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Experimental Mechanics @
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EM
Basics: Spectral Contents Analysis in PEA |
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Earlier developments were by Redner1
and by Sanford and Igenyar2. Essentially, for the point of
interest the light intensity is collected over a range of wavelengths to form
a spectrum. A theoretical model of the spectral contents of the point in a
fringe pattern is fitted to the experimental data using the fringe order as
the fitting parameter. The maximum fringe order that can be recognised is approximately equal to the number of
wavelengths at which intensity information is collected 3,4. Hence an RGB camera can be used to obtain
fringe orders up to about three5. No information about isoclinic angle is
available. Recent
work has produced significantly faster algorithms which do not need any a
priori knowledge of the range of fringe order being measured6. The University
of Sheffield has implemented the technology in a number of novel instruments. |
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Spectra
for fringe orders of 0.5, 2.25, & 5.75 |
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Obliquerscope
for measuring individual principal stresses in reflection coatings using
spectral contents analysis. |
1.
Redner, A.S., 1984,
‘Photoelastic measurements by means of computer assisted spectral contents
analysis’ Proc. 5th Int. Conf. Experimental Mechanics, Montreal, pp.421-7. 2.
Sanford, R.J., Igenyar,
V., 1985, ‘The measurement of the complete photoelastic fringe order using a
spectral scanner, Proc. SEM Spring Conf. Experimental Mechanics, pp. 160-8. 3.
Carazo-Alvarez, J., Haake, S.J., Patterson, E.A., 1994, 'Completely automated
photoelastic fringe analysis', Optics & Lasers in Engineering, 21:133-149
4.
Bhat, G.K., Redner, A.S., 1999, ‘Minimizing number of images required
in photoelastic multi-wavelength and phase-shifting analysis’,
Proc. SEM Spring Conf. Theor. Exptl.
& Comp. Mech., pp. 541-3. 5.
Petrucci etc 6. Pacey, M.N., Wang, X.Z., Haake, S.J., Patterson, E.A., 1999,‘The
application of evolutionary and maximum entropy algorithms to photoelastic
spectral analysis’, Experimental Mechanics, 38(4): 265-273. |
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