What is the solution for a string under tension with given boundary conditions?

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In summary: Those are what the problem wants you to find.In summary, the conversation discussed finding the equation for the motion of a string under tension, given specific boundary conditions. The solution involved using a Fourier series and determining the coefficients and frequency using the theory of Fourier analysis. The conversation also mentioned the use of separation of variables and the possibility of this being a preview of future material.
  • #1
maylie
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Homework Statement



A string of mass M and length L is attached to walls at either end, and is
under tension T. The string is held at rest in the following shape: y=B for L/2<x<3L/4
and y= 0 for the rest of the string. The string is released
at t =0.(a) Find y(x, t). You may express your answer as an infinite
series, so long as you have defined all the symbols in your series

Homework Equations


y(x)=Bsinkx
k=npi/L L =length of string n=mode no
Y(x,y)=[itex]\Sigma[/itex]Bsin(kx)cos(wt) (sm over all n)

The Attempt at a Solution


i don't understand how to incorporate the boundary conditions in given equation...i have been trying and all i come up with are two equations sin(3npix/2L) for 3l/4 and sin(kx) for L/2 ...Dont know how to go any further
 
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  • #2
maylie said:

Homework Statement



A string of mass M and length L is attached to walls at either end, and is
under tension T. The string is held at rest in the following shape: y=B for L/2<x<3L/4
and y= 0 for the rest of the string. The string is released
at t =0.(a) Find y(x, t). You may express your answer as an infinite
series, so long as you have defined all the symbols in your series

Homework Equations


y(x)=Bsinkx
k=npi/L L =length of string n=mode no
Y(x,y)=[itex]\Sigma[/itex]Bsin(kx)cos(wt) (sm over all n)

You probably mean$$
y(x,t)=\sum_{n=1}^\infty B_n \sin(\frac{n\pi} L x)\cos(\omega_n t)$$If you put ##t=0## and call your initial position of the string ##f(x)## you have$$
y(x,0)=f(x) = \sum_{n=1}^\infty B_n \sin(\frac{n\pi} L x)$$This is a Fourier series problem. Use that theory to figure out ##B_n##. We will just gloss over the fact that a continuous string can't be put in that initial shape.
 
  • #3
are you sure we have to use Fourier analysis because we arent taught this yet we had to use the above equations !
 
  • #4
Yes, I am sure. How did you get that solution in the first place? Did you use separation of variables? Fourier Series is standard material to go with that in problems like this. Maybe your teacher is trying to give you a "preview of coming attractions".
 
  • #5
no i used brute force . got it! thank you so much :)
 
  • #6
You're welcome. But you haven't "got it" until you know the formulas for ##B_n## and ##\omega_n##.
 

FAQ: What is the solution for a string under tension with given boundary conditions?

1. What is a continuous string equation?

A continuous string equation is a mathematical formula that describes the behavior of a string that is under tension and is constantly moving or changing in some way.

2. How is a continuous string equation different from a regular string equation?

A continuous string equation takes into account the dynamic behavior of a string, while a regular string equation only describes a static string.

3. What are some real-world applications of continuous string equations?

Continuous string equations are commonly used in fields such as physics, engineering, and music to model and understand the behavior of strings under different conditions, such as vibrations, bending, and tension.

4. What are the variables in a continuous string equation?

The variables in a continuous string equation depend on the specific equation being used, but they usually include parameters such as length, tension, density, and any external forces acting on the string.

5. Are there any limitations to continuous string equations?

While continuous string equations are useful for understanding the behavior of strings in certain scenarios, they may not be able to accurately model all real-world situations. For example, they may not take into account factors such as friction or non-linear behavior.

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