Block collision attached to spring

AI Thread Summary
The discussion revolves around a physics problem involving a block attached to a spring and a second block that collides inelastically after being released. The initial approach used conservation of energy to determine the velocity at the collision point, but it was pointed out that momentum conservation should be applied instead during the collision. The user attempted to calculate the distance the blocks slide after the collision using Newton's second law and kinematics, but faced challenges due to incorrect assumptions about constant acceleration. The conversation emphasizes the importance of correctly applying conservation laws before and after the collision, while noting that energy is not conserved during the collision itself. Ultimately, the user is guided to refine their calculations and correctly express the potential energy in terms of the distance beyond the collision point.
naianator
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Homework Statement



problems_MIT_boriskor_BKimages_10-mass-spring-two-block-collision.png


A block of mass m is attached to a spring with a force constant k, as in the above diagram. Initially, the spring is compressed a distance x from the equilibrium and the block is held at rest. Another block, of mass 2m, is placed a distance x/2 from the equilibrium as shown. After the spring is released, the blocks collide inelastically and slide together. How far (Δx) would the blocks slide beyond the collision point? Neglect friction between the blocks and the horizontal surface.

Homework Equations


U_spring = 1/2*k*x^2

K = 1/2*m*v^2

F = m*a

v_f^2 = v_0^2+2*a*x

The Attempt at a Solution


I used conservation of energy to find the velocity where the two blocks collide at x/2. I'm not sure about this though, because I don't think that conservation of momentum applies and I used 3m for the mass (assuming that the blocks had collided). Then I used N2L to find the acceleration based on the force (-kx) and mass (3m). I plugged that into the kinematics equation for final velocity and solved for delta x. I'm really not having any luck.

E_i = 1/2*k*x^2 = E_f = 1/2*m*v^2 + 1/2*k*x_f^2

at x/2 where m collides with 2m:

1/2*k*x^2 = 1/2*3m*v^2 + 1/8*k*x^2

k*x^2 = 3m*v^2 + 1/4*k*x^2

3/4*k*x^2 = 3*m*v^2

yielding

v = sqrt(k*x^2/(4*m))

by Newtons second law a = -k*x/(3*m)

and using kinematics (v_f^2 = v_0^2+2*a*x)

0 = k*x^2/(4*m) - 2*(k*x/(3*m))*delta(x)

x/4 = 2/3*delta(x)

delta(x) = 3/8*x

Am I way off base with this approach?
 
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naianator said:
I used conservation of energy to find the velocity where the two blocks collide at x/2.
You can use conservation of energy to find the velocity of mass m just before the collision. But energy is not conserved during the collision itself. (But what is conserved?)
 
Doc Al said:
You can use conservation of energy to find the velocity of mass m just before the collision. But energy is not conserved during the collision itself. (But what is conserved?)
momentum?
 
naianator said:

Homework Statement



problems_MIT_boriskor_BKimages_10-mass-spring-two-block-collision.png


A block of mass m is attached to a spring with a force constant k, as in the above diagram. Initially, the spring is compressed a distance x from the equilibrium and the block is held at rest. Another block, of mass 2m, is placed a distance x/2 from the equilibrium as shown. After the spring is released, the blocks collide inelastically and slide together. How far (Δx) would the blocks slide beyond the collision point? Neglect friction between the blocks and the horizontal surface.

Homework Equations


U_spring = 1/2*k*x^2

K = 1/2*m*v^2

F = m*a

v_f^2 = v_0^2+2*a*x

The Attempt at a Solution


I used conservation of energy to find the velocity where the two blocks collide at x/2. I'm not sure about this though, because I don't think that conservation of momentum applies and I used 3m for the mass (assuming that the blocks had collided). Then I used N2L to find the acceleration based on the force (-kx) and mass (3m). I plugged that into the kinematics equation for final velocity and solved for delta x. I'm really not having any luck.

E_i = 1/2*k*x^2 = E_f = 1/2*m*v^2 + 1/2*k*x_f^2

at x/2 where m collides with 2m:

1/2*k*x^2 = 1/2*3m*v^2 + 1/8*k*x^2

k*x^2 = 3m*v^2 + 1/4*k*x^2

3/4*k*x^2 = 3*m*v^2

yielding

v = sqrt(k*x^2/(4*m))

by Newtons second law a = -k*x/(3*m)

and using kinematics (v_f^2 = v_0^2+2*a*x)

0 = k*x^2/(4*m) - 2*(k*x/(3*m))*delta(x)

x/4 = 2/3*delta(x)

delta(x) = 3/8*x

Am I way off base with this approach?
According to what I did understand of your method to solve the problem.You have conserved energy in an inelastic collision which I don't think is valid.
Conservation of linear momentum however will hold true.I suggest you use that to find the final velocities of the blocks.

Edit:I'm sorry,I didn't see the earlier replies to the post.
 
naianator said:
momentum?
Yes!
 
Ellispson said:
According to what I did understand of your method to solve the problem.You have conserved energy in an inelastic collision which I don't think is valid.
Conservation of linear momentum however will hold true.I suggest you use that to find the final velocities of the blocks.
so according to conservation of momentum mass m has velocity sqrt(3*k*x^2/(4*m)) before the collision and according to conservation of momentum the blocks have velocity sqrt(3*k*x^2/(4*m))/3 after the collision. Can I find the acceleration and distance traveled with the same approach I tried before?
 
Doc Al said:
Yes!
so if I find the velocity of the masses after the collision can I use N2L and kinematics to find distance traveled?
 
naianator said:
so if I find the velocity of the masses after the collision can I use N2L and kinematics to find distance traveled?
I'm assuming not because I got another wrong answer
 
naianator said:
so according to conservation of momentum mass m has velocity sqrt(3*k*x^2/(4*m)) before the collision
I believe you mean conservation of energy here.

naianator said:
and according to conservation of momentum the blocks have velocity sqrt(3*k*x^2/(4*m))/3 after the collision.
Right.

naianator said:
Can I find the acceleration and distance traveled with the same approach I tried before?
No. That method was flawed since you assumed constant acceleration.

During the collision, energy is not conserved. But before and after the collision it is.

naianator said:
so if I find the velocity of the masses after the collision can I use N2L and kinematics to find distance traveled?
No, but see above for a hint.
 
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  • #10
Doc Al said:
I believe you mean conservation of energy here.Right.No. That method was flawed since you assumed constant acceleration.

During the collision, energy is not conserved. But before and after the collision it is.No, but see above for a hint.
ahhh so I can use conservation of energy again
 
  • #11
naianator said:
ahhh so I can use conservation of energy again
so is it 1/2*m*v^2 + 1/2*k*(x/2)^2 = 1/2*k*delta(x)^2

= x^2/12+x^2/4 = delta(x)^2

delta(x) = .57735?
 
  • #12
Doc Al said:
I believe you mean conservation of energy here.Right.No. That method was flawed since you assumed constant acceleration.

During the collision, energy is not conserved. But before and after the collision it is.No, but see above for a hint.

naianator said:
so is it 1/2*m*v^2 + 1/2*k*(x/2)^2 = 1/2*k*delta(x)^2

= x^2/12+x^2/4 = delta(x)^2

delta(x) = .57735?

Nope. So what am I doing wrong now?
 
  • #13
naianator said:
so is it 1/2*m*v^2 + 1/2*k*(x/2)^2 = 1/2*k*delta(x)^2
Make sure you have the right mass and speed for the KE term. And express the final PE term in terms of Δx properly. Δx is the distance beyond the collision point, not the final distance from equilibrium.
 
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  • #14
Doc Al said:
Make sure you have the right mass and speed for the KE term. And express the final PE term in terms of Δx properly. Δx is the distance beyond the collision point, not the final distance from equilibrium.
Got it, thanks.
 
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