Integrated Photoelasticity |
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Page 58
... perpendicular to uv , the amplitude ratio of the vibrations u and v is constant . The transformation of polarization of the incident light by a two - dimensional photoelastic model is carried out by moving the point , which represents ...
... perpendicular to uv , the amplitude ratio of the vibrations u and v is constant . The transformation of polarization of the incident light by a two - dimensional photoelastic model is carried out by moving the point , which represents ...
Page 60
... perpendicular to the secondary principal directions at this point . By the aid of the j - circle method Kuske has shown that for a nonhomogeneous photoelastic medium it is always possible to find two directions of the polarizer ...
... perpendicular to the secondary principal directions at this point . By the aid of the j - circle method Kuske has shown that for a nonhomogeneous photoelastic medium it is always possible to find two directions of the polarizer ...
Page 180
... perpendicular to the ray of light . The secondary principal directions form an angle of 45 ° with the rod axis z , and algebraically the area of the diagram of 12 equals zero ( Fig . 10-6 ) . Thus , by passing the light through the rod ...
... perpendicular to the ray of light . The secondary principal directions form an angle of 45 ° with the rod axis z , and algebraically the area of the diagram of 12 equals zero ( Fig . 10-6 ) . Thus , by passing the light through the rod ...
Contents
CHAPTER | 1 |
OPTICAL THEORY OF NONHOMOGENEOUS PHOTOELASTIC | 15 |
CHAPTER 3 | 38 |
Copyright | |
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angle of rotation anisotropy Application axial axis axisymmetric azimuth birefringent plate bisector calculated characteristic angle characteristic parameters characteristic phase retardation coefficients coincide considered constant cos² cylindrical shell dz dz elastic emergent light equations of photoelasticity Euler angles experimental data Figure hole incident light integral phase retardation integral Wertheim law integrated photoelasticity inverse problem investigating k₁ latter layer light ellipse light passes light ray light vector magnetophotoelasticity matrix membrane stresses middle surface Mueller matrix nomograph normal incidence optical anisotropy optical equations optical phenomena perpendicular photoelastic medium plane of polarization plane-polarized Poincaré sphere point of entrance polariscope primary characteristic directions ray of light reflection polariscope scattered light method secondary characteristic directions secondary principal directions secondary principal stress shear stress shells of revolution sin² Stokes parameters stress concentration stress distribution stress resultants thickness three-dimensional photoelastic transformation unitary unitary matrix values Verdet constant wavelength Wulff grid