Second order dynamic mesh technique is employed to solve gas dynamic equations which represent the different aspects of hyperbolic (nonlinear) equations. The value of the density, velocity, pressure and internal energy of the gas at t= 0.15s are computed using dynamic mesh technique and uniform mesh method. Their graphical comparison is given in £gures 1-4. We observe that the dynamic mesh graphs are more smooth than uniform mesh graphs. Therefore it is clear that the dynamic mesh technique gives better results than standard uniform mesh method.