How Do You Solve the Wave Equation Using Coefficient Equations?

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Homework Help Overview

The discussion revolves around solving the wave equation using coefficient equations, specifically focusing on the mathematical relationships and boundary conditions involved in the problem.

Discussion Character

  • Exploratory, Mathematical reasoning, Problem interpretation

Approaches and Questions Raised

  • Participants discuss calculating second derivatives and substituting them into the wave equation. There is an exploration of equating coefficients and seeking solutions in terms of sine functions. Questions arise regarding the next steps after establishing relationships between variables and boundary conditions.

Discussion Status

Some participants have provided insights into the derivation of normal mode frequencies and the implications of boundary conditions. There is acknowledgment of correctness in part (a), while part (b) remains less clear, prompting further inquiry into its requirements.

Contextual Notes

Participants are navigating the implications of quantization in the context of wave behavior on a string, as well as the relationship between wavelength and string length. There is a mention of homework constraints regarding the specific requirements of part (b).

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Homework Statement



[PLAIN]http://img33.imageshack.us/img33/8236/waveeq.jpg



The Attempt at a Solution



We calculate second differential with respect to x, and t, substitute into the wave equation.

We then equate the coefficients: [A''(x) + (w/v)^2A(x)]sin(wt)=0

We know from SHM equation that: A''(x) = -(w/v)^2A(x), and hence A''(x) = -k^2 A(x)

But where do we go from here? Any hints?

Also, what about part b?
 
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From A''(x) = -k^2 A(x), we seek a solution of the form A(x) = Csin(kx + psi)

Apply our boundary conditions of y(0,t) and y(L,t) both = 0.

We end up with sin(kL) = 0, where kL varies from 0 to 2PI, this implies that kL=nPI where n=1,2,3...

Because it's quantised, we can say k(n) = nPI/L, where n=1,2,3...

Since k = w/v, w(n) =nPI/L . vWhere w(n) are the normal mode frequencies.

Could someone verify this is correct?
 
Also, any clues for b)?
 
Looks good for part (a).
For (b), I'm not quite sure what they are getting at. In a sense, you already showed this in your derivation for part (a). Maybe they want you to think in terms of the wavelength λ and how it relates to the string length L.
 

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