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Nonlinear dynamic analysis of the perovskite solar cell under blast impacts based on the modified strain gradient theory

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Abstract

The perovskite solar cell (PSC) is one of the most burgeoning astronautic photovoltaic candidates with intrinsic microscales in thickness. One of the key concerns for the PSC within its operating status is nonlinear dynamic performance owing to ultra-thin structural attributes and dynamic impacts. This paper explores the size-dependent nonlinear dynamic behavior of the PSC under blast impacts. A multi-scale nonlinear dynamics framework is developed based on the modified strain gradient theory, extending the analytical nonlinear response analysis to microscale composites. Considering the von-Kármán geometric nonlinearity, the size-dependent motion equations are derived, and can be subsequently resolved by the fourth-order Runge–Kutta method to assess the transient response and blast impact resistance of the PSC. Diverse effects of the microplate theories, material length scale parameters, structural geometry, elastic foundations, damping, and blast impulses on the size-dependent nonlinear dynamic characteristics are systematically examined. Concluding remarks from the present study will be beneficial to the astronautic design and space deployment of the PSC energy harvesting devices with improved impact carrying capacity and safety.

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References

  1. NASA Artemis program n.d. https://www.nasa.gov/specials/artemis/. Accessed 6 Mar 2022

  2. Tiangong project n.d. http://en.cmse.gov.cn/missions/space_laboratory_missions/. Accessed 6 Mar 2022

  3. SpaceX Starlink n.d. https://www.starlink.com/premium. Accessed 6 Mar 2022

  4. BeiDou satellite system n.d. http://en.beidou.gov.cn/SYSTEMS/System/. Accessed 6 Mar 2022

  5. McLaughlin Green, C., Lomask, M.: Vanguard-a history, vol. 4202. NASA Special Publication (1970)

  6. Space qualified triple junction solar cell in Spectrolab n.d. http://www.spectrolab.com/photovoltaics/XTE-SF%20Data%20Sheet%20_12.23.19.pdf. Accessed 30 Jun 2021

  7. MicroLink Devices Achieves Certified 37.75% Solar Cell Power Conversion Efficiency n.d. http://mldevices.com/index.php/news/67-microlink-devices-achieves-certified-37-75-solar-cell-power-conversion-efficiency-microlink-devicesachieves-certified-37-75-solar-cell-power-conversion-efficiency. Accessed 11 Mar 2022

  8. Luque, A., Hegedus, S.: Handbook of Photovoltaic Science and Engineering. John Wiley & Sons, New York (2011)

    Google Scholar 

  9. Tu, Y., Wu, J., Xu, G., Yang, X., Cai, R., Gong, Q., Zhu, R., Huang, W.: Perovskite solar cells for space applications: progress and challenges. Adv. Mater. 33, 2006545 (2021)

    Article  Google Scholar 

  10. Green, M.A., Ho-Baillie, A., Snaith, H.J.: The emergence of perovskite solar cells. Nat. Photon. 8, 506 (2014)

    Article  Google Scholar 

  11. Cardinaletti, I., Vangerven, T., Nagels, S., Cornelissen, R., Schreurs, D., Hruby, J., Vodnik, J., Devisscher, D., Kesters, J., D’Haen, J.: Organic and perovskite solar cells for space applications. Sol. Energy Mater. Sol. Cells 182, 121–127 (2018)

    Article  Google Scholar 

  12. Best Research-Cell Efficiency Chart n.d. https://www.nrel.gov/pv/assets/pdfs/best-research-cell-efficiencies-rev220126.pdf. Accessed 11 Mar 2022

  13. Park, N.-G., Grätzel, M., Miyasaka, T., Zhu, K., Emery, K.: Towards stable and commercially available perovskite solar cells. Nat. Energy 1, 1–8 (2016)

    Article  Google Scholar 

  14. Kang, S., Jeong, J., Cho, S., Yoon, Y.J., Park, S., Lim, S., Kim, J.Y., Ko, H.: Ultrathin, lightweight and flexible perovskite solar cells with an excellent power-per-weight performance. J. Mater. Chem. A 7, 1107–1114 (2019)

    Article  Google Scholar 

  15. De Rossi, F., Taheri, B., Bonomo, M., Gupta, V., Renno, G., Nia, N.Y., Rech, P., Frost, C., Cazzaniga, C., Quagliotto, P.: Neutron irradiated perovskite films and solar cells on PET substrates. Nano Energy 93, 106879 (2022)

    Article  Google Scholar 

  16. Ho-Baillie, A.W., Sullivan, H.G., Bannerman, T.A., Talathi, H.P., Bing, J., Tang, S., Xu, A., Bhattacharyya, D., Cairns, I.H., McKenzie, D.R.: Deployment opportunities for space photovoltaics and the prospects for perovskite solar cells. Adv. Mater. Technol. 7, 2101059 (2022)

    Article  Google Scholar 

  17. Reb, L.K., Böhmer, M., Predeschly, B., Grott, S., Weindl, C.L., Ivandekic, G.I., Guo, R., Dreißigacker, C., Gernhäuser, R., Meyer, A.: Perovskite and organic solar cells on a rocket flight. Joule 4, 1880–1892 (2020)

    Article  Google Scholar 

  18. PSC in Satellite n.d. https://www.google.com/imgres?imgurl=https%3A%2F%2Fvcresearch.berkeley.edu%2Fsites%2Fdefault%2Ffiles%2Fnews_images%2Fsolar-satellite400.jpg&imgrefurl=https%3A%2F%2Fvcresearch.berkeley.edu%2Fnews%2Fresearch-brief-technology-could-bring-high-end-solar-masses&tbnid=9N5jCI7WyJPQkM&vet=12ahUKEwiA_Nid3cH2AhWbgGMGHUPyCaEQxiAoBXoECAAQJQ..i&docid=M2ay1ygwbIzEDM&w=400&h=259&itg=1&q=solar%20cell%20in%20satellite&ved=2ahUKEwiA_Nid3cH2AhWbgGMGHUPyCaEQxiAoBXoECAAQJQ. Accessed 1 Mar 2022

  19. PSC in Planetary space station n.d. https://www.google.com/imgres?imgurl=https%3A%2F%2Fs3.amazonaws.com%2Fsolarassets%2Fwp-content%2Fuploads%2F2019%2F06%2FISS20solar20panels.jpg&imgrefurl=https%3A%2F%2Fwww.solar.com%2Flearn%2Fhow-do-solar-panels-work%2F&tbnid=KGYRhxnmKCQJIM&vet=12ahUKEwjhlqKQ3cH2AhWBXWwGHRaqCbYQMygJegUIARC8AQ..i&docid=WTP8M_wBxa-drM&w=2000&h=1000&q=solar%20cell%20in%20satellite&ved=2ahUKEwjhlqKQ3cH2AhWBXWwGHRaqCbYQMygJegUIARC8AQ. Accessed 1 Mar 2022

  20. Ziegler, F., Fotiu, P., Irschik, H.: Structural dynamic plasticity effects due to impact or vibrational loadings. In: Structural Dynamics, pp. 3–10. Routledge (2022)

    Chapter  Google Scholar 

  21. Matveenko, V.P., Krommer, M., Belyaev, A.K., et al.: Dynamics and Control of Advanced Structures and Machines. Springer International Publishing (2019)

    Google Scholar 

  22. Bo, L., Gao, W., Yu, Y., Chen, X.: Geometrically nonlinear dynamic analysis of the stiffened perovskite solar cell subjected to biaxial velocity impacts. Nonlinear Dyn. 110, 281–311 (2022)

    Article  Google Scholar 

  23. Sun, G., Zhang, J., Li, S., Fang, J., Wang, E., Li, Q.: Dynamic response of sandwich panel with hierarchical honeycomb cores subject to blast loading. Thin-Walled Struct. 142, 499–515 (2019)

    Article  Google Scholar 

  24. Kazancı, Z.: A review on the response of blast loaded laminated composite plates. Prog. Aerosp. Sci. 81, 49–59 (2016)

    Article  Google Scholar 

  25. Bo, L., Li, Q., Chen, X., Gao, W.: Nonlinear dynamic instability of the perovskite solar cell under biaxial mechanical impacts. Eng. Fail. Anal. 139, 106444 (2022)

    Article  Google Scholar 

  26. Lyu, D., Ren, B., Li, S.: Failure modes and mechanisms for rechargeable Lithium-based batteries: a state-of-the-art review. Acta Mech. 230, 701–727 (2019)

    Article  Google Scholar 

  27. Fleck, N., Muller, G., Ashby, M.F., Hutchinson, J.W.: Strain gradient plasticity: theory and experiment. Acta Metall. Mater. 42, 475–487 (1994)

    Article  Google Scholar 

  28. Stölken, J.S., Evans, A.: A microbend test method for measuring the plasticity length scale. Acta Mater. 46, 5109–5115 (1998)

    Article  Google Scholar 

  29. Lam, D.C., Yang, F., Chong, A., Wang, J., Tong, P.: Experiments and theory in strain gradient elasticity. J. Mech. Phys. Solids 51, 1477–1508 (2003)

    Article  MATH  Google Scholar 

  30. Li, S.: On the micromechanics theory of Reissner-Mindlin plates. Acta Mech. 142, 47–99 (2000)

    Article  MATH  Google Scholar 

  31. Xi, S., Su, Y.: A phase field study of the grain-size effect on the thermomechanical behavior of polycrystalline NiTi thin films. Acta Mech. 232, 4545–4566 (2021)

    Article  MathSciNet  MATH  Google Scholar 

  32. Zhao, Z., Zhu, J., Chen, W.: Size-dependent vibrations and waves in piezoelectric nanostructures: a literature review. Int. J. Smart Nano Mater. 13, 391–431 (2022)

    Article  Google Scholar 

  33. Polyanskiy, A.M., Polyanskiy, V.A., Belyaev, A.K., Yakovlev, Y.A.: Relation of elastic properties, yield stress and ultimate strength of polycrystalline metals to their melting and evaporation parameters with account for nano and micro structure. Acta Mech. 229, 4863–4873 (2018)

    Article  MathSciNet  Google Scholar 

  34. Su, Y., Weng, G.J.: The frequency dependence of microstructure evolution in a ferroelectric nano-film during AC dynamic polarization switching. Acta Mech. 229, 795–805 (2018)

    Article  Google Scholar 

  35. Irschik, H., Heuer, R.: Analogies for simply supported nonlocal Kirchhoff plates of polygonal planform. Acta Mech. 229, 867–879 (2018)

    Article  MathSciNet  MATH  Google Scholar 

  36. Babaei, H., Eslami, M.R.: Thermally induced large deflection of FGM shallow micro-arches with integrated surface piezoelectric layers based on modified couple stress theory. Acta Mech. 230, 2363–2384 (2019)

    Article  MathSciNet  MATH  Google Scholar 

  37. Zhang, B., He, Y., Liu, D., Shen, L., Lei, J.: An efficient size-dependent plate theory for bending, buckling and free vibration analyses of functionally graded microplates resting on elastic foundation. Appl. Math. Model. 39, 3814–3845 (2015)

    Article  MathSciNet  MATH  Google Scholar 

  38. Fleck, N., Hutchinson, J.: A phenomenological theory for strain gradient effects in plasticity. J. Mech. Phys. Solids 41, 1825–1857 (1993)

    Article  MathSciNet  MATH  Google Scholar 

  39. Yang, F., Chong, A., Lam, D.C.C., Tong, P.: Couple stress based strain gradient theory for elasticity. Int. J. Solids Struct. 39, 2731–2743 (2002)

    Article  MATH  Google Scholar 

  40. Van Quyen, N., Duc, N.D.: Vibration and nonlinear dynamic response of nanocomposite multi-layer solar panel resting on elastic foundations. Thin-Walled Struct. 177, 109412 (2022)

    Article  Google Scholar 

  41. Dat, N.D., Quan, T.Q., Duc, N.D.: Vibration analysis of auxetic laminated plate with magneto-electro-elastic face sheets subjected to blast loading. Compos. Struct. 280, 114925 (2022)

    Article  Google Scholar 

  42. Quan, T.Q., Duc, N.D.: Analytical solutions for nonlinear vibration of porous functionally graded sandwich plate subjected to blast loading. Thin-Walled Struct. 170, 108606 (2022)

    Article  Google Scholar 

  43. Dat, N.D., Anh, V.M., Quan, T.Q., Duc, P.T., Duc, N.D.: Nonlinear stability and optimization of thin nanocomposite multilayer organic solar cell using Bees algorithm. Thin-Walled Struct. 149, 106520 (2020)

    Article  Google Scholar 

  44. Duc, N.D., Seung-Eock, K., Quan, T.Q., Long, D.D., Anh, V.M.: Nonlinear dynamic response and vibration of nanocomposite multilayer organic solar cell. Compos. Struct. 184, 1137–1144 (2018)

    Article  Google Scholar 

  45. Dinh Duc, N., Tuan, N.D., Tran, P., Quan, T.Q.: Nonlinear dynamic response and vibration of imperfect shear deformable functionally graded plates subjected to blast and thermal loads. Mech. Adv. Mater. Struct. 24, 318–329 (2017)

    Article  Google Scholar 

  46. Cong, P.H., Long, P.T., Van Nhat, N., Duc, N.D.: Geometrically nonlinear dynamic response of eccentrically stiffened circular cylindrical shells with negative poisson’s ratio in auxetic honeycombs core layer. Int. J. Mech. Sci. 152, 443–453 (2019)

    Article  Google Scholar 

  47. Nguyen, D.D., Tran, Q.Q., Nguyen, D.K.: New approach to investigate nonlinear dynamic response and vibration of imperfect functionally graded carbon nanotube reinforced composite double curved shallow shells subjected to blast load and temperature. Aerosp. Sci. Technol. 71, 360–372 (2017)

    Article  Google Scholar 

  48. Li, Q., Wu, D., Gao, W., Tin-Loi, F., Liu, Z., Cheng, J.: Static bending and free vibration of organic solar cell resting on Winkler-Pasternak elastic foundation through the modified strain gradient theory. Eur. J. Mech. -A/Solids 78, 103852 (2019)

    Article  MathSciNet  MATH  Google Scholar 

  49. Li, Q., Wu, D., Gao, W., Tin-Loi, F.: Size-dependent instability of organic solar cell resting on Winkler-Pasternak elastic foundation based on the modified strain gradient theory. Int. J. Mech. Sci. 177, 105306 (2020)

    Article  Google Scholar 

  50. Babaei, H., Kiani, Y., Eslami, M.R.: Vibrational behavior of thermally pre-/post-buckled FG-CNTRC beams on a nonlinear elastic foundation: a two-step perturbation technique. Acta Mech. 232, 3897–3915 (2021)

    Article  MathSciNet  MATH  Google Scholar 

  51. Babaei, H., Eslami, M.R.: Limit load analysis and imperfection sensitivity of porous FG micro-tubes surrounded by a nonlinear softening elastic medium. Acta Mech. 231, 4563–4583 (2020)

    Article  MathSciNet  MATH  Google Scholar 

  52. Gia Phi, B., Van Hieu, D., Sedighi, H.M., Sofiyev, A.H.: Size-dependent nonlinear vibration of functionally graded composite micro-beams reinforced by carbon nanotubes with piezoelectric layers in thermal environments. Acta Mech. (2022). https://doi.org/10.1007/s00707-022-03224-4

    Article  MathSciNet  MATH  Google Scholar 

  53. Karamanli, A.: Size-dependent behaviors of three directional functionally graded shear and normal deformable imperfect microplates. Compos. Struct. 257, 113076 (2021)

    Article  Google Scholar 

  54. Karamanli, A.: Structural behaviours of zigzag and armchair nanobeams using finite element doublet mechanics. Eur. J. Mech. A/Solids 89, 104287 (2021)

    Article  MathSciNet  MATH  Google Scholar 

  55. Radwan, A.F., Sobhy, M.: Transient instability analysis of viscoelastic sandwich CNTs-reinforced microplates exposed to 2D magnetic field and hygrothermal conditions. Compos. Struct. 245, 112349 (2020)

    Article  Google Scholar 

  56. Cuong-Le, T., Hoang-Le, M., Ferreira, A., Wahab, M.A.: Small size-effect isogeometric analysis for linear and nonlinear responses of porous metal foam microplate. Compos. Struct. 285, 115189 (2022)

    Article  Google Scholar 

  57. Li, F.-L., Fan, S.-J., Yuan, W.-H., Yang, L.: Size effects on the vibro-acoustic characteristics of different types of functionally graded sandwich microplates. Mech. Adv. Mater. Struct. (2022). https://doi.org/10.1080/15376494.2022.2060393

    Article  Google Scholar 

  58. Nguyen, N.V., Lee, J.: On the static and dynamic responses of smart piezoelectric functionally graded graphene platelet-reinforced microplates. Int. J. Mech. Sci. 197, 106310 (2021)

    Article  Google Scholar 

  59. Hung, P., Phung-Van, P., Thai, C.H.: A refined isogeometric plate analysis of porous metal foam microplates using modified strain gradient theory. Compos. Struct. 289, 115467 (2022)

    Article  Google Scholar 

  60. Phung-Van, P., Ferreira, A., Nguyen-Xuan, H., Thai, C.H.: A nonlocal strain gradient isogeometric nonlinear analysis of nanoporous metal foam plates. Eng. Anal. Bound. Elem. 130, 58–68 (2021)

    Article  MathSciNet  MATH  Google Scholar 

  61. Phung-Van, P., Ferreira, A., Nguyen-Xuan, H., Thai, C.H.: Scale-dependent nonlocal strain gradient isogeometric analysis of metal foam nanoscale plates with various porosity distributions. Compos. Struct. 268, 113949 (2021)

    Article  Google Scholar 

  62. Chen, X., Shen, H.-S., Huang, X.-H.: Thermo-mechanical postbuckling analysis of sandwich plates with functionally graded auxetic GRMMC core on elastic foundations. Compos. Struct. 279, 114796 (2022)

    Article  Google Scholar 

  63. Chen, X., Shen, H.-S., Xiang, Y.: Thermo-mechanical postbuckling analysis of sandwich cylindrical shells with functionally graded auxetic GRMMC core surrounded by an elastic medium. Thin-Walled Struct. 171, 108755 (2022)

    Article  Google Scholar 

  64. Ke, L.-L., Yang, J., Kitipornchai, S., Wang, Y.-S.: Axisymmetric postbuckling analysis of size-dependent functionally graded annular microplates using the physical neutral plane. Int. J. Eng. Sci. 81, 66–81 (2014)

    Article  MathSciNet  MATH  Google Scholar 

  65. Ke, L.-L., Wang, Y.-S., Yang, J., Kitipornchai, S.: The size-dependent vibration of embedded magneto-electro-elastic cylindrical nanoshells. Smart Mater. Struct. 23, 125036 (2014)

    Article  Google Scholar 

  66. Zhang, G., Gao, X.-L., Littlefield, A.: A non-classical model for circular cylindrical thin shells incorporating microstructure and surface energy effects. Acta Mech. 232, 2225–2248 (2021)

    Article  MathSciNet  MATH  Google Scholar 

  67. Chan, D.Q., Quan, T.Q., Phi, B.G., Van Hieu, D., Duc, N.D.: Buckling analysis and dynamic response of FGM sandwich cylindrical panels in thermal environments using nonlocal strain gradient theory. Acta Mech. (2022). https://doi.org/10.1007/s00707-022-03212-8

    Article  MathSciNet  MATH  Google Scholar 

  68. Reddy, J.N.: Mechanics of Laminated Composite Plates and Shells: Theory and Analysis. CRC Press, Boca Raton (2003)

    Book  Google Scholar 

  69. Xue, H., Fu, K., Wong, L.H., Birgersson, E., Stangl, R.: Modelling and loss analysis of meso-structured perovskite solar cells. J. Appl. Phys. 122, 083105 (2017)

    Article  Google Scholar 

  70. Jeon, N.J., Na, H., Jung, E.H., Yang, T.-Y., Lee, Y.G., Kim, G., Shin, H.-W., Seok, S.I., Lee, J., Seo, J.: A fluorene-terminated hole-transporting material for highly efficient and stable perovskite solar cells. Nat. Energy 3, 682–689 (2018)

    Article  Google Scholar 

  71. Jones R.M.: Mechanics of Composite Materials, pp. 164–165. (1998)

  72. Piggott, M.: Load Bearing Fibre Composites. Springer Science & Business Media, Berlin (2002)

    MATH  Google Scholar 

  73. Thai, H.-T., Choi, D.-H.: A refined plate theory for functionally graded plates resting on elastic foundation. Compos. Sci. Technol. 71, 1850–1858 (2011)

    Article  Google Scholar 

  74. Ekstrom, R.: Dynamic buckling of a rectangular orthotropic plate. AIAA J. 11, 1655–1659 (1973)

    Article  MATH  Google Scholar 

  75. Lam, N., Mendis, P., Ngo, T.: Response spectrum solutions for blast loading. Electron. J. Struct. Eng. 4, 28–44 (2004)

    Article  Google Scholar 

  76. Bulson, P.S.: Explosive Loading of Engineering Structures. CRC Press, Boca Raton (1997)

    Book  Google Scholar 

  77. Gupta, A.D., Gregory, F.H., Bitting, R.L., Bhattacharya, S.: Dynamic analysis of an explosively loaded hinged rectangular plate. Comput. Struct. 26, 339–344 (1987)

    Article  Google Scholar 

  78. Ramirez, C., Yadavalli, S.K., Garces, H.F., Zhou, Y., Padture, N.P.: Thermo-mechanical behavior of organic-inorganic halide perovskites for solar cells. Scripta Mater. 150, 36–41 (2018)

    Article  Google Scholar 

  79. Cardarelli, F.: Materials handbook. Springer (2000)

    Book  Google Scholar 

  80. Rakstys, K., Paek, S., Sohail, M., Gao, P., Cho, K.T., Gratia, P., Lee, Y., Dahmen, K.H., Nazeeruddin, M.K.: A highly hindered bithiophene-functionalized dispiro-oxepine derivative as an efficient hole transporting material for perovskite solar cells. J. Mater. Chem. A 4, 18259–18264 (2016)

    Article  Google Scholar 

  81. Tuyen, L.T.C., Jian, S.-R., Tien, N.T., Le, P.H.: Nanomechanical and material properties of fluorine-doped tin oxide thin films prepared by ultrasonic spray pyrolysis: effects of F-doping. Materials 12, 1665 (2019)

    Article  Google Scholar 

  82. Hosseini-Hashemi, S., Fadaee, M., Atashipour, S.R.: A new exact analytical approach for free vibration of Reissner-Mindlin functionally graded rectangular plates. Int. J. Mech. Sci. 53, 11–22 (2011)

    Article  Google Scholar 

  83. Matsunaga, H.: Free vibration and stability of functionally graded plates according to a 2-D higher-order deformation theory. Compos. Struct. 82, 499–512 (2008)

    Article  Google Scholar 

  84. Zhao, X., Lee, Y., Liew, K.M.: Free vibration analysis of functionally graded plates using the element-free kp-Ritz method. J. Sound Vib. 319, 918–939 (2009)

    Article  Google Scholar 

  85. Sobhy, M.: Buckling and free vibration of exponentially graded sandwich plates resting on elastic foundations under various boundary conditions. Compos. Struct. 99, 76–87 (2013)

    Article  Google Scholar 

  86. Xiang, Y., Wang, C., Kitipornchai, S.: Exact vibration solution for initially stressed Mindlin plates on Pasternak foundations. Int. J. Mech. Sci. 36, 311–316 (1994)

    Article  MATH  Google Scholar 

  87. Bo, L., Li, Q., Tian, Y., Wu, D., Yu, Y., Chen, X., Gao, W.: Nonlinear dynamic investigation of the perovskite solar cell with GPLR-FGP stiffeners under blast impact. Int. J. Mech. Sci. 213, 106866 (2022)

    Article  Google Scholar 

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Appendices

Appendix A

$$\begin{aligned} (\sigma_{xx} )_{l} & = (\lambda_{l} + 2\mu_{l} )\left[ {\frac{\partial u}{{\partial x}} + \frac{1}{2}\left( {\frac{{\partial w_{b} }}{\partial x} + \frac{{\partial w_{s} }}{\partial x}} \right)^{2} + \frac{1}{4}z\frac{{\partial^{2} w_{s} }}{{\partial x^{2} }} - z\frac{{\partial^{2} w_{b} }}{{\partial x^{2} }} - \frac{{5z^{3} }}{{3h^{2} }}\frac{{\partial^{2} w_{s} }}{{\partial x^{2} }}} \right] \\ & \quad + \lambda_{l} \left[ {\frac{\partial v}{{\partial y}} + \frac{1}{2}\left( {\frac{{\partial w_{b} }}{\partial y} + \frac{{\partial w_{s} }}{\partial y}} \right)^{2} + \frac{1}{4}z\frac{{\partial^{2} w_{s} }}{{\partial y^{2} }} - z\frac{{\partial^{2} w_{b} }}{{\partial y^{2} }} - \frac{{5z^{3} }}{{3h^{2} }}\frac{{\partial^{2} w_{s} }}{{\partial y^{2} }}} \right], \\ \end{aligned}$$
(A.1)
$$\begin{aligned} (\sigma_{yy} )_{l} & = (\lambda_{l} + 2\mu_{l} )\left[ {\frac{\partial v}{{\partial y}} + \frac{1}{2}\left( {\frac{{\partial w_{b} }}{\partial y} + \frac{{\partial w_{s} }}{\partial y}} \right)^{2} + \frac{1}{4}z\frac{{\partial^{2} w_{s} }}{{\partial y^{2} }} - z\frac{{\partial^{2} w_{b} }}{{\partial y^{2} }} - \frac{{5z^{3} }}{{3h^{2} }}\frac{{\partial^{2} w_{s} }}{{\partial y^{2} }}} \right] \\ & \quad + \lambda_{l} \left[ {\frac{\partial u}{{\partial x}} + \frac{1}{2}\left( {\frac{{\partial w_{b} }}{\partial x} + \frac{{\partial w_{s} }}{\partial x}} \right)^{2} + \frac{1}{4}z\frac{{\partial^{2} w_{s} }}{{\partial x^{2} }} - z\frac{{\partial^{2} w_{b} }}{{\partial x^{2} }} - \frac{{5z^{3} }}{{3h^{2} }}\frac{{\partial^{2} w_{s} }}{{\partial x^{2} }}} \right], \\ \end{aligned}$$
(A.2)
$$\begin{aligned} (\sigma_{zz} )_{l} & = \lambda_{l} \left[ {\frac{\partial u}{{\partial x}} + \frac{1}{2}\left( {\frac{{\partial w_{b} }}{\partial x} + \frac{{\partial w_{s} }}{\partial x}} \right)^{2} + \frac{1}{4}z\frac{{\partial^{2} w_{s} }}{{\partial x^{2} }} - z\frac{{\partial^{2} w_{b} }}{{\partial x^{2} }} - \frac{{5z^{3} }}{{3h^{2} }}\frac{{\partial^{2} w_{s} }}{{\partial x^{2} }}} \right] \\ & \quad + \lambda_{l} \left[ {\frac{\partial v}{{\partial y}} + \frac{1}{2}\left( {\frac{{\partial w_{b} }}{\partial y} + \frac{{\partial w_{s} }}{\partial y}} \right)^{2} + \frac{1}{4}z\frac{{\partial^{2} w_{s} }}{{\partial y^{2} }} - z\frac{{\partial^{2} w_{b} }}{{\partial y^{2} }} - \frac{{5z^{3} }}{{3h^{2} }}\frac{{\partial^{2} w_{s} }}{{\partial y^{2} }}} \right], \\ \end{aligned}$$
(A.3)
$$\begin{aligned} (\sigma_{xy} )_{l} & = 2\mu_{l} \left[ {\frac{1}{2}\left( {\frac{\partial u}{{\partial y}} + \frac{\partial v}{{\partial x}} + \frac{{\partial w_{b} }}{\partial y}\frac{{\partial w_{b} }}{\partial x} + \frac{{\partial w_{s} }}{\partial y}\frac{{\partial w_{b} }}{\partial x} + \frac{{\partial w_{b} }}{\partial y}\frac{{\partial w_{s} }}{\partial x} + \frac{{\partial w_{s} }}{\partial y}\frac{{\partial w_{s} }}{\partial x}} \right)} \right. \\ & \left. {\quad + \frac{1}{4}z\frac{{\partial^{2} w_{s} }}{\partial x\partial y} - z\frac{{\partial^{2} w_{b} }}{\partial x\partial y} - \frac{{5z^{3} }}{{3h^{2} }}\frac{{\partial^{2} w_{s} }}{\partial x\partial y}} \right], \\ \end{aligned}$$
(A.4)
$$(\sigma_{xz} )_{l} = \frac{5}{4}\mu_{l} \left( {1 - \frac{{4z^{2} }}{{h^{2} }}} \right)\frac{{\partial w_{s} }}{\partial x},$$
(A.5)
$$(\sigma_{yz} )_{l} = \frac{5}{4}\mu_{l} \left( {1 - \frac{{4z^{2} }}{{h^{2} }}} \right)\frac{{\partial w_{s} }}{\partial y},$$
(A.6)
$$\begin{aligned} (p_{x} )_{l} \; & = 2\mu _{l} l_{0}^{2} \left[ {\frac{{\partial ^{2} u}}{{\partial x^{2} }} + \frac{{\partial ^{2} v}}{{\partial x\partial y}} + \left( {\frac{{\partial w_{b} }}{{\partial y}} + \frac{{\partial w_{s} }}{{\partial y}}} \right)\left( {\frac{{\partial ^{2} w_{b} }}{{\partial x\partial y}} + \frac{{\partial ^{2} w_{s} }}{{\partial x\partial y}}} \right) + \left( {\frac{{\partial w_{b} }}{{\partial x}} + \frac{{\partial w_{s} }}{{\partial x}}} \right)\left( {\frac{{\partial ^{2} w_{b} }}{{\partial x^{2} }} + \frac{{\partial ^{2} w_{s} }}{{\partial x^{2} }}} \right)} \right. \\ & \quad \left. { + \frac{z}{4}\left( {\frac{{\partial ^{3} w_{s} }}{{\partial x\partial y^{2} }} + \frac{{\partial ^{3} w_{s} }}{{\partial x^{3} }}} \right) - z\left( {\frac{{\partial ^{3} w_{b} }}{{\partial x\partial y^{2} }} + \frac{{\partial ^{3} w_{b} }}{{\partial x^{3} }}} \right) - \frac{{5z^{3} }}{{3h^{2} }}\left( {\frac{{\partial ^{3} w_{s} }}{{\partial x^{3} }} + \frac{{\partial ^{3} w_{s} }}{{\partial x\partial y^{2} }}} \right)} \right], \\ \end{aligned}$$
(A.7)
$$\begin{aligned} (p_{y} )_{l} & = 2\mu_{l} l_{0}^{2} \left[ {\frac{{\partial^{2} u}}{\partial x\partial y} + \frac{{\partial^{2} v}}{{\partial y^{2} }} + \left( {\frac{{\partial w_{b} }}{\partial y} + \frac{{\partial w_{s} }}{\partial y}} \right)\left( {\frac{{\partial^{2} w_{b} }}{{\partial y^{2} }} + \frac{{\partial^{2} w_{s} }}{{\partial y^{2} }}} \right) + \left( {\frac{{\partial w_{b} }}{\partial x} + \frac{{\partial w_{s} }}{\partial x}} \right)\left( {\frac{{\partial^{2} w_{b} }}{\partial x\partial y} + \frac{{\partial^{2} w_{s} }}{\partial x\partial y}} \right)} \right. \\ & \left. {\quad + \frac{1}{4}z\left( {\frac{{\partial^{3} w_{s} }}{{\partial x^{2} \partial y}} + \frac{{\partial^{3} w_{s} }}{{\partial y^{3} }}} \right) - z\left( {\frac{{\partial^{3} w_{b} }}{{\partial x^{2} \partial y}} + \frac{{\partial^{3} w_{b} }}{{\partial y^{3} }}} \right) - \frac{5}{{3h^{2} }}z^{3} \left( {\frac{{\partial^{3} w_{s} }}{{\partial y^{3} }} + \frac{{\partial^{3} w_{s} }}{{\partial x^{2} \partial y}}} \right)} \right], \\ \end{aligned}$$
(A.8)
$$(p_{z} )_{l} = 2\mu_{l} l_{0}^{2} \left[ { - \left( {\frac{{\partial^{2} w_{b} }}{{\partial y^{2} }} + \frac{{\partial^{2} w_{b} }}{{\partial x^{2} }}} \right) + \left( {\frac{1}{4} - \frac{{5z^{2} }}{{h^{2} }}} \right)\left( {\frac{{\partial^{2} w_{s} }}{{\partial y^{2} }} + \frac{{\partial^{2} w_{s} }}{{\partial x^{2} }}} \right)} \right],$$
(A.9)
$$\begin{aligned} (\tau_{xxx}^{1} )_{l} & = 2\mu_{l} l_{1}^{2} \left[ {\frac{1}{5}\left( {2\frac{{\partial^{2} u}}{{\partial x^{2} }} - \frac{{\partial^{2} u}}{{\partial y^{2} }} - 2\frac{{\partial^{2} v}}{\partial x\partial y}} \right) - \frac{1}{5}\frac{{\partial^{2} w_{b} }}{{\partial y^{2} }}\frac{{\partial w_{b} }}{\partial x} - \frac{1}{5}\frac{{\partial^{2} w_{s} }}{{\partial y^{2} }}\frac{{\partial w_{b} }}{\partial x} - \frac{1}{5}\frac{{\partial^{2} w_{b} }}{{\partial y^{2} }}\frac{{\partial w_{s} }}{\partial x}} \right. \\ & \quad - \frac{1}{5}\frac{{\partial^{2} w_{s} }}{{\partial y^{2} }}\frac{{\partial w_{s} }}{\partial x} - \frac{2}{5}\frac{{\partial w_{b} }}{\partial y}\frac{{\partial^{2} w_{b} }}{\partial x\partial y} - \frac{2}{5}\frac{{\partial w_{s} }}{\partial y}\frac{{\partial^{2} w_{b} }}{\partial x\partial y} - \frac{2}{5}\frac{{\partial w_{b} }}{\partial y}\frac{{\partial^{2} w_{s} }}{\partial x\partial y} - \frac{2}{5}\frac{{\partial w_{s} }}{\partial y}\frac{{\partial^{2} w_{s} }}{\partial x\partial y} \\ & \quad + \frac{2}{5}\frac{{\partial w_{b} }}{\partial x}\frac{{\partial^{2} w_{b} }}{{\partial x^{2} }} + \frac{2}{5}\frac{{\partial w_{s} }}{\partial x}\frac{{\partial^{2} w_{b} }}{{\partial x^{2} }} + \frac{2}{5}\frac{{\partial w_{b} }}{\partial x}\frac{{\partial^{2} w_{s} }}{{\partial x^{2} }} + \frac{2}{5}\frac{{\partial w_{s} }}{\partial x}\frac{{\partial^{2} w_{s} }}{{\partial x^{2} }} \\ & \quad \left. { + z\left( {\frac{1}{10}\frac{{\partial^{3} w_{s} }}{{\partial x^{3} }} - \frac{3}{20}\frac{{\partial^{3} w_{s} }}{{\partial x\partial y^{2} }} + \frac{2}{{h^{2} }}\frac{{\partial w_{s} }}{\partial x}} \right) - \frac{1}{5}z\left( {2\frac{{\partial^{3} w_{b} }}{{\partial x^{3} }} - 3\frac{{\partial^{3} w_{b} }}{{\partial x\partial y^{2} }}} \right) - \frac{{z^{3} }}{{h^{2} }}\left( {\frac{2}{3}\frac{{\partial^{3} w_{s} }}{{\partial x^{3} }} - \frac{{\partial^{3} w_{s} }}{{\partial x\partial y^{2} }}} \right)} \right], \\ \end{aligned}$$
(A.10)
$$\begin{aligned} (\tau_{yyy}^{1} )_{l} & = 2\mu_{l} l_{1}^{2} \left[ {\frac{1}{5}\left( {2\frac{{\partial^{2} v}}{{\partial y^{2} }} - \frac{{\partial^{2} v}}{{\partial x^{2} }} - 2\frac{{\partial^{2} u}}{\partial x\partial y}} \right) + \frac{2}{5}\frac{{\partial w_{b} }}{\partial y}\frac{{\partial^{2} w_{b} }}{{\partial y^{2} }} + \frac{2}{5}\frac{{\partial w_{s} }}{\partial y}\frac{{\partial^{2} w_{b} }}{{\partial y^{2} }} + \frac{2}{5}\frac{{\partial^{2} w_{s} }}{{\partial y^{2} }}\frac{{\partial w_{b} }}{\partial y}} \right. \\ & \quad + \frac{2}{5}\frac{{\partial^{2} w_{s} }}{{\partial y^{2} }}\frac{{\partial w_{s} }}{\partial y} - \frac{2}{5}\frac{{\partial w_{b} }}{\partial x}\frac{{\partial^{2} w_{b} }}{\partial x\partial y} - \frac{2}{5}\frac{{\partial w_{s} }}{\partial x}\frac{{\partial^{2} w_{b} }}{\partial x\partial y} - \frac{2}{5}\frac{{\partial w_{b} }}{\partial x}\frac{{\partial^{2} w_{s} }}{\partial x\partial y} - \frac{2}{5}\frac{{\partial w_{s} }}{\partial x}\frac{{\partial^{2} w_{s} }}{\partial x\partial y} \\ & \quad - \frac{1}{5}\frac{{\partial w_{b} }}{\partial y}\frac{{\partial^{2} w_{b} }}{{\partial x^{2} }} - \frac{1}{5}\frac{{\partial w_{s} }}{\partial y}\frac{{\partial^{2} w_{b} }}{{\partial x^{2} }} - \frac{1}{5}\frac{{\partial w_{b} }}{\partial y}\frac{{\partial^{2} w_{s} }}{{\partial x^{2} }} - \frac{1}{5}\frac{{\partial w_{s} }}{\partial y}\frac{{\partial^{2} w_{s} }}{{\partial x^{2} }} \\ & \left. {\quad + z\left( {\frac{1}{10}\frac{{\partial^{3} w_{s} }}{{\partial y^{3} }} - \frac{3}{20}\frac{{\partial^{3} w_{s} }}{{\partial x^{2} \partial y}} + \frac{2}{{h^{2} }}\frac{{\partial w_{s} }}{\partial y}} \right) - \frac{1}{5}z\left( {2\frac{{\partial^{3} w_{b} }}{{\partial y^{3} }} - 3\frac{{\partial^{3} w_{b} }}{{\partial x^{2} \partial y}}} \right) - \frac{{z^{3} }}{{h^{2} }}\left( {\frac{2}{3}\frac{{\partial^{3} w_{s} }}{{\partial y^{3} }} - \frac{{\partial^{3} w_{s} }}{{\partial x^{2} \partial y}}} \right)} \right], \\ \end{aligned}$$
(A.11)
$$(\tau_{zzz}^{1} )_{l} = 2\mu_{l} l_{1}^{2} \left[ {\frac{1}{5}\left( {\frac{{\partial^{2} w_{b} }}{{\partial y^{2} }} + \frac{{\partial^{2} w_{b} }}{{\partial x^{2} }}} \right) - \left( {\frac{3}{10} - \frac{{2z^{2} }}{{h^{2} }}} \right)\left( {\frac{{\partial^{2} w_{s} }}{{\partial y^{2} }} + \frac{{\partial^{2} w_{s} }}{{\partial x^{2} }}} \right)} \right],$$
(A.12)
$$\begin{aligned} (\tau_{xxy}^{1} )_{l} & = (\tau_{xyx}^{1} )_{l} = (\tau_{yxx}^{1} )_{l} = 2\mu_{l} l_{1}^{2} \left[ {\frac{1}{15}\left( {8\frac{{\partial^{2} u}}{\partial x\partial y} + 4\frac{{\partial^{2} v}}{{\partial x^{2} }} - 3\frac{{\partial^{2} v}}{{\partial y^{2} }}} \right) - \frac{1}{5}\frac{{\partial w_{b} }}{\partial y}\frac{{\partial^{2} w_{b} }}{{\partial y^{2} }} - \frac{1}{5}\frac{{\partial w_{s} }}{\partial y}\frac{{\partial^{2} w_{b} }}{{\partial y^{2} }}} \right. \\ & \quad - \frac{1}{5}\frac{{\partial^{2} w_{s} }}{{\partial y^{2} }}\frac{{\partial w_{b} }}{\partial y} - \frac{1}{5}\frac{{\partial^{2} w_{s} }}{{\partial y^{2} }}\frac{{\partial w_{s} }}{\partial y} + \frac{8}{15}\frac{{\partial w_{b} }}{\partial x}\frac{{\partial^{2} w_{b} }}{\partial x\partial y} + \frac{8}{15}\frac{{\partial w_{s} }}{\partial x}\frac{{\partial^{2} w_{b} }}{\partial x\partial y} + \frac{8}{15}\frac{{\partial w_{b} }}{\partial x}\frac{{\partial^{2} w_{s} }}{\partial x\partial y} + \frac{8}{15}\frac{{\partial w_{s} }}{\partial x}\frac{{\partial^{2} w_{s} }}{\partial x\partial y} \\ & \quad + \frac{4}{15}\frac{{\partial w_{b} }}{\partial y}\frac{{\partial^{2} w_{b} }}{{\partial x^{2} }} + \frac{4}{15}\frac{{\partial w_{s} }}{\partial y}\frac{{\partial^{2} w_{b} }}{{\partial x^{2} }} + \frac{4}{15}\frac{{\partial w_{b} }}{\partial y}\frac{{\partial^{2} w_{s} }}{{\partial x^{2} }} + \frac{4}{15}\frac{{\partial w_{s} }}{\partial y}\frac{{\partial^{2} w_{s} }}{{\partial x^{2} }} \\ & \quad \left. {+ z\left( {\frac{1}{5}\frac{{\partial^{3} w_{s} }}{{\partial x^{2} \partial y}} - \frac{1}{20}\frac{{\partial^{3} w_{s} }}{{\partial y^{3} }} + \frac{2}{{3h^{2} }}\frac{{\partial w_{s} }}{\partial y}} \right) - \frac{1}{5}z\left( {4\frac{{\partial^{3} w_{b} }}{{\partial x^{2} \partial y}} - \frac{{\partial^{3} w_{b} }}{{\partial y^{3} }}} \right) - \frac{{z^{3} }}{{3h^{2} }}\left( {4\frac{{\partial^{3} w_{s} }}{{\partial x^{2} \partial y}} - \frac{{\partial^{3} w_{s} }}{{\partial y^{3} }}} \right)} \right], \\ \end{aligned}$$
(A.13)
$$(\tau_{xxz}^{1} )_{l} = (\tau_{xzx}^{1} )_{l} = (\tau_{zxx}^{1} )_{l} = 2\mu_{l} l_{1}^{2} \left[ { - \frac{1}{15}\left( {4\frac{{\partial^{2} w_{b} }}{{\partial x^{2} }} - \frac{{\partial^{2} w_{b} }}{{\partial y^{2} }}} \right) + \left( {\frac{1}{10} - \frac{{2z^{2} }}{{3h^{2} }}} \right)\left( {4\frac{{\partial^{2} w_{s} }}{{\partial x^{2} }} - \frac{{\partial^{2} w_{s} }}{{\partial y^{2} }}} \right)} \right],$$
(A.14)
$$\begin{aligned}& (\tau_{xyy}^{1} )_{l} = (\tau_{yxy}^{1} )_{l} = (\tau_{yyx}^{1} )_{l}\\ &\quad = 2\mu_{l} l_{1}^{2} \left[ { - \frac{1}{15}\left( {3\frac{{\partial^{2} u}}{{\partial x^{2} }} - 4\frac{{\partial^{2} u}}{{\partial y^{2} }} - 8\frac{{\partial^{2} v}}{\partial x\partial y}} \right) + \frac{4}{15}\frac{{\partial w_{b} }}{\partial x}\frac{{\partial^{2} w_{b} }}{{\partial y^{2} }} + \frac{4}{15}\frac{{\partial w_{b} }}{\partial x}\frac{{\partial^{2} w_{s} }}{{\partial y^{2} }}} \right. \\ & \qquad + \frac{4}{15}\frac{{\partial^{2} w_{b} }}{{\partial y^{2} }}\frac{{\partial w_{s} }}{\partial x} + \frac{4}{15}\frac{{\partial^{2} w_{s} }}{{\partial y^{2} }}\frac{{\partial w_{s} }}{\partial x} + \frac{8}{15}\frac{{\partial w_{b} }}{\partial y}\frac{{\partial^{2} w_{b} }}{\partial x\partial y} + \frac{8}{15}\frac{{\partial w_{s} }}{\partial y}\frac{{\partial^{2} w_{b} }}{\partial x\partial y} + \frac{8}{15}\frac{{\partial w_{b} }}{\partial y}\frac{{\partial^{2} w_{s} }}{\partial x\partial y} + \frac{8}{15}\frac{{\partial w_{s} }}{\partial y}\frac{{\partial^{2} w_{s} }}{\partial x\partial y} \\ & \qquad - \frac{1}{5}\frac{{\partial w_{b} }}{\partial x}\frac{{\partial^{2} w_{b} }}{{\partial x^{2} }} - \frac{1}{5}\frac{{\partial w_{s} }}{\partial x}\frac{{\partial^{2} w_{b} }}{{\partial x^{2} }} - \frac{1}{5}\frac{{\partial w_{b} }}{\partial x}\frac{{\partial^{2} w_{s} }}{{\partial x^{2} }} - \frac{1}{5}\frac{{\partial w_{s} }}{\partial x}\frac{{\partial^{2} w_{s} }}{{\partial x^{2} }} \\ & \left. {\qquad + z\left( { - \frac{1}{20}\frac{{\partial^{3} w_{s} }}{{\partial x^{3} }} + \frac{1}{5}\frac{{\partial^{3} w_{s} }}{{\partial x\partial y^{2} }} + \frac{2}{{3h^{2} }}\frac{{\partial w_{s} }}{\partial x}} \right) - \frac{1}{5}z\left( {4\frac{{\partial^{3} w_{b} }}{{\partial x\partial y^{2} }} - \frac{{\partial^{3} w_{b} }}{{\partial x^{3} }}} \right) - \frac{{z^{3} }}{{3h^{2} }}\left( {4\frac{{\partial^{3} w_{s} }}{{\partial x\partial y^{2} }} - \frac{{\partial^{3} w_{s} }}{{\partial x^{3} }}} \right)} \right], \\ \end{aligned}$$
(A.15)
$$(\tau_{xyz}^{1} )_{l} = (\tau_{yzx}^{1} )_{l} = (\tau_{yxz}^{1} )_{l} = (\tau_{xzy}^{1} )_{l} = (\tau_{zxy}^{1} )_{l} = (\tau_{zyx}^{1} )_{l} = 2\mu_{l} l_{1}^{2} \left[ { - \left( {\frac{1}{3}\frac{{\partial^{2} w_{b} }}{\partial x\partial y} - \frac{1}{2}\frac{{\partial^{2} w_{s} }}{\partial x\partial y}} \right) - \frac{{10z^{2} }}{{3h^{2} }}\frac{{\partial^{2} w_{s} }}{\partial x\partial y}} \right],$$
(A.16)
$$\begin{aligned} &(\tau_{xzz}^{1} )_{l} = (\tau_{zxz}^{1} )_{l} = (\tau_{zzx}^{1} )_{l} \\ &\quad = 2\mu_{l} l_{1}^{2} \left[ { - \frac{1}{15}\left( {3\frac{{\partial^{2} u}}{{\partial x^{2} }} + \frac{{\partial^{2} u}}{{\partial y^{2} }} + 2\frac{{\partial^{2} v}}{\partial x\partial y}} \right) - \frac{1}{15}\frac{{\partial w_{b} }}{\partial x}\frac{{\partial^{2} w_{b} }}{{\partial y^{2} }} - \frac{1}{15}\frac{{\partial w_{b} }}{\partial x}\frac{{\partial^{2} w_{s} }}{{\partial y^{2} }}} \right. \\ & \qquad - \frac{1}{15}\frac{{\partial^{2} w_{b} }}{{\partial y^{2} }}\frac{{\partial w_{s} }}{\partial x} - \frac{1}{15}\frac{{\partial^{2} w_{s} }}{{\partial y^{2} }}\frac{{\partial w_{s} }}{\partial x} - \frac{2}{15}\frac{{\partial w_{b} }}{\partial y}\frac{{\partial^{2} w_{b} }}{\partial x\partial y} - \frac{2}{15}\frac{{\partial w_{s} }}{\partial y}\frac{{\partial^{2} w_{b} }}{\partial x\partial y} - \frac{2}{15}\frac{{\partial w_{b} }}{\partial y}\frac{{\partial^{2} w_{s} }}{\partial x\partial y} - \frac{2}{15}\frac{{\partial w_{s} }}{\partial y}\frac{{\partial^{2} w_{s} }}{\partial x\partial y} \\ & \qquad - \frac{1}{5}\frac{{\partial w_{b} }}{\partial x}\frac{{\partial^{2} w_{b} }}{{\partial x^{2} }} - \frac{1}{5}\frac{{\partial w_{s} }}{\partial x}\frac{{\partial^{2} w_{b} }}{{\partial x^{2} }} - \frac{1}{5}\frac{{\partial w_{b} }}{\partial x}\frac{{\partial^{2} w_{s} }}{{\partial x^{2} }} - \frac{1}{5}\frac{{\partial w_{s} }}{\partial x}\frac{{\partial^{2} w_{s} }}{{\partial x^{2} }} \\ & \qquad - \left. { z\left( {\frac{1}{20}\frac{{\partial^{3} w_{s} }}{{\partial x^{3} }} + \frac{1}{20}\frac{{\partial^{3} w_{s} }}{{\partial x\partial y^{2} }} + \frac{8}{{3h^{2} }}\frac{{\partial w_{s} }}{\partial x}} \right) + \frac{1}{5}z\left( {\frac{{\partial^{3} w_{b} }}{{\partial x^{3} }} + \frac{{\partial^{3} w_{b} }}{{\partial x\partial y^{2} }}} \right) + \frac{{z^{3} }}{{3h^{2} }}\left( {\frac{{\partial^{3} w_{s} }}{{\partial x^{3} }} + \frac{{\partial^{3} w_{s} }}{{\partial x\partial y^{2} }}} \right)} \right], \\ \end{aligned}$$
(A.17)
$$(\tau_{yyz}^{1} )_{l} = (\tau_{yzy}^{1} )_{l} = (\tau_{zyy}^{1} )_{l} = 2\mu_{l} l_{1}^{2} \left[ { - \frac{1}{15}\left( {4\frac{{\partial^{2} w_{b} }}{{\partial y^{2} }} - \frac{{\partial^{2} w_{b} }}{{\partial x^{2} }}} \right) + \left( {\frac{1}{10} - \frac{{2z^{2} }}{{3h^{2} }}} \right)\left( {4\frac{{\partial^{2} w_{s} }}{{\partial y^{2} }} - \frac{{\partial^{2} w_{s} }}{{\partial x^{2} }}} \right)} \right],$$
(A.18)
$$\begin{aligned} &(\tau_{yzz}^{1} )_{l} = (\tau_{zyz}^{1} )_{l} = (\tau_{zzy}^{1} )_{l}\\ &\quad = 2\mu_{l} l_{1}^{2} \left[ { - \frac{1}{15}\left( {2\frac{{\partial^{2} u}}{\partial x\partial y} + \frac{{\partial^{2} v}}{{\partial x^{2} }} + 3\frac{{\partial^{2} v}}{{\partial y^{2} }}} \right) - \frac{1}{5}\frac{{\partial w_{b} }}{\partial y}\frac{{\partial^{2} w_{b} }}{{\partial y^{2} }} - \frac{1}{5}\frac{{\partial w_{s} }}{\partial y}\frac{{\partial^{2} w_{b} }}{{\partial y^{2} }}} \right. \\ & \qquad - \frac{1}{5}\frac{{\partial^{2} w_{s} }}{{\partial y^{2} }}\frac{{\partial w_{b} }}{\partial y} - \frac{1}{5}\frac{{\partial^{2} w_{s} }}{{\partial y^{2} }}\frac{{\partial w_{s} }}{\partial y} - \frac{2}{15}\frac{{\partial w_{b} }}{\partial x}\frac{{\partial^{2} w_{b} }}{\partial x\partial y} - \frac{2}{15}\frac{{\partial w_{s} }}{\partial x}\frac{{\partial^{2} w_{b} }}{\partial x\partial y} - \frac{2}{15}\frac{{\partial w_{b} }}{\partial x}\frac{{\partial^{2} w_{s} }}{\partial x\partial y} - \frac{2}{15}\frac{{\partial w_{s} }}{\partial x}\frac{{\partial^{2} w_{s} }}{\partial x\partial y} \\ & \qquad - \frac{1}{15}\frac{{\partial w_{b} }}{\partial y}\frac{{\partial^{2} w_{b} }}{{\partial x^{2} }} - \frac{1}{15}\frac{{\partial w_{s} }}{\partial y}\frac{{\partial^{2} w_{b} }}{{\partial x^{2} }} - \frac{1}{15}\frac{{\partial w_{b} }}{\partial y}\frac{{\partial^{2} w_{s} }}{{\partial x^{2} }} - \frac{1}{15}\frac{{\partial w_{s} }}{\partial y}\frac{{\partial^{2} w_{s} }}{{\partial x^{2} }} \\ & \qquad - \left. { z\left( {\frac{1}{20}\frac{{\partial^{3} w_{s} }}{{\partial x^{2} \partial y}} + \frac{1}{20}\frac{{\partial^{3} w_{s} }}{{\partial y^{3} }} + \frac{8}{{3h^{2} }}\frac{{\partial w_{s} }}{\partial y}} \right) + \frac{1}{5}z\left( {\frac{{\partial^{3} w_{b} }}{{\partial x^{2} \partial y}} + \frac{{\partial^{3} w_{b} }}{{\partial y^{3} }}} \right) + \frac{{z^{3} }}{{3h^{2} }}\left( {\frac{{\partial^{3} w_{s} }}{{\partial y^{3} }} + \frac{{\partial^{3} w_{s} }}{{\partial x^{2} \partial y}}} \right)} \right], \\ \end{aligned}$$
(A.19)
$$(m_{xx}^{(s)} )_{l} = 2\mu_{l} l_{2}^{2} \left[ {\frac{{\partial^{2} w_{b} }}{\partial x\partial y} + \left( {\frac{3}{8} + \frac{{5z^{2} }}{{2h^{2} }}} \right)\frac{{\partial^{2} w_{s} }}{\partial x\partial y}} \right],$$
(A.20)
$$(m_{yy}^{(s)} )_{l} = 2\mu_{l} l_{2}^{2} \left[ { - \frac{{\partial^{2} w_{b} }}{\partial x\partial y} - \left( {\frac{3}{8} + \frac{{5z^{2} }}{{2h^{2} }}} \right)\frac{{\partial^{2} w_{s} }}{\partial x\partial y}} \right],$$
(A.21)
$$(m_{xy}^{(s)} )_{l} = 2\mu_{l} l_{2}^{2} \left[ {\frac{1}{2}\left( {\frac{{\partial^{2} w_{b} }}{{\partial y^{2} }} - \frac{{\partial^{2} w_{b} }}{{\partial x^{2} }}} \right) + \left( {\frac{3}{16} + \frac{{5z^{2} }}{{4h^{2} }}} \right)\left( {\frac{{\partial^{2} w_{s} }}{{\partial y^{2} }} - \frac{{\partial^{2} w_{s} }}{{\partial x^{2} }}} \right)} \right],$$
(A.22)
$$(m_{xz}^{(s)} )_{l} = 2\mu_{l} l_{2}^{2} \left[ {\frac{1}{4}\left( {\frac{{\partial^{2} v}}{{\partial x^{2} }} - \frac{{\partial^{2} u}}{\partial x\partial y}} \right) + \frac{5z}{{2h^{2} }}\frac{{\partial w_{s} }}{\partial y}} \right],$$
(A.23)
$$(m_{yz}^{(s)} )_{l} = 2\mu_{l} l_{2}^{2} \left[ {\frac{1}{4}\left( {\frac{{\partial^{2} v}}{\partial x\partial y} - \frac{{\partial^{2} u}}{{\partial y^{2} }}} \right) - \frac{5z}{{2h^{2} }}\frac{{\partial w_{s} }}{\partial x}} \right].$$
(A.24)

Appendix B

$$\left[ \begin{gathered} N_{xx}^{0} \hfill \\ N_{xx}^{1} \hfill \\ N_{xx}^{3} \hfill \\ \end{gathered} \right] = \left[ {\begin{array}{*{20}c} {A_{0} } & \quad {A_{1} } & \quad {A_{3} } \\ {A_{1} } & \quad {A_{2} } & \quad {A_{4} } \\ {A_{3} } & \quad {A_{4} } & \quad {A_{6} } \\ \end{array} } \right]\left[ \begin{gathered} \frac{\partial u}{{\partial x}} + \frac{1}{2}\left( {\frac{{\partial w_{b} }}{\partial x} + \frac{{\partial w_{s} }}{\partial x}} \right)^{2} \\ \frac{1}{4}\frac{{\partial^{2} w_{s} }}{{\partial x^{2} }} - \frac{{\partial^{2} w_{b} }}{{\partial x^{2} }} \\ - \frac{5}{{3h^{2} }}\frac{{\partial^{2} w_{s} }}{{\partial x^{2} }} \\ \end{gathered} \right] + \left[ {\begin{array}{*{20}c} {F_{0} } & \quad {F_{1} } & \quad {F_{3} } \\ {F_{1} } & \quad {F_{2} } & \quad {F_{4} } \\ {F_{3} } & \quad {F_{4} } & \quad {F_{6} } \\ \end{array} } \right]\left[ \begin{gathered} \frac{\partial v}{{\partial y}} + \frac{1}{2}\left( {\frac{{\partial w_{b} }}{\partial y} + \frac{{\partial w_{s} }}{\partial y}} \right)^{2} \\ \frac{1}{4}\frac{{\partial^{2} w_{s} }}{{\partial y^{2} }} - \frac{{\partial^{2} w_{b} }}{{\partial y^{2} }} \\ - \frac{5}{{3h^{2} }}\frac{{\partial^{2} w_{s} }}{{\partial y^{2} }} \\ \end{gathered} \right],$$
(B.1)
$$\left[ \begin{gathered} N_{yy}^{0} \hfill \\ N_{yy}^{1} \hfill \\ N_{yy}^{3} \hfill \\ \end{gathered} \right] = \left[ {\begin{array}{*{20}c} {A_{0} } & \quad {A_{1} } & \quad {A_{3} } \\ {A_{1} } & \quad {A_{2} } & \quad {A_{4} } \\ {A_{3} } & \quad {A_{4} } & \quad {A_{6} } \\ \end{array} } \right]\left[ \begin{gathered} \frac{\partial v}{{\partial y}} + \frac{1}{2}\left( {\frac{{\partial w_{b} }}{\partial y} + \frac{{\partial w_{s} }}{\partial y}} \right)^{2} \\ \frac{1}{4}\frac{{\partial^{2} w_{s} }}{{\partial y^{2} }} - \frac{{\partial^{2} w_{b} }}{{\partial y^{2} }} \\ - \frac{5}{{3h^{2} }}\frac{{\partial^{2} w_{s} }}{{\partial y^{2} }} \\ \end{gathered} \right] + \left[ {\begin{array}{*{20}c} {F_{0} } & \quad {F_{1} } & \quad {F_{3} } \\ {F_{1} } & \quad {F_{2} } & \quad {F_{4} } \\ {F_{3} } & \quad {F_{4} } & \quad {F_{6} } \\ \end{array} } \right]\left[ \begin{gathered} \frac{\partial u}{{\partial x}} + \frac{1}{2}\left( {\frac{{\partial w_{b} }}{\partial x} + \frac{{\partial w_{s} }}{\partial x}} \right)^{2} \\ \frac{1}{4}\frac{{\partial^{2} w_{s} }}{{\partial x^{2} }} - \frac{{\partial^{2} w_{b} }}{{\partial x^{2} }} \\ - \frac{5}{{3h^{2} }}\frac{{\partial^{2} w_{s} }}{{\partial x^{2} }} \\ \end{gathered} \right],$$
(B.2)
$$\left[ \begin{gathered} N_{xy}^{0} \hfill \\ N_{xy}^{1} \hfill \\ N_{xy}^{3} \hfill \\ \end{gathered} \right] = \left[ {\begin{array}{*{20}c} {B_{0} } & \quad {B_{1} } & \quad {B_{3} } \\ {B_{1} } & \quad {B_{2} } & \quad {B_{4} } \\ {B_{3} } & \quad {B_{4} } & \quad {B_{6} } \\ \end{array} } \right]\left[ \begin{gathered} \frac{1}{2}\left( {\frac{\partial u}{{\partial y}} + \frac{\partial v}{{\partial x}} + \frac{{\partial w_{b} }}{\partial y}\frac{{\partial w_{b} }}{\partial x} + \frac{{\partial w_{s} }}{\partial y}\frac{{\partial w_{b} }}{\partial x} + \frac{{\partial w_{b} }}{\partial y}\frac{{\partial w_{s} }}{\partial x} + \frac{{\partial w_{s} }}{\partial y}\frac{{\partial w_{s} }}{\partial x}} \right) \\ \frac{1}{4}\frac{{\partial^{2} w_{s} }}{\partial x\partial y} - \frac{{\partial^{2} w_{b} }}{\partial x\partial y} \\ - \frac{5}{{3h^{2} }}\frac{{\partial^{2} w_{s} }}{\partial x\partial y} \\ \end{gathered} \right],$$
(B.3)
$$\left[ \begin{gathered} N_{xz}^{0} \hfill \\ N_{xz}^{2} \hfill \\ \end{gathered} \right] = \left[ {\begin{array}{*{20}c} {B_{0} } & \quad {B_{2} } \\ {B_{2} } & \quad {B_{4} } \\ \end{array} } \right]\left[ \begin{gathered} \frac{5}{8}\frac{{\partial w_{s} }}{\partial x} \\ - \frac{5}{{2h^{2} }}\frac{{\partial w_{s} }}{\partial x} \\ \end{gathered} \right],$$
(B.4)
$$\left[ \begin{gathered} N_{yz}^{0} \hfill \\ N_{yz}^{2} \hfill \\ \end{gathered} \right] = \left[ {\begin{array}{*{20}c} {B_{0} } & \quad {B_{2} } \\ {B_{2} } & \quad {B_{4} } \\ \end{array} } \right]\left[ \begin{gathered} \frac{5}{8}\frac{{\partial w_{s} }}{\partial y} \\ - \frac{5}{{2h^{2} }}\frac{{\partial w_{s} }}{\partial y} \\ \end{gathered} \right],$$
(B.5)
$$\left[ \begin{gathered} P_{x}^{0} \hfill \\ P_{x}^{1} \hfill \\ P_{x}^{3} \hfill \\ \end{gathered} \right] = \left[ {\begin{array}{*{20}c} {C_{0} } & \quad {C_{1} } & \quad {C_{3} } \\ {C_{1} } & \quad {C_{2} } & \quad {C_{4} } \\ {C_{3} } & \quad {C_{4} } & \quad {C_{6} } \\ \end{array} } \right]\left[ \begin{gathered} \frac{{\partial^{2} u}}{{\partial x^{2} }} + \frac{{\partial^{2} v}}{\partial x\partial y} + \left( {\frac{{\partial w_{b} }}{\partial y} + \frac{{\partial w_{s} }}{\partial y}} \right)\left( {\frac{{\partial^{2} w_{b} }}{\partial x\partial y} + \frac{{\partial^{2} w_{s} }}{\partial x\partial y}} \right) + \left( {\frac{{\partial w_{b} }}{\partial x} + \frac{{\partial w_{s} }}{\partial x}} \right)\left( {\frac{{\partial^{2} w_{b} }}{{\partial x^{2} }} + \frac{{\partial^{2} w_{s} }}{{\partial x^{2} }}} \right) \\ \frac{1}{4}\left( {\frac{{\partial^{3} w_{s} }}{{\partial x\partial y^{2} }} + \frac{{\partial^{3} w_{s} }}{{\partial x^{3} }}} \right) - \left( {\frac{{\partial^{3} w_{b} }}{{\partial x\partial y^{2} }} + \frac{{\partial^{3} w_{b} }}{{\partial x^{3} }}} \right) \\ - \frac{5}{{3h^{2} }}\left( {\frac{{\partial^{3} w_{s} }}{{\partial x^{3} }} + \frac{{\partial^{3} w_{s} }}{{\partial x\partial y^{2} }}} \right) \\ \end{gathered} \right],$$
(B.6)
$$\left[ \begin{gathered} P_{y}^{0} \hfill \\ P_{y}^{1} \hfill \\ P_{y}^{3} \hfill \\ \end{gathered} \right] = \left[ {\begin{array}{*{20}c} {C_{0} } & \quad {C_{1} } & \quad {C_{3} } \\ {C_{1} } & \quad {C_{2} } & \quad {C_{4} } \\ {C_{3} } & \quad {C_{4} } & \quad {C_{6} } \\ \end{array} } \right]\left[ \begin{gathered} \frac{{\partial^{2} u}}{\partial x\partial y} + \frac{{\partial^{2} v}}{{\partial y^{2} }} + \left( {\frac{{\partial w_{b} }}{\partial y} + \frac{{\partial w_{s} }}{\partial y}} \right)\left( {\frac{{\partial^{2} w_{b} }}{{\partial y^{2} }} + \frac{{\partial^{2} w_{s} }}{{\partial y^{2} }}} \right) + \left( {\frac{{\partial w_{b} }}{\partial x} + \frac{{\partial w_{s} }}{\partial x}} \right)\left( {\frac{{\partial^{2} w_{b} }}{\partial x\partial y} + \frac{{\partial^{2} w_{s} }}{\partial x\partial y}} \right) \\ \frac{1}{4}\left( {\frac{{\partial^{3} w_{s} }}{{\partial x^{2} \partial y}} + \frac{{\partial^{3} w_{s} }}{{\partial y^{3} }}} \right) - \left( {\frac{{\partial^{3} w_{b} }}{{\partial x^{2} \partial y}} + \frac{{\partial^{3} w_{b} }}{{\partial y^{3} }}} \right) \\ - \frac{5}{{3h^{2} }}\left( {\frac{{\partial^{3} w_{s} }}{{\partial y^{3} }} + \frac{{\partial^{3} w_{s} }}{{\partial x^{2} \partial y}}} \right) \\ \end{gathered} \right],$$
(B.7)
$$\left[ \begin{gathered} P_{z}^{0} \hfill \\ P_{z}^{2} \hfill \\ \end{gathered} \right] = \left[ {\begin{array}{*{20}c} {C_{0} } & \quad {C_{2} } \\ {C_{2} } & \quad {C_{4} } \\ \end{array} } \right]\left[ \begin{gathered} \frac{1}{4}\left( {\frac{{\partial^{2} w_{s} }}{{\partial x^{2} }} + \frac{{\partial^{2} w_{s} }}{{\partial y^{2} }}} \right) - \left( {\frac{{\partial^{2} w_{b} }}{{\partial x^{2} }} + \frac{{\partial^{2} w_{b} }}{{\partial y^{2} }}} \right) \\ - \frac{5}{{h^{2} }}\left( {\frac{{\partial^{2} w_{s} }}{{\partial x^{2} }} + \frac{{\partial^{2} w_{s} }}{{\partial y^{2} }}} \right) \\ \end{gathered} \right],$$
(B.8)
$$\left[ \begin{gathered} M_{xx}^{0} \hfill \\ M_{xx}^{2} \hfill \\ \end{gathered} \right] = \left[ {\begin{array}{*{20}c} {E_{0} } & \quad {E_{2} } \\ {E_{2} } & \quad {E_{4} } \\ \end{array} } \right]\left[ \begin{gathered} \frac{3}{8}\frac{{\partial^{2} w_{s} }}{\partial x\partial y} + \frac{{\partial^{2} w_{b} }}{\partial x\partial y} \\ \frac{5}{{2h^{2} }}\frac{{\partial^{2} w_{s} }}{\partial x\partial y} \\ \end{gathered} \right],$$
(B.9)
$$\left[ \begin{gathered} M_{xy}^{0} \hfill \\ M_{xy}^{2} \hfill \\ \end{gathered} \right] = - \left[ {\begin{array}{*{20}c} {E_{0} } & \quad {E_{2} } \\ {E_{2} } & \quad {E_{4} } \\ \end{array} } \right]\left[ \begin{gathered} \frac{3}{16}\left( {\frac{{\partial^{2} w_{s} }}{{\partial x^{2} }} - \frac{{\partial^{2} w_{s} }}{{\partial y^{2} }}} \right) + \frac{1}{2}\left( {\frac{{\partial^{2} w_{b} }}{{\partial x^{2} }} - \frac{{\partial^{2} w_{b} }}{{\partial y^{2} }}} \right) \\ \frac{5}{{4h^{2} }}\left( {\frac{{\partial^{2} w_{s} }}{{\partial x^{2} }} - \frac{{\partial^{2} w_{s} }}{{\partial y^{2} }}} \right) \\ \end{gathered} \right],$$
(B.10)
$$\left[ \begin{gathered} M_{xz}^{0} \hfill \\ M_{xz}^{1} \hfill \\ \end{gathered} \right] = \left[ {\begin{array}{*{20}c} {E_{0} } & \quad {E_{1} } \\ {E_{1} } & \quad {E_{2} } \\ \end{array} } \right]\left[ \begin{gathered} \frac{1}{4}\left( {\frac{{\partial^{2} v}}{{\partial x^{2} }} - \frac{{\partial^{2} u}}{\partial x\partial y}} \right) \\ \frac{5}{{2h^{2} }}\frac{{\partial w_{s} }}{\partial y} \\ \end{gathered} \right],$$
(B.11)
$$\left[ \begin{gathered} M_{yz}^{0} \hfill \\ M_{yz}^{1} \hfill \\ \end{gathered} \right] = - \left[ {\begin{array}{*{20}c} {E_{0} } & \quad {E_{1} } \\ {E_{1} } & \quad {E_{2} } \\ \end{array} } \right]\left[ \begin{gathered} \frac{1}{4}\left( {\frac{{\partial^{2} u}}{{\partial y^{2} }} - \frac{{\partial^{2} v}}{\partial x\partial y}} \right) \\ \frac{5}{{2h^{2} }}\frac{{\partial w_{s} }}{\partial x} \\ \end{gathered} \right],$$
(B.12)
$$\left[ \begin{gathered} T_{xxx}^{0} \hfill \\ T_{xxx}^{1} \hfill \\ T_{xxx}^{3} \hfill \\ \end{gathered} \right] = \left[ {\begin{array}{*{20}c} {D_{0} } & \quad {D_{1} } & \quad {D_{3} } \\ {D_{1} } & \quad {D_{2} } & \quad {D_{4} } \\ {D_{3} } & \quad {D_{4} } & \quad {D_{6} } \\ \end{array} } \right]\left[ \begin{gathered} \frac{1}{5}\left( {2\frac{{\partial^{2} u}}{{\partial x^{2} }} - \frac{{\partial^{2} u}}{{\partial y^{2} }} - 2\frac{{\partial^{2} v}}{\partial x\partial y}} \right) - \frac{1}{5}\frac{{\partial^{2} w_{b} }}{{\partial y^{2} }}\frac{{\partial w_{b} }}{\partial x} - \frac{1}{5}\frac{{\partial^{2} w_{s} }}{{\partial y^{2} }}\frac{{\partial w_{b} }}{\partial x} - \frac{1}{5}\frac{{\partial^{2} w_{b} }}{{\partial y^{2} }}\frac{{\partial w_{s} }}{\partial x} \\ - \frac{1}{5}\frac{{\partial^{2} w_{s} }}{{\partial y^{2} }}\frac{{\partial w_{s} }}{\partial x} - \frac{2}{5}\frac{{\partial w_{b} }}{\partial y}\frac{{\partial^{2} w_{b} }}{\partial x\partial y} - \frac{2}{5}\frac{{\partial w_{s} }}{\partial y}\frac{{\partial^{2} w_{b} }}{\partial x\partial y} - \frac{2}{5}\frac{{\partial w_{b} }}{\partial y}\frac{{\partial^{2} w_{s} }}{\partial x\partial y} - \frac{2}{5}\frac{{\partial w_{s} }}{\partial y}\frac{{\partial^{2} w_{s} }}{\partial x\partial y} \\ + \frac{2}{5}\frac{{\partial w_{b} }}{\partial x}\frac{{\partial^{2} w_{b} }}{{\partial x^{2} }} + \frac{2}{5}\frac{{\partial w_{s} }}{\partial x}\frac{{\partial^{2} w_{b} }}{{\partial x^{2} }} + \frac{2}{5}\frac{{\partial w_{b} }}{\partial x}\frac{{\partial^{2} w_{s} }}{{\partial x^{2} }} + \frac{2}{5}\frac{{\partial w_{s} }}{\partial x}\frac{{\partial^{2} w_{s} }}{{\partial x^{2} }} \\ \left( {\frac{1}{10}\frac{{\partial^{3} w_{s} }}{{\partial x^{3} }} - \frac{3}{20}\frac{{\partial^{3} w_{s} }}{{\partial x\partial y^{2} }} + \frac{2}{{h^{2} }}\frac{{\partial w_{s} }}{\partial x}} \right) - \frac{1}{5}\left( {2\frac{{\partial^{3} w_{b} }}{{\partial x^{3} }} - 3\frac{{\partial^{3} w_{b} }}{{\partial x\partial y^{2} }}} \right) \\ - \frac{1}{{h^{2} }}\left( {\frac{2}{3}\frac{{\partial^{3} w_{s} }}{{\partial x^{3} }} - \frac{{\partial^{3} w_{s} }}{{\partial x\partial y^{2} }}} \right) \\ \end{gathered} \right],$$
(B.13)
$$\left[ \begin{gathered} T_{xyx}^{0} \hfill \\ T_{xyx}^{1} \hfill \\ T_{xyx}^{3} \hfill \\ \end{gathered} \right] = \left[ {\begin{array}{*{20}c} {D_{0} } & \quad {D_{1} } & \quad {D_{3} } \\ {D_{1} } & \quad {D_{2} } & \quad {D_{4} } \\ {D_{3} } & \quad {D_{4} } & \quad {D_{6} } \\ \end{array} } \right]\left[ \begin{gathered} \frac{1}{15}\left( {\frac{{8\partial^{2} u}}{\partial x\partial y} + \frac{{4\partial^{2} v}}{{\partial x^{2} }} - 3\frac{{\partial^{2} v}}{{\partial y^{2} }}} \right) - \frac{1}{5}\frac{{\partial w_{b} }}{\partial y}\frac{{\partial^{2} w_{b} }}{{\partial y^{2} }} - \frac{1}{5}\frac{{\partial w_{s} }}{\partial y}\frac{{\partial^{2} w_{b} }}{{\partial y^{2} }} - \frac{1}{5}\frac{{\partial^{2} w_{s} }}{{\partial y^{2} }}\frac{{\partial w_{b} }}{\partial y} \\ - \frac{1}{5}\frac{{\partial^{2} w_{s} }}{{\partial y^{2} }}\frac{{\partial w_{s} }}{\partial y} + \frac{8}{15}\frac{{\partial w_{b} }}{\partial x}\frac{{\partial^{2} w_{b} }}{\partial x\partial y} + \frac{8}{15}\frac{{\partial w_{s} }}{\partial x}\frac{{\partial^{2} w_{b} }}{\partial x\partial y} + \frac{8}{15}\frac{{\partial w_{b} }}{\partial x}\frac{{\partial^{2} w_{s} }}{\partial x\partial y} + \frac{8}{15}\frac{{\partial w_{s} }}{\partial x}\frac{{\partial^{2} w_{s} }}{\partial x\partial y} \\ + \frac{4}{15}\frac{{\partial w_{b} }}{\partial y}\frac{{\partial^{2} w_{b} }}{{\partial x^{2} }} + \frac{4}{15}\frac{{\partial w_{s} }}{\partial y}\frac{{\partial^{2} w_{b} }}{{\partial x^{2} }} + \frac{4}{15}\frac{{\partial w_{b} }}{\partial y}\frac{{\partial^{2} w_{s} }}{{\partial x^{2} }} + \frac{4}{15}\frac{{\partial w_{s} }}{\partial y}\frac{{\partial^{2} w_{s} }}{{\partial x^{2} }} \\ \left( {\frac{1}{5}\frac{{\partial^{3} w_{s} }}{{\partial x^{2} \partial y}} - \frac{1}{20}\frac{{\partial^{3} w_{s} }}{{\partial y^{3} }} + \frac{2}{{3h^{2} }}\frac{{\partial w_{s} }}{\partial y}} \right) - \frac{1}{5}\left( {4\frac{{\partial^{3} w_{b} }}{{\partial x^{2} \partial y}} - \frac{{\partial^{3} w_{b} }}{{\partial y^{3} }}} \right) \\ - \frac{1}{{3h^{2} }}\left( {4\frac{{\partial^{3} w_{s} }}{{\partial x^{2} \partial y}} - \frac{{\partial^{3} w_{s} }}{{\partial y^{3} }}} \right) \\ \end{gathered} \right],$$
(B.14)
$$\left[ \begin{gathered} T_{xzx}^{0} \hfill \\ T_{xzx}^{2} \hfill \\ \end{gathered} \right] = \left[ {\begin{array}{*{20}c} {D_{0} } & \quad {D_{2} } \\ {D_{2} } & \quad {D_{4} } \\ \end{array} } \right]\left[ \begin{gathered} - \frac{1}{15}\left( {4\frac{{\partial^{2} w_{b} }}{{\partial x^{2} }} - \frac{{\partial^{2} w_{b} }}{{\partial y^{2} }}} \right) + \frac{1}{10}\left( {4\frac{{\partial^{2} w_{s} }}{{\partial x^{2} }} - \frac{{\partial^{2} w_{s} }}{{\partial y^{2} }}} \right) \\ - \frac{2}{{3h^{2} }}\left( {4\frac{{\partial^{2} w_{s} }}{{\partial x^{2} }} - \frac{{\partial^{2} w_{s} }}{{\partial y^{2} }}} \right) \\ \end{gathered} \right],$$
(B.15)
$$\left[ \begin{gathered} T_{yyx}^{0} \hfill \\ T_{yyx}^{1} \hfill \\ T_{yyx}^{3} \hfill \\ \end{gathered} \right] = \left[ {\begin{array}{*{20}c} {D_{0} } & \quad {D_{1} } & \quad {D_{3} } \\ {D_{1} } & \quad {D_{2} } & \quad {D_{4} } \\ {D_{3} } & \quad {D_{4} } & \quad {D_{6} } \\ \end{array} } \right]\left[ \begin{gathered} - \frac{1}{15}\left( {3\frac{{\partial^{2} u}}{{\partial x^{2} }} - 4\frac{{\partial^{2} u}}{{\partial y^{2} }} - 8\frac{{\partial^{2} v}}{\partial x\partial y}} \right) + \frac{4}{15}\frac{{\partial w_{b} }}{\partial x}\frac{{\partial^{2} w_{b} }}{{\partial y^{2} }} + \frac{4}{15}\frac{{\partial w_{b} }}{\partial x}\frac{{\partial^{2} w_{s} }}{{\partial y^{2} }} + \frac{4}{15}\frac{{\partial^{2} w_{b} }}{{\partial y^{2} }}\frac{{\partial w_{s} }}{\partial x} \\ + \frac{4}{15}\frac{{\partial^{2} w_{s} }}{{\partial y^{2} }}\frac{{\partial w_{s} }}{\partial x} + \frac{8}{15}\frac{{\partial w_{b} }}{\partial y}\frac{{\partial^{2} w_{b} }}{\partial x\partial y} + \frac{8}{15}\frac{{\partial w_{s} }}{\partial y}\frac{{\partial^{2} w_{b} }}{\partial x\partial y} + \frac{8}{15}\frac{{\partial w_{b} }}{\partial y}\frac{{\partial^{2} w_{s} }}{\partial x\partial y} + \frac{8}{15}\frac{{\partial w_{s} }}{\partial y}\frac{{\partial^{2} w_{s} }}{\partial x\partial y} \\ - \frac{1}{5}\frac{{\partial w_{b} }}{\partial x}\frac{{\partial^{2} w_{b} }}{{\partial x^{2} }} - \frac{1}{5}\frac{{\partial w_{s} }}{\partial x}\frac{{\partial^{2} w_{b} }}{{\partial x^{2} }} - \frac{1}{5}\frac{{\partial w_{b} }}{\partial x}\frac{{\partial^{2} w_{s} }}{{\partial x^{2} }} - \frac{1}{5}\frac{{\partial w_{s} }}{\partial x}\frac{{\partial^{2} w_{s} }}{{\partial x^{2} }} \\ \left( { - \frac{1}{20}\frac{{\partial^{3} w_{s} }}{{\partial x^{3} }} + \frac{1}{5}\frac{{\partial^{3} w_{s} }}{{\partial x\partial y^{2} }} + \frac{2}{{3h^{2} }}\frac{{\partial w_{s} }}{\partial x}} \right) - \frac{1}{5}\left( {4\frac{{\partial^{3} w_{b} }}{{\partial x\partial y^{2} }} - \frac{{\partial^{3} w_{b} }}{{\partial x^{3} }}} \right) \\ - \frac{1}{{3h^{2} }}\left( {4\frac{{\partial^{3} w_{s} }}{{\partial x\partial y^{2} }} - \frac{{\partial^{3} w_{s} }}{{\partial x^{3} }}} \right) \\ \end{gathered} \right],$$
(B.16)
$$\left[ \begin{gathered} T_{zzx}^{0} \hfill \\ T_{zzx}^{1} \hfill \\ T_{zzx}^{3} \hfill \\ \end{gathered} \right] = \left[ {\begin{array}{*{20}c} {D_{0} } & \quad {D_{1} } & \quad {D_{3} } \\ {D_{1} } & \quad {D_{2} } & \quad {D_{4} } \\ {D_{3} } & \quad {D_{4} } & \quad {D_{6} } \\ \end{array} } \right]\left[ \begin{gathered} - \frac{1}{15}\left( {3\frac{{\partial^{2} u}}{{\partial x^{2} }} + \frac{{\partial^{2} u}}{{\partial y^{2} }} + 2\frac{{\partial^{2} v}}{\partial x\partial y}} \right) - \frac{1}{15}\frac{{\partial w_{b} }}{\partial x}\frac{{\partial^{2} w_{b} }}{{\partial y^{2} }} - \frac{1}{15}\frac{{\partial w_{b} }}{\partial x}\frac{{\partial^{2} w_{s} }}{{\partial y^{2} }} - \frac{1}{15}\frac{{\partial^{2} w_{b} }}{{\partial y^{2} }}\frac{{\partial w_{s} }}{\partial x} \\ - \frac{1}{15}\frac{{\partial^{2} w_{s} }}{{\partial y^{2} }}\frac{{\partial w_{s} }}{\partial x} - \frac{2}{15}\frac{{\partial w_{b} }}{\partial y}\frac{{\partial^{2} w_{b} }}{\partial x\partial y} - \frac{2}{15}\frac{{\partial w_{s} }}{\partial y}\frac{{\partial^{2} w_{b} }}{\partial x\partial y} - \frac{2}{15}\frac{{\partial w_{b} }}{\partial y}\frac{{\partial^{2} w_{s} }}{\partial x\partial y} - \frac{2}{15}\frac{{\partial w_{s} }}{\partial y}\frac{{\partial^{2} w_{s} }}{\partial x\partial y} \\ - \frac{1}{5}\frac{{\partial w_{b} }}{\partial x}\frac{{\partial^{2} w_{b} }}{{\partial x^{2} }} - \frac{1}{5}\frac{{\partial w_{s} }}{\partial x}\frac{{\partial^{2} w_{b} }}{{\partial x^{2} }} - \frac{1}{5}\frac{{\partial w_{b} }}{\partial x}\frac{{\partial^{2} w_{s} }}{{\partial x^{2} }} - \frac{1}{5}\frac{{\partial w_{s} }}{\partial x}\frac{{\partial^{2} w_{s} }}{{\partial x^{2} }} \\ - \left( {\frac{1}{20}\frac{{\partial^{3} w_{s} }}{{\partial x^{3} }} + \frac{1}{20}\frac{{\partial^{3} w_{s} }}{{\partial x\partial y^{2} }} + \frac{8}{{3h^{2} }}\frac{{\partial w_{s} }}{\partial x}} \right) + \frac{1}{5}\left( {\frac{{\partial^{3} w_{b} }}{{\partial x^{3} }} + \frac{{\partial^{3} w_{b} }}{{\partial x\partial y^{2} }}} \right) \\ \frac{1}{{3h^{2} }}\left( {\frac{{\partial^{3} w_{s} }}{{\partial x^{3} }} + \frac{{\partial^{3} w_{s} }}{{\partial x\partial y^{2} }}} \right) \\ \end{gathered} \right],$$
(B.17)
$$\left[ \begin{gathered} T_{yzx}^{0} \hfill \\ T_{yzx}^{2} \hfill \\ \end{gathered} \right] = \left[ {\begin{array}{*{20}c} {D_{0} } & \quad {D_{2} } \\ {D_{2} } & \quad {D_{4} } \\ \end{array} } \right]\left[ \begin{gathered} - \left( {\frac{1}{3}\frac{{\partial^{2} w_{b} }}{\partial x\partial y} - \frac{1}{2}\frac{{\partial^{2} w_{s} }}{\partial x\partial y}} \right) \\ - \frac{10}{{3h^{2} }}\frac{{\partial^{2} w_{s} }}{\partial x\partial y} \\ \end{gathered} \right],$$
(B.18)
$$\begin{aligned}\left[ \begin{gathered} T_{yyy}^{0} \hfill \\ T_{yyy}^{1} \hfill \\ T_{yyy}^{3} \hfill \\ \end{gathered} \right] = &\left[ {\begin{array}{*{20}c} {D_{0} } & \quad {D_{1} } & \quad {D_{3} } \\ {D_{1} } & \quad {D_{2} } & \quad {D_{4} } \\ {D_{3} } & \quad {D_{4} } & \quad {D_{6} } \\ \end{array} } \right]\\ &\left[ \begin{gathered} \frac{1}{5}\left( {2\frac{{\partial^{2} v}}{{\partial y^{2} }} - \frac{{\partial^{2} v}}{{\partial x^{2} }} - 2\frac{{\partial^{2} u}}{\partial x\partial y}} \right) + \frac{2}{5}\frac{{\partial w_{b} }}{\partial y}\frac{{\partial^{2} w_{b} }}{{\partial y^{2} }} + \frac{2}{5}\frac{{\partial w_{s} }}{\partial y}\frac{{\partial^{2} w_{b} }}{{\partial y^{2} }} + \frac{2}{5}\frac{{\partial^{2} w_{s} }}{{\partial y^{2} }}\frac{{\partial w_{b} }}{\partial y} + \frac{2}{5}\frac{{\partial^{2} w_{s} }}{{\partial y^{2} }}\frac{{\partial w_{s} }}{\partial y} \\ - \frac{2}{5}\frac{{\partial w_{b} }}{\partial x}\frac{{\partial^{2} w_{b} }}{\partial x\partial y} - \frac{2}{5}\frac{{\partial w_{s} }}{\partial x}\frac{{\partial^{2} w_{b} }}{\partial x\partial y} - \frac{2}{5}\frac{{\partial w_{b} }}{\partial x}\frac{{\partial^{2} w_{s} }}{\partial x\partial y} - \frac{2}{5}\frac{{\partial w_{s} }}{\partial x}\frac{{\partial^{2} w_{s} }}{\partial x\partial y} \\ - \frac{1}{5}\frac{{\partial w_{b} }}{\partial y}\frac{{\partial^{2} w_{b} }}{{\partial x^{2} }} - \frac{1}{5}\frac{{\partial w_{s} }}{\partial y}\frac{{\partial^{2} w_{b} }}{{\partial x^{2} }} - \frac{1}{5}\frac{{\partial w_{b} }}{\partial y}\frac{{\partial^{2} w_{s} }}{{\partial x^{2} }} - \frac{1}{5}\frac{{\partial w_{s} }}{\partial y}\frac{{\partial^{2} w_{s} }}{{\partial x^{2} }} \\ \left( {\frac{1}{10}\frac{{\partial^{3} w_{s} }}{{\partial y^{3} }} - \frac{3}{20}\frac{{\partial^{3} w_{s} }}{{\partial x^{2} \partial y}} + \frac{2}{{h^{2} }}\frac{{\partial w_{s} }}{\partial y}} \right) - \frac{1}{5}\left( {2\frac{{\partial^{3} w_{b} }}{{\partial y^{3} }} - 3\frac{{\partial^{3} w_{b} }}{{\partial x^{2} \partial y}}} \right) \\ - \frac{1}{{h^{2} }}\left( {\frac{2}{3}\frac{{\partial^{3} w_{s} }}{{\partial y^{3} }} - \frac{{\partial^{3} w_{s} }}{{\partial x^{2} \partial y}}} \right) \\ \end{gathered} \right], \end{aligned}$$
(B.19)
$$\left[ \begin{gathered} T_{yzy}^{0} \hfill \\ T_{yzy}^{2} \hfill \\ \end{gathered} \right] = \left[ {\begin{array}{*{20}c} {D_{0} } & \quad {D_{2} } \\ {D_{2} } & \quad {D_{4} } \\ \end{array} } \right]\left[ \begin{gathered} \frac{1}{15}\left( {\frac{{\partial^{2} w_{b} }}{{\partial x^{2} }} - 4\frac{{\partial^{2} w_{b} }}{{\partial y^{2} }}} \right) - \frac{1}{10}\left( {\frac{{\partial^{2} w_{s} }}{{\partial x^{2} }} - 4\frac{{\partial^{2} w_{s} }}{{\partial y^{2} }}} \right) \\ \frac{2}{{3h^{2} }}\left( {\frac{{\partial^{2} w_{s} }}{{\partial x^{2} }} - 4\frac{{\partial^{2} w_{s} }}{{\partial y^{2} }}} \right) \\ \end{gathered} \right],$$
(B.20)
$$\begin{aligned} \left[ \begin{gathered} T_{zzy}^{0} \hfill \\ T_{zzy}^{1} \hfill \\ T_{zzy}^{3} \hfill \\ \end{gathered} \right] = & \left[ {\begin{array}{*{20}c} {D_{0} } & \quad {D_{1} } & \quad {D_{3} } \\ {D_{1} } & \quad {D_{2} } & \quad {D_{4} } \\ {D_{3} } & \quad {D_{4} } & \quad {D_{6} } \\ \end{array} } \right]\\ &\left[ \begin{gathered} - \frac{1}{15}\left( {2\frac{{\partial^{2} u}}{\partial x\partial y} + \frac{{\partial^{2} v}}{{\partial x^{2} }} + 3\frac{{\partial^{2} v}}{{\partial y^{2} }}} \right) - \frac{1}{5}\frac{{\partial w_{b} }}{\partial y}\frac{{\partial^{2} w_{b} }}{{\partial y^{2} }} - \frac{1}{5}\frac{{\partial w_{s} }}{\partial y}\frac{{\partial^{2} w_{b} }}{{\partial y^{2} }} - \frac{1}{5}\frac{{\partial^{2} w_{s} }}{{\partial y^{2} }}\frac{{\partial w_{b} }}{\partial y} \\ - \frac{1}{5}\frac{{\partial^{2} w_{s} }}{{\partial y^{2} }}\frac{{\partial w_{s} }}{\partial y} - \frac{2}{15}\frac{{\partial w_{b} }}{\partial x}\frac{{\partial^{2} w_{b} }}{\partial x\partial y} - \frac{2}{15}\frac{{\partial w_{s} }}{\partial x}\frac{{\partial^{2} w_{b} }}{\partial x\partial y} - \frac{2}{15}\frac{{\partial w_{b} }}{\partial x}\frac{{\partial^{2} w_{s} }}{\partial x\partial y} - \frac{2}{15}\frac{{\partial w_{s} }}{\partial x}\frac{{\partial^{2} w_{s} }}{\partial x\partial y} \\ - \frac{1}{15}\frac{{\partial w_{b} }}{\partial y}\frac{{\partial^{2} w_{b} }}{{\partial x^{2} }} - \frac{1}{15}\frac{{\partial w_{s} }}{\partial y}\frac{{\partial^{2} w_{b} }}{{\partial x^{2} }} - \frac{1}{15}\frac{{\partial w_{b} }}{\partial y}\frac{{\partial^{2} w_{s} }}{{\partial x^{2} }} - \frac{1}{15}\frac{{\partial w_{s} }}{\partial y}\frac{{\partial^{2} w_{s} }}{{\partial x^{2} }} \\ - \left( {\frac{1}{20}\frac{{\partial^{3} w_{s} }}{{\partial x^{2} \partial y}} + \frac{1}{20}\frac{{\partial^{3} w_{s} }}{{\partial y^{3} }} + \frac{8}{{3h^{2} }}\frac{{\partial w_{s} }}{\partial y}} \right) + \frac{1}{5}\left( {\frac{{\partial^{3} w_{b} }}{{\partial x^{2} \partial y}} + \frac{{\partial^{3} w_{b} }}{{\partial y^{3} }}} \right) \\ \frac{1}{{3h^{2} }}\left( {\frac{{\partial^{3} w_{s} }}{{\partial y^{3} }} + \frac{{\partial^{3} w_{s} }}{{\partial x^{2} \partial y}}} \right) \\ \end{gathered} \right], \end{aligned}$$
(B.21)
$$\left[ \begin{gathered} T_{zzz}^{0} \hfill \\ T_{zzz}^{2} \hfill \\ \end{gathered} \right] = \left[ {\begin{array}{*{20}c} {D_{0} } & \quad {D_{2} } \\ {D_{2} } & \quad {D_{4} } \\ \end{array} } \right]\left[ \begin{gathered} \frac{1}{5}\left( {\frac{{\partial^{2} w_{b} }}{{\partial x^{2} }} + \frac{{\partial^{2} w_{b} }}{{\partial y^{2} }}} \right) - \frac{3}{10}\left( {\frac{{\partial^{2} w_{s} }}{{\partial x^{2} }} + \frac{{\partial^{2} w_{s} }}{{\partial y^{2} }}} \right) \\ \frac{2}{{h^{2} }}\left( {\frac{{\partial^{2} w_{s} }}{{\partial x^{2} }} + \frac{{\partial^{2} w_{s} }}{{\partial y^{2} }}} \right) \\ \end{gathered} \right],$$
(B.22)

where

$$\begin{gathered} A_{i} = \sum\limits_{l = 1}^{k} {\int_{{z_{l} }}^{{z_{l + 1} }} {(\lambda_{l} + 2\mu_{l} )z^{i} {\text{d}}z, \;\, } } i = 0,1,2,3,4,6, \;\, B_{i} = \sum\limits_{l = 1}^{k} {\int_{{z_{l} }}^{{z_{l + 1} }} {2\mu_{l} z^{i} {\text{d}}z, \;\, } } i = 0,1,2,3,4,6, \hfill \\ C_{i} = \sum\limits_{l = 1}^{k} {\int_{{z_{l} }}^{{z_{l + 1} }} {2\mu_{l} l_{0}^{2} z^{i} {\text{d}}z, \;\, } } i = 0,1,2,3,4,6, \;\, D_{i} = \sum\limits_{l = 1}^{k} {\int_{{z_{l} }}^{{z_{l + 1} }} {2\mu_{l} l_{1}^{2} z^{i} {\text{d}}z, \;\, } } i = 0,1,2,3,4,6, \hfill \\ E_{i} = \sum\limits_{l = 1}^{k} {\int_{{z_{l} }}^{{z_{l + 1} }} {2\mu_{l} l_{2}^{2} z^{i} {\text{d}}z, \;\, } } i = 0,1,2,3,4,6, \, F_{i} = \sum\limits_{l = 1}^{k} {\int_{{z_{l} }}^{{z_{l + 1} }} {\lambda_{l} z^{i} {\text{d}}z, \;\, } } i = 0,1,2,3,4,6. \hfill \\ \end{gathered}$$
(B.23)

Appendix C

$$\begin{aligned} L_{11} & = - \frac{1}{2}B_{0} \phi_{m}^{\prime } \psi_{n}^{\prime \prime } - A_{0} \psi_{n} \phi_{m}^{(3)} + C_{0} \psi_{n}^{\prime \prime } \phi_{m}^{(3)} + \frac{2}{3}D_{0} \psi_{n}^{\prime \prime } \phi_{m}^{(3)} + \frac{1}{8}E_{0} \psi_{n}^{\prime \prime } \phi_{m}^{(3)} \\ & \quad + \frac{4}{15}D_{0} \phi_{m}^{\prime } \psi_{n}^{(4)} + \frac{1}{8}E_{0} \phi_{m}^{\prime } \psi_{n}^{(4)} + C_{0} \psi_{n} \phi_{m}^{(5)} + \frac{2}{5}D_{0} \psi_{n} \phi_{m}^{(5)} , \\ \end{aligned}$$
(C.1)
$$\begin{aligned} L_{12} & = - \frac{1}{2}B_{0} \phi_{m}^{\prime } \psi_{n}^{\prime \prime } - F_{0} \phi_{m}^{\prime } \psi_{n}^{\prime \prime } + C_{0} \psi_{n}^{\prime \prime } \phi_{m}^{(3)} + \frac{2}{15}D_{0} \psi_{n}^{\prime \prime } \phi_{m}^{(3)} \\ & \quad - \frac{1}{8}E_{0} \psi_{n}^{\prime \prime } \phi_{m}^{(3)} + C_{0} \phi_{m}^{\prime } \psi_{n}^{(4)} + \frac{2}{15}D_{0} \phi_{m}^{\prime } \psi_{n}^{(4)} - \frac{1}{8}E_{0} \phi_{m}^{\prime } \psi_{n}^{(4)} , \\ \end{aligned}$$
(C.2)
$$\begin{aligned} L_{13} & = B_{1} \phi_{m}^{\prime } \psi_{n}^{\prime \prime } + F_{1} \phi_{m}^{\prime } \psi_{n}^{\prime \prime } + A_{1} \psi_{n} \phi_{m}^{(3)} - 2C_{1} \psi_{n}^{\prime \prime } \phi_{m}^{(3)} - \frac{4}{5}D_{1} \psi_{n}^{\prime \prime } \phi_{m}^{(3)} \\ & \quad - C_{1} \phi_{m}^{\prime } \psi_{n}^{(4)} - \frac{2}{5}D_{1} \phi_{m}^{\prime } \psi_{n}^{(4)} - C_{1} \psi_{n} \phi_{m}^{(5)} - \frac{2}{5}D_{1} \psi_{n} \phi_{m}^{(5)} , \\ \end{aligned}$$
(C.3)
$$\begin{aligned} L_{14} & = - \frac{1}{2}B_{0} \phi_{m} \phi_{m}^{\prime } \psi_{n}^{\prime 2} - F_{0} \phi_{m} \phi_{m}^{\prime } \psi_{n}^{\prime 2} - A_{0} \psi_{n}^{2} \phi_{m}^{\prime } \phi_{m}^{\prime \prime } + 5C_{0} \phi_{m}^{\prime } \psi_{n}^{\prime 2} \phi_{m}^{\prime \prime } + \frac{16}{{15}}D_{0} \phi_{m}^{\prime } \psi_{n}^{\prime 2} \phi_{m}^{\prime \prime } \\ & \quad - \frac{1}{2}B_{0} \phi_{m} \psi_{n} \phi_{m}^{\prime } \psi_{n}^{\prime \prime } + 2C_{0} \psi_{n} \phi_{m}^{\prime } \phi_{m}^{\prime \prime } \psi_{n}^{\prime \prime } + \frac{5}{3}D_{0} \psi_{n} \phi_{m}^{\prime } \phi_{m}^{\prime \prime } \psi_{n}^{\prime \prime } + 2C_{0} \phi_{m} \phi_{m}^{\prime } \psi_{n}^{\prime \prime 2} + \frac{8}{15}D_{0} \phi_{m} \phi_{m}^{\prime } \psi_{n}^{\prime \prime 2} \\ & \quad + C_{0} \phi_{m} \psi_{n}^{\prime 2} \phi_{m}^{(3)} + \frac{2}{15}D_{0} \phi_{m} \psi_{n}^{\prime 2} \phi_{m}^{(3)} + 3C_{0} \psi_{n}^{2} \phi_{m}^{\prime \prime } \phi_{m}^{(3)} + \frac{6}{5}D_{0} \psi_{n}^{2} \phi_{m}^{\prime \prime } \phi_{m}^{(3)} + \frac{1}{3}D_{0} \phi_{m} \psi_{n} \psi_{n}^{\prime \prime } \phi_{m}^{(3)} \\ & \quad + 2C_{0} \phi_{m} \phi_{m}^{\prime } \psi_{n}^{\prime } \psi_{n}^{(3)} + \frac{4}{5}D_{0} \phi_{m} \phi_{m}^{\prime } \psi_{n}^{\prime } \psi_{n}^{(3)} + C_{0} \psi_{n}^{2} \phi_{m}^{\prime } \phi_{m}^{(4)} + \frac{2}{5}D_{0} \psi_{n}^{2} \phi_{m}^{\prime } \phi_{m}^{(4)} + \frac{4}{15}D_{0} \phi_{m} \psi_{n} \phi_{m}^{\prime } \psi_{n}^{(4)} , \\ \end{aligned}$$
(C.4)
$$\begin{aligned} L_{15} & = - \frac{1}{4}B_{1} \phi_{m}^{\prime } \psi_{n}^{\prime \prime } + \frac{{5B_{3} \phi_{m}^{\prime } \psi_{n}^{\prime \prime } }}{{3h^{2} }} + \frac{{2D_{1} \phi_{m}^{\prime } \psi_{n}^{\prime \prime } }}{{h^{2} }} - \frac{1}{4}F_{1} \phi_{m}^{\prime } \psi_{n}^{\prime \prime } + \frac{{5F_{3} \phi_{m}^{\prime } \psi_{n}^{\prime \prime } }}{{3h^{2} }} - \frac{1}{4}A_{1} \psi_{n} \phi_{m}^{(3)} \\ & \quad + \frac{{5A_{3} \psi_{n} \phi_{m}^{(3)} }}{{3h^{2} }} + \frac{{2D_{1} \psi_{n} \phi_{m}^{(3)} }}{{h^{2} }} + \frac{1}{2}C_{1} \psi_{n}^{\prime \prime } \phi_{m}^{(3)} - \frac{{10C_{3} \psi_{n}^{\prime \prime } \phi_{m}^{(3)} }}{{3h^{2} }} + \frac{1}{5}D_{1} \psi_{n}^{\prime \prime } \phi_{m}^{(3)} - \frac{{4D_{3} \psi_{n}^{\prime \prime } \phi_{m}^{(3)} }}{{3h^{2} }} \\ & \quad + \frac{1}{4}C_{1} \phi_{m}^{\prime } \psi_{n}^{(4)} - \frac{{5C_{3} \phi_{m}^{\prime } \psi_{n}^{(4)} }}{{3h^{2} }} + \frac{1}{10}D_{1} \phi_{m}^{\prime } \psi_{n}^{(4)} - \frac{{2D_{3} \phi_{m}^{\prime } \psi_{n}^{(4)} }}{{3h^{2} }} + \frac{1}{4}C_{1} \psi_{n} \phi_{m}^{(5)} - \frac{{5C_{3} \psi_{n} \phi_{m}^{(5)} }}{{3h^{2} }} \\ & \quad + \frac{1}{10}D_{1} \psi_{n} \phi_{m}^{(5)} - \frac{{2D_{3} \psi_{n} \phi_{m}^{(5)} }}{{3h^{2} }}, \\ \end{aligned}$$
(C.5)
$$\begin{aligned} L_{16} & = - B_{0} \phi_{m} \phi_{m}^{\prime } \psi_{n}^{\prime 2} - 2F_{0} \phi_{m} \phi_{m}^{\prime } \psi_{n}^{\prime 2} - 2A_{0} \psi_{n}^{2} \phi_{m}^{\prime } \phi_{m}^{\prime \prime } + 10C_{0} \phi_{m}^{\prime } \psi_{n}^{\prime 2} \phi_{m}^{\prime \prime } + \frac{32}{{15}}D_{0} \phi_{m}^{\prime } \psi_{n}^{\prime 2} \phi_{m}^{\prime \prime } \\ & \quad - B_{0} \phi_{m} \psi_{n} \phi_{m}^{\prime } \psi_{n}^{\prime \prime } + 4C_{0} \psi_{n} \phi_{m}^{\prime } \phi_{m}^{\prime \prime } \psi_{n}^{\prime \prime } + \frac{10}{3}D_{0} \psi_{n} \phi_{m}^{\prime } \phi_{m}^{\prime \prime } \psi_{n}^{\prime \prime } + 4C_{0} \phi_{m} \phi_{m}^{\prime } \psi_{n}^{\prime \prime 2} + \frac{16}{{15}}D_{0} \phi_{m} \phi_{m}^{\prime } \psi_{n}^{\prime \prime 2} \\ & \quad + 2C_{0} \phi_{m} \psi_{n}^{\prime 2} \phi_{m}^{(3)} + \frac{4}{15}D_{0} \phi_{m} \psi_{n}^{\prime 2} \phi_{m}^{(3)} + 6C_{0} \psi_{n}^{2} \phi_{m}^{\prime \prime } \phi_{m}^{(3)} + \frac{12}{5}D_{0} \psi_{n}^{2} \phi_{m}^{\prime \prime } \phi_{m}^{(3)} + \frac{2}{3}D_{0} \phi_{m} \psi_{n} \psi_{n}^{\prime \prime } \phi_{m}^{(3)} \\ & \quad + 4C_{0} \phi_{m} \phi_{m}^{\prime } \psi_{n}^{\prime } \psi_{n}^{(3)} + \frac{8}{5}D_{0} \phi_{m} \phi_{m}^{\prime } \psi_{n}^{\prime } \psi_{n}^{(3)} + 2C_{0} \psi_{n}^{2} \phi_{m}^{\prime } \phi_{m}^{(4)} + \frac{4}{5}D_{0} \psi_{n}^{2} \phi_{m}^{\prime } \phi_{m}^{(4)} + \frac{8}{15}D_{0} \phi_{m} \psi_{n} \phi_{m}^{\prime } \psi_{n}^{(4)} , \\ \end{aligned}$$
(C.6)
$$\begin{aligned} L_{17} & = - \frac{1}{2}B_{0} \phi_{m} \phi_{m}^{\prime } \psi_{n}^{\prime 2} - F_{0} \phi_{m} \phi_{m}^{\prime } \psi_{n}^{\prime 2} - A_{0} \psi_{n}^{2} \phi_{m}^{\prime } \phi_{m}^{\prime \prime } + 5C_{0} \phi_{m}^{\prime } \psi_{n}^{\prime 2} \phi_{m}^{\prime \prime } + \frac{16}{{15}}D_{0} \phi_{m}^{\prime } \psi_{n}^{\prime 2} \phi_{m}^{\prime \prime } \\ & \quad - \frac{1}{2}B_{0} \phi_{m} \psi_{n} \phi_{m}^{\prime } \psi_{n}^{\prime \prime } + 2C_{0} \psi_{n} \phi_{m}^{\prime } \phi_{m}^{\prime \prime } \psi_{n}^{\prime \prime } + \frac{5}{3}D_{0} \psi_{n} \phi_{m}^{\prime } \phi_{m}^{\prime \prime } \psi_{n}^{\prime \prime } + 2C_{0} \phi_{m} \phi_{m}^{\prime } \psi_{n}^{\prime \prime 2} + \frac{8}{15}D_{0} \phi_{m} \phi_{m}^{\prime } \psi_{n}^{\prime \prime 2} \\ & \quad + C_{0} \phi_{m} \psi_{n}^{\prime 2} \phi_{m}^{(3)} + \frac{2}{15}D_{0} \phi_{m} \psi_{n}^{\prime 2} \phi_{m}^{(3)} + 3C_{0} \psi_{n}^{2} \phi_{m}^{\prime \prime } \phi_{m}^{(3)} + \frac{6}{5}D_{0} \psi_{n}^{2} \phi_{m}^{\prime \prime } \phi_{m}^{(3)} + \frac{1}{3}D_{0} \phi_{m} \psi_{n} \psi_{n}^{\prime \prime } \phi_{m}^{(3)} \\ & \quad + 2C_{0} \phi_{m} \phi_{m}^{\prime } \psi_{n}^{\prime } \psi_{n}^{(3)} + \frac{4}{5}D_{0} \phi_{m} \phi_{m}^{\prime } \psi_{n}^{\prime } \psi_{n}^{(3)} + C_{0} \psi_{n}^{2} \phi_{m}^{\prime } \phi_{m}^{(4)} + \frac{2}{5}D_{0} \psi_{n}^{2} \phi_{m}^{\prime } \phi_{m}^{(4)} + \frac{4}{15}D_{0} \phi_{m} \psi_{n} \phi_{m}^{\prime } \psi_{n}^{(4)} , \\ \end{aligned}$$
(C.7)
$$L_{111} = I_{0} \psi_{n} \phi_{m}^{\prime } , \, L_{112} = - I_{1} \psi_{n} \phi_{m}^{\prime } , \, L_{113} = I_{2} \psi_{n} \phi_{m}^{\prime } ,$$
(C.8)
$$\begin{aligned} L_{21} & = - \frac{1}{2}B_{0} \psi_{n}^{\prime } \phi_{m}^{\prime \prime } - F_{0} \psi_{n}^{\prime } \phi_{m}^{\prime \prime } + C_{0} \phi_{m}^{\prime \prime } \psi_{n}^{(3)} + \frac{2}{15}D_{0} \phi_{m}^{\prime \prime } \psi_{n}^{(3)} - \frac{1}{8}E_{0} \phi_{m}^{\prime \prime } \psi_{n}^{(3)} + C_{0} \psi_{n}^{\prime } \phi_{m}^{(4)} \\ & \quad + \frac{2}{15}D_{0} \psi_{n}^{\prime } \phi_{m}^{(4)} - \frac{1}{8}E_{0} \psi_{n}^{\prime } \phi_{m}^{(4)} , \\ \end{aligned}$$
(C.9)
$$\begin{aligned} L_{22} & = - \frac{1}{2}B_{0} \psi_{n}^{\prime } \phi_{m}^{\prime \prime } - A_{0} \phi_{m} \psi_{n}^{(3)} + C_{0} \phi_{m}^{\prime \prime } \psi_{n}^{(3)} + \frac{2}{3}D_{0} \phi_{m}^{\prime \prime } \psi_{n}^{(3)} + \frac{1}{8}E_{0} \phi_{m}^{\prime \prime } \psi_{n}^{(3)} + \frac{4}{15}D_{0} \psi_{n}^{\prime } \phi_{m}^{(4)} \\ & + \frac{1}{8}E_{0} \psi_{n}^{\prime } \phi_{m}^{(4)} + C_{0} \phi_{m} \psi_{n}^{(5)} + \frac{2}{5}D_{0} \phi_{m} \psi_{n}^{(5)} , \\ \end{aligned}$$
(C.10)
$$\begin{aligned} L_{23} & = B_{1} \psi_{n}^{\prime } \phi_{m}^{\prime \prime } + F_{1} \psi_{n}^{\prime } \phi_{m}^{\prime \prime } + A_{1} \phi_{m} \psi_{n}^{(3)} - 2C_{1} \phi_{m}^{\prime \prime } \psi_{n}^{(3)} - \frac{4}{5}D_{1} \phi_{m}^{\prime \prime } \psi_{n}^{(3)} - C_{1} \psi_{n}^{\prime } \phi_{m}^{(4)} - \frac{2}{5}D_{1} \psi_{n}^{\prime } \phi_{m}^{(4)} \\ & - C_{1} \phi_{m} \psi_{n}^{(5)} - \frac{2}{5}D_{1} \phi_{m} \psi_{n}^{(5)} , \\ \end{aligned}$$
(C.11)
$$\begin{aligned} L_{24} & = - \frac{1}{2}B_{0} \psi_{n} \phi_{m}^{\prime 2} \psi_{n}^{\prime } - F_{0} \psi_{n} \phi_{m}^{\prime 2} \psi_{n}^{\prime } - \frac{1}{2}B_{0} \phi_{m} \psi_{n} \psi_{n}^{\prime } \phi_{m}^{\prime \prime } + 2C_{0} \psi_{n} \psi_{n}^{\prime } \phi_{m}^{\prime \prime 2} + \frac{8}{15}D_{0} \psi_{n} \psi_{n}^{\prime } \phi_{m}^{\prime \prime 2} \\ & \quad - A_{0} \phi_{m}^{2} \psi_{n}^{\prime } \psi_{n}^{\prime \prime } + 5C_{0} \phi_{m}^{\prime 2} \psi_{n}^{\prime } \psi_{n}^{\prime \prime } + \frac{16}{{15}}D_{0} \phi_{m}^{\prime 2} \psi_{n}^{\prime } \psi_{n}^{\prime \prime } + 2C_{0} \phi_{m} \psi_{n}^{\prime } \phi_{m}^{\prime \prime } \psi_{n}^{\prime \prime } + \frac{5}{3}D_{0} \phi_{m} \psi_{n}^{\prime } \phi_{m}^{\prime \prime } \psi_{n}^{\prime \prime } \\ & \quad + 2C_{0} \psi_{n} \phi_{m}^{\prime } \psi_{n}^{\prime } \phi_{m}^{(3)} + \frac{4}{5}D_{0} \psi_{n} \phi_{m}^{\prime } \psi_{n}^{\prime } \phi_{m}^{(3)} + C_{0} \psi_{n} \phi_{m}^{\prime 2} \psi_{n}^{(3)} + \frac{2}{15}D_{0} \psi_{n} \phi_{m}^{\prime 2} 2\psi_{n}^{(3)} + \frac{1}{3}D_{0} \phi_{m} \psi_{n} \phi_{m}^{\prime \prime } \psi_{n}^{(3)} \\ & \quad + 3C_{0} \phi_{m}^{2} \psi_{n}^{\prime \prime } \psi_{n}^{(3)} + \frac{6}{5}D_{0} \phi_{m}^{2} \psi_{n}^{\prime \prime } \psi_{n}^{(3)} + \frac{4}{15}D_{0} \phi_{m} \psi_{n} \psi_{n}^{\prime } \phi_{m}^{(4)} + C_{0} \phi_{m}^{2} \psi_{n}^{\prime } \psi_{n}^{(4)} + \frac{2}{5}D_{0} \phi_{m}^{2} \psi_{n}^{\prime } \psi_{n}^{(4)} , \\ \end{aligned}$$
(C.12)
$$\begin{aligned} L_{25} & = - \frac{1}{4}B_{1} \psi_{n}^{\prime } \phi_{m}^{\prime \prime } + \frac{{5B_{3} \psi_{n}^{\prime } \phi_{m}^{\prime \prime } }}{{3h^{2} }} + \frac{{2D_{1} \psi_{n}^{\prime } \phi_{m}^{\prime \prime } }}{{h^{2} }} - \frac{1}{4}F_{1} \psi_{n}^{\prime } \phi_{m}^{\prime \prime } + \frac{{5F_{3} \psi_{n}^{\prime } \phi_{m}^{\prime \prime } }}{{3h^{2} }} - \frac{1}{4}A_{1} \phi_{m} \psi_{n}^{(3)} \\ & \quad + \frac{{5A_{3} \phi_{m} \psi_{n}^{(3)} }}{{3h^{2} }} + \frac{{2D_{1} \phi_{m} \psi_{n}^{(3)} }}{{h^{2} }} + \frac{1}{2}C_{1} \phi_{m}^{\prime \prime } \psi_{n}^{(3)} - \frac{{10C_{3} \phi_{m}^{\prime \prime } \psi_{n}^{(3)} }}{{3h^{2} }} + \frac{1}{5}D_{1} \phi_{m}^{\prime \prime } \psi_{n}^{(3)} - \frac{{4D_{3} \phi_{m}^{\prime \prime } \psi_{n}^{(3)} }}{{3h^{2} }} \\ & \quad + \frac{1}{4}C_{1} \psi_{n}^{\prime } \phi_{m}^{(4)} - \frac{{5C_{3} \psi_{n}^{\prime } \phi_{m}^{(4)} }}{{3h^{2} }} + \frac{1}{10}D_{1} \psi_{n}^{\prime } \phi_{m}^{(4)} - \frac{{2D_{3} \psi_{n}^{\prime } \phi_{m}^{(4)} }}{{3h^{2} }} + \frac{1}{4}C_{1} \phi_{m} \psi_{n}^{(5)} - \frac{{5C_{3} \phi_{m} \psi_{n}^{(5)} }}{{3h^{2} }} \\ & \quad + \frac{1}{10}D_{1} \phi_{m} \psi_{n}^{(5)} - \frac{{2D_{3} \phi_{m} \psi_{n}^{(5)} }}{{3h^{2} }}, \\ \end{aligned}$$
(C.13)
$$\begin{aligned} L_{26} & = - B_{0} \psi_{n} \phi_{m}^{\prime 2} \psi_{n}^{\prime } - 2F_{0} \psi_{n} \phi_{m}^{\prime 2} \psi_{n}^{\prime } - B_{0} \phi_{m} \psi_{n} \psi_{n}^{\prime } \phi_{m}^{\prime \prime } + 4C_{0} \psi_{n} \psi_{n}^{\prime } \phi_{m}^{\prime \prime 2} + \frac{16}{{15}}D_{0} \psi_{n} \psi_{n}^{\prime } \phi_{m}^{\prime \prime 2} \\ & \quad - 2A_{0} \phi_{m}^{2} \psi_{n}^{\prime } \psi_{n}^{\prime \prime } + 10C_{0} \phi_{m}^{\prime 2} \psi_{n}^{\prime } \psi_{n}^{\prime \prime } + \frac{32}{{15}}D_{0} \phi_{m}^{\prime 2} \psi_{n}^{\prime } \psi_{n}^{\prime \prime } + 4C_{0} \phi_{m} \psi_{n}^{\prime } \phi_{m}^{\prime \prime } \psi_{n}^{\prime \prime } + \frac{10}{3}D_{0} \phi_{m} \psi_{n}^{\prime } \phi_{m}^{\prime \prime } \psi_{n}^{\prime \prime } \\ & \quad + 4C_{0} \psi_{n} \phi_{m}^{\prime } \psi_{n}^{\prime } \phi_{m}^{(3)} + \frac{8}{5}D_{0} \psi_{n} \phi_{m}^{\prime } \psi_{n}^{\prime } \phi_{m}^{(3)} + 2C_{0} \psi_{n} \phi_{m}^{\prime 2} \psi_{n}^{(3)} + \frac{4}{15}D_{0} \psi_{n} \phi_{m}^{\prime 2} \psi_{n}^{(3)} + \frac{2}{3}D_{0} \phi_{m} \psi_{n} \phi_{m}^{\prime \prime } \psi_{n}^{(3)} \\ & \quad + 6C_{0} \phi_{m}^{2} \psi_{n}^{\prime \prime } \psi_{n}^{(3)} + \frac{12}{5}D_{0} \phi_{m}^{2} \psi_{n}^{\prime \prime } \psi_{n}^{(3)} + \frac{8}{15}D_{0} \phi_{m} \psi_{n} \psi_{n}^{\prime } \phi_{m}^{(4)} + 2C_{0} \phi_{m}^{2} \psi_{n}^{\prime } \psi_{n}^{(4)} + \frac{4}{5}D_{0} \phi_{m}^{2} \psi_{n}^{\prime } \psi_{n}^{(4)} , \\ \end{aligned}$$
(C.14)
$$\begin{aligned} L_{27} & = - \frac{1}{2}B_{0} \psi_{n} \phi_{m}^{\prime 2} \psi_{n}^{\prime } - F_{0} \psi_{n} \phi_{m}^{\prime 2} \psi_{n}^{\prime } - \frac{1}{2}B_{0} \phi_{m} \psi_{n} \psi_{n}^{\prime } \phi_{m}^{\prime \prime } + 2C_{0} \psi_{n} \psi_{n}^{\prime } \phi_{m}^{\prime 2} + \frac{8}{15}D_{0} \psi_{n} \psi_{n}^{\prime } \phi_{m}^{\prime 2} \\ & \quad - A_{0} \phi_{m}^{2} \psi_{n}^{\prime } \psi_{n}^{\prime \prime } + 5C_{0} \phi_{m}^{\prime 2} \psi_{n}^{\prime } \psi_{n}^{\prime \prime } + \frac{16}{{15}}D_{0} \phi_{m}^{\prime 2} \psi_{n}^{\prime } \psi_{n}^{\prime \prime } + 2C_{0} \phi_{m} \psi_{n}^{\prime } \phi_{m}^{\prime \prime } \psi_{n}^{\prime \prime } + \frac{5}{3}D_{0} \phi_{m} \psi_{n}^{\prime } \phi_{m}^{\prime \prime } \psi_{n}^{\prime \prime } \\ & \quad + 2C_{0} \psi_{n} \phi_{m}^{\prime } \psi_{n}^{\prime } \phi_{m}^{(3)} + \frac{4}{5}D_{0} \psi_{n} \phi_{m}^{\prime } \psi_{n}^{\prime } \phi_{m}^{(3)} + C_{0} \psi_{n} \phi_{m}^{\prime 2} \psi_{n}^{(3)} + \frac{2}{15}D_{0} \psi_{n} \phi_{m}^{\prime 2} \psi_{n}^{(3)} + \frac{1}{3}D_{0} \phi_{m} \psi_{n} \phi_{m}^{\prime \prime } \psi_{n}^{(3)} \\ & \quad + 3C_{0} \phi_{m}^{2} \psi_{n}^{\prime \prime } \psi_{n}^{(3)} + \frac{6}{5}D_{0} \phi_{m}^{2} \psi_{n}^{\prime \prime } \psi_{n}^{(3)} + \frac{4}{15}D_{0} \phi_{m} \psi_{n} \psi_{n}^{\prime } \phi_{m}^{(4)} + C_{0} \phi_{m}^{2} \psi_{n}^{\prime } \psi_{n}^{(4)} + \frac{2}{5}D_{0} \phi_{m}^{2} \psi_{n}^{\prime } \psi_{n}^{(4)} , \\ \end{aligned}$$
(C.15)
$$L_{211} = I_{0} \phi_{m} \psi_{n}^{\prime } , \, L_{212} = - I_{1} \phi_{m} \psi_{n}^{\prime } , \, L_{213} = I_{2} \phi_{m} \psi_{n}^{\prime } ,$$
(C.16)
$$\begin{aligned} L_{31} & = - B_{1} \phi_{m}^{\prime \prime } \psi_{n}^{\prime \prime } - F_{1} \phi_{m}^{\prime \prime } \psi_{n}^{\prime \prime } - A_{1} \psi_{n} \phi_{m}^{(4)} + 2C_{1} \psi_{n}^{\prime \prime } \phi_{m}^{(4)} + \frac{4}{5}D_{1} \psi_{n}^{\prime \prime } \phi_{m}^{(4)} + C_{1} \phi_{m}^{\prime \prime } \psi_{n}^{(4)} \\ & \quad + \frac{2}{5}D_{1} \phi_{m}^{\prime \prime } \psi_{n}^{(4)} + C_{1} \psi_{n} \phi_{m}^{(6)} + \frac{2}{5}D_{1} \psi_{n} \phi_{m}^{(6)} , \\ \end{aligned}$$
(C.17)
$$\begin{aligned} L_{32} & = - B_{1} \phi_{m}^{\prime \prime } \psi_{n}^{\prime \prime } - F_{1} \phi_{m}^{\prime \prime } \psi_{n}^{\prime \prime } + C_{1} \psi_{n}^{\prime \prime } \phi_{m}^{(4)} + \frac{2}{5}D_{1} \psi_{n}^{\prime \prime } \phi_{m}^{(4)} - A_{1} \phi_{m} \psi_{n}^{(4)} + 2C_{1} \phi_{m}^{\prime \prime } \psi_{n}^{(4)} \\ & \quad + \frac{4}{5}D_{1} \phi_{m}^{\prime \prime } \psi_{n}^{(4)} + C_{1} \phi_{m} \psi_{n}^{(6)} + \frac{2}{5}D_{1} \phi_{m} \psi_{n}^{(6)} , \\ \end{aligned}$$
(C.18)
$$\begin{aligned} L_{33} & = k_{w} \phi_{m} \psi_{n} - k_{p} \psi_{n} \phi_{m}^{\prime \prime } - k_{p} \phi_{m} \psi_{n}^{\prime \prime } + 2B_{2} \phi_{m}^{\prime \prime } \psi_{n}^{\prime \prime } + 2C_{0} \phi_{m}^{\prime \prime } \psi_{n}^{\prime \prime } + \frac{8}{15}D_{0} \phi_{m}^{\prime \prime } \psi_{n}^{\prime \prime } + E_{0} \phi_{m}^{\prime \prime } \psi_{n}^{\prime \prime } \\ & \quad + 2F_{2} \phi_{m}^{\prime \prime } \psi_{n}^{\prime \prime } + A_{2} \psi_{n} \phi_{m}^{(4)} + C_{0} \psi_{n} \phi_{m}^{(4)} + \frac{4}{15}D_{0} \psi_{n} \phi_{m}^{(4)} + \frac{1}{2}E_{0} \psi_{n} \phi_{m}^{(4)} - 3C_{2} \psi_{n}^{\prime \prime } \phi_{m}^{(4)} \\ & \quad - \frac{6}{5}D_{2} \psi_{n}^{\prime \prime } \phi_{m}^{(4)} + A_{2} \phi_{m} \psi_{n}^{(4)} + C_{0} \phi_{m} \psi_{n}^{(4)} + \frac{4}{15}D_{0} \phi_{m} \psi_{n}^{(4)} + \frac{1}{2}E_{0} \phi_{m} \psi_{n}^{(4)} - 3C_{2} \phi_{m}^{\prime \prime } \psi_{n}^{(4)} \\ & \quad - \frac{6}{5}D_{2} \phi_{m}^{\prime \prime } \psi_{n}^{(4)} - C_{2} \psi_{n} \phi_{m}^{(6)} - \frac{2}{5}D_{2} \psi_{n} \phi_{m}^{(6)} - C_{2} \phi_{m} \psi_{n}^{(6)} - \frac{2}{5}D_{2} \phi_{m} \psi_{n}^{(6)} , \\ \end{aligned}$$
(C.19)
$$L_{34} = - B_{0} \phi_{m}^{\prime 2} \psi_{n}^{\prime 2} - A_{0} \psi_{n}^{2} \phi_{m}^{\prime \prime 2} - F_{0} \phi_{m} \psi_{n} \phi_{m}^{\prime \prime } \psi_{n}^{\prime \prime } ,$$
(C.20)
$$L_{35} = - B_{0} \phi_{m}^{\prime 2} \psi_{n}^{\prime 2} - F_{0} \phi_{m} \psi_{n} \phi_{m}^{\prime \prime } \psi_{n}^{\prime \prime } - A_{0} \phi_{m}^{2} \psi_{n}^{\prime \prime 2} ,$$
(C.21)
$$\begin{aligned} L_{{36}} & = B_{1} \phi _{m} ^{{\prime 2}} \psi _{n} ^{{\prime 2}} - 2F_{1} \phi _{m} ^{{\prime 2}} \psi _{n} ^{{\prime 2}} - B_{1} \phi _{m} \psi _{n} ^{{\prime 2}} \phi _{m} ^{{\prime \prime }} - F_{1} \phi _{m} \psi _{n} ^{{\prime 2}} \phi _{m} ^{{\prime \prime }} + 7C_{1} \psi _{n} ^{{\prime 2}} \phi _{m} ^{{\prime 2}} + \frac{8}{5}D_{1} \psi _{n} ^{{\prime 2}} \phi _{m} ^{{\prime 2}} \\ & \quad - B_{1} \psi _{n} \phi _{m} ^{{\prime 2}} \psi _{n} ^{{\prime \prime }} - F_{1} \psi _{n} \phi _{m} ^{{\prime 2}} \psi _{n} ^{{\prime \prime }} - B_{1} \phi _{m} \psi _{n} \phi _{m} ^{{\prime \prime }} \psi _{n} ^{{\prime \prime }} + 2F_{1} \phi _{m} \psi _{n} \phi _{m} ^{{\prime \prime }} \psi _{n} ^{{\prime \prime }} + 4C_{1} \psi _{n} \phi _{m} ^{{\prime \prime 2}} \psi _{n} ^{{\prime \prime }} \\ & \quad + \frac{{11}}{5}D_{1} \psi _{n} \phi _{m} ^{{\prime \prime 2}} \psi _{n} ^{{\prime \prime }} + 7C_{1} \phi _{m} ^{{\prime 2}} \psi _{n} ^{{\prime \prime 2}} + \frac{8}{5}D_{1} \phi _{m} ^{{\prime 2}} \psi _{n} ^{{\prime \prime 2}} + 4C_{1} \phi _{m} \phi _{m} ^{{\prime \prime }} \psi _{n} ^{{\prime \prime 2}} + \frac{{11}}{5}D_{1} \phi _{m} \phi _{m} ^{{\prime \prime }} \psi _{n} ^{{\prime \prime 2}} \\ & \quad - A_{1} \psi _{n} ^{2} \phi _{m} ^{\prime } \phi _{m} ^{{(3)}} + 8C_{1} \phi _{m} ^{\prime } \psi _{n} ^{{\prime 2}} \phi _{m} ^{{(3)}} + 2D_{1} \phi _{m} ^{\prime } \psi _{n} ^{{\prime 2}} \phi _{m} ^{{(3)}} + 4C_{1} \psi _{n} \phi _{m} ^{\prime } \psi _{n} ^{{\prime \prime }} \phi _{m} ^{{(3)}} + \frac{{14}}{5}D_{1} \psi _{n} \phi _{m} ^{\prime } \psi _{n} ^{{\prime \prime }} \phi _{m} ^{{(3)}} \\ & \quad + 3C_{1} \psi _{n} ^{2} \phi _{m} ^{{(3)2}} + \frac{6}{5}D_{1} \psi _{n} ^{2} \phi _{m} ^{{(3)2}} - A_{1} \phi _{m} ^{2} \psi _{n} ^{\prime } \psi _{n} ^{{(3)}} + 8C_{1} \phi _{m} ^{{\prime 2}} \psi _{n} ^{\prime } \psi _{n} ^{{(3)}} + 2D_{1} \phi _{m} ^{{\prime 2}} \psi _{n} ^{\prime } \psi _{n} ^{{(3)}} \\ & \quad + 4C_{1} \phi _{m} \psi _{n} ^{\prime } \phi _{m} ^{{\prime \prime }} \psi _{n} ^{{(3)}} + \frac{{14}}{5}D_{1} \phi _{m} \psi _{n} ^{\prime } \phi _{m} ^{{\prime \prime }} \psi _{n} ^{{(3)}} + 3C_{1} \phi _{m} ^{2} \psi _{n} ^{{(3)2}} + \frac{6}{5}D_{1} \phi _{m} ^{2} \psi _{n} ^{{(3)2}} + C_{1} \phi _{m} \psi _{n} ^{{\prime 2}} \phi _{m} ^{{(4)}} \\ & \quad + \frac{2}{5}D_{1} \phi _{m} \psi _{n} ^{{\prime 2}} \phi _{m} ^{{(4)}} + 4C_{1} \psi _{n} ^{2} \phi _{m} ^{{\prime \prime }} \phi _{m} ^{{(4)}} + \frac{8}{5}D_{1} \psi _{n} ^{2} \phi _{m} ^{{\prime \prime }} \phi _{m} ^{{(4)}} + \frac{3}{5}D_{1} \phi _{m} \psi _{n} \psi _{n} ^{{\prime \prime }} \phi _{m} ^{{(4)}} + C_{1} \psi _{n} \phi _{m} ^{{\prime 2}} \psi _{n} ^{{(4)}} \\ & \quad + \frac{2}{5}D_{1} \psi _{n} \phi _{m} ^{{\prime 2}} \psi _{n} ^{{(4)}} + \frac{3}{5}D_{1} \phi _{m} \psi _{n} \phi _{m} ^{{\prime \prime }} \psi _{n} ^{{(4)}} + 4C_{1} \phi _{m} ^{2} \psi _{n} ^{{\prime \prime }} \psi _{n} ^{{(4)}} + \frac{8}{5}D_{1} \phi _{m} ^{2} \psi _{n} ^{{\prime \prime }} \psi _{n} ^{{(4)}} + C_{1} \psi _{n} ^{2} \phi _{m} ^{\prime } \phi _{m} ^{{(5)}} \\ & \quad + \frac{2}{5}D_{1} \psi _{n} ^{2} \phi _{m} ^{\prime } \phi _{m} ^{{(5)}} + C_{1} \phi _{m} ^{2} \psi _{n} ^{\prime } \psi _{n} ^{{(5)}} + \frac{2}{5}D_{1} \phi _{m} ^{2} \psi _{n} ^{\prime } \psi _{n} ^{{(5)}} , \\ \end{aligned}$$
(C.22)
$$\begin{aligned} L_{37} & = - B_{0} \phi_{m} \psi_{n} \phi_{m}^{\prime 2} \psi_{n}^{\prime 2} - \frac{1}{2}A_{0} \psi_{n}^{3} \phi_{m}^{\prime 2} \phi_{m}^{\prime \prime } - \frac{1}{2}F_{0} \phi_{m}^{2} \psi_{n} \psi_{n}^{\prime 2} \phi_{m}^{\prime \prime } - \frac{1}{2}F_{0} \phi_{m} \psi_{n}^{2} \phi_{m}^{\prime 2} \psi_{n}^{\prime \prime } \\ & \quad - \frac{1}{2}A_{0} \phi_{m}^{3} \psi_{n}^{\prime 2} \psi_{n}^{\prime \prime } , \\ \end{aligned}$$
(C.23)
$$\begin{aligned} L_{38} & = k_{w} \phi_{m} \psi_{n} - k_{p} \psi_{n} \phi_{m}^{\prime \prime } - \frac{1}{2}B_{2} \phi_{m}^{\prime \prime } \psi_{n}^{\prime \prime } + \frac{{10B_{4} \phi_{m}^{\prime \prime } \psi_{n}^{\prime \prime } }}{{3h^{2} }} - \frac{1}{2}C_{0} \phi_{m}^{\prime \prime } \psi_{n}^{\prime \prime } + \frac{{10C_{2} \phi_{m}^{\prime \prime } \psi_{n}^{\prime \prime } }}{{h^{2} }} \\ & \quad - \frac{4}{5}D_{0} \phi_{m}^{\prime \prime } \psi_{n}^{\prime \prime } + \frac{{28D_{2} \phi_{m}^{\prime \prime } \psi_{n}^{\prime \prime } }}{{3h^{2} }} + \frac{3}{8}E_{0} \phi_{m}^{\prime \prime } \psi_{n}^{\prime \prime } + \frac{{5E_{2} \phi_{m}^{\prime \prime } \psi_{n}^{\prime \prime } }}{{2h^{2} }} - \frac{1}{2}F_{2} \phi_{m}^{\prime \prime } \psi_{n}^{\prime \prime } + \frac{{10F_{4} \phi_{m}^{\prime \prime } \psi_{n}^{\prime \prime } }}{{3h^{2} }} \\ & \quad - \frac{1}{4}A_{2} \psi_{n} \phi_{m}^{(4)} + \frac{{5A_{4} \psi_{n} \phi_{m}^{(4)} }}{{3h^{2} }} - \frac{1}{4}C_{0} \psi_{n} \phi_{m}^{(4)} + \frac{{5C_{2} \psi_{n} \phi_{m}^{(4)} }}{{h^{2} }} - \frac{2}{5}D_{0} \psi_{n} \phi_{m}^{(4)} + \frac{{14D_{2} \psi_{n} \phi_{m}^{(4)} }}{{3h^{2} }} \\ & \quad + \frac{3}{16}E_{0} \psi_{n} \phi_{m}^{(4)} + \frac{{5E_{2} \psi_{n} \phi_{m}^{(4)} }}{{4h^{2} }} + \frac{3}{4}C_{2} \psi_{n}^{\prime \prime } \phi_{m}^{(4)} - \frac{{5C_{4} \psi_{n}^{\prime \prime } \phi_{m}^{(4)} }}{{h^{2} }} + \frac{3}{10}D_{2} \psi_{n}^{\prime \prime } \phi_{m}^{(4)} - \frac{{2D_{4} \psi_{n}^{\prime \prime } \phi_{m}^{(4)} }}{{h^{2} }} \\ & \quad - \frac{1}{4}A_{2} \phi_{m} \psi_{n}^{(4)} + \frac{{5A_{4} \phi_{m} \psi_{n}^{(4)} }}{{3h^{2} }} - \frac{1}{4}C_{0} \phi_{m} \psi_{n}^{(4)} + \frac{{5C_{2} \phi_{m} \psi_{n}^{(4)} }}{{h^{2} }} - \frac{2}{5}D_{0} \phi_{m} \psi_{n}^{(4)} + \frac{{14D_{2} \phi_{m} \psi_{n}^{(4)} }}{{3h^{2} }} \\ & \quad + \frac{3}{16}E_{0} \phi_{m} \psi_{n}^{(4)} + \frac{{5E_{2} \phi_{m} \psi_{n}^{(4)} }}{{4h^{2} }} + \frac{3}{4}C_{2} \phi_{m}^{\prime \prime } \psi_{n}^{(4)} - \frac{{5C_{4} \phi_{m}^{\prime \prime } \psi_{n}^{(4)} }}{{h^{2} }} + \frac{3}{10}D_{2} \phi_{m}^{\prime \prime } \psi_{n}^{(4)} - \frac{{2D_{4} \phi_{m}^{\prime \prime } \psi_{n}^{(4)} }}{{h^{2} }} \\ & \quad + \frac{1}{4}C_{2} \psi_{n} \phi_{m}^{(6)} - \frac{{5C_{4} \psi_{n} \phi_{m}^{(6)} }}{{3h^{2} }} + \frac{1}{10}D_{2} \psi_{n} \phi_{m}^{(6)} - \frac{{2D_{4} \psi_{n} \phi_{m}^{(6)} }}{{3h^{2} }} + \frac{1}{4}C_{2} \phi_{m} \psi_{n}^{(6)} - \frac{{5C_{4} \phi_{m} \psi_{n}^{(6)} }}{{3h^{2} }} \\ & \quad + \frac{1}{10}D_{2} \phi_{m} \psi_{n}^{(6)} - \frac{{2D_{4} \phi_{m} \psi_{n}^{(6)} }}{{3h^{2} }} - k_{p} \phi_{m} \psi_{n}^{\prime \prime } , \\ \end{aligned}$$
(C.24)
$$L_{39} = - B_{0} \phi_{m}^{\prime 2} \psi_{n}^{\prime 2} - A_{0} \psi_{n}^{2} \phi_{m}^{\prime \prime 2} - F_{0} \phi_{m} \psi_{n} \phi_{m}^{\prime \prime } \psi_{n}^{\prime \prime } ,$$
(C.25)
$$L_{390} = - B_{0} \phi_{m}^{\prime 2} \psi_{n}^{\prime 2} - F_{0} \phi_{m} \psi_{n} \phi_{m}^{\prime \prime } \psi_{n}^{\prime \prime } - A_{0} \phi_{m}^{2} \psi_{n}^{\prime \prime 2},$$
(C.26)
$$\begin{aligned} L_{391} & = - \frac{1}{2}B_{1} \phi_{m}^{\prime 2} \psi_{n}^{\prime 2} + \frac{{10B_{3} \phi_{m}^{\prime 2} \psi_{n}^{\prime 2} }}{{3h^{2} }} - 4F_{1} \phi_{m}^{\prime 2} \psi_{n}^{\prime 2} - 2B_{1} \phi_{m} \psi_{n}^{\prime 2} \phi_{m}^{\prime \prime } - 2F_{1} \phi_{m} \psi_{n}^{\prime 2} \phi_{m}^{\prime \prime } \\ & \quad - \frac{5}{4}A_{1} \psi_{n}^{2} \phi_{m}^{\prime \prime 2} + \frac{{5A_{3} \psi_{n}^{2} \phi_{m}^{\prime \prime 2} }}{{3h^{2} }} + 14C_{1} \psi_{n}^{\prime 2} \phi_{m}^{\prime \prime 2} + \frac{16}{5}D_{1} \psi_{n}^{\prime 2} \phi_{m}^{\prime \prime 2} - 2B_{1} \psi_{n} \phi_{m}^{\prime 2} \psi_{n}^{\prime \prime } \\ & \quad - 2F_{1} \psi_{n} \phi_{m}^{\prime 2} \psi_{n}^{\prime \prime } - 2B_{1} \phi_{m} \psi_{n} \phi_{m}^{\prime \prime } \psi_{n}^{\prime \prime } + \frac{3}{2}F_{1} \phi_{m} \psi_{n} \phi_{m}^{\prime \prime } \psi_{n}^{\prime \prime } + \frac{{10F_{3} \phi_{m} \psi_{n} \phi_{m}^{\prime \prime } \psi_{n}^{\prime \prime } }}{{3h^{2} }} + 8C_{1} \psi_{n} \phi_{m}^{\prime \prime 2} \psi_{n}^{\prime \prime } \\ & \quad + \frac{22}{5}D_{1} \psi_{n} \phi_{m}^{\prime \prime 2} \psi_{n}^{\prime \prime } - \frac{5}{4}A_{1} \phi_{m}^{2} \psi_{n}^{\prime \prime 2} + \frac{{5A_{3} \phi_{m}^{2} \psi_{n}^{\prime \prime 2} }}{{3h^{2} }} + 14C_{1} \phi_{m}^{\prime 2} \psi_{n}^{\prime \prime 2} + \frac{16}{5}D_{1} \phi_{m}^{\prime 2} \psi_{n}^{\prime \prime 2} + 8C_{1} \phi_{m} \phi_{m}^{\prime \prime } \psi_{n}^{\prime \prime 2} \\ & \quad + \frac{22}{5}D_{1} \phi_{m} \phi_{m}^{\prime \prime } \psi_{n}^{\prime \prime 2} - 2A_{1} \psi_{n}^{2} \phi_{m}^{\prime } \phi_{m}^{(3)} + 16C_{1} \phi_{m}^{\prime } \psi_{n}^{\prime 2} \phi_{m}^{(3)} + 4D_{1} \phi_{m}^{\prime } \psi_{n}^{\prime 2} \phi_{m}^{(3)} + 8C_{1} \psi_{n} \phi_{m}^{\prime } \psi_{n}^{\prime \prime } \phi_{m}^{(3)} \\ & \quad + \frac{28}{5}D_{1} \psi_{n} \phi_{m}^{\prime } \psi_{n}^{\prime \prime } \phi_{m}^{(3)} + 6C_{1} \psi_{n}^{2} \phi_{m}^{(3)2} + \frac{12}{5}D_{1} \psi_{n}^{2} \phi_{m}^{(3)2} - 2A_{1} \phi_{m}^{2} \psi_{n}^{\prime } \psi_{n}^{(3)} + 16C_{1} \phi_{m}^{\prime 2} \psi_{n}^{\prime } \psi_{n}^{(3)} \\ & \quad + 4D_{1} \phi_{m}^{\prime 2} \psi_{n}^{\prime } \psi_{n}^{(3)} + 8C_{1} \phi_{m} \psi_{n}^{\prime } \phi_{m}^{\prime \prime } \psi_{n}^{(3)} + \frac{28}{5}D_{1} \phi_{m} \psi_{n}^{\prime } \phi_{m}^{\prime \prime } \psi_{n}^{(3)} + 6C_{1} \phi_{m}^{2} \psi_{n}^{(3)2} + \frac{12}{5}D_{1} \phi_{m}^{2} \psi_{n}^{(3)2} \\ & \quad + 2C_{1} \phi_{m} \psi_{n}^{\prime 2} \phi_{m}^{(4)} + \frac{4}{5}D_{1} \phi_{m} \psi_{n}^{\prime 2} \phi_{m}^{(4)} + 8C_{1} \psi_{n}^{2} \phi_{m}^{\prime \prime } \phi_{m}^{(4)} + \frac{16}{5}D_{1} \psi_{n}^{2} \phi_{m}^{\prime \prime } \phi_{m}^{(4)} + \frac{6}{5}D_{1} \phi_{m} \psi_{n} \psi_{n}^{\prime \prime } \phi_{m}^{(4)} \\ & \quad + 2C_{1} \psi_{n} \phi_{m}^{\prime 2} \psi_{n}^{(4)} + \frac{4}{5}D_{1} \psi_{n} \phi_{m}^{\prime 2} \psi_{n}^{(4)} + \frac{6}{5}D_{1} \phi_{m} \psi_{n} \phi_{m}^{\prime \prime } \psi_{n}^{(4)} + 8C_{1} \phi_{m}^{2} \psi_{n}^{\prime \prime } \psi_{n}^{(4)} + \frac{16}{5}D_{1} \phi_{m}^{2} \psi_{n}^{\prime \prime } \psi_{n}^{(4)} \\ & \quad + 2C_{1} \psi_{n}^{2} \phi_{m}^{\prime } \phi_{m}^{(5)} + \frac{4}{5}D_{1} \psi_{n}^{2} \phi_{m}^{\prime } \phi_{m}^{(5)} + 2C_{1} \phi_{m}^{2} \psi_{n}^{\prime } \psi_{n}^{(5)} + \frac{4}{5}D_{1} \phi_{m}^{2} \psi_{n}^{\prime } \psi_{n}^{(5)} , \\ \end{aligned}$$
(C.27)
$$\begin{aligned} L_{392} & = - 3B_{0} \phi_{m} \psi_{n} \phi_{m}^{\prime 2} \psi_{n}^{\prime 2} - \frac{3}{2}A_{0} \psi_{n}^{3} \phi_{m}^{\prime 2} \phi_{m}^{\prime \prime } - \frac{3}{2}F_{0} \phi_{m}^{2} \psi_{n} \psi_{n}^{\prime 2} \phi_{m}^{\prime \prime } - \frac{3}{2}F_{0} \phi_{m} \psi_{n}^{2} \phi_{m}^{\prime 2} \psi_{n}^{\prime \prime } \\ & \quad - \frac{3}{2}A_{0} \phi_{m}^{3} \psi_{n}^{\prime 2} \psi_{n}^{\prime \prime } , \\ \end{aligned}$$
(C.28)
$$\begin{aligned} L_{393} & = - \frac{3}{2}B_{1} \phi_{m}^{\prime 2} \psi_{n}^{\prime 2} + \frac{{10B_{3} \phi_{m}^{\prime 2} \psi_{n}^{\prime 2} }}{{3h^{2} }} - 2F_{1} \phi_{m}^{\prime 2} \psi_{n}^{\prime 2} - B_{1} \phi_{m} \psi_{n}^{\prime 2} \phi_{m}^{\prime \prime } - F_{1} \phi_{m} \psi_{n}^{\prime 2} \phi_{m}^{\prime \prime } \\ & \quad - \frac{5}{4}A_{1} \psi_{n}^{2} \phi_{m}^{\prime \prime 2} + \frac{{5A_{3} \psi_{n}^{2} \phi_{m}^{\prime \prime 2} }}{{3h^{2} }} + 7C_{1} \psi_{n}^{\prime 2} \phi_{m}^{\prime \prime 2} + \frac{8}{5}D_{1} \psi_{n}^{\prime 2} \phi_{m}^{\prime \prime 2} - B_{1} \psi_{n} \phi_{m}^{\prime 2} \psi_{n}^{\prime \prime } - F_{1} \psi_{n} \phi_{m}^{\prime 2} \psi_{n}^{\prime \prime } \\ & \quad - B_{1} \phi_{m} \psi_{n} \phi_{m}^{\prime \prime } \psi_{n}^{\prime \prime } - \frac{1}{2}F_{1} \phi_{m} \psi_{n} \phi_{m}^{\prime \prime } \psi_{n}^{\prime \prime } + \frac{{10F_{3} \phi_{m} \psi_{n} \phi_{m}^{\prime \prime } \psi_{n}^{\prime \prime } }}{{3h^{2} }} + 4C_{1} \psi_{n} \phi_{m}^{\prime \prime 2} \psi_{n}^{\prime \prime } + \frac{11}{5}D_{1} \psi_{n} \phi_{m}^{\prime \prime 2} \psi_{n}^{\prime \prime } \\ & \quad - \frac{5}{4}A_{1} \phi_{m}^{2} \psi_{n}^{\prime \prime 2} + \frac{{5A_{3} \phi_{m}^{2} \psi_{n}^{\prime \prime 2} }}{{3h^{2} }} + 7C_{1} \phi_{m}^{\prime 2} \psi_{n}^{\prime \prime 2} + \frac{8}{5}D_{1} \phi_{m}^{\prime 2} \psi_{n}^{\prime \prime 2} + 4C_{1} \phi_{m} \phi_{m}^{\prime \prime } \psi_{n}^{\prime \prime 2} + \frac{11}{5}D_{1} \phi_{m} \phi_{m}^{\prime \prime } \psi_{n}^{\prime \prime 2} \\ & \quad - A_{1} \psi_{n}^{2} \phi_{m}^{\prime } \phi_{m}^{(3)} + 8C_{1} \phi_{m}^{\prime } \psi_{n}^{\prime 2} \phi_{m}^{(3)} + 2D_{1} \phi_{m}^{\prime } \psi_{n}^{\prime 2} \phi_{m}^{(3)} + 4C_{1} \psi_{n} \phi_{m}^{\prime } \psi_{n}^{\prime \prime } \phi_{m}^{(3)} + \frac{14}{5}D_{1} \psi_{n} \phi_{m}^{\prime } \psi_{n}^{\prime \prime } \phi_{m}^{(3)} \\ & \quad + 3C_{1} \psi_{n}^{2} \phi_{m}^{(3)2} + \frac{6}{5}D_{1} \psi_{n}^{2} \phi_{m}^{(3)2} - A_{1} \phi_{m}^{2} \psi_{n}^{\prime } \psi_{n}^{(3)} + 8C_{1} \phi_{m}^{\prime 2} \psi_{n}^{\prime } \psi_{n}^{(3)} + 2D_{1} \phi_{m}^{\prime 2} \psi_{n}^{\prime } \psi_{n}^{(3)} \\ & \quad + 4C_{1} \phi_{m} \psi_{n}^{\prime } \phi_{m}^{\prime \prime } \psi_{n}^{(3)} + \frac{14}{5}D_{1} \phi_{m} \psi_{n}^{\prime } \phi_{m}^{\prime \prime } \psi_{n}^{(3)} + 3C_{1} \phi_{m}^{2} \psi_{n}^{(3)2} + \frac{6}{5}D_{1} \phi_{m}^{2} \psi_{n}^{(3)2} + C_{1} \phi_{m} \psi_{n}^{\prime 2} \phi_{m}^{(4)} \\ & \quad c + \frac{2}{5}D_{1} \phi_{m} \psi_{n}^{\prime 2} \phi_{m}^{(4)} + 4C_{1} \psi_{n}^{2} \phi_{m}^{\prime \prime } \phi_{m}^{(4)} + \frac{8}{5}D_{1} \psi_{n}^{2} \phi_{m}^{\prime \prime } \phi_{m}^{(4)} + \frac{3}{5}D_{1} \phi_{m} \psi_{n} \psi_{n}^{\prime \prime } \phi_{m}^{(4)} + C_{1} \psi_{n} \phi_{m}^{\prime 2} \psi_{n}^{(4)} \\ & \quad + \frac{2}{5}D_{1} \psi_{n} \phi_{m}^{\prime 2} \psi_{n}^{(4)} + \frac{3}{5}D_{1} \phi_{m} \psi_{n} \phi_{m}^{\prime \prime } \psi_{n}^{(4)} + 4C_{1} \phi_{m}^{2} \psi_{n}^{\prime \prime } \psi_{n}^{(4)} + \frac{8}{5}D_{1} \phi_{m}^{2} \psi_{n}^{\prime \prime } \psi_{n}^{(4)} \\ & \quad + C_{1} \psi_{n}^{2} \phi_{m}^{\prime } \phi_{m}^{(5)} + \frac{2}{5}D_{1} \psi_{n}^{2} \phi_{m}^{\prime } \phi_{m}^{(5)} + C_{1} \phi_{m}^{2} \psi_{n}^{\prime } \psi_{n}^{(5)} + \frac{2}{5}D_{1} \phi_{m}^{2} \psi_{n}^{\prime } \psi_{n}^{(5)} , \\ \end{aligned}$$
(C.29)
$$\begin{aligned} L_{394} = - 3B_{0} \phi_{m} \psi_{n} \phi_{m}^{\prime 2} \psi_{n}^{\prime 2} - \frac{3}{2}A_{0} \psi_{n}^{3} \phi_{m}^{\prime 2} \phi_{m}^{\prime \prime } - \frac{3}{2}F_{0} \phi_{m}^{2} \psi_{n} \psi_{n}^{\prime 2} \phi_{m}^{\prime \prime } - \frac{3}{2}F_{0} \phi_{m} \psi_{n}^{2} \phi_{m}^{\prime 2} \psi_{n}^{\prime \prime } - \frac{3}{2}A_{0} \phi_{m}^{3} \psi_{n}^{\prime 2} \psi_{n}^{\prime \prime } , \\ \end{aligned}$$
(C.30)
$$\begin{aligned} L_{395} & { = } - B_{0} \phi_{m} \psi_{n} \phi_{m}^{\prime 2} \psi_{n}^{\prime 2} - \frac{1}{2}A_{0} \psi_{n}^{3} \phi_{m}^{\prime 2} \phi_{m}^{\prime \prime } - \frac{1}{2}F_{0} \phi_{m}^{2} \psi_{n} \psi_{n}^{\prime 2} \phi_{m}^{\prime \prime } - \frac{1}{2}F_{0} \phi_{m} \psi_{n}^{2} \phi_{m}^{\prime 2} \psi_{n}^{\prime \prime } \\ & \quad - \frac{1}{2}A_{0} \phi_{m}^{3} \psi_{n}^{\prime 2} \psi_{n}^{\prime \prime } , \\ \end{aligned}$$
(C.31)
$$\begin{gathered} L_{311} = C_{d} I_{0} \phi_{m} \psi_{n} ,L_{312} = C_{d} I_{0} \phi_{m} \psi_{n} ,L_{313} = I_{1} \psi_{n} \phi_{m}^{\prime \prime } ,L_{314} = I_{1} \phi_{m} \psi_{n}^{\prime \prime } , \hfill \\ L_{315} = I_{0} \phi_{m} \psi_{n} - I_{3} \psi_{n} \phi_{m}^{\prime \prime } - I_{3} \phi_{m} \psi_{n}^{\prime \prime } ,L_{316} = I_{0} \phi_{m} \psi_{n} + I_{5} \psi_{n} \phi_{m}^{\prime \prime } + I_{5} \phi_{m} \psi_{n}^{\prime \prime } , \hfill \\ \end{gathered}$$
(C.32)
$$\begin{aligned} L_{41} & = \frac{1}{4}B_{1} \phi_{m}^{\prime \prime } \psi_{n}^{\prime \prime } - \frac{{5B_{3} \phi_{m}^{\prime \prime } \psi_{n}^{\prime \prime } }}{{3h^{2} }} - \frac{{2D_{1} \phi_{m}^{\prime \prime } \psi_{n}^{\prime \prime } }}{{h^{2} }} + \frac{1}{4}F_{1} \phi_{m}^{\prime \prime } \psi_{n}^{\prime \prime } - \frac{{5F_{3} \phi_{m}^{\prime \prime } \psi_{n}^{\prime \prime } }}{{3h^{2} }} + \frac{1}{4}A_{1} \psi_{n} \phi_{m}^{(4)} \\ & \quad - \frac{{5A_{3} \psi_{n} \phi_{m}^{(4)} }}{{3h^{2} }} - \frac{{2D_{1} \psi_{n} \phi_{m}^{(4)} }}{{h^{2} }} - \frac{1}{2}C_{1} \psi_{n}^{\prime \prime } \phi_{m}^{(4)} + \frac{{10C_{3} \psi_{n}^{\prime \prime } \phi_{m}^{(4)} }}{{3h^{2} }} - \frac{1}{5}D_{1} \psi_{n}^{\prime \prime } \phi_{m}^{(4)} + \frac{{4D_{3} \psi_{n}^{\prime \prime } \phi_{m}^{(4)} }}{{3h^{2} }} \\ & \quad - \frac{1}{4}C_{1} \phi_{m}^{\prime \prime } \psi_{n}^{(4)} + \frac{{5C_{3} \phi_{m}^{\prime \prime } \psi_{n}^{(4)} }}{{3h^{2} }} - \frac{1}{10}D_{1} \phi_{m}^{\prime \prime } \psi_{n}^{(4)} + \frac{{2D_{3} \phi_{m}^{\prime \prime } \psi_{n}^{(4)} }}{{3h^{2} }} - \frac{1}{4}C_{1} \psi_{n} \phi_{m}^{(6)} + \frac{{5C_{3} \psi_{n} \phi_{m}^{(6)} }}{{3h^{2} }} \\ & \quad - \frac{1}{10}D_{1} \psi_{n} \phi_{m}^{(6)} + \frac{{2D_{3} \psi_{n} \phi_{m}^{(6)} }}{{3h^{2} }}, \\ \end{aligned}$$
(C.33)
$$\begin{aligned} L_{42} & = \frac{1}{4}B_{1} \phi_{m}^{\prime \prime } \psi_{n}^{\prime \prime } - \frac{{5B_{3} \phi_{m}^{\prime \prime } \psi_{n}^{\prime \prime } }}{{3h^{2} }} - \frac{{2D_{1} \phi_{m}^{\prime \prime } \psi_{n}^{\prime \prime } }}{{h^{2} }} + \frac{1}{4}F_{1} \phi_{m}^{\prime \prime } \psi_{n}^{\prime \prime } - \frac{{5F_{3} \phi_{m}^{\prime \prime } \psi_{n}^{\prime \prime } }}{{3h^{2} }} - \frac{1}{4}C_{1} \psi_{n}^{\prime \prime } \phi_{m}^{(4)} \\ & \quad + \frac{{5C_{3} \psi_{n}^{\prime \prime } \phi_{m}^{(4)} }}{{3h^{2} }} - \frac{1}{10}D_{1} \psi_{n}^{\prime \prime } \phi_{m}^{(4)} + \frac{{2D_{3} \psi_{n}^{\prime \prime } \phi_{m}^{(4)} }}{{3h^{2} }} + \frac{1}{4}A_{1} \phi_{m} \psi_{n}^{(4)} - \frac{{5A_{3} \phi_{m} \psi_{n}^{(4)} }}{{3h^{2} }} - \frac{{2D_{1} \phi_{m} \psi_{n}^{(4)} }}{{h^{2} }} \\ & \quad - \frac{1}{2}C_{1} \phi_{m}^{\prime \prime } \psi_{n}^{(4)} + \frac{{10C_{3} \phi_{m}^{\prime \prime } \psi_{n}^{(4)} }}{{3h^{2} }} - \frac{1}{5}D_{1} \phi_{m}^{\prime \prime } \psi_{n}^{(4)} + \frac{{4D_{3} \phi_{m}^{\prime \prime } \psi_{n}^{(4)} }}{{3h^{2} }} - \frac{1}{4}C_{1} \phi_{m} \psi_{n}^{(6)} + \frac{{5C_{3} \phi_{m} \psi_{n}^{(6)} }}{{3h^{2} }} \\ & \quad - \frac{1}{10}D_{1} \phi_{m} \psi_{n}^{(6)} + \frac{{2D_{3} \phi_{m} \psi_{n}^{(6)} }}{{3h^{2} }}, \\ \end{aligned}$$
(C.34)
$$\begin{aligned} L_{43} & = k_{w} \phi_{m} \psi_{n} - k_{p} \psi_{n} \phi_{m}^{\prime \prime } - k_{p} \phi_{m} \psi_{n}^{\prime \prime } - \frac{1}{2}B_{2} \phi_{m}^{\prime \prime } \psi_{n}^{\prime \prime } + \frac{{10B_{4} \phi_{m}^{\prime \prime } \psi_{n}^{\prime \prime } }}{{3h^{2} }} - \frac{1}{2}C_{0} \phi_{m}^{\prime \prime } \psi_{n}^{\prime \prime } + \frac{{10C_{2} \phi_{m}^{\prime \prime } \psi_{n}^{\prime \prime } }}{{h^{2} }} \\ & \quad - \frac{4}{5}D_{0} \phi_{m}^{\prime \prime } \psi_{n}^{\prime \prime } + \frac{{28D_{2} \phi_{m}^{\prime \prime } \psi_{n}^{\prime \prime } }}{{3h^{2} }} + \frac{3}{8}E_{0} \phi_{m}^{\prime \prime } \psi_{n}^{\prime \prime } + \frac{{5E_{2} \phi_{m}^{\prime \prime } \psi_{n}^{\prime \prime } }}{{2h^{2} }} - \frac{1}{2}F_{2} \phi_{m}^{\prime \prime } \psi_{n}^{\prime \prime } + \frac{{10F_{4} \phi_{m}^{\prime \prime } \psi_{n}^{\prime \prime } }}{{3h^{2} }} \\ & \quad - \frac{1}{4}A_{2} \psi_{n} \phi_{m}^{(4)} + \frac{{5A_{4} \psi_{n} \phi_{m}^{(4)} }}{{3h^{2} }} - \frac{1}{4}C_{0} \psi_{n} \phi_{m}^{(4)} + \frac{{5C_{2} \psi_{n} \phi_{m}^{(4)} }}{{h^{2} }} - \frac{2}{5}D_{0} \psi_{n} \phi_{m}^{(4)} + \frac{{14D_{2} \psi_{n} \phi_{m}^{(4)} }}{{3h^{2} }} \\ & \quad + \frac{3}{16}E_{0} \psi_{n} \phi_{m}^{(4)} + \frac{{5E_{2} \psi_{n} \phi_{m}^{(4)} }}{{4h^{2} }} + \frac{3}{4}C_{2} \psi_{n}^{\prime \prime } \phi_{m}^{(4)} - \frac{{5C_{4} \psi_{n}^{\prime \prime } \phi_{m}^{(4)} }}{{h^{2} }} + \frac{3}{10}D_{2} \psi_{n}^{\prime \prime } \phi_{m}^{(4)} - \frac{{2D_{4} \psi_{n}^{\prime \prime } \phi_{m}^{(4)} }}{{h^{2} }} \\ & \quad - \frac{1}{4}A_{2} \phi_{m} \psi_{n}^{(4)} + \frac{{5A_{4} \phi_{m} \psi_{n}^{(4)} }}{{3h^{2} }} - \frac{1}{4}C_{0} \phi_{m} \psi_{n}^{(4)} + \frac{{5C_{2} \phi_{m} \psi_{n}^{(4)} }}{{h^{2} }} - \frac{2}{5}D_{0} \phi_{m} \psi_{n}^{(4)} + \frac{{14D_{2} \phi_{m} \psi_{n}^{(4)} }}{{3h^{2} }} \\ & \quad + \frac{3}{16}E_{0} \phi_{m} \psi_{n}^{(4)} + \frac{{5E_{2} \phi_{m} \psi_{n}^{(4)} }}{{4h^{2} }} + \frac{3}{4}C_{2} \phi_{m}^{\prime \prime } \psi_{n}^{(4)} - \frac{{5C_{4} \phi_{m}^{\prime \prime } \psi_{n}^{(4)} }}{{h^{2} }} + \frac{3}{10}D_{2} \phi_{m}^{\prime \prime } \psi_{n}^{(4)} - \frac{{2D_{4} \phi_{m}^{\prime \prime } \psi_{n}^{(4)} }}{{h^{2} }} \\ & \quad + \frac{1}{4}C_{2} \psi_{n} \phi_{m}^{(6)} - \frac{{5C_{4} \psi_{n} \phi_{m}^{(6)} }}{{3h^{2} }} + \frac{1}{10}D_{2} \psi_{n} \phi_{m}^{(6)} - \frac{{2D_{4} \psi_{n} \phi_{m}^{(6)} }}{{3h^{2} }} + \frac{1}{4}C_{2} \phi_{m} \psi_{n}^{(6)} - \frac{{5C_{4} \phi_{m} \psi_{n}^{(6)} }}{{3h^{2} }} \\ & \quad + \frac{1}{10}D_{2} \phi_{m} \psi_{n}^{(6)} - \frac{{2D_{4} \phi_{m} \psi_{n}^{(6)} }}{{3h^{2} }}, \\ \end{aligned}$$
(C.35)
$$L_{44} = - B_{0} \phi_{m}^{\prime 2} \psi_{n}^{\prime 2} - A_{0} \psi_{n}^{2} \phi_{m}^{\prime \prime 2} - F_{0} \phi_{m} \psi_{n} \phi_{m}^{\prime \prime } \psi_{n}^{\prime \prime } ,$$
(C.36)
$$L_{45} { = } - B_{0} \phi_{m}^{\prime 2} \psi_{n}^{\prime 2} - F_{0} \phi_{m} \psi_{n} \phi_{m}^{\prime \prime } \psi_{n}^{\prime \prime } - A_{0} \phi_{m}^{2} \psi_{n}^{\prime \prime 2} ,$$
(C.37)
$$\begin{aligned} L_{{46}} & = \frac{9}{4}B_{1} \phi _{m} ^{{\prime 2}} \psi _{n} ^{{\prime 2}} - \frac{{5B_{3} \phi _{m} ^{{\prime 2}} \psi _{n} ^{{\prime 2}} }}{{3h^{2} }} - \frac{{8D_{1} \phi _{m} ^{{\prime 2}} \psi _{n} ^{{\prime 2}} }}{{3h^{2} }} + \frac{1}{2}F_{1} \phi _{m} ^{{\prime 2}} \psi _{n} ^{{\prime 2}} - \frac{{10F_{3} \phi _{m} ^{{\prime 2}} \psi _{n} ^{{\prime 2}} }}{{3h^{2} }} + \frac{1}{4}B_{1} \phi _{m} \psi _{n} ^{{\prime 2}} \phi _{m} ^{{\prime \prime }} \\ & \quad - \frac{{5B_{3} \phi _{m} \psi _{n} ^{{\prime 2}} \phi _{m} ^{{\prime \prime }} }}{{3h^{2} }} - \frac{{2D_{1} \phi _{m} \psi _{n} ^{{\prime 2}} \phi _{m} ^{{\prime \prime }} }}{{h^{2} }} + \frac{1}{4}F_{1} \phi _{m} \psi _{n} ^{{\prime 2}} \phi _{m} ^{{\prime \prime }} - \frac{{5F_{3} \phi _{m} \psi _{n} ^{{\prime 2}} \phi _{m} ^{{\prime \prime }} }}{{3h^{2} }} + \frac{5}{4}A_{1} \psi _{n} ^{2} \phi _{m} ^{{\prime \prime 2}} - \frac{{5A_{3} \psi _{n} ^{2} \phi _{m} ^{{\prime \prime 2}} }}{{3h^{2} }} \\ & \quad - \frac{{2D_{1} \psi _{n} ^{2} \phi _{m} ^{{\prime \prime 2}} }}{{h^{2} }} - \frac{7}{4}C_{1} \psi _{n} ^{{\prime 2}} \phi _{m} ^{{\prime \prime 2}} + \frac{{35C_{3} \psi _{n} ^{{\prime 2}} \phi _{m} ^{{\prime \prime 2}} }}{{3h^{2} }} - \frac{2}{5}D_{1} \psi _{n} ^{{\prime 2}} \phi _{m} ^{{\prime \prime 2}} + \frac{{8D_{3} \psi _{n} ^{{\prime 2}} \phi _{m} ^{{\prime \prime 2}} }}{{3h^{2} }} + \frac{1}{4}B_{1} \psi _{n} \phi _{m} ^{{\prime 2}} \psi _{n} ^{{\prime \prime }} \\ & \quad - \frac{{5B_{3} \psi _{n} \phi _{m} ^{{\prime 2}} \psi _{n} ^{{\prime \prime }} }}{{3h^{2} }} - \frac{{2D_{1} \psi _{n} \phi _{m} ^{{\prime 2}} \psi _{n} ^{{\prime \prime }} }}{{h^{2} }} + \frac{1}{4}F_{1} \psi _{n} \phi _{m} ^{{\prime 2}} \psi _{n} ^{{\prime \prime }} - \frac{{5F_{3} \psi _{n} \phi _{m} ^{{\prime 2}} \psi _{n} ^{{\prime \prime }} }}{{3h^{2} }} + \frac{1}{4}B_{1} \phi _{m} \psi _{n} \phi _{m} ^{{\prime \prime }} \psi _{n} ^{{\prime \prime }} \\ & \quad - \frac{{5B_{3} \phi _{m} \psi _{n} \phi _{m} ^{{\prime \prime }} \psi _{n} ^{{\prime \prime }} }}{{3h^{2} }} - \frac{{4D_{1} \phi _{m} \psi _{n} \phi _{m} ^{{\prime \prime }} \psi _{n} ^{{\prime \prime }} }}{{3h^{2} }} + 2F_{1} \phi _{m} \psi _{n} \phi _{m} ^{{\prime \prime }} \psi _{n} ^{{\prime \prime }} - C_{1} \psi _{n} \phi _{m} ^{{\prime \prime 2}} \psi _{n} ^{{\prime \prime }} + \frac{{20C_{3} \psi _{n} \phi _{m} ^{{\prime \prime 2}} \psi _{n} ^{{\prime \prime }} }}{{3h^{2} }} \\ & \quad - \frac{{11}}{{20}}D_{1} \psi _{n} \phi _{m} ^{{\prime \prime 2}} \psi _{n} ^{{\prime \prime }} + \frac{{11D_{3} \psi _{n} \phi _{m} ^{{\prime \prime 2}} \psi _{n} ^{{\prime \prime }} }}{{3h^{2} }} + \frac{5}{4}A_{1} \phi _{m} ^{2} \psi _{n} ^{{\prime \prime 2}} - \frac{{5A_{3} \phi _{m} ^{2} \psi _{n} ^{{\prime \prime 2}} }}{{3h^{2} }} - \frac{{2D_{1} \phi _{m} ^{2} \psi _{n} ^{{\prime \prime 2}} }}{{h^{2} }} - \frac{7}{4}C_{1} \phi _{m} ^{{\prime 2}} \psi _{n} ^{{\prime \prime 2}} \\ & \quad + \frac{{35C_{3} \phi _{m} ^{{\prime 2}} \psi _{n} ^{{\prime \prime 2}} }}{{3h^{2} }} - \frac{2}{5}D_{1} \phi _{m} ^{{\prime 2}} \psi _{n} ^{{\prime \prime 2}} + \frac{{8D_{3} \phi _{m} ^{{\prime 2}} \psi _{n} ^{{\prime \prime 2}} }}{{3h^{2} }} - C_{1} \phi _{m} \phi _{m} ^{{\prime \prime }} \psi _{n} ^{{\prime \prime 2}} + \frac{{20C_{3} \phi _{m} \phi _{m} ^{{\prime \prime }} \psi _{n} ^{{\prime \prime 2}} }}{{3h^{2} }} - \frac{{11}}{{20}}D_{1} \phi _{m} \phi _{m} ^{{\prime \prime }} \psi _{n} ^{{\prime \prime 2}} \\ & \quad + \frac{{11D_{3} \phi _{m} \phi _{m} ^{{\prime \prime }} \psi _{n} ^{{\prime \prime 2}} }}{{3h^{2} }} + \frac{1}{4}A_{1} \psi _{n} ^{2} \phi _{m} ^{\prime } \phi _{m} ^{{(3)}} - \frac{{5A_{3} \psi _{n} ^{2} \phi _{m} ^{\prime } \phi _{m} ^{{(3)}} }}{{3h^{2} }} - \frac{{2D_{1} \psi _{n} ^{2} \phi _{m} ^{\prime } \phi _{m} ^{{(3)}} }}{{h^{2} }} - 2C_{1} \phi _{m} ^{\prime } \psi _{n} ^{{\prime 2}} \phi _{m} ^{{(3)}} \\ & \quad + \frac{{40C_{3} \phi _{m} ^{\prime } \psi _{n} ^{{\prime 2}} \phi _{m} ^{{(3)}} }}{{3h^{2} }} - \frac{1}{2}D_{1} \phi _{m} ^{\prime } \psi _{n} ^{{\prime 2}} \phi _{m} ^{{(3)}} + \frac{{10D_{3} \phi _{m} ^{\prime } \psi _{n} ^{{\prime 2}} \phi _{m} ^{{(3)}} }}{{3h^{2} }} - C_{1} \psi _{n} \phi _{m} ^{\prime } \psi _{n} ^{{\prime \prime }} \phi _{m} ^{{(3)}} + \frac{{20C_{3} \psi _{n} \phi _{m} ^{\prime } \psi _{n} ^{{\prime \prime }} \phi _{m} ^{{(3)}} }}{{3h^{2} }} \\ & \quad - \frac{7}{{10}}D_{1} \psi _{n} \phi _{m} ^{\prime } \psi _{n} ^{{\prime \prime }} \phi _{m} ^{{(3)}} + \frac{{14D_{3} \psi _{n} \phi _{m} ^{\prime } \psi _{n} ^{{\prime \prime }} \phi _{m} ^{{(3)}} }}{{3h^{2} }} - \frac{3}{4}C_{1} \psi _{n} ^{2} \phi _{m} ^{{(3)2}} + \frac{{5C_{3} \psi _{n} ^{2} \phi _{m} ^{{(3)2}} }}{{h^{2} }} - \frac{3}{{10}}D_{1} \psi _{n} ^{2} \phi _{m} ^{{(3)2}} \\ & \quad + \frac{{2D_{3} \psi _{n} ^{2} \phi _{m} ^{{(3)2}} }}{{h^{2} }} + \frac{1}{4}A_{1} \phi _{m} ^{2} \psi _{n} ^{\prime } \psi _{n} ^{{(3)}} - \frac{{5A_{3} \phi _{m} ^{2} \psi _{n} ^{\prime } \psi _{n} ^{{(3)}} }}{{3h^{2} }} - \frac{{2D_{1} \phi _{m} ^{2} \psi _{n} ^{\prime } \psi _{n} ^{{(3)}} }}{{h^{2} }} - 2C_{1} \phi _{m} ^{{\prime 2}} \psi _{n} ^{\prime } \psi _{n} ^{{(3)}} \\ & \quad + \frac{{40C_{3} \phi _{m} ^{{\prime 2}} \psi _{n} ^{\prime } \psi _{n} ^{{(3)}} }}{{3h^{2} }} - \frac{1}{2}D_{1} \phi _{m} ^{{\prime 2}} \psi _{n} ^{\prime } \psi _{n} ^{{(3)}} + \frac{{10D_{3} \phi _{m} ^{{\prime 2}} \psi _{n} ^{\prime } \psi _{n} ^{{(3)}} }}{{3h^{2} }} - C_{1} \phi _{m} \psi _{n} ^{\prime } \phi _{m} ^{{\prime \prime }} \psi _{n} ^{{(3)}} + \frac{{20C_{3} \phi _{m} \psi _{n} ^{\prime } \phi _{m} ^{{\prime \prime }} \psi _{n} ^{{(3)}} }}{{3h^{2} }} \\ & \quad - \frac{7}{{10}}D_{1} \phi _{m} \psi _{n} ^{\prime } \phi _{m} ^{{\prime \prime }} \psi _{n} ^{{(3)}} + \frac{{14D_{3} \phi _{m} \psi _{n} ^{\prime } \phi _{m} ^{{\prime \prime }} \psi _{n} ^{{(3)}} }}{{3h^{2} }} - \frac{3}{4}C_{1} \phi _{m} ^{2} \psi _{n} ^{{(3)2}} + \frac{{5C_{3} \phi _{m} ^{2} \psi _{n} ^{{(3)2}} }}{{h^{2} }} - \frac{3}{{10}}D_{1} \phi _{m} ^{2} \psi _{n} ^{{(3)2}} \\ & \quad + \frac{{2D_{3} \phi _{m} ^{2} \psi _{n} ^{{(3)2}} }}{{h^{2} }} - \frac{1}{4}C_{1} \phi _{m} \psi _{n} ^{{\prime 2}} \phi _{m} ^{{(4)}} + \frac{{5C_{3} \phi _{m} \psi _{n} ^{{\prime 2}} \phi _{m} ^{{(4)}} }}{{3h^{2} }} - \frac{1}{{10}}D_{1} \phi _{m} \psi _{n} ^{{\prime 2}} \phi _{m} ^{{(4)}} + \frac{{2D_{3} \phi _{m} \psi _{n} ^{{\prime 2}} \phi _{m} ^{{(4)}} }}{{3h^{2} }} \\ & \quad - C_{1} \psi _{n} ^{2} \phi _{m} ^{{\prime \prime }} \phi _{m} ^{{(4)}} + \frac{{20C_{3} \psi _{n} ^{2} \phi _{m} ^{{\prime \prime }} \phi _{m} ^{{(4)}} }}{{3h^{2} }} - \frac{2}{5}D_{1} \psi _{n} ^{2} \phi _{m} ^{{\prime \prime }} \phi _{m} ^{{(4)}} + \frac{{8D_{3} \psi _{n} ^{2} \phi _{m} ^{{\prime \prime }} \phi _{m} ^{{(4)}} }}{{3h^{2} }} - \frac{3}{{20}}D_{1} \phi _{m} \psi _{n} \psi _{n} ^{{\prime \prime }} \phi _{m} ^{{(4)}} \\ & \quad + \frac{{D_{3} \phi _{m} \psi _{n} \psi _{n} ^{{\prime \prime }} \phi _{m} ^{{(4)}} }}{{h^{2} }} - \frac{1}{4}C_{1} \psi _{n} \phi _{m} ^{{\prime 2}} \psi _{n} ^{{(4)}} + \frac{{5C_{3} \psi _{n} \phi _{m} ^{{\prime 2}} \psi _{n} ^{{(4)}} }}{{3h^{2} }} - \frac{1}{{10}}D_{1} \psi _{n} \phi _{m} ^{{\prime 2}} \psi _{n} ^{{(4)}} + \frac{{2D_{3} \psi _{n} \phi _{m} ^{{\prime 2}} \psi _{n} ^{{(4)}} }}{{3h^{2} }} \\ & \quad - \frac{3}{{20}}D_{1} \phi _{m} \psi _{n} \phi _{m} ^{{\prime \prime }} \psi _{n} ^{{(4)}} + \frac{{D_{3} \phi _{m} \psi _{n} \phi _{m} ^{{\prime \prime }} \psi _{n} ^{{(4)}} }}{{h^{2} }} - C_{1} \phi _{m} ^{2} \psi _{n} ^{{\prime \prime }} \psi _{n} ^{{(4)}} + \frac{{20C_{3} \phi _{m} ^{2} \psi _{n} ^{{\prime \prime }} \psi _{n} ^{{(4)}} }}{{3h^{2} }} - \frac{2}{5}D_{1} \phi _{m} ^{2} \psi _{n} ^{{\prime \prime }} \psi _{n} ^{{(4)}} \\ & \quad + \frac{{8D_{3} \phi _{m} ^{2} \psi _{n} ^{{\prime \prime }} \psi _{n} ^{{(4)}} }}{{3h^{2} }} - \frac{1}{4}C_{1} \psi _{n} ^{2} \phi _{m} ^{\prime } \phi _{m} ^{{(5)}} + \frac{{5C_{3} \psi _{n} ^{2} \phi _{m} ^{\prime } \phi _{m} ^{{(5)}} }}{{3h^{2} }} - \frac{1}{{10}}D_{1} \psi _{n} ^{2} \phi _{m} ^{\prime } \phi _{m} ^{{(5)}} + \frac{{2D_{3} \psi _{n} ^{2} \phi _{m} ^{\prime } \phi _{m} ^{{(5)}} }}{{3h^{2} }} \\ & \quad - \frac{1}{4}C_{1} \phi _{m} ^{2} \psi _{n} ^{\prime } \psi _{n} ^{{(5)}} + \frac{{5C_{3} \phi _{m} ^{2} \psi _{n} ^{\prime } \psi _{n} ^{{(5)}} }}{{3h^{2} }} - \frac{1}{{10}}D_{1} \phi _{m} ^{2} \psi _{n} ^{\prime } \psi _{n} ^{{(5)}} + \frac{{2D_{3} \phi _{m} ^{2} \psi _{n} ^{\prime } \psi _{n} ^{{(5)}} }}{{3h^{2} }}, \\ \end{aligned}$$
(C.38)
$$\begin{aligned} L_{47} = - B_{0} \phi_{m} \psi_{n} \phi_{m}^{\prime 2} \psi_{n}^{\prime 2} - \frac{1}{2}A_{0} \psi_{n}^{3} \phi_{m}^{\prime 2} \phi_{m}^{\prime \prime } - \frac{1}{2}F_{0} \phi_{m}^{2} \psi_{n} \psi_{n}^{\prime 2} \phi_{m}^{\prime \prime } - \frac{1}{2}F_{0} \phi_{m} \psi_{n}^{2} \phi_{m}^{\prime 2} \psi_{n}^{\prime \prime } - \frac{1}{2}A_{0} \phi_{m}^{3} \psi_{n}^{\prime 2} \psi_{n}^{\prime \prime } , \\ \end{aligned}$$
(C.39)
$$\begin{aligned} L_{{48}} & = k_{w} \phi _{m} \psi _{n} - k_{p} \psi _{n} \phi _{m} ^{{\prime \prime }} - \frac{{25}}{{32}}B_{0} \psi _{n} \phi _{m} ^{{\prime \prime }} + \frac{{25B_{2} \psi _{n} \phi _{m} ^{{\prime \prime }} }}{{4h^{2} }} - \frac{{25B_{4} \psi _{n} \phi _{m} ^{{\prime \prime }} }}{{2h^{4} }} - \frac{{80D_{2} \psi _{n} \phi _{m} ^{{\prime \prime }} }}{{3h^{4} }} - \frac{{25E_{2} \psi _{n} \phi _{m} ^{{\prime \prime }} }}{{2h^{4} }} \\ & \quad - k_{p} \phi _{m} \psi _{n} ^{{\prime \prime }} - \frac{{25}}{{32}}B_{0} \phi _{m} \psi _{n} ^{{\prime \prime }} + \frac{{25B_{2} \phi _{m} \psi _{n} ^{{\prime \prime }} }}{{4h^{2} }} - \frac{{25B_{4} \phi _{m} \psi _{n} ^{{\prime \prime }} }}{{2h^{4} }} - \frac{{80D_{2} \phi _{m} \psi _{n} ^{{\prime \prime }} }}{{3h^{4} }} - \frac{{25E_{2} \phi _{m} \psi _{n} ^{{\prime \prime }} }}{{2h^{4} }} + \frac{1}{8}B_{2} \phi _{m} ^{{\prime \prime }} \psi _{n} ^{{\prime \prime }} \\ & \quad - \frac{{5B_{4} \phi _{m} ^{{\prime \prime }} \psi _{n} ^{{\prime \prime }} }}{{3h^{2} }} + \frac{{50B_{6} \phi _{m} ^{{\prime \prime }} \psi _{n} ^{{\prime \prime }} }}{{9h^{4} }} + \frac{1}{8}C_{0} \phi _{m} ^{{\prime \prime }} \psi _{n} ^{{\prime \prime }} - \frac{{5C_{2} \phi _{m} ^{{\prime \prime }} \psi _{n} ^{{\prime \prime }} }}{{h^{2} }} + \frac{{50C_{4} \phi _{m} ^{{\prime \prime }} \psi _{n} ^{{\prime \prime }} }}{{h^{4} }} + \frac{6}{5}D_{0} \phi _{m} ^{{\prime \prime }} \psi _{n} ^{{\prime \prime }} \\ & \quad - \frac{{18D_{2} \phi _{m} ^{{\prime \prime }} \psi _{n} ^{{\prime \prime }} }}{{h^{2} }} + \frac{{200D_{4} \phi _{m} ^{{\prime \prime }} \psi _{n} ^{{\prime \prime }} }}{{3h^{4} }} + \frac{9}{{64}}E_{0} \phi _{m} ^{{\prime \prime }} \psi _{n} ^{{\prime \prime }} + \frac{{15E_{2} \phi _{m} ^{{\prime \prime }} \psi _{n} ^{{\prime \prime }} }}{{8h^{2} }} + \frac{{25E_{4} \phi _{m} ^{{\prime \prime }} \psi _{n} ^{{\prime \prime }} }}{{4h^{4} }} + \frac{1}{8}F_{2} \phi _{m} ^{{\prime \prime }} \psi _{n} ^{{\prime \prime }} \\ & \quad - \frac{{5F_{4} \phi _{m} ^{{\prime \prime }} \psi _{n} ^{{\prime \prime }} }}{{3h^{2} }} + \frac{{50F_{6} \phi _{m} ^{{\prime \prime }} \psi _{n} ^{{\prime \prime }} }}{{9h^{4} }} + \frac{1}{{16}}A_{2} \psi _{n} \phi _{m} ^{{(4)}} - \frac{{5A_{4} \psi _{n} \phi _{m} ^{{(4)}} }}{{6h^{2} }} + \frac{{25A_{6} \psi _{n} \phi _{m} ^{{(4)}} }}{{9h^{4} }} + \frac{1}{{16}}C_{0} \psi _{n} \phi _{m} ^{{(4)}} \\ & \quad - \frac{{5C_{2} \psi _{n} \phi _{m} ^{{(4)}} }}{{2h^{2} }} + \frac{{25C_{4} \psi _{n} \phi _{m} ^{{(4)}} }}{{h^{4} }} + \frac{3}{5}D_{0} \psi _{n} \phi _{m} ^{{(4)}} - \frac{{9D_{2} \psi _{n} \phi _{m} ^{{(4)}} }}{{h^{2} }} + \frac{{100D_{4} \psi _{n} \phi _{m} ^{{(4)}} }}{{3h^{4} }} + \frac{9}{{128}}E_{0} \psi _{n} \phi _{m} ^{{(4)}} \\ & \quad + \frac{{15E_{2} \psi _{n} \phi _{m} ^{{(4)}} }}{{16h^{2} }} + \frac{{25E_{4} \psi _{n} \phi _{m} ^{{(4)}} }}{{8h^{4} }} - \frac{3}{{16}}C_{2} \psi _{n} ^{{\prime \prime }} \phi _{m} ^{{(4)}} + \frac{{5C_{4} \psi _{n} ^{{\prime \prime }} \phi _{m} ^{{(4)}} }}{{2h^{2} }} - \frac{{25C_{6} \psi _{n} ^{{\prime \prime }} \phi _{m} ^{{(4)}} }}{{3h^{4} }} - \frac{3}{{40}}D_{2} \psi _{n} ^{{\prime \prime }} \phi _{m} ^{{(4)}} \\ & \quad + \frac{{D_{4} \psi _{n} ^{{\prime \prime }} \phi _{m} ^{{(4)}} }}{{h^{2} }} - \frac{{10D_{6} \psi _{n} ^{{\prime \prime }} \phi _{m} ^{{(4)}} }}{{3h^{4} }} + \frac{1}{{16}}A_{2} \phi _{m} \psi _{n} ^{{(4)}} - \frac{{5A_{4} \phi _{m} \psi _{n} ^{{(4)}} }}{{6h^{2} }} + \frac{{25A_{6} \phi _{m} \psi _{n} ^{{(4)}} }}{{9h^{4} }} + \frac{1}{{16}}C_{0} \phi _{m} \psi _{n} ^{{(4)}} \\ & \quad - \frac{{5C_{2} \phi _{m} \psi _{n} ^{{(4)}} }}{{2h^{2} }} + \frac{{25C_{4} \phi _{m} \psi _{n} ^{{(4)}} }}{{h^{4} }} + \frac{3}{5}D_{0} \phi _{m} \psi _{n} ^{{(4)}} - \frac{{9D_{2} \phi _{m} \psi _{n} ^{{(4)}} }}{{h^{2} }} + \frac{{100D_{4} \phi _{m} \psi _{n} ^{{(4)}} }}{{3h^{4} }} + \frac{9}{{128}}E_{0} \phi _{m} \psi _{n} ^{{(4)}} \\ & \quad + \frac{{15E_{2} \phi _{m} \psi _{n} ^{{(4)}} }}{{16h^{2} }} + \frac{{25E_{4} \phi _{m} \psi _{n} ^{{(4)}} }}{{8h^{4} }} - \frac{3}{{16}}C_{2} \phi _{m} ^{{\prime \prime }} \psi _{n} ^{{(4)}} + \frac{{5C_{4} \phi _{m} ^{{\prime \prime }} \psi _{n} ^{{(4)}} }}{{2h^{2} }} - \frac{{25C_{6} \phi _{m} ^{{\prime \prime }} \psi _{n} ^{{(4)}} }}{{3h^{4} }} - \frac{3}{{40}}D_{2} \phi _{m} ^{{\prime \prime }} \psi _{n} ^{{(4)}} \\ & \quad + \frac{{D_{4} \phi _{m} ^{{\prime \prime }} \psi _{n} ^{{(4)}} }}{{h^{2} }} - \frac{{10D_{6} \phi _{m} ^{{\prime \prime }} \psi _{n} ^{{(4)}} }}{{3h^{4} }} - \frac{1}{{16}}C_{2} \psi _{n} \phi _{m} ^{{(6)}} + \frac{{5C_{4} \psi _{n} \phi _{m} ^{{(6)}} }}{{6h^{2} }} - \frac{{25C_{6} \psi _{n} \phi _{m} ^{{(6)}} }}{{9h^{4} }} - \frac{1}{{40}}D_{2} \psi _{n} \phi _{m} ^{{(6)}} \\ & \quad + \frac{{D_{4} \psi _{n} \phi _{m} ^{{(6)}} }}{{3h^{2} }} - \frac{{10D_{6} \psi _{n} \phi _{m} ^{{(6)}} }}{{9h^{4} }} - \frac{1}{{16}}C_{2} \phi _{m} \psi _{n} ^{{(6)}} + \frac{{5C_{4} \phi _{m} \psi _{n} ^{{(6)}} }}{{6h^{2} }} - \frac{{25C_{6} \phi _{m} \psi _{n} ^{{(6)}} }}{{9h^{4} }} - \frac{1}{{40}}D_{2} \phi _{m} \psi _{n} ^{{(6)}} \\ & \quad + \frac{{D_{4} \phi _{m} \psi _{n} ^{{(6)}} }}{{3h^{2} }} - \frac{{10D_{6} \phi _{m} \psi _{n} ^{{(6)}} }}{{9h^{4} }}, \\ \end{aligned}$$
(C.40)
$$L_{49} { = } - B_{0} \phi_{m}^{\prime 2} \psi_{n}^{\prime 2} - A_{0} \psi_{n}^{2} \phi_{m}^{\prime \prime 2} - F_{0} \phi_{m} \psi_{n} \phi_{m}^{\prime \prime } \psi_{n}^{\prime \prime } ,$$
(C.41)
$$L_{490} = - B_{0} \phi_{m}^{\prime 2} \psi_{n}^{\prime 2} - F_{0} \phi_{m} \psi_{n} \phi_{m}^{\prime \prime } \psi_{n}^{\prime \prime } - A_{0} \phi_{m}^{2} \psi_{n}^{\prime \prime 2} ,$$
(C.42)
$$\begin{aligned} L_{{491}} & = 2B_{1} \phi _{m} ^{{\prime 2}} \psi _{n} ^{{\prime 2}} - \frac{{16D_{1} \phi _{m} ^{{\prime 2}} \psi _{n} ^{{\prime 2}} }}{{3h^{2} }} + F_{1} \phi _{m} ^{{\prime 2}} \psi _{n} ^{{\prime 2}} - \frac{{20F_{3} \phi _{m} ^{{\prime 2}} \psi _{n} ^{{\prime 2}} }}{{3h^{2} }} + \frac{1}{2}B_{1} \phi _{m} \psi _{n} ^{{\prime 2}} \phi _{m} ^{{\prime \prime }} - \frac{{10B_{3} \phi _{m} \psi _{n} ^{{\prime 2}} \phi _{m} ^{{\prime \prime }} }}{{3h^{2} }} \\ & \quad - \frac{{4D_{1} \phi _{m} \psi _{n} ^{{\prime 2}} \phi _{m} ^{{\prime \prime }} }}{{h^{2} }} + \frac{1}{2}F_{1} \phi _{m} \psi _{n} ^{{\prime 2}} \phi _{m} ^{{\prime \prime }} - \frac{{10F_{3} \phi _{m} \psi _{n} ^{{\prime 2}} \phi _{m} ^{{\prime \prime }} }}{{3h^{2} }} + \frac{5}{4}A_{1} \psi _{n} ^{2} \phi _{m} ^{{\prime \prime 2}} - \frac{{5A_{3} \psi _{n} ^{2} \phi _{m} ^{{\prime \prime 2}} }}{{3h^{2} }} - \frac{{4D_{1} \psi _{n} ^{2} \phi _{m} ^{{\prime \prime 2}} }}{{h^{2} }} \\ & \quad - \frac{7}{2}C_{1} \psi _{n} ^{{\prime 2}} \phi _{m} ^{{\prime \prime 2}} + \frac{{70C_{3} \psi _{n} ^{{\prime 2}} \phi _{m} ^{{\prime \prime 2}} }}{{3h^{2} }} - \frac{4}{5}D_{1} \psi _{n} ^{{\prime 2}} \phi _{m} ^{{\prime \prime 2}} + \frac{{16D_{3} \psi _{n} ^{{\prime 2}} \phi _{m} ^{{\prime \prime 2}} }}{{3h^{2} }} + \frac{1}{2}B_{1} \psi _{n} \phi _{m} ^{{\prime 2}} \psi _{n} ^{{\prime \prime }} - \frac{{10B_{3} \psi _{n} \phi _{m} ^{{\prime 2}} \psi _{n} ^{{\prime \prime }} }}{{3h^{2} }} \\ & \quad - \frac{{4D_{1} \psi _{n} \phi _{m} ^{{\prime 2}} \psi _{n} ^{{\prime \prime }} }}{{h^{2} }} + \frac{1}{2}F_{1} \psi _{n} \phi _{m} ^{{\prime 2}} \psi _{n} ^{{\prime \prime }} - \frac{{10F_{3} \psi _{n} \phi _{m} ^{{\prime 2}} \psi _{n} ^{{\prime \prime }} }}{{3h^{2} }} + \frac{1}{2}B_{1} \phi _{m} \psi _{n} \phi _{m} ^{{\prime \prime }} \psi _{n} ^{{\prime \prime }} - \frac{{10B_{3} \phi _{m} \psi _{n} \phi _{m} ^{{\prime \prime }} \psi _{n} ^{{\prime \prime }} }}{{3h^{2} }} \\ & \quad - \frac{{8D_{1} \phi _{m} \psi _{n} \phi _{m} ^{{\prime \prime }} \psi _{n} ^{{\prime \prime }} }}{{3h^{2} }} + \frac{3}{2}F_{1} \phi _{m} \psi _{n} \phi _{m} ^{{\prime \prime }} \psi _{n} ^{{\prime \prime }} + \frac{{10F_{3} \phi _{m} \psi _{n} \phi _{m} ^{{\prime \prime }} \psi _{n} ^{{\prime \prime }} }}{{3h^{2} }} - 2C_{1} \psi _{n} \phi _{m} ^{{\prime \prime 2}} \psi _{n} ^{{\prime \prime }} + \frac{{40C_{3} \psi _{n} \phi _{m} ^{{\prime \prime 2}} \psi _{n} ^{{\prime \prime }} }}{{3h^{2} }} \\ & \quad - \frac{{11}}{{10}}D_{1} \psi _{n} \phi _{m} ^{{\prime \prime 2}} \psi _{n} ^{{\prime \prime }} + \frac{{22D_{3} \psi _{n} \phi _{m} ^{{\prime \prime 2}} \psi _{n} ^{{\prime \prime }} }}{{3h^{2} }} + \frac{5}{4}A_{1} \phi _{m} ^{2} \psi _{n} ^{{\prime \prime 2}} - \frac{{5A_{3} \phi _{m} ^{2} \psi _{n} ^{{\prime \prime 2}} }}{{3h^{2} }} - \frac{{4D_{1} \phi _{m} ^{2} \psi _{n} ^{{\prime \prime 2}} }}{{h^{2} }} - \frac{7}{2}C_{1} \phi _{m} ^{{\prime 2}} \psi _{n} ^{{\prime \prime 2}} \\ & \quad + \frac{{70C_{3} \phi _{m} ^{{\prime 2}} \psi _{n} ^{{\prime \prime 2}} }}{{3h^{2} }} - \frac{4}{5}D_{1} \phi _{m} ^{{\prime 2}} \psi _{n} ^{{\prime \prime 2}} + \frac{{16D_{3} \phi _{m} ^{{\prime 2}} \psi _{n} ^{{\prime \prime 2}} }}{{3h^{2} }} - 2C_{1} \phi _{m} \phi _{m} ^{{\prime \prime }} \psi _{n} ^{{\prime \prime 2}} + \frac{{40C_{3} \phi _{m} \phi _{m} ^{{\prime \prime }} \psi _{n} ^{{\prime \prime 2}} }}{{3h^{2} }} \\ & \quad - \frac{{11}}{{10}}D_{1} \phi _{m} \phi _{m} ^{{\prime \prime }} \psi _{n} ^{{\prime \prime 2}} + \frac{{22D_{3} \phi _{m} \phi _{m} ^{{\prime \prime }} \psi _{n} ^{{\prime \prime 2}} }}{{3h^{2} }} + \frac{1}{2}A_{1} \psi _{n} ^{2} \phi _{m} ^{\prime } \phi _{m} ^{{(3)}} - \frac{{10A_{3} \psi _{n} ^{2} \phi _{m} ^{\prime } \phi _{m} ^{{(3)}} }}{{3h^{2} }} - \frac{{4D_{1} \psi _{n} ^{2} \phi _{m} ^{\prime } \phi _{m} ^{{(3)}} }}{{h^{2} }} \\ & \quad - 4C_{1} \phi _{m} ^{\prime } \psi _{n} ^{{\prime 2}} \phi _{m} ^{{(3)}} + \frac{{80C_{3} \phi _{m} ^{\prime } \psi _{n} ^{{\prime 2}} \phi _{m} ^{{(3)}} }}{{3h^{2} }} - D_{1} \phi _{m} ^{\prime } \psi _{n} ^{{\prime 2}} \phi _{m} ^{{(3)}} + \frac{{20D_{3} \phi _{m} ^{\prime } \psi _{n} ^{{\prime 2}} \phi _{m} ^{{(3)}} }}{{3h^{2} }} - 2C_{1} \psi _{n} \phi _{m} ^{\prime } \psi _{n} ^{{\prime \prime }} \phi _{m} ^{{(3)}} \\ & \quad + \frac{{40C_{3} \psi _{n} \phi _{m} ^{\prime } \psi _{n} ^{{\prime \prime }} \phi _{m} ^{{(3)}} }}{{3h^{2} }} - \frac{7}{5}D_{1} \psi _{n} \phi _{m} ^{\prime } \psi _{n} ^{{\prime \prime }} \phi _{m} ^{{(3)}} + \frac{{28D_{3} \psi _{n} \phi _{m} ^{\prime } \psi _{n} ^{{\prime \prime }} \phi _{m} ^{{(3)}} }}{{3h^{2} }} - \frac{3}{2}C_{1} \psi _{n} ^{2} \phi _{m} ^{{(3)2}} + \frac{{10C_{3} \psi _{n} ^{2} \phi _{m} ^{{(3)2}} }}{{h^{2} }} \\ & \quad - \frac{3}{5}D_{1} \psi _{n} ^{2} \phi _{m} ^{{(3)2}} + \frac{{4D_{3} \psi _{n} ^{2} \phi _{m} ^{{(3)2}} }}{{h^{2} }} + \frac{1}{2}A_{1} \phi _{m} ^{2} \psi _{n} ^{\prime } \psi _{n} ^{{(3)}} - \frac{{10A_{3} \phi _{m} ^{2} \psi _{n} ^{\prime } \psi _{n} ^{{(3)}} }}{{3h^{2} }} - \frac{{4D_{1} \phi _{m} ^{2} \psi _{n} ^{\prime } \psi _{n} ^{{(3)}} }}{{h^{2} }} \\ & \quad - 4C_{1} \phi _{m} ^{{\prime 2}} \psi _{n} ^{\prime } \psi _{n} ^{{(3)}} + \frac{{80C_{3} \phi _{m} ^{{\prime 2}} \psi _{n} ^{\prime } \psi _{n} ^{{(3)}} }}{{3h^{2} }} - D_{1} \phi _{m} ^{{\prime 2}} \psi _{n} ^{\prime } \psi _{n} ^{{(3)}} + \frac{{20D_{3} \phi _{m} ^{{\prime 2}} \psi _{n} ^{\prime } \psi _{n} ^{{(3)}} }}{{3h^{2} }} - 2C_{1} \phi _{m} \psi _{n} ^{\prime } \phi _{m} ^{{\prime \prime }} \psi _{n} ^{{(3)}} \\ & \quad + \frac{{40C_{3} \phi _{m} \psi _{n} ^{\prime } \phi _{m} ^{{\prime \prime }} \psi _{n} ^{{(3)}} }}{{3h^{2} }} - \frac{7}{5}D_{1} \phi _{m} \psi _{n} ^{\prime } \phi _{m} ^{{\prime \prime }} \psi _{n} ^{{(3)}} + \frac{{28D_{3} \phi _{m} \psi _{n} ^{\prime } \phi _{m} ^{{\prime \prime }} \psi _{n} ^{{(3)}} }}{{3h^{2} }} - \frac{3}{2}C_{1} \phi _{m} ^{2} \psi _{n} ^{{(3)2}} + \frac{{10C_{3} \phi _{m} ^{2} \psi _{n} ^{{(3)2}} }}{{h^{2} }} \\ & \quad - \frac{3}{5}D_{1} \phi _{m} ^{2} \psi _{n} ^{{(3)2}} + \frac{{4D_{3} \phi _{m} ^{2} \psi _{n} ^{{(3)2}} }}{{h^{2} }} - \frac{1}{2}C_{1} \phi _{m} \psi _{n} ^{{\prime 2}} \phi _{m} ^{{(4)}} + \frac{{10C_{3} \phi _{m} \psi _{n} ^{{\prime 2}} \phi _{m} ^{{(4)}} }}{{3h^{2} }} - \frac{1}{5}D_{1} \phi _{m} \psi _{n} ^{{\prime 2}} \phi _{m} ^{{(4)}} \\ & \quad + \frac{{4D_{3} \phi _{m} \psi _{n} ^{{\prime 2}} \phi _{m} ^{{(4)}} }}{{3h^{2} }} - 2C_{1} \psi _{n} ^{2} \phi _{m} ^{{\prime \prime }} \phi _{m} ^{{(4)}} + \frac{{40C_{3} \psi _{n} ^{2} \phi _{m} ^{{\prime \prime }} \phi _{m} ^{{(4)}} }}{{3h^{2} }} - \frac{4}{5} D_{1} \psi _{n} ^{2} \phi _{m} ^{{\prime \prime }} \phi _{m} ^{{(4)}} + \frac{{16D_{3} \psi _{n} ^{2} \phi _{m} ^{{\prime \prime }} \phi _{m} ^{{(4)}} }}{{3h^{2} }} \\ & \quad - \frac{3}{{10}}D_{1} \phi _{m} \psi _{n} \psi _{n} ^{{\prime \prime }} \phi _{m} ^{{(4)}} + \frac{{2D_{3} \phi _{m} \psi _{n} \psi _{n} ^{{\prime \prime }} \phi _{m} ^{{(4)}} }}{{h^{2} }} - \frac{1}{2}C_{1} \psi _{n} \phi _{m} ^{{\prime 2}} \psi _{n} ^{{(4)}} + \frac{{10C_{3} \psi _{n} \phi _{m} ^{{\prime 2}} \psi _{n} ^{{(4)}} }}{{3h^{2} }} - \frac{1}{5}D_{1} \psi _{n} \phi _{m} ^{{\prime 2}} \psi _{n} ^{{(4)}} \\ & \quad + \frac{{4D_{3} \psi _{n} \phi _{m} ^{{\prime 2}} \psi _{n} ^{{(4)}} }}{{3h^{2} }} - \frac{3}{{10}}D_{1} \phi _{m} \psi _{n} \phi _{m} ^{{\prime \prime }} \psi _{n} ^{{(4)}} + \frac{{2D_{3} \phi _{m} \psi _{n} \phi _{m} ^{{\prime \prime }} \psi _{n} ^{{(4)}} }}{{h^{2} }} - 2C_{1} \phi _{m} ^{2} \psi _{n} ^{{\prime \prime }} \psi _{n} ^{{(4)}} + \frac{{40C_{3} \phi _{m} ^{2} \psi _{n} ^{{\prime \prime }} \psi _{n} ^{{(4)}} }}{{3h^{2} }} \\ & \quad - \frac{4}{5}D_{1} \phi _{m} ^{2} \psi _{n} ^{{\prime \prime }} \psi _{n} ^{{(4)}} + \frac{{16D_{3} \phi _{m} ^{2} \psi _{n} ^{{\prime \prime }} \psi _{n} ^{{(4)}} }}{{3h^{2} }} - \frac{1}{2}C_{1} \psi _{n} ^{2} \phi _{m} ^{\prime } \phi _{m} ^{{(5)}} + \frac{{10C_{3} \psi _{n} ^{2} \phi _{m} ^{\prime } \phi _{m} ^{{(5)}} }}{{3h^{2} }} - \frac{1}{5}D_{1} \psi _{n} ^{2} \phi _{m} ^{\prime } \phi _{m} ^{{(5)}} \\ & \quad + \frac{{4D_{3} \psi _{n} ^{2} \phi _{m} ^{\prime } \phi _{m} ^{{(5)}} }}{{3h^{2} }} - \frac{1}{2}C_{1} \phi _{m} ^{2} \psi _{n} ^{\prime } \psi _{n} ^{{(5)}} + \frac{{10C_{3} \phi _{m} ^{2} \psi _{n} ^{\prime } \psi _{n} ^{{(5)}} }}{{3h^{2} }} - \frac{1}{5}D_{1} \phi _{m} ^{2} \psi _{n} ^{\prime } \psi _{n} ^{{(5)}} + \frac{{4D_{3} \phi _{m} ^{2} \psi _{n} ^{\prime } \psi _{n} ^{{(5)}} }}{{3h^{2} }}, \\ \end{aligned}$$
(C.43)
$$\begin{aligned} L_{492} & = - 3B_{0} \phi_{m} \psi_{n} \phi_{m}^{\prime 2} \psi_{n}^{\prime 2} - \frac{3}{2}A_{0} \psi_{n}^{3} \phi_{m}^{\prime 2} \phi_{m}^{\prime \prime } - \frac{3}{2}F_{0} \phi_{m}^{2} \psi_{n} \psi_{n}^{\prime 2} \phi_{m}^{\prime \prime } - \frac{3}{2}F_{0} \phi_{m} \psi_{n}^{2} \phi_{m}^{\prime 2} \psi_{n}^{\prime \prime } \\ & \quad - \frac{3}{2}A_{0} \phi_{m}^{3} \psi_{n}^{\prime 2} \psi_{n}^{\prime \prime } , \\ \end{aligned}$$
(C.44)
$$\begin{aligned} L_{{493}} & = - \frac{1}{4}B_{1} \phi _{m} ^{{\prime 2}} \psi _{n} ^{{\prime 2}} + \frac{{5B_{3} \phi _{m} ^{{\prime 2}} \psi _{n} ^{{\prime 2}} }}{{3h^{2} }} - \frac{{8D_{1} \phi _{m} ^{{\prime 2}} \psi _{n} ^{{\prime 2}} }}{{3h^{2} }} + \frac{1}{2}F_{1} \phi _{m} ^{{\prime 2}} \psi _{n} ^{{\prime 2}} - \frac{{10F_{3} \phi _{m} ^{{\prime 2}} \psi _{n} ^{{\prime 2}} }}{{3h^{2} }} + \frac{1}{4}B_{1} \phi _{m} \psi _{n} ^{{\prime 2}} \phi _{m} ^{{\prime \prime }} \\ & \quad - \frac{{5B_{3} \phi _{m} \psi _{n} ^{{\prime 2}} \phi _{m} ^{{\prime \prime }} }}{{3h^{2} }} - \frac{{2D_{1} \phi _{m} \psi _{n} ^{{\prime 2}} \phi _{m} ^{{\prime \prime }} }}{{h^{2} }} + \frac{1}{4}F_{1} \phi _{m} \psi _{n} ^{{\prime 2}} \phi _{m} ^{{\prime \prime }} - \frac{{5F_{3} \phi _{m} \psi _{n} ^{{\prime 2}} \phi _{m} ^{{\prime \prime }} }}{{3h^{2} }} - \frac{{2D_{1} \psi _{n} ^{2} \phi _{m} ^{{\prime \prime 2}} }}{{h^{2} }} - \frac{7}{4}C_{1} \psi _{n} ^{{\prime 2}} \phi _{m} ^{{\prime \prime 2}} \\ & \quad + \frac{{35C_{3} \psi _{n} ^{{\prime 2}} \phi _{m} ^{{\prime \prime 2}} }}{{3h^{2} }} - \frac{2}{5}D_{1} \psi _{n} ^{{\prime 2}} \phi _{m} ^{{\prime \prime 2}} + \frac{{8D_{3} \psi _{n} ^{{\prime 2}} \phi _{m} ^{{\prime \prime 2}} }}{{3h^{2} }} + \frac{1}{4}B_{1} \psi _{n} \phi _{m} ^{{\prime 2}} \psi _{n} ^{{\prime \prime }} - \frac{{5B_{3} \psi _{n} \phi _{m} ^{{\prime 2}} \psi _{n} ^{{\prime \prime }} }}{{3h^{2} }} - \frac{{2D_{1} \psi _{n} \phi _{m} ^{{\prime 2}} \psi _{n} ^{{\prime \prime }} }}{{h^{2} }} \\ & \quad + \frac{1}{4}F_{1} \psi _{n} \phi _{m} ^{{\prime 2}} \psi _{n} ^{{\prime \prime }} - \frac{{5F_{3} \psi _{n} \phi _{m} ^{{\prime 2}} \psi _{n} ^{{\prime \prime }} }}{{3h^{2} }} + \frac{1}{4}B_{1} \phi _{m} \psi _{n} \phi _{m} ^{{\prime \prime }} \psi _{n} ^{{\prime \prime }} - \frac{{5B_{3} \phi _{m} \psi _{n} \phi _{m} ^{{\prime \prime }} \psi _{n} ^{{\prime \prime }} }}{{3h^{2} }} - \frac{{4D_{1} \phi _{m} \psi _{n} \phi _{m} ^{{\prime \prime }} \psi _{n} ^{{\prime \prime }} }}{{3h^{2} }} \\ & \quad - \frac{1}{2}F_{1} \phi _{m} \psi _{n} \phi _{m} ^{{\prime \prime }} \psi _{n} ^{{\prime \prime }} + \frac{{10F_{3} \phi _{m} \psi _{n} \phi _{m} ^{{\prime \prime }} \psi _{n} ^{{\prime \prime }} }}{{3h^{2} }} - C_{1} \psi _{n} \phi _{m} ^{{\prime \prime 2}} \psi _{n} ^{{\prime \prime }} + \frac{{20C_{3} \psi _{n} \phi _{m} ^{{\prime \prime 2}} \psi _{n} ^{{\prime \prime }} }}{{3h^{2} }} - \frac{{11}}{{20}}D_{1} \psi _{n} \phi _{m} ^{{\prime \prime 2}} \psi _{n} ^{{\prime \prime }} \\ & \quad + \frac{{11D_{3} \psi _{n} \phi _{m} ^{{\prime \prime 2}} \psi _{n} ^{{\prime \prime }} }}{{3h^{2} }} - \frac{{2D_{1} \phi _{m} ^{2} \psi _{n} ^{{\prime \prime 2}} }}{{h^{2} }} - \frac{7}{4}C_{1} \phi _{m} ^{{\prime 2}} \psi _{n} ^{{\prime \prime 2}} + \frac{{35C_{3} \phi _{m} ^{{\prime 2}} \psi _{n} ^{{\prime \prime 2}} }}{{3h^{2} }} - \frac{2}{5}D_{1} \phi _{m} ^{{\prime 2}} \psi _{n} ^{{\prime \prime 2}} + \frac{{8D_{3} \phi _{m} ^{{\prime 2}} \psi _{n} ^{{\prime \prime 2}} }}{{3h^{2} }} \\ & \quad - C_{1} \phi _{m} \phi _{m} ^{{\prime \prime }} \psi _{n} ^{{\prime \prime 2}} + \frac{{20C_{3} \phi _{m} \phi _{m} ^{{\prime \prime }} \psi _{n} ^{{\prime \prime 2}} }}{{3h^{2} }} - \frac{{11}}{{20}}D_{1} \phi _{m} \phi _{m} ^{{\prime \prime }} \psi _{n} ^{{\prime \prime 2}} + \frac{{11D_{3} \phi _{m} \phi _{m} ^{{\prime \prime }} \psi _{n} ^{{\prime \prime 2}} }}{{3h^{2} }} + \frac{1}{4}A_{1} \psi _{n} ^{2} \phi _{m} ^{\prime } \phi _{m} ^{{(3)}} \\ & \quad - \frac{{5A_{3} \psi _{n} ^{2} \phi _{m} ^{\prime } \phi _{m} ^{{(3)}} }}{{3h^{2} }} - \frac{{2D_{1} \psi _{n} ^{2} \phi _{m} ^{\prime } \phi _{m} ^{{(3)}} }}{{h^{2} }} - 2C_{1} \phi _{m} ^{\prime } \psi _{n} ^{{\prime 2}} \phi _{m} ^{{(3)}} + \frac{{40C_{3} \phi _{m} ^{\prime } \psi _{n} ^{{\prime 2}} \phi _{m} ^{{(3)}} }}{{3h^{2} }} - \frac{1}{2}D_{1} \phi _{m} ^{\prime } \psi _{n} ^{{\prime 2}} \phi _{m} ^{{(3)}} \\ & \quad + \frac{{10D_{3} \phi _{m} ^{\prime } \psi _{n} ^{{\prime 2}} \phi _{m} ^{{(3)}} }}{{3h^{2} }} - C_{1} \psi _{n} \phi _{m} ^{\prime } \psi _{n} ^{{\prime \prime }} \phi _{m} ^{{(3)}} + \frac{{20C_{3} \psi _{n} \phi _{m} ^{\prime } \psi _{n} ^{{\prime \prime }} \phi _{m} ^{{(3)}} }}{{3h^{2} }} - \frac{7}{{10}}D_{1} \psi _{n} \phi _{m} ^{\prime } \psi _{n} ^{{\prime \prime }} \phi _{m} ^{{(3)}} \\ & \quad + \frac{{14D_{3} \psi _{n} \phi _{m} ^{\prime } \psi _{n} ^{{\prime \prime }} \phi _{m} ^{{(3)}} }}{{3h^{2} }} - \frac{3}{4}C_{1} \psi _{n} ^{2} \phi _{m} ^{{(3)2}} + \frac{{5C_{3} \psi _{n} ^{2} \phi _{m} ^{{(3)2}} }}{{h^{2} }} - \frac{3}{{10}}D_{1} \psi _{n} ^{2} \phi _{m} ^{{(3)2}} + \frac{{2D_{3} \psi _{n} ^{2} \phi _{m} ^{{(3)2}} }}{{h^{2} }} \\ & \quad + \frac{1}{4}A_{1} \phi _{m} ^{2} \psi _{n} ^{\prime } \psi _{n} ^{{(3)}} - \frac{{5A_{3} \phi _{m} ^{2} \psi _{n} ^{\prime } \psi _{n} ^{{(3)}} }}{{3h^{2} }} - \frac{{2D_{1} \phi _{m} ^{2} \psi _{n} ^{\prime } \psi _{n} ^{{(3)}} }}{{h^{2} }} - 2C_{1} \phi _{m} ^{{\prime 2}} \psi _{n} ^{\prime } \psi _{n} ^{{(3)}} + \frac{{40C_{3} \phi _{m} ^{{\prime 2}} \psi _{n} ^{\prime } \psi _{n} ^{{(3)}} }}{{3h^{2} }} \\ & \quad - \frac{1}{2}D_{1} \phi _{m} ^{{\prime 2}} \psi _{n} ^{\prime } \psi _{n} ^{{(3)}} + \frac{{10D_{3} \phi _{m} ^{{\prime 2}} \psi _{n} ^{\prime } \psi _{n} ^{{(3)}} }}{{3h^{2} }} - C_{1} \phi _{m} \psi _{n} ^{\prime } \phi _{m} ^{{\prime \prime }} \psi _{n} ^{{(3)}} + \frac{{20C_{3} \phi _{m} \psi _{n} ^{\prime } \phi _{m} ^{{\prime \prime }} \psi _{n} ^{{(3)}} }}{{3h^{2} }} \\ & \quad - \frac{7}{{10}}D_{1} \phi _{m} \psi _{n} ^{\prime } \phi _{m} ^{{\prime \prime }} \psi _{n} ^{{(3)}} + \frac{{14D_{3} \phi _{m} \psi _{n} ^{\prime } \phi _{m} ^{{\prime \prime }} \psi _{n} ^{{(3)}} }}{{3h^{2} }} - \frac{3}{4}C_{1} \phi _{m} ^{2} \psi _{n} ^{{(3)2}} + \frac{{5C_{3} \phi _{m} ^{2} \psi _{n} ^{{(3)2}} }}{{h^{2} }} - \frac{3}{{10}}D_{1} \phi _{m} ^{2} \psi _{n} ^{{(3)2}} \\ & \quad + \frac{{2D_{3} \phi _{m} ^{2} \psi _{n} ^{{(3)2}} }}{{h^{2} }} - \frac{1}{4}C_{1} \phi _{m} \psi _{n} ^{{\prime 2}} \phi _{m} ^{{(4)}} + \frac{{5C_{3} \phi _{m} \psi _{n} ^{{\prime 2}} \phi _{m} ^{{(4)}} }}{{3h^{2} }} - \frac{1}{{10}}D_{1} \phi _{m} \psi _{n} ^{{\prime 2}} \phi _{m} ^{{(4)}} + \frac{{2D_{3} \phi _{m} \psi _{n} ^{{\prime 2}} \phi _{m} ^{{(4)}} }}{{3h^{2} }} \\ & \quad - C_{1} \psi _{n} ^{2} \phi _{m} ^{{\prime \prime }} \phi _{m} ^{{(4)}} + \frac{{20C_{3} \psi _{n} ^{2} \phi _{m} ^{{\prime \prime }} \phi _{m} ^{{(4)}} }}{{3h^{2} }} - \frac{2}{5}D_{1} \psi _{n} ^{2} \phi _{m} ^{{\prime \prime }} \phi _{m} ^{{(4)}} + \frac{{8D_{3} \psi _{n} ^{2} \phi _{m} ^{{\prime \prime }} \phi _{m} ^{{(4)}} }}{{3h^{2} }} - \frac{3}{{20}}D_{1} \phi _{m} \psi _{n} \psi _{n} ^{{\prime \prime }} \phi _{m} ^{{(4)}} \\ & \quad + \frac{{D_{3} \phi _{m} \psi _{n} \psi _{n} ^{{\prime \prime }} \phi _{m} ^{{(4)}} }}{{h^{2} }} - \frac{1}{4}C_{1} \psi _{n} \phi _{m} ^{{\prime 2}} \psi _{n} ^{{(4)}} + \frac{{5C_{3} \psi _{n} \phi _{m} ^{{\prime 2}} \psi _{n} ^{{(4)}} }}{{3h^{2} }} - \frac{1}{{10}}D_{1} \psi _{n} \phi _{m} ^{{\prime 2}} \psi _{n} ^{{(4)}} + \frac{{2D_{3} \psi _{n} \phi _{m} ^{{\prime 2}} \psi _{n} ^{{(4)}} }}{{3h^{2} }} \\ & \quad - \frac{3}{{20}}D_{1} \phi _{m} \psi _{n} \phi _{m} ^{{\prime \prime }} \psi _{n} ^{{(4)}} + \frac{{D_{3} \phi _{m} \psi _{n} \phi _{m} ^{{\prime \prime }} \psi _{n} ^{{(4)}} }}{{h^{2} }} - C_{1} \phi _{m} ^{2} \psi _{n} ^{{\prime \prime }} \psi _{n} ^{{(4)}} + \frac{{20C_{3} \phi _{m} ^{2} \psi _{n} ^{{\prime \prime }} \psi _{n} ^{{(4)}} }}{{3h^{2} }} - \frac{2}{5}D_{1} \phi _{m} ^{2} \psi _{n} ^{{\prime \prime }} \psi _{n} ^{{(4)}} \\ & \quad + \frac{{8D_{3} \phi _{m} ^{2} \psi _{n} ^{{\prime \prime }} \psi _{n} ^{{(4)}} }}{{3h^{2} }} - \frac{1}{4}C_{1} \psi _{n} ^{2} \phi _{m} ^{\prime } \phi _{m} ^{{(5)}} + \frac{{5C_{3} \psi _{n} ^{2} \phi _{m} ^{\prime } \phi _{m} ^{{(5)}} }}{{3h^{2} }} - \frac{1}{{10}}D_{1} \psi _{n} ^{2} \phi _{m} ^{\prime } \phi _{m} ^{{(5)}} + \frac{{2D_{3} \psi _{n} ^{2} \phi _{m} ^{\prime } \phi _{m} ^{{(5)}} }}{{3h^{2} }} \\ & \quad - \frac{1}{4}C_{1} \phi _{m} ^{2} \psi _{n} ^{\prime } \psi _{n} ^{{(5)}} + \frac{{5C_{3} \phi _{m} ^{2} \psi _{n} ^{\prime } \psi _{n} ^{{(5)}} }}{{3h^{2} }} - \frac{1}{{10}}D_{1} \phi _{m} ^{2} \psi _{n} ^{\prime } \psi _{n} ^{{(5)}} + \frac{{2D_{3} \phi _{m} ^{2} \psi _{n} ^{\prime } \psi _{n} ^{{(5)}} }}{{3h^{2} }}, \\ \end{aligned}$$
(C.45)
$$\begin{aligned} L_{494} & = - 3B_{0} \phi_{m} \psi_{n} \phi_{m}^{\prime 2} \psi_{n}^{\prime 2} - \frac{3}{2}A_{0} \psi_{n}^{3} \phi_{m}^{\prime 2} \phi_{m}^{\prime \prime } - \frac{3}{2}F_{0} \phi_{m}^{2} \psi_{n} \psi_{n}^{\prime 2} \phi_{m}^{\prime \prime } - \frac{3}{2}F_{0} \phi_{m} \psi_{n}^{2} \phi_{m}^{\prime 2} \psi_{n}^{\prime \prime } \\ & \quad - \frac{3}{2}A_{0} \phi_{m}^{3} \psi_{n}^{\prime 2} \psi_{n}^{\prime \prime } , \\ \end{aligned}$$
(C.46)
$$\begin{aligned} L_{495} & = - B_{0} \phi_{m} \psi_{n} \phi_{m}^{\prime 2} \psi_{n}^{\prime 2} - \frac{1}{2}A_{0} \psi_{n}^{3} \phi_{m}^{\prime 2} \phi_{m}^{\prime \prime } - \frac{1}{2}F_{0} \phi_{m}^{2} \psi_{n} \psi_{n}^{\prime 2} \phi_{m}^{\prime \prime } - \frac{1}{2}F_{0} \phi_{m} \psi_{n}^{2} \phi_{m}^{\prime 2} \psi_{n}^{\prime \prime } \\ & \quad - \frac{1}{2}A_{0} \phi_{m}^{3} \psi_{n}^{\prime 2} \psi_{n}^{\prime \prime } , \\ \end{aligned}$$
(C.47)
$$\begin{gathered} L_{411} = C_{d} I_{0} \phi_{m} \psi_{n} ,\;\, L_{412} = C_{d} I_{0} \phi_{m} \psi_{n} , \;\, L_{413} = - I_{2} \psi_{n} \phi_{m}^{\prime \prime } , \;\, L_{414} = - I_{2} \phi_{m} \psi_{n}^{\prime \prime } , \hfill \\ L_{415} = I_{0} \phi_{m} \psi_{n} + I_{5} \psi_{n} \phi_{m}^{\prime \prime } + I_{5} \phi_{m} \psi_{n}^{\prime \prime } , \;\, L_{416} = I_{0} \phi_{m} \psi_{n} - I_{4} \psi_{n} \phi_{m}^{\prime \prime } - I_{4} \phi_{m} \psi_{n}^{\prime \prime } . \hfill \\ \end{gathered}$$
(C.48)

Appendix D

$$Li_{11} = \int_{{S_{a} }} {L_{11} \phi_{m}^{\prime } \psi_{n} {\text{d}}S_{a} } , \, Li_{12} = \int_{{S_{a} }} {L_{12} \phi_{m}^{\prime } \psi_{n} {\text{d}}S_{a} } , \, Li_{13} = \int_{{S_{a} }} {L_{13} \phi_{m}^{\prime } \psi_{n} {\text{d}}S_{a} } , \, Li_{14} = \int_{{S_{a} }} {L_{14} \phi_{m}^{\prime } \psi_{n} {\text{d}}S_{a} } ,$$
(D.1)
$$Li_{15} = \int_{{S_{a} }} {L_{15} \phi_{m}^{\prime } \psi_{n} {\text{d}}S_{a} } , \, Li_{16} = \int_{{S_{a} }} {L_{16} \phi_{m}^{\prime } \psi_{n} {\text{d}}S_{a} } , \, Li_{17} = \int_{{S_{a} }} {L_{17} \phi_{m}^{\prime } \psi_{n} {\text{d}}S_{a} } , \, Li_{111} = \int_{{S_{a} }} {L_{111} \phi_{m}^{\prime } \psi_{n} {\text{d}}S_{a} } ,$$
(D.2)
$$Li_{112} = \int_{{S_{a} }} {L_{112} \phi_{m}^{\prime } \psi_{n} {\text{d}}S_{a} } ,Li_{113} = \int_{{S_{a} }} {L_{113} \phi_{m}^{\prime } \psi_{n} {\text{d}}S_{a} } ,$$
(D.3)
$$Li_{21} = \int_{{S_{a} }} {L_{21} \phi_{m} \psi_{n}^{\prime } {\text{d}}S_{a} } , \, Li_{22} = \int_{{S_{a} }} {L_{22} \phi_{m} \psi_{n}^{\prime } {\text{d}}S_{a} } , \, Li_{23} = \int_{{S_{a} }} {L_{23} \phi_{m} \psi_{n}^{\prime } {\text{d}}S_{a} } , \, Li_{24} = \int_{{S_{a} }} {L_{24} \phi_{m} \psi_{n}^{\prime } {\text{d}}S_{a} } ,$$
(D.4)
$$Li_{25} = \int_{{S_{a} }} {L_{25} \phi_{m} \psi_{n}^{\prime } {\text{d}}S_{a} } , \, Li_{26} = \int_{{S_{a} }} {L_{26} \phi_{m} \psi_{n}^{\prime } {\text{d}}S_{a} } , \, Li_{27} = \int_{{S_{a} }} {L_{27} \phi_{m} \psi_{n}^{\prime } {\text{d}}S_{a} } , \, Li_{211} = \int_{{S_{a} }} {L_{211} \phi_{m} \psi_{n}^{\prime } {\text{d}}S_{a} } ,$$
(D.5)
$$Li_{212} = \int_{{S_{a} }} {L_{212} \phi_{m} \psi_{n}^{\prime } {\text{d}}S_{a} } , \, Li_{213} = \int_{{S_{a} }} {L_{213} \phi_{m} \psi_{n}^{\prime } {\text{d}}S_{a} } ,$$
(D.6)
$$Li_{31} = \int_{{S_{a} }} {L_{31} \phi_{m} \psi_{n} {\text{d}}S_{a} } , \, Li_{32} = \int_{{S_{a} }} {L_{32} \phi_{m} \psi_{n} {\text{d}}S_{a} } , \, Li_{33} = \int_{{S_{a} }} {L_{33} \phi_{m} \psi_{n} {\text{d}}S_{a} } , \, Li_{34} = \int_{{S_{a} }} {L_{34} \phi_{m} \psi_{n} {\text{d}}S_{a} } ,$$
(D.7)
$$Li_{35} = \int_{{S_{a} }} {L_{35} \phi_{m} \psi_{n} {\text{d}}S_{a} } , \, Li_{36} = \int_{{S_{a} }} {L_{36} \phi_{m} \psi_{n} {\text{d}}S_{a} } , \, Li_{37} = \int_{{S_{a} }} {L_{37} \phi_{m} \psi_{n} {\text{d}}S_{a} } , \, Li_{38} = \int_{{S_{a} }} {L_{38} \phi_{m} \psi_{n} {\text{d}}S_{a} } ,$$
(D.8)
$$Li_{39} = \int_{{S_{a} }} {L_{39} \phi_{m} \psi_{n} {\text{d}}S_{a} } , \, Li_{390} = \int_{{S_{a} }} {L_{390} \phi_{m} \psi_{n} {\text{d}}S_{a} } , \, Li_{391} = \int_{{S_{a} }} {L_{391} \phi_{m} \psi_{n} {\text{d}}S_{a} } , \, Li_{392} = \int_{{S_{a} }} {L_{392} \phi_{m} \psi_{n} {\text{d}}S_{a} } ,$$
(D.9)
$$Li_{393} = \int_{{S_{a} }} {L_{393} \phi_{m} \psi_{n} d{\text{d}}_{a} } , \, Li_{394} = \int_{{S_{a} }} {L_{394} \phi_{m} \psi_{n} {\text{d}}S_{a} } ,Li_{395} = \int_{{S_{a} }} {L_{395} \phi_{m} \psi_{n} {\text{d}}S_{a} } ,Li_{311} = \int_{{S_{a} }} {L_{311} \phi_{m} \psi_{n} {\text{d}}S_{a} } ,$$
(D.10)
$$Li_{312} = \int_{{S_{a} }} {L_{312} \phi_{m} \psi_{n} {\text{d}}S_{a} } , \, Li_{313} = \int_{{S_{a} }} {L_{313} \phi_{m} \psi_{n} {\text{d}}S_{a} } , \, Li_{314} = \int_{{S_{a} }} {L_{314} \phi_{m} \psi_{n} {\text{d}}S_{a} } ,Li_{315} = \int_{{S_{a} }} {L_{315} \phi_{m} \psi_{n} {\text{d}}S_{a} } ,$$
(D.11)
$$Li_{316} = \int_{{S_{a} }} {L_{316} \phi_{m} \psi_{n} {\text{d}}S_{a} } , \, Li_{q} = \int_{{S_{a} }} {\phi_{m} \psi_{n} {\text{d}}S_{a} } ,$$
(D.12)
$$Li_{41} = \int_{{S_{a} }} {L_{41} \phi_{m} \psi_{n} d{\text{d}}_{a} } , \, Li_{42} = \int_{{S_{a} }} {L_{42} \phi_{m} \psi_{n} {\text{d}}S_{a} } , \, Li_{43} = \int_{{S_{a} }} {L_{43} \phi_{m} \psi_{n} {\text{d}}S_{a} } , \, Li_{44} = \int_{{S_{a} }} {L_{44} \phi_{m} \psi_{n} {\text{d}}S_{a} } ,$$
(D.13)
$$Li_{45} = \int_{{S_{a} }} {L_{45} \phi_{m} \psi_{n} {\text{d}}S_{a} } , \, Li_{46} = \int_{{S_{a} }} {L_{46} \phi_{m} \psi_{n} {\text{d}}S_{a} } , \, Li_{47} = \int_{{S_{a} }} {L_{47} \phi_{m} \psi_{n} {\text{d}}S_{a} } , \, Li_{48} = \int_{{S_{a} }} {L_{48} \phi_{m} \psi_{n} {\text{d}}S_{a} } ,$$
(D.14)
$$Li_{49} = \int_{{S_{a} }} {L_{49} \phi_{m} \psi_{n} {\text{d}}S_{a} } , \, Li_{490} = \int_{{S_{a} }} {L_{490} \phi_{m} \psi_{n} {\text{d}}S_{a} } , \, Li_{491} = \int_{{S_{a} }} {L_{491} \phi_{m} \psi_{n} {\text{d}}S_{a} } , \, Li_{492} = \int_{{S_{a} }} {L_{492} \phi_{m} \psi_{n} {\text{d}}S_{a} } ,$$
(D.15)
$$Li_{493} = \int_{{S_{a} }} {L_{493} \phi_{m} \psi_{n} {\text{d}}S_{a} } , \, Li_{494} = \int_{{S_{a} }} {L_{494} \phi_{m} \psi_{n} {\text{d}}S_{a} } ,Li_{495} = \int_{{S_{a} }} {L_{495} \phi_{m} \psi_{n} {\text{d}}S_{a} } ,Li_{411} = \int_{{S_{a} }} {L_{411} \phi_{m} \psi_{n} {\text{d}}S_{a} } ,$$
(D.16)
$$Li_{412} = \int_{{S_{a} }} {L_{412} \phi_{m} \psi_{n} {\text{d}}S_{a} } , \, Li_{413} = \int_{{S_{a} }} {L_{413} \phi_{m} \psi_{n} {\text{d}}S_{a} } ,Li_{414} = \int_{{S_{a} }} {L_{414} \phi_{m} \psi_{n} {\text{d}}S_{a} } ,Li_{415} = \int_{{S_{a} }} {L_{415} \phi_{m} \psi_{n} {\text{d}}S_{a} } ,$$
(D.17)
$$Li_{416} = \int_{{S_{a} }} {L_{416} \phi_{m} \psi_{n} {\text{d}}S_{a} }.$$
(D.18)

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Bo, L. Nonlinear dynamic analysis of the perovskite solar cell under blast impacts based on the modified strain gradient theory. Acta Mech 234, 1649–1685 (2023). https://doi.org/10.1007/s00707-022-03444-8

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