Initial Conditions
For instance for
%MATHMODE{ \gamma=1.2,\; Q_0=50,\; E_0=50 }%
two different exact solutions under the assumption of a stationary detonation wave are plotted in
Fig. 2.1. Herein,
f denotes the
overdrive parameter, which is defined with respect to the corresponding Chapman-Jouguet velocity by
%MATHMODE{ f:=\left(\frac{d^\star}{d_{_{CJ}}}\right)^2=\left(\frac{D}{D_{_{CJ}}}\right)^2\;. }%
Figure 2.1: Stationary ZND solutions. The abscissae display the normalized distance behind detonation front. Top:
f =1.0, bottom:
f =1.8.
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RalfDeiterding - 14 Dec 2004