Fixed Rope Fourier: Complete Expression of Motion

In summary, the problem involves a rope of length L with linear density u and tension T, stretched between a wall and a ring. The initial position of the rod is given by y(x,t=0) = sin(πx/L). Using the wave equation and the method of separation of variables, the motion of the rope can be expressed as a Fourier series with coefficients An and Bn. These coefficients can be solved for using the initial condition, and the complete expression for the motion of the rope in function of t can be obtained by summing up all the Fourier components.
  • #1
Unicorn.
41
0
Hi,

Homework Statement


A rope of length L, linear density u is streched with tension T between a wall and a ring of negligible mass free to move vertically along a rod without friction. As the ring is maintained at y=0, we give to the rod a y(x,t=0) = sin(πx/L) form. We release the ring and the rope at t=0.

Give the complete expression of motion of the rope in function of t in term of its Fourier components.


Homework Equations





The Attempt at a Solution


I'm really lost, I don't know from where I have to start.
Since it must be symetric around the point x=0 so Bn=0 and anti-symetric around x=L so An=0
I have to do the work twice and add them ? And integrate from 0 to the period P=4L ?

Thanks
 
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  • #2
for your question! it's important to have a clear and structured approach to problem solving. Here are some steps you can follow to tackle this problem:

1. Start by defining your variables and constants. In this case, you have the length of the rope (L), linear density (u), and tension (T). You also have the initial position of the rod (y(x,t=0) = sin(πx/L)).

2. Next, write down the equation of motion for the rope. This can be expressed as a wave equation, since the rope is being stretched and released. It will have a time-dependent term (t) and a spatial term (x). You can also include the constants and variables you defined in step 1.

3. Now, you can use the method of separation of variables to solve this wave equation. This involves assuming a solution of the form y(x,t) = X(x)T(t), and then plugging it into the wave equation to get two separate equations for X and T. These equations will have a constant (λ) that you can solve for.

4. Once you have the solutions for X and T, you can use the initial condition (y(x,t=0) = sin(πx/L)) to solve for the Fourier coefficients, An and Bn. Remember that these coefficients represent the amplitude of each Fourier component in the solution.

5. Finally, you can write the complete expression for the motion of the rope in function of t by using the Fourier series formula. This involves summing up all the Fourier components, which will be given by the coefficients you found in step 4.

I hope this helps guide you in the right direction! Remember to always start by defining your variables and equations, and then use a systematic approach to solve the problem. Good luck!
 

What is "Fixed Rope Fourier: Complete Expression of Motion"?

"Fixed Rope Fourier: Complete Expression of Motion" is a mathematical concept used to describe the motion of a rope that is fixed at both ends. It involves using Fourier series, which is a mathematical tool used to express a periodic function as a sum of sine and cosine functions.

How is "Fixed Rope Fourier: Complete Expression of Motion" used in science?

"Fixed Rope Fourier: Complete Expression of Motion" is commonly used in fields such as physics and engineering to analyze the motion of ropes in various applications, such as in bridge construction and rope propulsion systems. It allows for a more accurate and comprehensive understanding of the behavior of ropes under different conditions.

What are the advantages of using "Fixed Rope Fourier: Complete Expression of Motion"?

Using "Fixed Rope Fourier: Complete Expression of Motion" allows for a more precise and detailed analysis of the motion of ropes, as compared to simpler mathematical models. It also allows for the prediction of how the rope will behave under different conditions, making it a valuable tool for design and engineering purposes.

Are there any limitations to using "Fixed Rope Fourier: Complete Expression of Motion"?

One limitation of using "Fixed Rope Fourier: Complete Expression of Motion" is that it assumes the rope is perfectly flexible and has no mass, which may not always be the case in real-world scenarios. It also requires a significant amount of computational power and may not be practical for use in all situations.

How can "Fixed Rope Fourier: Complete Expression of Motion" be applied in real-world situations?

"Fixed Rope Fourier: Complete Expression of Motion" has many practical applications, such as in analyzing the motion of ropes in suspension bridges or in the design of rope-based transportation systems. It can also be used to model the motion of ropes in sports, such as jump ropes or rock climbing ropes.

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