Vibrating String kinetic energy

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SUMMARY

The kinetic energy of a vibrating string segment is defined by the equation ΔK = (1/2)Δm(∂y/∂t)², where μ = Δm/Δx. For a string of length L fixed at both ends, the total kinetic energy in the nth mode of vibration is proportional to n²A_n². The maximum kinetic energy occurs when the wave function is at its peak, specifically when y(x,t) = Asin(ω₀(t - x/ν)). This discussion clarifies the relationship between the mode of vibration and the kinetic energy of the string.

PREREQUISITES
  • Understanding of wave functions in physics
  • Familiarity with angular frequency (ω₀) and its role in vibrations
  • Knowledge of kinetic energy equations in classical mechanics
  • Basic calculus for integration and differentiation
NEXT STEPS
  • Study the derivation of wave functions for vibrating strings
  • Learn about the relationship between frequency and mode of vibration
  • Explore the principles of energy conservation in oscillatory systems
  • Investigate the effects of tension and mass density on string vibrations
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Students studying physics, particularly those focusing on wave mechanics, as well as educators and anyone interested in the dynamics of vibrating strings and their energy properties.

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Homework Statement


The kinetic energy of a segment of length \Delta x and mass \Delta m of a vibrating string is given by \Delta K = \frac{1}{2} \Delta m (\frac{\partial y}{\partial t})^2 = \frac{1}{2} \mu (\frac{\partial y}{\partial t})^2 \Delta x, where \mu = \frac{\Delta m}{\Delta x}.

a. find the total kinetic energy of the nth mode of vibration of a string of length L fixed at both ends.

b. Give the maximum kinetic energy of the string.

c. What is the wave function when the kinetic energy has its maximum value?

d. Show that the maximum kinetic energy in the nth mode is proportional to n^2 A_n^2.


Homework Equations


Pretty much given.


The Attempt at a Solution


I have tried numerous times to get a start on this problem but I can't seem to figure it out. Neither can my older brother or other peers :frown:.
 
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Ok, I can't answer them all, but here's what I can answer:

We might as well work with differentials
\frac{dK}{dx}=\frac{1}{2} \mu (\frac{\partial y}{\partial t})^2

Ok, the next bit is hand-wavy. For a vibrating string

y(x,t) = Asin(\omega_{0} (t - x/\nu ))

where omega is the angular frequency- you may have seen it in some slightly different but equivalent form.

\frac{\partial y}{\partial t} = A\omega cos(\omega_{0} (t - x/\nu ))

At t=0:
\frac{\partial y}{\partial t} = A\omega cos(\omega_{0} x/\nu )

Then:
\frac{dK}{dx}=\frac{1}{2} \mu (\frac{\partial y}{\partial t})^2 = \frac{1}{2} \mu (A \omega_{0} )^2 cos^2(\omega_{0} x/\nu )

So, in one wavelength:

\int_{0}^{\lambda } \frac{1}{2} (A\omega_{0} )^2 cos^2(\omega_{0} x/\nu )dx

You will see that the integral is equal to:

\frac{1}{4} \lamda \mu (A\omega_{0} )^2

\omega_{0} is the angular frequency of the first normal mode, and the frequency of the nth normal mode is n\omega_{0}. Some of the results follow directly from that.

As a matter of interest- what book are you using?
 
Last edited:
qspeechc said:
As a matter of interest- what book are you using?

Physics for Scientists and Engineers vol.5 by Paul A. Tipler
 
I think I understand now. Thanks for the help.
 
? What is the smallest possible 'unit' that can be in all of this.
 

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