Mechanics of Biological Systems and Materials, Volume 4: by Morteza Khaleghi, Ivo Dobrev (auth.), François Barthelat, PDF

By Morteza Khaleghi, Ivo Dobrev (auth.), François Barthelat, Pablo Zavattieri, Chad S. Korach, Barton C. Prorok, K. Jane Grande-Allen (eds.)

ISBN-10: 3319007769

ISBN-13: 9783319007762

ISBN-10: 3319007777

ISBN-13: 9783319007779

Mechanics of organic platforms and fabrics, quantity four: Proceedings of the 2013 Annual convention on Experimental and utilized Mechanics, the fourth quantity of 8 from the convention, brings jointly contributions to this significant region of study and engineering. the gathering provides early findings and case stories on quite a lot of parts, together with:

Structure-Function & layout of sentimental organic Tissues

Soft Tissue Biomechanics: Nanoscale to Physiological Control

Bone Mechanics

Biomimetic Materials

Residual Stresses in organic Materials

Cells

Cellulose Materials

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Additional info for Mechanics of Biological Systems and Materials, Volume 4: Proceedings of the 2013 Annual Conference on Experimental and Applied Mechanics

Sample text

In direct methods, cohesive law is essentially obtained from the results of fracture experiments [11–13, 20–22] and using the concept of J-integral approach. While these techniques are valuable, they, however, are expensive in terms of experimental procedure and often need additional experimental setup. The inverse methods represent another type of approach which consists in modeling the experiment using finite elements, and identifying the parameters of the cohesive law which produce the best match between the model and the experiments [11, 23–25].

We further discuss the validity of this assumption in Sect. 3. Since the substrates are considered to be rigid, they only rotate about the hinge point O located at the end of the beams (Fig. 2). 1) Where x is the position from the hinge point, L is the distance from the line of action of the pulling force to the hinge point O, and Δ is the pins separation displacement. 2) 0 Where B is the thickness of the substrates, b is the length of the bond line, and tðxÞ denotes the traction function which is unknown and is to be determined.

In order to meet this assumption, the deformation of the substrate during the course of the loading should be negligible compared to that of the adhesive layer. We further discuss the validity of this assumption in Sect. 3. Since the substrates are considered to be rigid, they only rotate about the hinge point O located at the end of the beams (Fig. 2). 1) Where x is the position from the hinge point, L is the distance from the line of action of the pulling force to the hinge point O, and Δ is the pins separation displacement.

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Mechanics of Biological Systems and Materials, Volume 4: Proceedings of the 2013 Annual Conference on Experimental and Applied Mechanics by Morteza Khaleghi, Ivo Dobrev (auth.), François Barthelat, Pablo Zavattieri, Chad S. Korach, Barton C. Prorok, K. Jane Grande-Allen (eds.)


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