By Helena Jin, Sanichiro Yoshida, Luciano Lamberti, Ming-Tzer Lin
Advancement of Optical equipment 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 crucial zone of analysis and engineering. the gathering provides early findings and case reports on a variety of optical equipment starting from conventional photoelasticity and interferometry to more moderen DIC and DVC suggestions, and comprises papers within the following common technical examine parts:
Advanced optical interferometry
Developments in picture correlation (Digital &Volumetric )
Full box Methods
Novel Optical equipment for Stress/Strain Analysis
Advances in Optical tools
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Additional resources for Advancement of Optical Methods in Experimental Mechanics, Volume 3: Proceedings of the 2015 Annual Conference on Experimental and Applied Mechanics
Cox, The elasticity and strength of paper and other fibrous materials. Br. J. Appl. Phys. 3, 72–79 (1952) 4. R. Piggott, Failure processes in the fibre-polymer interphase. Compos. Sci. Technol. 42, 57–76 (1991) 5. A. R. Tyson, Tensile properties of fibre-reinforced metal: copper/tungsten and copper/molybdenum. J. Mech. Phys. Solids 13, 329–350 (1965) 6. M. A. A. J. R. Jones, Measurement of micro stress fields in epoxy matrix around a fibre using phase-stepping automated photoelasticity. Compos.
In some tests, additional pressed pellets of PETN were also epoxied to the RP-2 detonator. In general, only 10 % of the available chemical energy of the high explosive contributed to the strength of the blast wave. Additional shock tube characterization, including evidence of boundary layer growth under certain conditions, is discussed elsewhere . After explosive detonation, a planar blast wave is generated due to the shock tube confinement. This blast wave propagates the length of the tube until impinging upon the rupture disc.
The explosive charge consisted of an RP-2 with an additional 40-mg pellet of pressed PETN. 3 Stereomicroscope DIC The stereomicroscope DIC system was positioned to view the rupture disc installed at the shock tube exit (Fig. 3). The system was mounted on an optical table perpendicular to the shock tube axis to protect the system from direct exposure to the gas-dynamic shock and explosive detonation product gases after the rupture event. An Olympus SZX16 microscope was mounted horizontally, coupling two Shimadzu HPV-2 high-speed cameras to its optical ports (Fig.