I. Introduction
Near-surface nuclear explosions cause destructive damage and destroy to surroundings especially injuries and deaths to people, and the blast wave of nuclear explosion is one of the most serious destruction on target structure. When a nuclear bomb explodes in the air near the ground, the surrounding air is subjected to high temperature and pressure. Due to the low initial density and pressure of the surrounding air, the rarefaction wave propagates backward to the explosion products and the pressure at the point where the rarefaction wave arrives decreases rapidly, and the explosion products disperse rapidly around, forming a strong compression wave. The density, temperature, and pressure of the nearby atmosphere increase sharply. This change makes the shock wave have a strong destructive effect on the objects in the surroundings. The formation of nuclear explosion shock wave is the result of superposition of a series of compression waves. Under the condition of free propagation of shock wave, the blast shock wave intensity gradually attenuates with the distance, and finally attenuates to sound wave. When the shock wave impacts obstacles in the process of propagation, the reflection of shock wave will occur. When the incident wave is vertical to the surface of obstacles, the normal reflection of shock wave will be formed. To accurately evaluate the damage effect, the parameters of flow field after normal reflected shock wave should be investigated [1].