With what speed does the projectile leave the barrel

In summary, the conversation discusses the use of a toy gun that projects a 4.8 g soft rubber sphere using a spring. The spring constant is 12.0 N/m, the barrel is 14.3 cm long, and there is a constant frictional force of 0.028 N between the barrel and projectile. The speed at which the projectile leaves the barrel can be calculated using the formula V_f = sqrtKX_i^2 - 2fL/m, which gives an answer of 2.98 m/s when the spring is compressed 6.5 cm. The conversation also mentions the use of energy conservation as the only applicable method to solve this problem.
  • #1
BunDa4Th
188
0
A toy gun uses a spring to project a 4.8 g soft rubber sphere horizontally. The spring constant is 12.0 N/m, the barrel of the gun is 14.3 cm long, and a constant frictional force of 0.028 N exists between barrel and projectile. With what speed does the projectile leave the barrel if the spring was compressed 6.5 cm for this launch?

the answer is 2.98 m/s

i was wondering if there is an easier way to solve this equation? i did this the first time and got 3.02 m/s but forgot how i did it.

the second time i did it i used this formula V_f = sqrtKX_i^2 - 2fL/m

V_f= sqrt ((12)(.065)^2 - 2(.028)(.143)/(4.8 x 10^-3)) = 2.98

I was wonder if anyone can tell me is there an easier way to doing this in a simple way. I know there is one which gave me the answer 3.02 i just forgot to write it down and forgot it just now.
 
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  • #2
Are you sure the answer is 2.98? Can you calrify how you arrive at the above eqn?
 
Last edited:
  • #3
the way i got that is

W_nc = (KE + PE_g + PE_s)_f - (KE + PE_g + PEs) = deltaKE + deltaPE_g + deltaPE_s

since gun barrel is horizontal, the gravitational potential energy is constant
deltaPE_g = mg(y_f - y_i) = 0. the elastic potential energy is
PE_s = 1/2kx^2 x = distance spring compress

deltaPE_s = 1/2k(0 - x_i^2) = -1/2kx_i^2

i got this from the book i read.
 
  • #4
oh yea forgot this part Wnc = (fcos180*)L = -fL L= length of barrel

-fL = (1/2mv^2 - 0) + (0) + (-1/2kx_i^2) solve for v^2 then input the numbers given.
 
  • #5
Well. ya. I do think that energy conservation is the only one method that will allow you to arrive at this answer. What other methods do you think is applicable in this case? Guess, there is no shortcut for this though..

One alternative that would have come to mind would be to use forces. However, ur force is not a constant force. It changes as ur extension of the spring changes, so basically, forces is being ruled out. Thus, the only way to get around this question is by using energy conservation.
 
  • #6
Oh thanks a lot. I guess I will have to remember all this for the test.
 

Related to With what speed does the projectile leave the barrel

1. What is the formula for calculating the speed of a projectile leaving the barrel?

The formula for calculating the speed of a projectile leaving the barrel is v = sqrt(2gh), where v is the velocity, g is the acceleration due to gravity, and h is the height of the barrel.

2. How does the mass of the projectile affect its speed leaving the barrel?

The mass of the projectile does not affect its speed leaving the barrel. The velocity of the projectile is determined by the force applied to it and the distance it travels in the barrel.

3. What factors can impact the speed of a projectile leaving the barrel?

The speed of a projectile leaving the barrel can be impacted by factors such as the force applied to it, the distance it travels in the barrel, air resistance, and the weight and shape of the projectile.

4. Is the speed of a projectile leaving the barrel constant?

No, the speed of a projectile leaving the barrel is not constant. It is affected by external factors such as air resistance and can also decrease over time due to gravity.

5. Can the speed of a projectile leaving the barrel be greater than the speed of sound?

Yes, the speed of a projectile leaving the barrel can be greater than the speed of sound. However, this would require a very powerful force and is not common in everyday scenarios.

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