Photoelasticity

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A picture created using photoelasticity, of plastic utensils

Photoelasticity is an experimental method to determine the stress distribution in a material. The method is mostly used in cases where mathematical methods become quite cumbersome. Unlike the analytical methods of stress determination, photoelasticity gives a fairly accurate picture of stress distribution, even around abrupt discontinuities in a material. The method is an important tool for determining critical stress points in a material, and is used for determining stress concentration in irregular geometries.

History

The photoelastic phenomenon was first described by the Scottish physicist David Brewster[1] .[2] Photoelasticity developed at the beginning of the twentieth century with the works of E.G.Coker and L.N.G. Filon of University of London. Their book Treatise on Photoelasticity published in 1930 by the Cambridge Press became a standard text on the subject. Between 1930 and 1940 many other books in Russian, German and French appeared on the subject.

At the same time much development occurred in the field. Great improvements were achieved in the technique and the equipment was simplified. With the improvement in technology the scope of photoelasticity was extended to three dimensional state of stress. Many practical problems were solved using photoelasticity, and it soon became popular. A number of photoelastic laboratories were established in educational institutions and industries.

With the advent of digital polariscope using light-emitting diodes, continuous monitoring of structures under load became possible. This led to the development of dynamic photoelasticity. Dynamic photoelasticity has contributed greatly to the study of complex phenomena such as fracture of materials.

Principles

Tension lines in plastic protractor seen under cross-polarized light.

The method is based on the property of birefringence exhibited by certain transparent materials. Birefringence is a property where a ray of light passing through a birefringent material experiences two refractive indices. The property of birefringence (or double refraction) is observed in many optical crystals. Upon the application of stresses, photoelastic materials exhibit the property of birefringence, and the magnitude of the refractive indices at each point in the material is directly related to the state of stresses at that point. Information such as maximum shear stress and its orientation are available by analyzing the birefringence with an instrument called polariscope.

When a ray of light passes through a photoelastic material, its electromagnetic wave components gets resolved along the two principal stress directions and each of these components experiences different refractive indices due to the birefringence. The difference in the refractive indices leads to a relative phase retardation between the two components. Assuming a thin specimen made of isotropic materials, where two-dimensional photoelasticity is applicable. The magnitude of the relative retardation is given by the stress-optic law:[3]

\Delta ={\frac {2\pi t}{\lambda }}C(\sigma _{{1}}-\sigma _{{2}})

where Δ is the induced retardation, C is the stress-optic coefficient, t is the specimen thickness, σ1 and σ2 are the first and second principal stresses, respectively. The retardation changes the polarization of transmitted light. The polariscope combines the different polarization states of light waves before and after passing the specimen. Due to optical interference of the two waves, a fringe pattern is revealed. The number of fringe order N is denoted as

N={\frac {\Delta }{2\pi }}

which depends on relative retardation. By studying the fringe pattern one can determine the state of stress at various points in the material.

For materials that do not show photoelastic behavior, it is still possible to study the stress distribution in such materials. The first step is to build a model using photoelastic materials, which has similar geometry as the real structure to be investigated. The loading is then applied in the same way to ensure that the stress distribution in the model is similar to the stress in the real structure.

Isoclinics and isochromatics

Isoclinics are the loci of the points in the specimen along which the principal stresses are in the same direction.

Isochromatics are the loci of the points along which the difference in the first and second principal stress remains the same. Thus they are the lines which join the points with equal maximum shear stress magnitude.[4]

Two-dimensional photoelasticity

Photoelasticity

Photoelasticity can be applied both to three dimensional and two dimensional state of stress. But the application of photoelasticty to the three dimensional state of stress is more involved as compared to the state of two-dimensional or plane-stress system. So the present section deals with application of photoelasticity in investigation of a plane stress system. This condition is achieved when the thickness of the prototype is much smaller as compared to dimensions in the plane. Thus one is only concerned with stresses acting parallel to the plane of the model, as other stress components are zero. The experimental setup varies from experiment to experiment. The two basic kinds of setup used are plane polariscope and circular polariscope.

The working principle of two-dimensional photoelasticity allows the measurement of retardation, which can be converted to the difference between the first and second principal stress and their orientation. To further get values of each stress component, a technique called stress-separation is required.[5] Several theoretical and experimental methods are utilized to provide additional information to solve individual stress components.

Plane polariscope

The setup consists of two linear polarizers and a light source. The light source can either emit monochromatic light or white light depending upon the experiment. First the light is passed through the first polarizer which converts the light into plane polarized light. The apparatus is set up in such a way that this plane polarized light then passes through the stressed specimen. This light then follows, at each point of the specimen, the direction of principal stress at that point. The light is then made to pass through the analyzer and we finally get the fringe pattern. (e/_)

The fringe pattern in a plane polariscope setup consists of both the isochromatics and the isoclinics. The isoclinics change with the orientation of the polariscope while there is no change in the isochromatics.

Transmission Circular Polariscope
The same device functions as a plane polariscoe when quarter wave plates are taken aside or rotated so their axes parallel to polarization axes

Circular polariscope

In a circular polariscope setup two quarter-wave plates are added to the experimental setup of the plane polariscope. The first quarter-wave plate is placed in between the polarizer and the specimen and the second quarter-wave plate is placed between the specimen and the analyzer. The effect of adding the quarter-wave plate after the source-side polarizer is that we get circularly polarized light passing through the sample. The analyzer-side quarter-wave plate converts the circular polarization state back to linear before the light passes through the analyzer.

The basic advantage of a circular polariscope over a plane polariscope is that in a circular polariscope setup we only get the isochromatics and not the isoclinics. This eliminates the problem of differentiating between the isoclinics and the isochromatics.

Applications

Photoelasticity has been used for a variety of stress analyses and even for routine use in design, particularly before the advent of numerical methods, such as for instance finite elements or boundary elements.[6] Digitization of polariscopy enables fast image acquisition and data processing, which allows its industrial applications to control quality of manufacturing process for materials such as glass[7] and polymer.[8] Dentistry utilizes photoelasticity to analyze strain in denture materials.[9]

Photoelastic model to validate the stiffener model. Isochromatic fringe patterns around a steel platelet in a photo-elastic two-part epoxy resin.

Photoelasticity can successfully be used to investigate the highly localized stress state within masonry[10][11] [12] or in proximity of a rigid line inclusion (stiffener) embedded in an elastic medium.[13] In the former case, the problem is nonlinear due to the contacts between bricks, while in the latter case the elastic solution is singular, so that numerical methods may fail to provide correct results. These can be obtained through photoelastic techniques. Dynamic photoelasticity integrated with high-speed photography is utilized to investigate fracture behavior in materials.[14]

See also

References

  1. ↑ D. Brewster, Experiments on the depolarization of light as exhibited by various mineral, animal and vegetable bodies with a reference of the phenomena to the general principle of polarization, Phil. Tras. 1815, pp.29-53.
  2. ↑ D. Brewster, On the communication of the structure of doubly-refracting crystals to glass, murite of soda, flour spar, and other substances by mechanical compression and dilation, Phil. Tras. 1816, pp.156-178.
  3. ↑ Dally, J.W. and Riley, W.F., Experimental Stress Analysis, 3rd edition, McGraw-Hill Inc., 1991
  4. ↑ Ramesh, K., Digital Photoelasticity, Springer, 2000
  5. ↑ Fernandez M.S-B., Calderon, J.M.A., Diez, P.M.B and Segura, I.I.C, Stress-separation techniques in photoelasticity: A review. The Journal of Strain Analysis for Engineering Design, 2010, 45:1 [doi:10.1243/03093247JSA583]
  6. ↑ Frocht, M.M., Photoelasticity. J. Wiley and Sons, London, 1965
  7. ↑ Ajovalasit, A., Petrucci, G., Scafidi, M., RGB photoelasticity applied to the analysis of membrane residual stress in glass, Measurement Science and Technology, 2012, 23-2, no. 025601
  8. ↑ Kramer, S., Beiermann, B., Davis, D., Sottos, N., White, S., Moore, J., Characterization of mechanochemically active polymers using combined photoelasticity and fluorescence measurements, SEM Annual Conference and Exposition on Experimental and Applied Mechanics, 2010, 2, pp.896-907.
  9. ↑ Fernandes, C.P., Glantz, P.-O.J., Svensson, S.A., Bergmark, A. Reflection photoelasticity: A new method for studies of clinical mechanics in prosthetic dentistry Dental Materials, 2003, 19-2, pp.106-117.
  10. ↑ D. Bigoni and G. Noselli, Localized stress percolation through dry masonry walls. Part I - Experiments. European Journal of Mechanics A/Solids, 2010, 29, 291-298.
  11. ↑ D. Bigoni and G. Noselli, Localized stress percolation through dry masonry walls. Part II - Modelling. European Journal of Mechanics A/Solids, 2010, 29, pp.299-307.
  12. ↑ Bigoni, D. Nonlinear Solid Mechanics: Bifurcation Theory and Material Instability. Cambridge University Press, 2012 . ISBN 9781107025417.
  13. ↑ G. Noselli, F. Dal Corso and D. Bigoni, The stress intensity near a stiffener disclosed by photoelasticity. International Journal of Fracture, 2010, 166, 91–103.
  14. ↑ Shukla, A., High-speed fracture studies on bimaterial interfaces using photoelasticity - A review, Journal of Strain Analysis for Engineering Design, 2012, 36-2, 119-142.

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