Work and Power of the Friction Force in an F=-bυ damped oscillation

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Discussion Overview

The discussion revolves around the work and power of the friction force in a damped oscillation described by the equation F=-bυ. Participants explore how to calculate the work done by this force over a specified interval and the corresponding power, while also considering alternative perspectives on energy dissipation in damped systems.

Discussion Character

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

Main Points Raised

  • One participant seeks to calculate the work done by the friction force F=-bυ over a distance and expresses uncertainty about deriving the power equation P=Fυ.
  • Another participant confirms the relationship P=Fυ by breaking it down into force times speed, equating it to work done per time.
  • A different participant mentions difficulty in calculating work done during a specific time interval (T/2) and refers to the integral W=\int_{0}^{A}Fds.
  • One participant argues that the frictional force does not do work and suggests analyzing the problem from an energy perspective, proposing to calculate the difference in kinetic energy to assess energy dissipation.
  • Another participant counters that in underdamped oscillations, the work done by friction reflects the energy lost by the system, proposing a specific equation for work based on energy states.
  • A later reply provides a mathematical expression for velocity in the underdamped case and discusses energy loss, while noting that potential energy must also be considered in broader contexts.

Areas of Agreement / Disagreement

Participants express differing views on whether the frictional force does work and how to approach the calculation of energy loss in damped oscillations. There is no consensus on the correct method or interpretation of the frictional force's role.

Contextual Notes

Some participants' arguments depend on specific assumptions about the system's behavior and the definitions of work and energy in the context of damped oscillations. The discussion includes unresolved mathematical steps and varying interpretations of energy dissipation.

Who May Find This Useful

This discussion may be of interest to those studying damped oscillations, energy dissipation in mechanical systems, or the mathematical modeling of forces in physics.

karkas
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Hey there forum!

Consider a damped oscillation in which the friction force is F=-bυ.
What I want to ask is how do you calculate the work done by this force for any x interval along a line and what is the Power of the work done by this force?

I already know that Power P of the work done due to a force F is P=Fυ, therefore substituting would give P=-bυ2. But I cannot derive the equation P=Fυ from my equations.

Thanks in advance!
 
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Hey there karkas! :smile:
karkas said:
I cannot derive the equation P=Fυ from my equations.

Fv = force times speed = force times distance per time = work done per time = energy per time = power = P :wink:
 
Yea, thanks tiny-tim ! I got that solved too, but I'm kinda still stuck as to calculating the work done by the force F=-bυ, say during T/2 of the oscillation.

All I know is that W=\int_{0}^{A}Fds but can't work on it. Doesn't really matter though, since the question that I wabted to answer is answered now!
 
Perhaps it's a minor point, but the frictional force does not do work. It's better to do these calculations from the energy perspective. For a damped oscillator:

http://en.wikipedia.org/wiki/Damping

You can calculate v(t) and from that, the kinetic energy. The difference between the kinetic energy at time t and time '0' is the cumulative amount of dissipated energy from friction. You can also calculate this in terms of the power (energy * time) if you wish.
 
Boy, you're a genius! Thanks for changing my perspective, that's hella much wiser. But I think that in a damped oscillation (the underdamped one) there is a work of the frictional force and it expresses the energy lost by the system.

So in such an oscillation, where A=A_0 e^{-kt}, k=b/2m the work done by the frictional forces equals to W= E - E_0 = 1/2 DA^2 - 1/2DA_0^2 right?
 
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I'm not sure I'm following you, but for the underdamped case where x(t) = x_0 exp (-ct/2m)cos (w_d t), the velocity is then v(t) = x_0 * c/2m * w_d * exp (-ct/2m) sin(w_d t) and the frictional loss of energy g(t)= 1/2m(v_0^2-v(t)^2) which may reduce to your result every 1/2 period.

Edit- this is true for the restrcited case x = 0. Otherwise, the potential energy of the spring [1/2 kx(t)^2] has to be included.

In any case, I'm glad to be of help!
 
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