![]() | ![]() | ![]() | 2.1 Characterization of the system of equations | Contents | Index |
has two distinct and real eigenvalues lambda1<0<lambda2,
such that we are dealing with a strictly hyperbolic system. We note that the celerity of gravitational waves c=sqrt(gh) takes the place the speed of sound has in gas dynamics and the Froude number Fr=|u|/c is the analogue to the Mach number.
Let us reduce the system to a diagonal form. For this we need the right eigenvectors ri satisfying J-lambdai*I)*ri=0 which form the columns of the following matrix R,
with the inverse
The diagonalization of the jacobian J (denoting Lambda=diag(lambda1,lambda2)) can be written as:
In the linear case, i.e. when the Jacobian is constant, we have
where R-1*dQ=dW defines the characteristic variables Wi which are advected along characteristic lines with respective wave speeds lambdai.
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![]() | ![]() | ![]() | 2.1 Characterization of the system of equations | Contents | Index |