By Helena Jin, Sanichiro Yoshida, Luciano Lamberti, Ming-Tzer Lin
Advancement of Optical tools in Experimental Mechanics, quantity three of the court cases of the 2015SEM Annual Conference& Exposition on Experimental and utilized Mechanics, the 3rd quantity of 9 from the convention, brings jointly contributions to this significant quarter of study and engineering. the gathering provides early findings and case reports on quite a lot of optical equipment starting from conventional photoelasticity and interferometry to more moderen DIC and DVC concepts, and contains papers within the following basic technical study components:
Advanced optical interferometry
Developments in photo correlation (Digital &Volumetric )
Full box Methods
Novel Optical equipment for Stress/Strain Analysis
Advances in Optical tools
Read or Download Advancement of Optical Methods in Experimental Mechanics, Volume 3: Proceedings of the 2015 Annual Conference on Experimental and Applied Mechanics PDF
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Additional info for Advancement of Optical Methods in Experimental Mechanics, Volume 3: Proceedings of the 2015 Annual Conference on Experimental and Applied Mechanics
Shear tests were conducted on a 530 kN servo-hydraulic Tinius Olsen load frame. 5 mm/min was applied to the impactor. The displacement was increased at a constant rate until specimen failure. Two specimens for each layup were tested for repeatability assessment. To compensate limitations of 2D characterization, coupons of different widths were considered to capture potential edge effects. It was shown that, with the width increase, the results of testing, quantified by maximal breaking load, quickly converge to an asymptotic solution.
6) where, Ci is the stress-optic coefficient for each wavelength. Substituting Eq. 5) into Eq. 7) Phase unwrapping can be performed by searching fringe order Ni , which is consistent with Eq. 7). 8) By finding the set of fringe orders Ni , which make the value of E minimum, the unwrapped phase ı’i can be obtained using Eq. 5). In searching the set of Ni , taking the inequalities N1 > N2 > N3 into account, the set of Ni that does not satisfy the inequalities is excluded. 9) 30 T. Sakai et al. Fig.
Between 2 quarterwave plates, a birefringent material as a single fiber embedded epoxy resin with retardation ı whose fast axis subtends as angle ® with the ox axis. , the isoclinic parameter. Similarly, the retardation • of the specimen, that is, the isochromatic parameter relates the principal stress difference as ı D 2N D2 C d . 1) where N is the isochromatic fringe order, C¢ is the stress-optic coefficient, d the thickness of the specimen, œ is the wavelength of the monochromatic incident light, and 1 and 2 are the principal stresses.