Abstract
A new method that combines phase shifting photoelasticity and transmission Coherent Gradient Sensing (CGS) is developed to determine the tensorial stress field in thin plates of photoelastic materials. A six step phase shifting photoelasticity method determines principal stress directions and the difference of principal stresses. The transmission CGS method utilizes a standard four step phase shifting method to measure the x and y first derivatives of the sum of principal stresses. These stress derivatives are numerically integrated using a weighted preconditioned conjugate gradient (PCG) algorithm, which is also used for the phase unwrapping of the photoelastic and CGS phases. With full-field measurement of the sum and difference of principal stresses, the principal stresses may be separated, followed by the Cartesian and polar coordinate stresses using the principal stress directions. The method is demonstrated for a compressed polycarbonate plate with a side V-shaped notch. The experimental stress fields compare well with theoretical stress fields derived from Williams solution for a thin plate with an angular corner.
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Abbreviations
- A x,y :
-
magnitude of \(\boldsymbol{E}\) along x and y axes
- c i :
-
constant of integration
- C :
-
relative photoelastic constant
- C f :
-
fitting parameter for V-notch stress solution
- d shear :
-
shearing distance in CGS
- D 1,2 :
-
absolute photoelastic constants
- D 3,4 :
-
photoelastic constants related to D 1,2, ν, E, and n
- E :
-
Young’s modulus
- \(\boldsymbol{E}\) :
-
electric field vector
- I :
-
intensity (irradiance)
- h :
-
specimen thickness
- h d :
-
phase discontinuity height
- k :
-
wave number
- n o :
-
isotropic index of refraction
- n i :
-
principal index of refraction (\(i=\lbrace 1,2,3\rbrace\))
- N :
-
photoelastic fringe order
- p :
-
pitch of Ronchi gratings
- R x,y :
-
reflection coefficients along x and y directions for the non-polarizing beamsplitter
- T x,y :
-
transmission coefficients along x and y directions for the non-polarizing beamsplitter
- α :
-
isoclinic angle
- β :
-
angle of ouput polarizer
- γ :
-
small angle of first order diffraction in CGS
- δ :
-
isochromatic phase
- \(\tilde{{\mathit\Delta}}\) :
-
Ronchi grating separation
- θ :
-
polar angle
- λ :
-
wavelength
- ν :
-
Possion’s ratio
- ξ :
-
fast axis angle of input λ/4 plate
- ρ :
-
angle of input polarizer
- σ 1,2 :
-
principal stresses
- σ ab :
-
in-plane stresses (Cartesian for \((a,b)=\lbrace1,2\rbrace\) and polar for \((a,b)=\lbrace r,\theta\rbrace\))
- ϕ :
-
fast axis angle of output λ/4 plate
- ϕ x,y :
-
arbitrary phase constant in initial electric field
- φ diff :
-
phase related to σ 1 − σ 2
- φ sum :
-
phase related to σ 1 + σ 2
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Acknowledgements
We gratefully acknowledge the support of the National Science Foundation (DMR # 0520565) through the Center for Science and Engineering of Materials (CSEM) at the California Institute of Technology, of the American Society for Engineering Education National Defense Science and Engineering Graduate (NDSEG) Fellowship Program, and of the National Science Foundation Graduate Research Fellowship Program. We thank Prof. E.A. Patterson for valuable discussions during this project.
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Kramer, S.L.B., Mello, M., Ravichandran, G. et al. Phase Shifting Full-Field Interferometric Methods for Determination of In-Plane Tensorial Stress. Exp Mech 49, 303–315 (2009). https://doi.org/10.1007/s11340-009-9230-0
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DOI: https://doi.org/10.1007/s11340-009-9230-0