Wave Equation for a Vibrating String

In summary: You got:sin(pi/4) at...0?I don't see how they would get a sin(pi/4) at...0?No, I don't see how they would get a sin(pi/4) at...0.
  • #1
forestmine
203
0

Homework Statement



A string of length l has a zero initial velocity and a displacement y[itex]_{0}[/itex](x) as shown. (This initial displacement might be caused by stopping the string at the center and plucking half of it). Find the displacement as a function of x and t.

See the following link for the figure. It's the first one on the page.

http://web.physics.ucsb.edu/~physCS33/spring2011/hw1.pdf

Homework Equations





The Attempt at a Solution



Now, to be honest with you all, I'm not really having trouble with the process. I understand how to find a form for y given the boundary conditions, and in fact I come up with,

y=Bn * sin(n[itex]\pi[/itex]x/l) * cos(n[itex]\pi[/itex]vt/l)

where Bn is equal to the Fourier sine series,

Bn=2/l ∫ f(x)*sin(2[itex]\pi[/itex]nx/l)dx.

My problem is that my answer doesn't look like that in the book, or the answer on the page I linked above. They might be equivalent, and I'm just not seeing it?

I got y=2h/[itex]\pi^{2}[/itex] [itex]\sum[/itex]1/n[itex]^{2}[/itex] [2sin([itex]\pi[/itex]n/2) - sin([itex]\pi[/itex]n] sin(n[itex]\pi[/itex]x/l) cos (n[itex]\pi[/itex]vt/l).

I got Bn from setting f(x)=y[itex]_{0}[/itex](x) = 4hx/l for 0<x<l/4 and 2h-4hx/l for l/4<x<l/2.

Now my main question is -- way back to pre-algebra -- are my f(x) equations correct? I've done the Fourier series integrals over and over again, and can't find any errors, and so I'm left to think that I must have concluded f(x) incorrectly.

Sorry for the pretty silly question, but I'm at a loss here!

Thanks so much.
 
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  • #2
You got:

y=2h/[itex]\pi^{2}[/itex] [itex]\sum[/itex]1/n[itex]^{2}[/itex] [2sin([itex]\pi[/itex]n/2) - sin([itex]\pi[/itex]n] sin(n[itex]\pi[/itex]x/l) cos (n[itex]\pi[/itex]vt/l).

Here - let me tidy that up...

You got:
$$y(x,t)=\frac{2h}{\pi^2}\sum A_n \sin_{n=1}^\infty \frac{n\pi x}{l} \cos \frac{n\pi vt}{l}\\ A_n=\frac{1}{n^2}\left[\sin\frac{\pi n}{2} - \sin\pi n \right]$$

They got $$y(x,t)=\frac{8h}{\pi^2}\sum_{n=1}^\infty A_n\sin\frac{n\pi x}{l}\cos\frac{n\pi v t}{l}\\ A_n= \frac{1}{n^2}\left[ \sin\frac{n\pi}{4}-\sin\frac{n\pi}{2}\right]$$

Now my main question is -- way back to pre-algebra -- are my f(x) equations correct? I've done the Fourier series integrals over and over again, and can't find any errors, and so I'm left to think that I must have concluded f(x) incorrectly.
Well ... I didn't see your f(x) or details of your working - but you have clearly missed something out.
What did you use for y(x,0)?
 
  • #3
Yes, your f(x) equations are correct as you can verify by checking their values at their end points.
 
  • #4
LCKurtz said:
Yes, your f(x) equations are correct as you can verify by checking their values at their end points.

That's exactly what I did, but I guess I just convinced myself there was something I wasn't seeing there. Thanks for the confirmation!
 
  • #5
Simon Bridge said:
You got:

Well ... I didn't see your f(x) or details of your working - but you have clearly missed something out.
What did you use for y(x,0)?

I used y= 4hx/l for 0<x<l/4

2h-4hx/l for l/4<x<l/2

0 for l/2<x<l

So this basically gave me two equations for An, where the first is equal to

An = 2/l (from 0 to l/4)∫(4hx/l)*sin(2[itex]\pi[/itex]nx/l)dx

and the second, for l/4<x<l/2

An = 2/l ∫(2h-4hx/l)*sin(2[itex]\pi[/itex]nx/l)dx

Do those look ok?


Sorry for the awful formatting!
 
  • #6
forestmine said:
I used y= 4hx/l for 0<x<l/4

2h-4hx/l for l/4<x<l/2

0 for l/2<x<l

So this basically gave me two equations for An, where the first is equal to

An = 2/l (from 0 to l/4)∫(4hx/l)*sin(2[itex]\pi[/itex]nx/l)dx

and the second, for l/4<x<l/2

An = 2/l ∫(2h-4hx/l)*sin(2[itex]\pi[/itex]nx/l)dx

Do those look ok?
I'll have to check it later ... got to go.
LCKurtz should be able to help meantime.

Sorry for the awful formatting!
If you use the quote button on any of my posts, you'll see how I did that :)
It's worth the effort to learn and you aren't doing anything very complicated.
 
  • #7
Simon Bridge said:
You got:

Here - let me tidy that up...

You got:
$$y(x,t)=\frac{2h}{\pi^2}\sum A_n \sin_{n=1}^\infty \frac{n\pi x}{l} \cos \frac{n\pi vt}{l}\\ A_n=\frac{1}{n^2}\left[\sin\frac{\pi n}{2} - \sin\pi n \right]$$

They got $$y(x,t)=\frac{8h}{\pi^2}\sum_{n=1}^\infty A_n\sin\frac{n\pi x}{l}\cos\frac{n\pi v t}{l}\\ A_n= \frac{1}{n^2}\left[ \sin\frac{n\pi}{4}-\sin\frac{n\pi}{2}\right]$$

So actually, my An includes the prefactor of 2h/[itex]\pi[/itex][itex]^{2}[/itex]. There's on the other hand, is independent of the constants out front. That's why I was thinking that maybe the two answers are equivalent, in that they factored those pre-factors out, but then the fact that our sin terms are different is throwing me.

I've recalculated the An integrals in my previous post over and over again, and I still can't find an error. I don't see how they would get a sin(pi/4) at all.
 
  • #8
forestmine said:
I've recalculated the An integrals in my previous post over and over again, and I still can't find an error. I don't see how they would get a sin(pi/4) at all.

I can't bring myself to crunch through all the steps, but I would certainly expect expressions like ##\sin\frac\pi 4## since one of the boundaries is ##\frac l 4##. That caused me to look at your formula:

An = 2/l (from 0 to l/4)∫(4hx/l)*sin(2πnx/l)dx

Are you sure that "2" belongs there?
 
  • #9
LCKurtz said:
I can't bring myself to crunch through all the steps, but I would certainly expect expressions like ##\sin\frac\pi 4## since one of the boundaries is ##\frac l 4##. That caused me to look at your formula:

An = 2/l (from 0 to l/4)∫(4hx/l)*sin(2πnx/l)dx

Are you sure that "2" belongs there?

I'm almost certain the 2pi factor belongs there. At least it certainly does in the equations for the coefficients of a Fourier series, where the 2pi emerges from ω. Unless for some reason those equations are modified in this case? I know the book tends to leave off the 2pi, but that's when they're assuming a period of 2pi, which is of course not the case here.

That's why I can't see how they'd get ##\sin\frac\pi 4##, as there'd always be a 2 to cancel with the 4.
 
  • #10
And if that 2 weren't there, to cancel the 4 you would get answers like they claim. That alone should suggest you are wrong. I'm suggesting it too. Perhaps you should look up the FS formulas again.
 
  • #11
LCKurtz said:
And if that 2 weren't there, to cancel the 4 you would get answers like they claim. That alone should suggest you are wrong. I'm suggesting it too. Perhaps you should look up the FS formulas again.

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

Everything I've looked up suggests the 2 should be there. I'm also pretty sure I've been using the 2 in all my Fourier coefficients calculations up until now. :( I thought the two arises from the fact that ω=2pi/T.

I'm sorry. I guess I'll run through the problem again without the 2, but I don't see why it shouldn't be there...
 
  • #12
There they are using ##P## for the whole period. Most writeups use ##2p=P## so ##p## is a half period. In your problem ##p = l## is a half period.
 
  • #13
LCKurtz said:
There they are using ##P## for the whole period. Most writeups use ##2p=P## so ##p## is a half period. In your problem ##p = l## is a half period.
Yep, I just got that. Makes sense now. Thank you so much!

Although, can I ask, how would one know (without knowing the answer) that the period is in fact 2l and not l, like I wrongly assumed it was, just from reading the problem/looking at the image. Ah man, feeling rather stupid.
 
  • #14
forestmine said:
Yep, I just got that. Makes sense now. Thank you so much!

Although, can I ask, how would one know (without knowing the answer) that the period is in fact 2l and not l, like I wrongly assumed it was, just from reading the problem/looking at the image. Ah man, feeling rather stupid.

Since your string is on the interval ##[0,l]## and you are doing a half range sine expansion for it, that tells you that you are imagining the odd extension of the string to ##[-l,0]## extended periodically. So the period must be ##2l##.
 
  • #15
LCKurtz said:
Since your string is on the interval ##[0,l]## and you are doing a half range sine expansion for it, that tells you that you are imagining the odd extension of the string to ##[-l,0]## extended periodically. So the period must be ##2l##.


Hm, ok, fair enough. Thank you so much for all the help. I knew it was going to come down to something silly.
 
  • #16
Hm, I was able to work through the problem, correcting for the period, and it looks like I'm now only off by a factor of 2. A friend of mine is also having the same problem. Not sure if we can chalk it up textbook error, or just something we're not seeing...

Ah nevermind, feeling rather silly. Got it all straightened out. Thanks all for the help!
 
Last edited:

What is the wave equation for a vibrating string?

The wave equation for a vibrating string is a mathematical formula that describes the motion of a string when it is plucked or strummed. It is commonly used in physics and engineering to study the behavior of strings and other elastic materials.

What are the variables in the wave equation for a vibrating string?

The variables in the wave equation for a vibrating string include the tension of the string, the linear density of the string, the length of the string, and the wave speed. These variables determine the frequency and wavelength of the waves produced by the string.

How is the wave equation for a vibrating string derived?

The wave equation for a vibrating string is derived from Newton's second law of motion and Hooke's law. It takes into account the forces acting on the string, such as tension and restoring force, and combines them to describe the motion of the string over time.

What are the applications of the wave equation for a vibrating string?

The wave equation for a vibrating string has many practical applications, including the design and analysis of musical instruments, the study of seismic waves, and the development of technologies such as sonar and ultrasound.

Can the wave equation for a vibrating string be applied to other systems?

Yes, the wave equation for a vibrating string can be applied to other systems that exhibit wave-like behavior, such as ropes, springs, and membranes. It can also be extended to more complex systems, such as electromagnetic waves and quantum mechanical systems.

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