Abstract

The “super-gun” class of weaponry has been around for a long time. However, its unusual physics is largely ignored to this day in mainstream physics. We study an example of such a “super gun”, the “Paris gun”. We first look into the historic accounts of the firing distance of such a gun and try to reconcile it with our physical understanding of ballistics. We do this by looking into the drag component in the equations of motion for ballistic movement, which is usually neglected. The drag component of the equations of motion is the main reason for symmetry breaking in ballistics. We study ballistics for several air density profiles and discuss the results. We then proceed to look into the effects of muzzle velocity as well as mass and ground temperature on the optimal firing angle and firing range. We find that, even in the simplest case of fixed air density, the effects of including drag are far reaching. We also determine that in the “sensible” range of projectile mass, the muzzle velocity is the most important factor in determining the maximal firing range. We have found that even the simplest of complications that include air density, shifts the optimal angle from the schoolbook’s 45-degree angle, ground temperature plays a major role. While the optimal angle changes by a mere two degrees in response to a huge change in ground temperature, the maximal distance is largely affected. Muzzle velocity is perhaps the most influential variable when working within a sensible projectile mass range. In the current essay, this principle is described and examples are provided where students can apply them. For each problem, we provide both the force consideration solution approach and the energy consideration solution approach.

Highlights

  • One late-March morning in 1918, a high-pitched whistle pierced the streets of Paris, followed promptly by an explosion

  • Figure shows the four flavors discussed: Ballistic motion insimplest vacuum, angle for firing distance should no doubt depend on the ground temperature, even in the Ballistic motion a constant airthe density, and lastly, the andmakes barometric air density exponential case. in using temperature profile of exponential the atmosphere the temperature profiles dependence even more pronounced [6,7,8,9]

  • Figure displays the results of our numerical simulation for the initial conditions optimal angle for firing distance should no doubt depend on the ground temperature, even in the corresponding to the “Paris which are given in the aboveprofile

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Summary

Introduction

One late-March morning in 1918, a high-pitched whistle pierced the streets of Paris, followed promptly by an explosion. This came as a surprise to many Parisians, literally “out of the blue” [1] While they were used by that stage of World War I to explosions following the thunders of artillery, or the rickety humming of a biplane on a bomb run, this shelling was relatively stealthy, having little to no forewarning in the way of sound effects. This led to the widespread belief among the shelled citizenry that they were targeted by a high-flying Zeppelin air-ship [1,2]. The purpose of this work is to examine the effect of the atmosphere on a long-range shell [4,5,6,11]

Accounting for Air Resistance
Atmospheric or Barometric—Choose Your Flavor
Temperature
Specifications for the
So which angle isthere best?
Optimal angle
Findings
Conclusions
Full Text
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