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
Figure 2.1: Stationary ZND solutions. The abscissae display the normalized distance behind detonation front. Top: 
f =1.0, bottom: 
f =1.8. 
-- 
RalfDeiterding - 14 Dec 2004