Abstract
We describe a compact finite-difference discretization and Gaussian-radial basis function for the two-dimensional local fractional elliptic PDEs that describe anomalous diffusion-convection of groundwater contamination. Precisely estimating pollutant concentration over a long period helps protect water reservoirs. The local fractional partial differential equations and their discretization described here are the generalization of the integer order elliptic partial differential equations and their high-order scheme. The high-order discretization of fractal gradient and anomalous diffusion on a non-uniformly spaced nine-point single-cell grid network gives the result in small computing time. The new scheme is supported by a detailed convergence analysis describing the monotone property and a strongly connected Jacobian (iteration) matrix graph. The computational illustration of various anomalous diffusion-convection models demonstrates the proposed methodology’s effectiveness.
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Acknowledgements
This research work was presented at the XIII Annual International Conference of the Georgian Mathematical Union at Batumi Shota Rustaveli State University, 4–9 September 2023.
Funding
N. Jha is partially supported by the Science & Engineering Research Board, Government of India (MTR/2022/000485). S. Verma acknowledges South Asian University, New Delhi for providing travel grant and Council of Scientific & Industrial Research Grant-in-aid (No. 09/1112(0009)/2020-EMR-I) in the form of research fellowship.
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Appendices
Appendix 1. Expression of weight coefficients in equation (5.2) and (5.3)
\(a_{l}^{(0)}\) | \(\left( p_{l}-1\right) \left\{ 2 c^{2} h_{l} / 3+h_{l+1}^{-1}\right\}\) | \(b_{m}^{(0)}\) | \(\left( q_{m}-1\right) \left\{ 2 c^{2} k_{m} / 3+k_{m+1}^{-1}\right\}\) |
\(a_{l+1}^{(0)}\) | \(\left\{ c^{2} h_{l}\left( p_{l}+2\right) / 3+h_{l+1}^{-1}\right\} /\left( p_{l}+1\right)\) | \(b_{m+1}^{(0)}\) | \(\left\{ c^{2} k_{m}\left( q_{m}+2\right) / 3+h_{l+1}^{-1}\right\} /\left( 1+q_{m}\right)\) |
\(a_{l-1}^{(0)}\) | \(-p_{l}\left\{ c^{2} h_{l}\left( 2 p_{l}+1\right) / 3+h_{l}^{-1}\right\} /\left( p_{l}+1\right)\) | \(b_{m-1}^{(0)}\) | \(-q_{m}\left\{ c^{2} k_{m}\left( 2 q_{m}+1\right) / 3-k_{m}^{-1}\right\} /\left( q_{m}+1\right)\) |
\(a_{l}^{(1)}\) | \(\left( p_{l}+1\right) \left\{ c^{2} h_{l}\left( p_{l}+2\right) / 3-h_{l+1}^{-1}\right\}\) | \(b_{m}^{(1)}\) | \(\left( q_{m}+1\right) \left\{ c^{2} k_{m}\left( q_{m}+2\right) / 3-k_{m+1}^{-1}\right\}\) |
\(a_{l+1}^{(1)}\) | \(\left( 2 p_{l}+1\right) \left[ 1 /\left\{ h_{l+1}\left( p_{l}+1\right) \right\} -2 c^{2} h_{l} / 3\right]\) | \(b_{m+1}^{(1)}\) | \(\left( 2 q_{m}+1\right) \left[ 1 /\left\{ k_{m+1}\left( 1+q_{m}\right) \right\} -2 c^{2} k_{m} / 3\right]\) |
\(a_{l-1}^{(1)}\) | \(p_{l}\left[ 1 /\left\{ h_{l}\left( 1+p_{l}\right) \right\} +c^{2} h_{l}\left( 1-p_{l}\right) / 3\right]\) | \(b_{m-1}^{(1)}\) | \(q_{m}\left[ 1 /\left\{ k_{m}\left( 1+q_{m}\right) \right\} +c^{2} k_{m}\left( 1-q_{m}\right) / 3\right]\) |
\(a_{l}^{(2)}\) | \(\left( p_{l}+1\right) \left\{ 1 / h_{l}-c^{2} h_{l}\left( 2 p_{l}+1\right) / 3\right\} / p_{l}\) | \(b_{m}^{(2)}\) | \(\left( q_{m}+1\right) \left\{ 1 / k_{m}-c^{2} k_{m}\left( 2 q_{m}+1\right) / 3\right\} / q_{m}\) |
\(a_{l+1}^{(2)}\) | \(-\left[ 1 /\left\{ h_{l}\left( p_{l}+1\right) \right\} +c^{2} h_{l}\left( p_{l}-1\right) / 3\right] / p_{l}\) | \(b_{m+1}^{(2)}\) | \(-\left[ 1 /\left\{ k_{m}\left( q_{m}+1\right) \right\} +c^{2} k_{m}\left( q_{m}-1\right) / 3\right] / q_{m}\) |
\(a_{l-1}^{(2)}\) | \(\left( p_{l}+2\right) \left[ 2 c^{2} h_{l} / 3-1 /\left\{ h_{l}\left( p_{l}+1\right) \right\} \right]\) | \(b_{m-1}^{(2)}\) | \(\left( q_{m}+2\right) \left[ 2 c^{2} k_{m} / 3-1 /\left\{ k_{m}\left( q_{m}+1\right) \right\} \right]\) |
\(a_{l}^{(3)}\) | \(2\left( 2 p_{l}^{2}-7 p_{l}+2\right) c^{2} /\left( 3 p_{l}\right) -2 /\left( p_{l} h_{l}^{2}\right)\) | \(b_{m}^{(3)}\) | \(2\left( 2 q_{m}^{2}-7 q_{m}+2\right) c^{2} /\left( 3 q_{m}\right) -2 /\left( q_{m} k_{m}^{2}\right)\) |
\(a_{l+1}^{(3)}\) | \(2\left\{ \left( p_{l}^{2}+4 p_{l}-2\right) c^{2} / 3+h_{l}^{-2}\right\} /\left\{ p_{l}\left( p_{l}+1\right) \right\}\) | \(b_{m+1}^{(3)}\) | \(2\left\{ \left( q_{m}^{2}+4 q_{m}-2\right) c^{2} / 3+k_{m}^{-2}\right\} /\left\{ q_{m}\left( q_{m}+1\right) \right\}\) |
\(a_{l-1}^{(3)}\) | \(2\left\{ -\left( 2 p_{l}^{2}-4 p_{l}-1\right) c^{2} / 3+h_{l}^{-2}\right\} /\left( p_{l}+1\right)\) | \(b_{m-1}^{(3)}\) | \(2\left\{ -\left( 2 q_{m}^{2}-4 q_{m}-1\right) c^{2} / 3+k_{m}^{-2}\right\} /\left( q_{m}+1\right)\) |
Appendix 2. Expression of weight coefficients in equation (6.5) and (6.6)
\(\rho _{0}\) | \(\left( \rho _{2}-\rho _{1} p_{l}\right) /\left[ \left( p_{l}+1\right) P_{l, m}^{x}\right]\) | \(\sigma _{0}\) | \(\left( \sigma _{2}-\sigma _{1} q_{m}\right) /\left[ \left( q_{m}+1\right) Q_{l, m}^{y}\right]\) |
\(\rho _{1}\) | \(-\frac{\rho _{2} t_{1}-\left( t_{0} \rho _{2}+3 c^{2} p^{+} h_{l} p_{l} q_{m}\right) P_{l, m} Q_{l, m}}{t_{1}-t_{0} P_{l, m} Q_{l, m}}\) | \(\sigma _{1}\) | \(-\frac{\sigma _{2} t_{1}-\left( t_{0} \sigma _{2}+3 c^{2} q^{+} k_{l} p_{l} q_{m}\right) P_{l, m} Q_{l, m}}{t_{1}-t_{0} P_{l, m} Q_{l, m}}\) |
\(\rho _{2}\) | \(\frac{p_{l} q_{m}\left\{ t_{0}\left( 6 c^{2} h_{l} p_{l} P_{l, m}+P_{l, m}^{x}\right) P_{l, m} Q_{l, m}-t_{1} P_{l, m}^{x}\right\} p^{+}}{2 t_{0}\left( t_{1}-t_{0} P_{l, m} Q_{l, m}\right) \left( p_{l}+1\right) P_{l, m}}\) | \(\sigma _{2}\) | \(\frac{p_{l} q_{m}\left\{ t_{0}\left( 6 c^{2} k_{m} q_{m} Q_{l, m}+Q_{l, m}^{y}\right) P_{l, m} Q_{l, m}-t_{1} Q_{l, m}^{y}\right\} q^{+}}{2 t_{0}\left( t_{1}-t_{0} P_{l, m} Q_{l, m}\right) \left( q_{m}+1\right) Q_{l, m}}\) |
\(\rho _{3}\) | \(\rho _{0} h_{l}\left( p_{l}+1\right) Q_{l, m}^{x} /\left[ k_{m}\left( q_{m}+1\right) \right]\) | \(\sigma _{3}\) | \(\sigma _{0} k_{m}\left( q_{m}+1\right) P_{l, m}^{y} /\left[ h_{l}\left( p_{l}+1\right) \right]\) |
\(\rho _{4}\) | \(\frac{t_{2} h_{l} p_{l} q_{m} P_{l, m} Q_{l, m}}{2 t_{0}\left( t_{1}-t_{0} P_{l, m} Q_{l, m}\right) k_{m}\left( p_{l}+1\right) P_{l, m}}\) | \(\sigma _{4}\) | \(\frac{t_{2} k_{m} p_{l} q_{m}\left( P_{l, m}\right) ^{2}}{2 t_{0}\left( t_{1}-t_{0} P_{l, m} Q_{l, m}\right) h_{l}\left( q_{m}+1\right) P_{l, m}}\) |
\(t_{0}\) | \(2 p_{l}^{2} q_{m}^{2}-p_{l}^{2} q_{m}-p_{l} q_{m}^{2}+2 p_{l}^{2}+8 p_{l} q_{m}+2 q_{m}^{2}-p_{l}-q_{m}+2\) | ||
\(t_{1}\) | \(h_{l} q_{m}\left( p_{l}-1\right) p^{+} Q_{l, m} P_{l, m}^{x}+k_{m} p_{l}\left( q_{m}-1\right) q^{+} P_{l, m} Q_{l, m}^{y}\) | ||
\(t_{2}\) | \(h_{l} q_{m}\left( p_{l}-1\right) p^{+2} Q_{l, m} P_{l, m}^{x}+\left( t_{0} h_{l} p^{+} Q_{l, m}^{x}+k_{m} p_{l}\left( q_{m}-1\right) p^{+} q^{+} Q_{l, m}^{y}-t_{0} p^{+} Q_{l, m}\right.\) |
Appendix 3. Values of coefficients in equation (6.8)
\(Z_{10}\) | \(h_{l}\left\{ a_{l+1}^{(0)}\left( k_{m} b_{m}^{(0)} t_{11}+t_{10}\right) +h_{l} a_{l+1}^{(3)} t_{20}\right\}\) | \(Z_{21}\) | \(a_{l-1}^{(0)} b_{m+1}^{(0)}\) |
\(Z_{20}\) | \(h_{l}\left\{ a_{l-1}^{(0)}\left( k_{m} b_{m}^{(0)} t_{11}+t_{10}\right) +h_{l} a_{l-1}^{(3)} t_{20}\right\}\) | \(Z_{22}\) | \(a_{l-1}^{(0)} b_{m-1}^{(0)}\) |
\(Z_{01}\) | \(k_{m}\left\{ b_{m+1}^{(0)}\left( h_{l} a_{l}^{(0)} t_{11}+t_{01}\right) +k_{m} b_{m+1}^{(3)} t_{02}\right\}\) | \(Z_{11}\) | \(a_{l+1}^{(0)} b_{m+1}^{(0)}\) |
\(Z_{02}\) | \(k_{m}\left\{ b_{m-1}^{(0)}\left( h_{l} a_{l}^{(0)} t_{11}+t_{01}\right) +k_{m} b_{m-1}^{(3)} t_{02}\right\}\) | \(Z_{12}\) | \(a_{l+1}^{(0)} b_{m-1}^{(0)}\) |
\(Z_{00}\) | \(1+h_{l} a_{l}^{(0)} t_{10}+k_{m} b_{m}^{(0)} t_{01}+h_{l} k_{m} a_{l}^{(0)} b_{m}^{(0)} t_{11}+h_{l}^{2} a_{l}^{(3)} t_{20}+k_{m}^{2} b_{m}^{(3)} t_{02}\) | ||
\(t_{10}\) | \(\left( p_{l}-1\right) / 3-h_{l} P_{l, m}^{x}\left( p_{l}^{2}+p_{l}+1\right) /\left( 18 P_{l, m}\right)\) | ||
\(t_{01}\) | \(\left( q_{m}-1\right) / 3-k_{m} Q_{l, m}^{y}\left( q_{m}^{2}+q_{m}+1\right) /\left( 18 Q_{l, m}\right)\) | ||
\(t_{11}\) | \(\left( q_{m}-1\right) \left( p_{l}-1\right) / 9\) | ||
\(t_{20}\) | \(\left( p_{l}^{2}-p_{l}+1\right) / 12\) | ||
\(t_{02}\) | \(\left( q_{m}^{2}-q_{m}+1\right) / 12\) | ||
\(\mathcal {C}_{10}\) | \(\left( p_{l}-1\right) \left\{ 3 P_{l, m}+k_{m}\left( q_{m}-1\right) P_{l, m}^{y}+h_{l}\left( p_{l}-1\right) P_{l, m}^{x}\right\}\) | ||
\(\mathcal {C}_{01}\) | \(\left( q_{l}-1\right) \left\{ 3 Q_{l, m}+k_{m}\left( q_{m}-1\right) Q_{l, m}^{y}+h_{l}\left( p_{l}-1\right) Q_{l, m}^{x}\right\}\) | ||
\(\mathcal {C}_{11}\) | \(\left( p_{l}-1\right) \left( q_{l}-1\right) \left( P_{l, m}+Q_{l, m}\right)\) | ||
\(\mathcal {C}_{12}\) | \(p^{+} h_{l} P_{l, m}^{x} Q_{l, m}-\left[ 2\left( p_{l}-1\right) \left\{ 3 Q_{l, m}-\left( 1-q_{m}\right) k_{m} Q_{l, m}^{y}\right\} +3 p^{-} h_{l} Q_{l, m}^{x}\right] P_{l, m}\) | ||
\(\mathcal {C}_{21}\) | \(q^{+} k_{m} P_{l, m} Q_{l, m}^{y}-\left[ 2\left( q_{m}-1\right) \left\{ 3 P_{l, m}-\left( 1-p_{l}\right) h_{l} P_{l, m}^{x}\right\} +3 q^{-} k_{m} P_{l, m}^{y}\right] Q_{l, m}\) | ||
\(\mathcal {C}_{22}\) | \(q^{-} h_{l}^{2} P_{l, m}+p^{-} k_{m}^{2} Q_{l, m}\) | ||
\(\mathcal {C}_{20}\) | \(12\left( c^{2} h_{l}^{2} p^{+}-3\right) P_{l, m}^{2} Q_{l, m}+2 p^{+} h_{l}^{2}\left( P_{l, m}^{x}\right) ^{2} Q_{l, m}- \Bigg [4 h_{l} k_{m}\left( p_{l}-1\right) \left( q_{l}-1\right) P_{l, m}^{x y} Q_{l, m}+3\Bigg \{4 k_{m}\left( q_{m}- 1\right) P_{l, m}^{y}+4 h_{l}\left( p_{l}-1\right) P_{l, m}^{x}+q^{-} k_{m}^{2} P_{l, m}^{y y}+p^{-} h_{l}^{2} P_{l, m}^{x x}\Bigg \} Q_{l, m}-2 q^{+} k_{m}^{2} P_{l, m}^{y} Q_{l, m}^{y}\Bigg ] P_{l, m}\) | ||
\(\mathcal {C}_{02}\) | \(12\left( c^{2} k_{m}^{2} q^{+}-3\right) P_{l, m} Q_{l, m}^{2}+2 q^{+} k_{m}^{2} P_{l, m}\left( Q_{l, m}^{y}\right) ^{2}-\Bigg [4 h_{l} k_{m}\left( p_{l}-1\right) \left( q_{l}-1\right) P_{l, m} Q_{l, m}^{x y}+3\Bigg \{4 k_{m}\left( q_{l}- 1\right) Q_{l, m}^{y}+4 h_{l}\left( p_{l}-1\right) Q_{l, m}^{x}+q^{-} k_{m}^{2} Q_{l, m}^{y y}+p^{-} h_{l}^{2} Q_{l, m}^{x x}\Bigg \} P_{l, m}-2 p^{+} h_{l}^{2} P_{l, m}^{x} Q_{l, m}^{x}\Bigg ] Q_{l, m}\) |
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Jha, N., Verma, S. GAUSSIAN-RBF INTERPOLANT AND THIRD-ORDER COMPACT DISCRETIZATION OF 2D ANOMALOUS DIFFUSION-CONVECTION MODEL ON A MESH-MAPPED NON-UNIFORM GRID NETWORK. J Math Sci (2024). https://doi.org/10.1007/s10958-024-07014-2
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DOI: https://doi.org/10.1007/s10958-024-07014-2