Abstract:Recent experimental and numerical studies of weak Mach reflections are examined. It is shown that the fundamental reason for the von Neumann paradox is that his theory of Mach reflection is based on the assumption that the flow downstream of the reflected wave and the Mach shock near the wave triple point is uniform. The assumption is shown to be valid for strong Mach reflection which agrees with experiment, but invalid for weak Mach reflection whicb does not agree with experiment. It is also shown that viscou… Show more
“….." bivariate form B~satisiies'the "bounds ' --' '~~~~~-In order to show t@ we construct sub-and super-solutions. We shalI show that for every J < c and M > I/e, the functions J@ -g and M@ -g are sub-and super-solutions respectively to (23), where~satisfies (15). This is equivalent to showing that Jand M@ are sub-and super-solutions to…”
Section: Theorem 13 For Every F C W Them Ezids a Function V E %$ Sumentioning
confidence: 99%
“…In particular, we may now suppose f is given by (15), then the solution of (21), which we have found, is the solution we want, save for the possibility that Bg does not coincide with B for our weak solution v. We rule this out in the next section.…”
Section: Theorem 13 For Every F C W Them Ezids a Function V E %$ Sumentioning
confidence: 99%
“…The first integral in (33) can be estimated using the fact that ii is bounded from below by e & Therefore, there exists a Cl >0 such that where -the bivariate forna B is defined by (16) and f by (15 The theory in this paper also maybe extended to unbounded domains 0:…”
Section: Theorem 12 the Operator T Is Coercivementioning
confidence: 99%
“…We handle this by supposing~to be an arbitrary function, in (21), (not related to g by (15)), and then letting~be the function defined by (15) to obtain the existence of a weak solution for problem (14).…”
Section: Definition 3 Let F G L'(q) a Function V E %! Is Called A Wmentioning
confidence: 99%
“….. gas dynamics equations iq the form of a particularly simple nonlinearity, and may give a description of the transition between regular and Mach reflection for weak" shocks. This phenomenon has been extensively studied numerically and experimentally (see, for example, [5], [15]); however, there are only a few related aimIytical results. We mention Morawetz's study of a full-pot entialequation model, [10], which is in the same spirit as the TSD model.…”
We prove a theorem on existence of a weak solution of the Dirichlet problem for a quasilinear elliptic equation with a degeneracy on one part of the boundary. The degeneracy is of a type ("Keldysh type") associated with singular behavior -blow-up of a derivativeat the boundary. We define an associated operator which is continuous: pseudo-monotone and coercive and show that a weak.solution &playing singular behavior at the boundary e~sts.
“….." bivariate form B~satisiies'the "bounds ' --' '~~~~~-In order to show t@ we construct sub-and super-solutions. We shalI show that for every J < c and M > I/e, the functions J@ -g and M@ -g are sub-and super-solutions respectively to (23), where~satisfies (15). This is equivalent to showing that Jand M@ are sub-and super-solutions to…”
Section: Theorem 13 For Every F C W Them Ezids a Function V E %$ Sumentioning
confidence: 99%
“…In particular, we may now suppose f is given by (15), then the solution of (21), which we have found, is the solution we want, save for the possibility that Bg does not coincide with B for our weak solution v. We rule this out in the next section.…”
Section: Theorem 13 For Every F C W Them Ezids a Function V E %$ Sumentioning
confidence: 99%
“…The first integral in (33) can be estimated using the fact that ii is bounded from below by e & Therefore, there exists a Cl >0 such that where -the bivariate forna B is defined by (16) and f by (15 The theory in this paper also maybe extended to unbounded domains 0:…”
Section: Theorem 12 the Operator T Is Coercivementioning
confidence: 99%
“…We handle this by supposing~to be an arbitrary function, in (21), (not related to g by (15)), and then letting~be the function defined by (15) to obtain the existence of a weak solution for problem (14).…”
Section: Definition 3 Let F G L'(q) a Function V E %! Is Called A Wmentioning
confidence: 99%
“….. gas dynamics equations iq the form of a particularly simple nonlinearity, and may give a description of the transition between regular and Mach reflection for weak" shocks. This phenomenon has been extensively studied numerically and experimentally (see, for example, [5], [15]); however, there are only a few related aimIytical results. We mention Morawetz's study of a full-pot entialequation model, [10], which is in the same spirit as the TSD model.…”
We prove a theorem on existence of a weak solution of the Dirichlet problem for a quasilinear elliptic equation with a degeneracy on one part of the boundary. The degeneracy is of a type ("Keldysh type") associated with singular behavior -blow-up of a derivativeat the boundary. We define an associated operator which is continuous: pseudo-monotone and coercive and show that a weak.solution &playing singular behavior at the boundary e~sts.
We prove a theorem on existence of a weak solution of the Dirichlet problem for a quasilinear elliptic equation with a degeneracy on one part of the boundary. The degeneracy is of a type (``Keldysh type'') associated with singular behavior blow-up of a derivative at the boundary. We define an associated operator which is continuous, pseudo-monotone and coercive and show that a weak solution displaying singular behavior at the boundary exists. 1996 Academic Press, Inc. Contents 1. Introduction. 2. The degenerate boundary and the comparison principle. 2.1. Singularities in the solution. 2.2. The comparison principle. 3. A linear model equation. 3.1. Existence of a weak solution in a Hilbert space. 4. The weighted Sobolev space setting. 4.1. Modification of the problem. 4.2. Embeddings of the Hilbert space H : . 4.3. Weak formulation of the modified problem. 5. Existence of a weak solution. 5.1. Properties of T. 5.2. Bounds on the weak solution. 6. Conclusions. Appendix: Compactness of the embedding.
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