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Helena Jin, Cesar Sciammarella, Sanichiro Yoshida, Luciano's Advancement of Optical Methods in Experimental Mechanics, PDF

By Helena Jin, Cesar Sciammarella, Sanichiro Yoshida, Luciano Lamberti

ISBN-10: 3319415999

ISBN-13: 9783319415994

ISBN-10: 3319416006

ISBN-13: 9783319416007

Advancement of Optical tools in Experimental Mechanics, quantity three: complaints of the 2014 Annual convention on Experimental and utilized Mechanics, the 3rd quantity of 8 from the convention, brings jointly contributions to this significant region of analysis and engineering.  the gathering offers early findings and case reviews on quite a lot of optical tools starting from conventional photoelasticity and interferometry to more moderen DIC and DVC options, and contains papers within the following common technical examine areas:

·        complex optical tools for frontier applications

·        complex optical interferometry

·        Optical size structures utilizing polarized light

·        Optical tools for complicated production

·        electronic picture correlation

·        Optical equipment on the micro/nano-scale

·        third-dimensional imaging and volumetric correlation

·        Imaging equipment for thermomechanics applications

·        Opto-acoustical equipment in experimental mechanics

·        Optical measurements in difficult environments

·        Optical tools for inverse problems

·        Advances in optical methods

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Additional resources for Advancement of Optical Methods in Experimental Mechanics, Volume 3: Proceedings of the 2016 Annual Conference on Experimental and Applied Mechanics 

Example text

12a) and 17 orders in the v-pattern (Fig. 12c). Therefore, the horizontal diameter of the disk will expand by about 5 μm under the action of the applied load while the vertical diameter of the specimen will contract by about 21 μm. The computer generated patterns have been obtained utilizing a solution taken from the theory of elasticity [21]. The difference between theory and experiment is due to the modality of load application. A. Sciammarella and L. 222 μm 3300 N Fig. 12 (a) Recorded u-pattern; (b) computer generated u-pattern; (c) recorded v-pattern; (d) computer generated v-pattern Fig.

It is well known that the lower limit of Eq. 61) is obtained when the window function is a Gaussian function. In the present case, the sensor gives Ip(x, y) and it is necessary to locally smooth this function by introducing a band pass filter that will render the approximated energy ratio defined in Eq. 60) optimum. Hence, in the previously derived equations the recorded Ip(x, y) can be replaced by: I pb ðx; yÞ ¼ I p ∗∗gðx; yÞ ð1:62Þ where the upper script b indicates a band pass filtered version of the recorded signal and g(x, y) is a selected band pass filter.

Instead of seeking to achieve smoothing by doing the differentiation over a large area, here the differentiation is done over a very small area, with controlled smoothing achieved by filtering both the raw phase data and the subsequent strain results. 32 J. S. Schajer Fig. 5 Study of the effects of strain filtering template size and number of repetitions. From left to right, the template sizes in each column are 3 Â 3, 9 Â 9 and 15 Â 15. From top to bottom, the numbers of repetitions in each row are 1, 5, 10 and 15.

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Advancement of Optical Methods in Experimental Mechanics, Volume 3: Proceedings of the 2016 Annual Conference on Experimental and Applied Mechanics  by Helena Jin, Cesar Sciammarella, Sanichiro Yoshida, Luciano Lamberti


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