Understanding derivation of kinetic energy from impulse?

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Discussion Overview

The discussion revolves around the derivation of kinetic energy from the concept of impulse, exploring the relationship between force, momentum, and kinetic energy. Participants examine the integration of impulse with respect to velocity and its implications for understanding kinetic energy.

Discussion Character

  • Exploratory
  • Technical explanation
  • Conceptual clarification
  • Debate/contested

Main Points Raised

  • One participant questions the meaning of integrating impulse with respect to velocity, expressing confusion about transitioning from a time domain to a velocity domain.
  • Another participant explains that work can be derived from impulse by manipulating the relationships between force, momentum, and displacement, ultimately leading to the expression for kinetic energy.
  • A third participant reflects on their misunderstanding, noting that they initially focused on time integration rather than work, which clarified their understanding of the relationship between force and kinetic energy.
  • A different participant raises a question about simply calculating final velocity to determine kinetic energy, suggesting that momentum may not directly correlate with kinetic energy.

Areas of Agreement / Disagreement

Participants express differing views on the approach to understanding kinetic energy and impulse, with some focusing on integration techniques while others question the necessity of such derivations. The discussion remains unresolved regarding the best method to relate momentum and kinetic energy.

Contextual Notes

Participants highlight the complexity of transitioning between different domains (time to velocity) and the potential misconceptions that arise from focusing on time-based integrals. There is also an acknowledgment that momentum and kinetic energy may not have a straightforward relationship.

Who May Find This Useful

This discussion may be useful for students and enthusiasts of physics who are grappling with the concepts of impulse, momentum, and kinetic energy, particularly in the context of integration and the relationships between these concepts.

richsmith
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I have a question that annoys my basic understanding of kinetic energy.

I know if I have a force-time plot then the area under the curve is equivalent to the impulse imparted on an object (in units Newton-Seconds). I know that this is also equivalent to the change in momentum of the object i.e. Ft = delta mV

I know that i can get these values from the plot by simply intgrating the Force function wrt to time. Now I want to determine the kinetic energy involved in this event. I know that k.e. = 1/2mV^2 so I know that is simply the integral of the impulse w.r.t. to velocity

Now that is the part conceptually I don't really grasp. What does it really mean to integrate with respect to velocity? This means I am suddenly on a velocity :rolleyes: domain, not time, and I don't really understand this?

Thanks.
 
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While impulse is ∫Fdt, work is ∫Fdx. Since force can be viewed as the rate of change of momentum, you have F = dp/dt = m dv/dt. Thus:
W = ∫Fdx = ∫m (dv/dt) * dx = m∫dv*(dx/dt) = m∫v dv = ½mv² (which is kinetic energy).

Make sense?
 
After some head scratching yes it does, finaly.

I think my mistake has always been trying to integrate wrt time. I really had to step back and ask myself what i was after, work that is, which is not a time integral.

Manipulating dv/dt to dx/dt and then subbing in V now makes it algebraicly understandable.

Thanks a lot.

Richard.
 
I have a question that annoys my basic understanding of kinetic energy.

Similar to questions which annoys my basic understanding of electrostatics?

Why not just calculate the final velocity of the body and then calculate the K.E.

Take as a caveat that the momentum of a body might not be directly proportional to K.E possesed by it.
 

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