Download Dynamics of Detonations and Explosions: Detonations (Vol. by A. L. Kuhl, J. C. Leyer, A. A. Borisov, W. A. Sirignano PDF

By A. L. Kuhl, J. C. Leyer, A. A. Borisov, W. A. Sirignano

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Additional info for Dynamics of Detonations and Explosions: Detonations (Vol. 133, Progress in Astronautics and Aeronautics)

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The normal direction to the surface at u is given precisely by u, thus we need to know the local behaviour around u in the orthogonal directions to u. 1. Let u be an eigenvector of A associated with the eigenvalue λ . The spectrum of A and that of J p (u) are related in the following way: 1. An eigenvalue λ of A corresponds to the eigenvalue 0 for J p (u) 2. An eigenvector w associated with μ of A corresponds to the eigenvector I − P(u) w with eigenvalue λ −μ u p for J p (u) and this includes the particular case where μ = λ , the case of complex eigenvalues and eigenvectors, as well as the case of generalized eigenvectors.

6 and compare the actual number of iterations with the a priori estimates. 5 Repeat the previous exercise using now any of the other iterative methods and compare. 01y = 6 , 208 404 , y= . Solution: x = 404 , y = −200 . Solution: x = − 3 3 40 3 Linear Systems: Numerical Simulations Compare with the solution given by other iterative methods of your choice and also with the exact solution. 9). Keep in mind that, since the matrices are symmetric we may use them as matrix M. 51) to compute the optimal values of τ and α .

Even if we have several eigenvectors linearly independent (say {ui }qi=1 , where q = mg ) associated with the eigenvalue, any solution of the q form x(t) = ∑ ai (t)ui is a constant: substituting in Eq. 1), we have i=1 q ∑ a˙i (t)ui + i=1 λmin q λmin q a (t)u − i i ∑ ∑ ai (t)ui = 0 x p i=1 x p i=1 q ⇐⇒ ∑ a˙i (t)ui = 0 ⇐⇒ ∀i, a˙i = 0. 19) i=1 Thus, any point of eigenspace Umin is a fixed point. We suppose thus that a general solution has components outside Umin . Those can be of two types: outside U¯min and inside U¯min − Umin .

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