How can I find the wave equation u(x,t) of a string

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The wave equation U(x,t) for a vibrating string with linear density d and tension p is derived using the initial displacement U0(x) = a1*sin(2*pi*x/L) + a2*sin(4*pi*x/L). The solution is expressed as a sum of sine and cosine functions: U(x,t) = ΣBn*cos(n*pi*a*t/L)*sin(n*pi*x/L). The coefficients Bn are calculated using the integral Bn = (2/L)∫U0(x)*sin(n*pi*x/L)dx, resulting in specific values for B2 and B4 corresponding to a1 and a2, respectively. The discussion emphasizes the importance of applying boundary conditions and correctly interpreting the coefficients.

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Mutatis
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Find the wave equation U(x,t) of a vibrating string with linear density d, tension p, initial velocity zero, weight L and initial displacement

U0(x) = a1*sin(2*pi*x/L)+a2*sin(4*pi*x/L).


Guys, please help me with this task. I did the following procedure:

The U(x,t) solution must me a sum of sine and cosine functions, like

ΣBn*cos(n*pi*a*t/L)*sin(n*pi*x/L).

Then Bn is found with Bn=∫U0(x)*sin(n*pi*x/L)dx. I'm a little lost with all these substitiution that leads me to big integrals with no solution.
 
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Just apply the given boundary conditions to your general expression.
 
I did, but the answer is a sum of sine and cosine times Bn term which is still in terms of a1 and a2. I'm very confused. I did the calculus through Maple.
 
Mutatis said:
I did, but the answer is a sum of sine and cosine times Bn term which is still in terms of a1 and a2. I'm very confused. I did the calculus through Maple.
Please post your working. If I cannot see it then I cannot know what you have wrong or exactly where you are stuck.
Apart from one differentiation, you should not need any calculus.
 
Ok, that was how I did. The ##U(x,t)## solution must me a sum of sine and cosine functions, then $$ U\left(u,t\right) = \sum_{n=0}^\infty B_n \cos\left( \frac {n \pi a t} {L} \right) \sin\left( \frac {n \pi a t} {L} \right)$$ and ##B_n## can be found using $$ B_n = \frac 2 L \int_0^L f(x)\sin\left( \frac {n \pi a t}{L} \right)\, dx$$.
To get ##B_n## I applied ##f(x)## on the second equation above: $$B_n = \frac 2 L \{ a_1 \int_0^L \sin\left( \frac {2 x \pi }{L} \right) \sin\left( \frac {n x \pi }{L} \right) \, dx + a_2 \int_0^L \sin\left( \frac {4 x \pi }{L} \right) \sin\left( \frac {n x \pi }{L} \right) \, dx \}$$. These two integrals I used Maple to get the result, and it returned me: $$B_n = \frac {a_1} {\pi} \left[ \frac {\sin \left( n \pi - 2 \pi \right)} {\left( n - 2 \right)} - \frac {\sin \left( n \pi - 2 \pi \right)} {\left( n + 2 \right)} \right] + \frac {a_1} {\pi} \left[ \frac {\sin \left( n \pi - 4 \pi \right)} {\left( n - 4 \right)} - \frac {\sin \left( n \pi + 4 \pi \right)} {\left( n + 4 \right)} \right] $$. That was I found. Should I apply the ##B_n## on the ##U(x,t)## equation now?
 
Last edited:
Mutatis said:
and Bn can be found using
Sure, but that's a sledgehammer to crack a nut.
You have at t=0 ##a_1\sin(2\pi x/L)+a_2\sin(4\pi x/L)=\Sigma B_n\sin(n\pi x/L)##.
Can you not write down the values of the Bn by inspection?
 
I've tried it. But that's what is getting me confuse. ##B_n = a_1, a_2## then? Thank you the help. It's the first exercise that I'm really stuck about vibrating waves.
 
The wave equation is $$ U(x,t) = a_1 \cos \left( \frac {2 \pi x a t} {L} \right) \sin \left( \frac {2 \pi x} {L} \right) + a_2 \cos \left( \frac {4 \pi x a t} {L} \right) \sin \left( \frac {4 \pi x} {L} \right) $$ with ##n = 2,4##. Do you have some tip to find ##a_1## and ##a_2##?
 
Mutatis said:
I've tried it. But that's what is getting me confuse. ##B_n = a_1, a_2## then?.
Well, B2=a1, B4=a2, and the rest are zero.
Mutatis said:
Do you have some tip to find a1 and a2
Those are given unknowns. You are not expected to find values for them. You have the answer already.
 
  • #10
Thank you!
 

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