1966
DOI: 10.1115/1.3625016
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Introduction to the Mechanics of a Continuous Medium

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Cited by 73 publications
(92 citation statements)
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“…13 demonstrate a good agreement of the experimental data with our theoretical model at short distances from the crack tips. Some disagreement between experimental and theoretical results at distances away from the crack tips is due to an asymptotical character of the expressions used for stress tensor components [41] that are valid only for short distances. Fig.13(a) shows that external compressive stress partially compensates for tensile residual stress acting near the tip of crack 1.…”
Section: Theoretical Model Of Photoacoustic Thermoelastic E® Ect Nearmentioning
confidence: 99%
“…13 demonstrate a good agreement of the experimental data with our theoretical model at short distances from the crack tips. Some disagreement between experimental and theoretical results at distances away from the crack tips is due to an asymptotical character of the expressions used for stress tensor components [41] that are valid only for short distances. Fig.13(a) shows that external compressive stress partially compensates for tensile residual stress acting near the tip of crack 1.…”
Section: Theoretical Model Of Photoacoustic Thermoelastic E® Ect Nearmentioning
confidence: 99%
“…(8) Heat transfer, associated with diffusion of heat dQ from region of higher temperature T h to lower temperature T l , with entropy change:…”
Section: Entropy In Friction and Wear Processesmentioning
confidence: 99%
“…The equation of motion and the geodesic line equation in nonmetrical manifold can be derived from the Sedov variational principle [13] which is the generalization of the least action principle: δS(q) + δW (q) = 0 (15) where S(q) is the holonomic functional called action andW (q) is the nonholonomic functional, i.e. δδ ′W ≡ δ ′ δW .…”
Section: Appendixmentioning
confidence: 99%
“…As the result the motion of the systems subjected to dissipative forces on the metric manifold is equivalent to the free motion of the test particle on the nonmetric (generalized path) manifold. Note that the equation of motion and the geodesic line equation in the nonmetrical manifold can be derived from Sedov variational principle [13] which is the generalization of the least action principle.…”
Section: Introductionmentioning
confidence: 99%
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