<p><BR/>Replying to:<BR/><DIV CLASS='Discussion_PostQuote'>Forgive my obstinacy but. wouldn't the gas expand in both directions until the projectile exits the muzzle end of the barrel?Replying to:<BR/><DIV CLASS='Discussion_PostQuote'></p><p>No. There is high pressure, hot rapidly expanding gas behiing the projectile (while in the bore) and much cooler, lower pressure gas being compressed and expelled from the barrel ahead of the projectile. The pressure behind the projectile, due to combustion of the propellant, is MUCH higher and the gas is MUCH hotter than the gas in front of the projectile. Flame temperatures of the propellants involved are on the order of 3500K.</p><p>Replying to:<BR/><DIV CLASS='Discussion_PostQuote'> And if this is the case then, depending on how long the barrel were wouldn't the accelerations which are high, try to move the umbrella down at the same rate as the projectile moves up and thus create its own reaction mass/force with a portion of it's acceleration over a time transient? </DIV></p><p>One way to look at this problem is to consider the effect of the gas pressure on the projectile and on the breech of the gun. The pressures are the same. The effective areas are the same. There is a frictional component between the projectile and the bore which is reacted as a retarding force on the gun,but that can be safely neglected in a first-order analysis. So basically the force on the projectile equals the force on the gun, although they are in opposite directions. But the gun is usually MUCH more massive than the projectile, and so the acceleration of the gun is correspondingly less. When the bullet exits the muzzle, the gas from the combustion of the propellant expands very rapidly and exits the muzzle at the local speed of sound (in the hot gas) which adds substantially to the momentum of the material expelled from the barrel (projectile plus gas) and contributed to recoil. But what is conserved is momentum, not acceleration or speed. The rearward momenteum of the gun is equal to the forward momentum of the projectile and expelled gasses. Because the gun is MUCH heavier than the projectile and gasses, the speed of the gun is MUCH lower. (Momentum is mass times velocity).</p><p> Replying to:<BR/><DIV CLASS='Discussion_PostQuote'> Also I'm not positive what the shock wave shape of a parachute moving thru air is but isn't its reaction force more a function of the volume of air that the canopy displaces with the velocity of the of the parachute being more a limited factor in the equation past an optimal acceleration? In short if the equation for the distribution of the forces with respect to time were plotted wouldn't the up (parachute reaction) side be an exponentially increasing force while the down (projectile mass) side be more constant and thus create a net gain? <br />Posted by BBRAZEAU</DIV></p><p>The reaction force of a parachute is a funtion of two major things. One is velocity, which determines dynamics pressure (dynamic pressure is 1/2*air density*velocity^2). The other is projected area normala to the velocity. The reation force from the parachute, since the area is basically constant, will be primarily dependent on the velocity. </p><p>I don't understand your last sentence. But at the moment that the projectile leaves the barrel, if one assumes that the parachute is stationary with respect to the atomosphere, the reaction will be determined completely by conservation of momentum, the momentum of the projectile and expelled gasses, and there will be no aerodynamic effect. Aerodynamics will only be non-zero once the parachute has accelerated and has a velocity relative to the air, which creates drag. </p><p><br /><br /> </p> <div class="Discussion_UserSignature"> </div>