Elastic collision problem (μk) is the target variable

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SUMMARY

The discussion centers on the elastic collision problem involving two objects, A and B, each with mass m. Object A is suspended and released from height h, colliding elastically with object B, which then slides a distance d on a rough surface. The key equations used include momentum conservation (mA)(vA1) = (mB)(vB2) and energy conservation, leading to the expression (μk) = (2gh - v^2)/(2g)(d). The conclusion emphasizes that energy is conserved in elastic collisions, and the energy lost to friction must be accounted for to solve for the distance d.

PREREQUISITES
  • Understanding of elastic collisions and momentum conservation
  • Familiarity with gravitational potential energy and kinetic energy equations
  • Knowledge of frictional forces and the coefficient of kinetic friction (μk)
  • Ability to manipulate algebraic equations involving energy and distance
NEXT STEPS
  • Study the principles of elastic collisions in detail
  • Learn how to apply conservation of momentum and energy in collision problems
  • Explore the effects of friction on motion and energy loss
  • Investigate the relationship between height, distance, and the coefficient of kinetic friction in similar problems
USEFUL FOR

Students studying physics, particularly those focusing on mechanics and collision theory, as well as educators looking for examples of elastic collisions and energy conservation principles.

PedroPicapiedra
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Homework Statement


Two certain small objects A and B, each have mass m. A is suspended using a lightweight, inelastic string, and B is placed on a rough horizontal floor in a position where it is in contact with the vertically suspended A. Next, A is raised to height h above its original position while the string is kept taut, and then is gently released. A collides elastically with B, which then slides along the floor distance d before coming to a rest
20180601_122238.png


Homework Equations


(mA)(vA1)+(mB)(vB1) = (mA)(vA2)+(mA)(vA2)
K1 + U1 + W other = K2 + U2

The Attempt at a Solution


To my understanding, in collision problems the momentum is always conserved. However, energy is not necessarily conserved.
So I used the momentum equation and and inserted the variables. Since object B is at rest before the collision, and object A is at rest after the collision; I got rid of (mB)(vB1) and (mA)(vA2).
Therefore:
(mA)(vA1) = (mB)(vB2) since both masses are equal I got that both velocities are equal.
(vA1) = (vB2)

Then I use the energy equation where

K1 = 0
U1 = mgh
W other = (Ff)(d) = (μk)(n) = (μk)(-mg)
K2 = 1/2mv^2
U2 = 0

Thus
mgh - (μk)(mg)(d) = 1/2mv^2
gh - (μk)(g)(d) = 1/2v^2
h - (μk)(d) = (v^2)/(2g)
(μk) = (2gh - v^2)/(2g)(d)

I don' really know where I went wrong. But I think my energy equation is wrong.

The answer is supposed to be h/d.

Thank you.
 

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You are correct that A is at rest after the collision. Also, energy is conserved except that energy is lost as B slides along the floor (that energy goes into heat). Write an expression for the total energy just before A is released and another expression for the total energy right after the collision. Then relate the energy lost due to friction to the distance B slides.
 
PedroPicapiedra said:

Homework Statement


Two certain small objects A and B, each have mass m. A is suspended using a lightweight, inelastic string, and B is placed on a rough horizontal floor in a position where it is in contact with the vertically suspended A. Next, A is raised to height h above its original position while the string is kept taut, and then is gently released. A collides elastically with B, which then slides along the floor distance d before coming to a rest
View attachment 226460

Homework Equations


(mA)(vA1)+(mB)(vB1) = (mA)(vA2)+(mA)(vA2)
K1 + U1 + W other = K2 + U2

The Attempt at a Solution


To my understanding, in collision problems the momentum is always conserved. However, energy is not necessarily conserved.
So I used the momentum equation and and inserted the variables. Since object B is at rest before the collision, and object A is at rest after the collision; I got rid of (mB)(vB1) and (mA)(vA2).
Therefore:
(mA)(vA1) = (mB)(vB2) since both masses are equal I got that both velocities are equal.
(vA1) = (vB2)

Then I use the energy equation where

K1 = 0
U1 = mgh
W other = (Ff)(d) = (μk)(n) = (μk)(-mg)
K2 = 1/2mv^2
U2 = 0

Thus
mgh - (μk)(mg)(d) = 1/2mv^2
gh - (μk)(g)(d) = 1/2v^2
h - (μk)(d) = (v^2)/(2g)
(μk) = (2gh - v^2)/(2g)(d)

I don' really know where I went wrong. But I think my energy equation is wrong.

The answer is supposed to be h/d.

Thank you.
The problem states that the collision is elastic. That means that no energy is lost in the collision, so energy is conserved.
The mass A is not necessarily at rest after the collision, but you can use conservation of energy and conservation of momentum to figure out what its velocity is. In this case, your two wrong assumptions canceled out and you got the right answer anyway. All of A's momentum is transferred to B. That will not happen if the two masses are different or if collision is not head on.

I don't understand what "W other" means, or how you are trying to use it in an energy equation. Energy is lost to friction as B slides to a stop, so you could equate the work the block does against friction to its initial kinetic energy and solve for d.
 

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