Damped oscillator energy dissipated per cycle.

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SUMMARY

The discussion focuses on calculating the energy dissipated by a damping force during one cycle of a damped oscillator, specifically using the formula 2*pi*m*B*w*A^2. The natural frequency is equal to the driving frequency, and the damping force is represented as F=-bv. The key equations include the total energy of the oscillator, given by (1/2)*m*w^2*A^2, and the relationship between velocity and amplitude. The solution involves integrating the sinusoidal velocity to account for the energy loss accurately.

PREREQUISITES
  • Understanding of damped oscillators and their dynamics
  • Familiarity with sinusoidal functions and their derivatives
  • Knowledge of energy concepts in mechanical systems
  • Proficiency in calculus, particularly integration techniques
NEXT STEPS
  • Study the derivation of energy dissipation in damped harmonic oscillators
  • Learn about the role of damping coefficients in oscillatory motion
  • Explore the integration of sinusoidal functions for energy calculations
  • Investigate the impact of varying amplitude on energy dissipation
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Students studying physics, particularly those focusing on mechanics and oscillatory systems, as well as educators seeking to explain energy dissipation in damped oscillators.

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Homework Statement


Sinusoidal driving force driving a damped oscillator (mass = m).
Natural frequency is assumed to equal the drive frequency = w
Time has elapsed to the point any transients have dissipated.

Show that the energy dissipated by the damping force [F=-bv] during one cycle is equal to

2*pi*m*B*w*A^2


Homework Equations



Total energy = (1/2)*m*w^2*A^2

A=amplitude

x=Acos(w*t-d)

v=A*w*sin(w*t-d)

d=delta=phase shift

B=Beta=Damping coefficient = b/(2*m)

The Attempt at a Solution



I am explicitly told in a hint that the rate at which the force does work is F*v.

My reasoning is,

Rate of work done by force = rate of energy dissipation. Work done by the non-conservative damping force must be = the change in energy of the oscillator. This rate times the time period desired will give the energy loss in in that amount of time. The time in question is one period (2*pi)/w .

(F*v)*t

(-bv*v)*(2*pi)/w

(-b(A*w)^2)*(2*pi)/w where I have said v^2=(A*w)^2

-2*pi*(2*m*B)*w*A^2 substituting b=B*2*m , the result at which I am stuck.

The negative sign may be disregarded I believe, because the problem asks for the energy dissipated, and the oscillator is losing energy. Bu the extra factor of 2 confuses me. I believe am close.
 
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Found the mistake. Don't multiply by time, you must integrate the full sinusoidal velocity to get an (pi/2) factor.
 

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