Understanding the Relationship between Kinetic Energy and Momentum in Collisions

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Discussion Overview

The discussion revolves around the relationship between kinetic energy and momentum in collisions, specifically addressing the implications of conservation laws in elastic and inelastic collisions. Participants explore the mathematical formulations of kinetic energy and momentum, and the conditions under which they are conserved or transformed during collisions.

Discussion Character

  • Exploratory
  • Technical explanation
  • Debate/contested
  • Mathematical reasoning

Main Points Raised

  • One participant expresses confusion about the kinetic energy formula and its implications during a collision, questioning how kinetic energy can seemingly double in a specific scenario.
  • Another participant explains that the scenario described is an inelastic collision, where both kinetic energy and momentum cannot be conserved simultaneously.
  • A different participant challenges the assumption that one object can receive all the momentum in a collision, emphasizing that this would violate conservation of energy.
  • Discussion includes the classification of collisions as elastic or inelastic, with a note that inelastic collisions result in energy loss to other forms, while elastic collisions conserve kinetic energy.
  • One participant introduces the concept of the coefficient of restitution to explain energy loss in inelastic collisions.
  • Another participant confirms that two objects can have the same momentum but different kinetic energies, asserting that this is inevitable if the objects have different masses.

Areas of Agreement / Disagreement

Participants express differing views on the implications of kinetic energy and momentum conservation in collisions. There is no consensus on the specific scenarios discussed, and multiple competing interpretations of the principles involved remain evident.

Contextual Notes

Participants highlight limitations in understanding the integration of kinetic energy and momentum conservation, as well as the conditions under which these principles apply. Some assumptions about collision types and energy transformations are not fully resolved.

Who May Find This Useful

This discussion may be of interest to students and enthusiasts of physics, particularly those exploring concepts related to mechanics, energy conservation, and collision dynamics.

stevo1
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I am having problems with the kinetic energy formula KE = 1/2 mv^2.
If an object of 1kg travels at a speed of 1ms its kinetic energy is 1/2 * 1 * 1^2 = 0.5J.
But if it collides with an object of 0.5kg which is stationary, to conserve momentum which is equal to mass * velocity = 1 * 1 = 1kgms the new speed of the 0.5kg object = momentum / mass = 1/0.5 = 2ms. The kinetic energy of this new object is equal to 1/2 * 0.5 * 2^2 = 1/4 * 4 = 1J. This is double the energy of the initial object which is impossible. It does not make sense to me that the faster an object travels a disproportionate amount of energy is required. I think that the origin of KE (1/2 mv^2), the integration of F=ma, is something that cannot be integrated in reality, only in theory, if momentum is to be conserved.
Can anyone shed any light on this?

Thanks
Stephen Lewis
 
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What you're doigng is describing what is called an inelastic collsion, in an inelsatic collsion both kinetic energy and momentum cannot be conserved here's the one-diemsnional proof

Imagine two objects of masses [itex]m_1[/itex] and [itex]m_2[/itex], traveling with velocities of [itex]v_1[/itex] and [itex]v_2[/itex] which after collding inelastically form a new object of [itex]m_3[/itex], traveling at velocity [itex]m_3[/itex], which due to the conservations of mass must equal [itex]m_1 + m_2[/itex]

We can say this due to the conservation of momentum:

[tex]m_3v_3 = m_1v_1 + m_2v_2[/tex]

therefore:

[tex]v_3 = \frac{m_1v_1 + m_2v_2}{m_3}[/tex]

We can also say that due to the conservation of energy:

[tex]\frac{1}{2}m_3{v_3}^2 = \frac{1}{2}m_1{v_1}^2 + \frac{1}{2}m_2{v_2}^2[/tex]

therefore:

[tex]v_3 = \sqrt{\frac{m_1{v_1}^2 + m_2{v_2}^2}{m_3}}[/tex]

combing the equations we get:

[tex]\frac{m_1v_1 + m_2v_2}{m_3} = \sqrt{\frac{m_1{v_1}^2 + m_2{v_2}^2}{m_3}}[/tex]

square and mutiply [itex]{m_3}^2[/itex] byboth sides,substitue in [itex]m_3 = m_1 + m_2[/itex] and mutiply out:

[tex]{m_1}^2{v_1}^2 + {m_2}^2{v_2}^2 + 2m_1m_2v_1v_2 = {m_1}^2{v_1}^2 + {m_2}^2{v_2}^2 + m_1m_2{v_1}^2 + m_1m_2v_2^2[/tex]

Simply eliminate and you get:

[tex]2v_1v_2 = v_1^2 + v_2^2[/tex]

Which can be re-arranged as:

[tex]v_1^2 - 2v_1v_2 + v_2^2 = 0[/tex]

using the quadratic formula we can solve for [itex]v_1[/itex]

And we find that:

[tex]v_1 = v_2[/tex]


So for an inelastic collision the intial velcoties of the two colliding objects must be the same, hence no collision.

Therfore the nergy must take some other form rtaher than kinetic energy.
 
stevo1 said:
I am having problems with the kinetic energy formula KE = 1/2 mv^2.
If an object of 1kg travels at a speed of 1ms its kinetic energy is 1/2 * 1 * 1^2 = 0.5J.
OK.
But if it collides with an object of 0.5kg which is stationary, to conserve momentum which is equal to mass * velocity = 1 * 1 = 1kgms the new speed of the 0.5kg object = momentum / mass = 1/0.5 = 2ms.
Says who? During the collision the total momentum is conserved. In this case, the total momentum equals 1 kg-m/s. The situation you describe, where the struck object gets all the momentum, cannot happen--it would violate conservation of energy (assuming there is no energy source--like an explosive--involved). It could happen, but only if the two objects were the same mass.
The kinetic energy of this new object is equal to 1/2 * 0.5 * 2^2 = 1/4 * 4 = 1J. This is double the energy of the initial object which is impossible.
Right. It won't happen.
It does not make sense to me that the faster an object travels a disproportionate amount of energy is required. I think that the origin of KE (1/2 mv^2), the integration of F=ma, is something that cannot be integrated in reality, only in theory, if momentum is to be conserved.
It works just fine, done correctly. :smile:
 
super-elastic collision

One more note. Collisions are often classified as elastic or inelastic. In a purely elastic collision, the KE is conserved. In a more realistic inelastic collision, some of that energy is lost to thermal energy and deformation of the objects: so the total KE after the collision is less than what it was before the collision.

The example you gave--in which the total KE increased--would be a super-elastic collision. This would require an additional source of energy.
 
You need to consider Newton's coefficient of Restitution

e = Relative Speed of separation/Relative Speed of Approach

Where e is the the coefficient of resitution. This is used when there is a energy loss. i.e. the collision is inelastic.

Yes youth!
 
Thanks to all those who replied.
Sorry for the long delay in this reply.

One final thing, could two objects possesses the same momentum but hold different kinetic energies, for example an object of 1kg mass traveling at 1ms, KE = 1/2 * 1 * 1^2 = 0.5J and momentum = 1 * 1 = 1kgms and an object of 0.5kg mass traveling at 2ms KE = 1/2 * 0.5 * 2^2 = 1J and momentum = 0.5 * 2 = 1kgms.
Is this possible? If so, can you explain why?

Many thanks

Stephen Lewis
 
stevo1 said:
One final thing, could two objects possesses the same momentum but hold different kinetic energies,...
...
Is this possible? If so, can you explain why?
It's not only possible, but if the objects have different masses it's inevitable. Momentum and kinetic energy are two entirely different concepts.
 
Thanks Doc Al, very interesting.
 

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