“…In many cases the hypothesis makes it possible to select a unique solution of the problem [8,11]. In particular, this is the case for solutions to Equations (18) when the discontinuity structure is described by (19) with m = 0 [11].…”
Section: Long Waves In Nonlinear Media With Dispersion and Dissipatiomentioning
confidence: 99%
“…Riemann waves in elastic media were considered in [18, 3, 5, Chapter III]. In the case of small-amplitude waves in weakly anisotropic media it follows [15,17,19, Chapter 3; Section 7.4.5] from (1), (7) that…”
Section: Riemann and Shock Waves Solution Of Piston Problemmentioning
confidence: 99%
“…The set of values behind the shock u + for which the solution of the structure problem (19) exists for a given value ahead of the shock u − was investigated in [33,36]. It consist of intervals and separate points.…”
Section: Long Waves In Nonlinear Media With Dispersion and Dissipatiomentioning
One-dimensional selfsimilar problems for waves in an elastic half-space generated by a sudden change of the boundary stress (the "piston" problem) and problems of disintegration of an arbitrary discontinuity are considered. For the case when small-amplitude waves are generated in a medium with small anisotropy a qualitative analysis shows that these problems have nonunique solutions when it is assumed that the solutions involve Riemann waves and evolutionary discontinuities. The above-mentioned problems are considered as limits of properly formulated problems for visco-elastic media when the viscosity tends to zero or (what is the same) that time tends to infinity. It is numerically found that all above-mentioned inviscid solutions can represent the asymptotics of visco-elastic solutions. The type of asymptotics depends on those details of the visco-elastic problem formulation which are absent when formulating inviscid selfsimilar problems. Similar considerations are made for elastic media with dispersion along with dissipation which are manifested in small-scale processes. In such media the number of available asymptotics (as t → ∞) for the above-mentioned solutions depends on a relation between dispersion and dissipation and can be large. Thus, two possible causes for the nonuniqueness of solutions to the equations of elasticity theory are investigated.
“…In many cases the hypothesis makes it possible to select a unique solution of the problem [8,11]. In particular, this is the case for solutions to Equations (18) when the discontinuity structure is described by (19) with m = 0 [11].…”
Section: Long Waves In Nonlinear Media With Dispersion and Dissipatiomentioning
confidence: 99%
“…Riemann waves in elastic media were considered in [18, 3, 5, Chapter III]. In the case of small-amplitude waves in weakly anisotropic media it follows [15,17,19, Chapter 3; Section 7.4.5] from (1), (7) that…”
Section: Riemann and Shock Waves Solution Of Piston Problemmentioning
confidence: 99%
“…The set of values behind the shock u + for which the solution of the structure problem (19) exists for a given value ahead of the shock u − was investigated in [33,36]. It consist of intervals and separate points.…”
Section: Long Waves In Nonlinear Media With Dispersion and Dissipatiomentioning
One-dimensional selfsimilar problems for waves in an elastic half-space generated by a sudden change of the boundary stress (the "piston" problem) and problems of disintegration of an arbitrary discontinuity are considered. For the case when small-amplitude waves are generated in a medium with small anisotropy a qualitative analysis shows that these problems have nonunique solutions when it is assumed that the solutions involve Riemann waves and evolutionary discontinuities. The above-mentioned problems are considered as limits of properly formulated problems for visco-elastic media when the viscosity tends to zero or (what is the same) that time tends to infinity. It is numerically found that all above-mentioned inviscid solutions can represent the asymptotics of visco-elastic solutions. The type of asymptotics depends on those details of the visco-elastic problem formulation which are absent when formulating inviscid selfsimilar problems. Similar considerations are made for elastic media with dispersion along with dissipation which are manifested in small-scale processes. In such media the number of available asymptotics (as t → ∞) for the above-mentioned solutions depends on a relation between dispersion and dissipation and can be large. Thus, two possible causes for the nonuniqueness of solutions to the equations of elasticity theory are investigated.
“…Эти решения изучены в рабо-тах [21], [25]. Подставив (1.5) в (1.3), получим систему обыкновенных диффе-ренциальных уравнений для u α :…”
unclassified
“…Интегральные кривые волн Римана касаются собственных векторов матрицы R α,β и на плоскости (u 1 , u 2 ) образуют два ортогональных семейства кривых (рис. 1.1) [21], [22], [25]. Оси u 1 и u 2 для множества интегральных кривых являются осями симметрии.…”
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