Bullets - Then and Now - Simscale Incompressible Run

 In today's post, I would like to present you a comparative analysis of the aerodynamics of gas flow around medieval bullets and bullets that we deal with today. We will try to answer the question why the shape of the bullet has changed so significantly.

Bullets  - then and now in SimScale 

To simplify the analysis, our projectile will be stationary and the gas flowing around it will have the muzzle velocity of the bullet from the gun barrel (usually it is over 530 m / s). We assume a speed on Inlet of 570 m / s. As an outlet, we assume an atmospheric pressure of 1 bar ABS. The walls are defined as SLIP, which eliminates unnecessary turbulence on the border of the gas and the walls of the model. All defined boundary conditions are presented in the figure below.

BC's of Incompressible flow on SimScale 

As I mentioned before, we will be dealing with two types of bullets. Ball with a diameter of 24 mm and a pistol bullet with a diameter of also 24 mm.
Types of bullets used in simulation 

Due to the simplification of the analysis to the linear gas model, we assume the analysis as incompressible. We establish the turbulence model as k-omega SST.

Type of analysis definition in SimScale 

The figure below shows the model boundary conditions defined in the analysis.
BC's defined in SimScale 

As can be seen below, the shape of the projectile has a decisive influence on the distribution of gas velocity during flight. First of all, you can notice the different shape of the maximum speed as well as the shape and length of the formed "tail".For the ball, it can be seen that the fields of maximum velocity form "wings", while in the case of the classic shape, the maximum values are more "glued" to the solid.

Velocity distribution on cross-section in SimScale 

Also when it comes to the shape of the gas flow. It is more stabilized and more similar to laminar in the case of a bullet from "our time".
Vectors of gas flow shape in SimScale

The size and shape of the maximum velocities (over 600 m / s) are also different in both cases. The ball causes greater resistance and less stabilizes the gas stream, which means that the "cloud" of maximum values is greater for the medieval solution. The tail length for velocities above 500 m / s is also substantially different in the two cases. The tail of the ball is several times longer than that of the pistol bullet.

Velocity isosurfaces in SimScale









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