I'm trying to find position as a function of time for a fired bullet, but I'm missing something because I end up with a dimensionalized exponent in the final result...
I start with
-F_d = ma (1)
F_d = drag force
m= mass of bullet
a= acceleration
assume F_d is porportional to the square of the velocity in (2)
F_d = C*rho*A*v^2/2 (2)
C = coefficient of drag
rho = density of medium
A= crass sectional area of bullet
v = velocity of bullet
by eq(1&2) with initial condition that @ t=0, v= v_o
C*rho*A/(2m)*INT(t,0)[dt] = -INT(v,v_o)[dv/v^2]
which yeilds
v= [C*rho*A/(2m)*t + 1/v_o]^(-1) eq(3)
for the sake of simplicity let
z=C*rho*A/(2m)
then
dx/dt = v
INT(x,0)[dx] = INT(t,0)[ v dt]
x= 1/z*ln( 1 + z*v_o*t)
Edit: Nevermind I exponentiated it after the previous step and just became confused...Its funny how writing it out a second time made me realize that.
Originally posted by joe shmoVery simply joe, you forgot to take into consideration the bullet's ogive when you made your calculations. I made the same mistake when i was your age.
I'm trying to find position as a function of time for a fired bullet, but I'm missing something because I end up with a dimensionalized exponent in the final result...
I start with
-F_d = ma (1)
F_d = drag force
m= mass of bullet
a= acceleration
assume F_d is porportional to the square of the velocity in (2)
F_d = C*rho*A*v^2/2 (2)
C ...[text shortened]... ep and just became confused...Its funny how writing it out a second time made me realize that.
GRANNY.
Originally posted by smw6869The shape of the bullet is accounted for in the coefficient of drag. The equation predicts the velocity of the bullet at a hundred yards within 0.5% of the manufacturers experimental results at that range...so i'm happy with it.
Very simply joe, you forgot to take into consideration the bullet's ogive when you made your calculations. I made the same mistake when i was your age.
GRANNY.
Originally posted by joe shmoI have nothing to contribute on this but have a question.
I'm trying to find position as a function of time for a fired bullet, but I'm missing something because I end up with a dimensionalized exponent in the final result...
I start with
-F_d = ma (1)
F_d = drag force
m= mass of bullet
a= acceleration
assume F_d is porportional to the square of the velocity in (2)
F_d = C*rho*A*v^2/2 (2)
C ...[text shortened]... ep and just became confused...Its funny how writing it out a second time made me realize that.
Does the drag coefficient differ depending on whether the bullet velocity exceeds Mach 1? The charts I have looked at indicate that muzzle velocity is >Mach 1 generally. So, MV would decrease to below Mach 1 at some point, and then, do drag considerations change at this point?
http://en.wikipedia.org/wiki/External_ballistics#The_transonic_problem
Originally posted by JS357Yeah, the coefficient of drag is a function of the Mach number. The coefficient is pretty constant for a projectile at M<.9, around Mach = 1 a sharp increase occurs, and with M>1 it decreases non-linearly, appearing to sort of leveling off after M>6.
I have nothing to contribute on this but have a question.
Does the drag coefficient differ depending on whether the bullet velocity exceeds Mach 1? The charts I have looked at indicate that muzzle velocity is >Mach 1 generally. So, MV would decrease to below Mach 1 at some point, and then, do drag considerations change at this point?
http://en.wikipedia.org/wiki/External_ballistics#The_transonic_problem
The equation I derrived doesnt take this curve into consideration(the Reynolds number was > 10^4, and M>2 througout the range distance). So I just used the maximum C around M =1.