D'alembert solution for the semi-infinite string

In summary, the solution of the wave equation using d'Alembert solution for a semi-infinite string is given by u(x,t)=\frac{1}{2c}\left( \int^{x+ct}_{x-ct} dy\, b(y) - \int^{-x+ct}_{-x-ct} dy\, b(y) \right), where b(y)=\frac{y^2}{1+y^3}. For x \geq ct, the solution is u(x,t)=\dfrac{1}{6c}\ln\left[\dfrac{1+(x+ct)^{3}}{1+(x-ct)^{3}}\right], and
  • #1
bobred
173
0

Homework Statement


Find the solution of the wave equation using d'Alembert solution.

Homework Equations


[itex]u(0,t)=0[/itex][/B] and [itex]u(x,0)=0[/itex]
[tex]u_t(x,0)=\frac{x^2}{1+x^3}, \, x\geq0[/tex]
[tex]u_t(x,0)=0, \, x<0[/tex]


The Attempt at a Solution


For a semi infinite string we have the solution
[tex]u(x,t)=\frac{1}{2}\left( a(x-ct)+a(x+ct)-a(-x-ct)-a(-x+ct) \right)+\frac{1}{2c}\left( \int^{x+ct}_{x-ct} dy\, b(y) - \int^{-x+ct}_{-x-ct} dy\, b(y) \right)[/tex]
with [itex]u(x,0)=a(x)=0[/itex] so
[tex]u(x,t)=\frac{1}{2c}\left( \int^{x+ct}_{x-ct} dy\, b(y) - \int^{-x+ct}_{-x-ct} dy\, b(y) \right)[/tex]
where

[tex]b(y)=\frac{y^2}{1+y^3}[/tex]

Is this right?
 
Last edited:
  • #3
Thsi is what I came up with
for [tex]x \geq ct[/tex]
[tex]u(x,t)=\dfrac{1}{6c}\ln\left[\dfrac{1+(x+ct)^{3}}{1+(x-ct)^{3}}\right][/tex]
and [tex]x < ct[/tex]
[tex]u(x,t)=\dfrac{1}{6c}\left[\ln\left(\dfrac{1+(x+ct)^{3}}{1+(ct-x)^{3}}\right)\right][/tex]
 

Related to D'alembert solution for the semi-infinite string

1. What is the D'alembert solution for the semi-infinite string?

The D'alembert solution for the semi-infinite string is a mathematical solution that describes the displacement of a string that is fixed at one end and free at the other end. It takes into account the initial conditions of the string and the wave equation.

2. How is the D'alembert solution derived?

The D'alembert solution is derived from the wave equation, which is a partial differential equation that describes the motion of a wave. By solving the wave equation with the given initial conditions, the D'alembert solution can be obtained.

3. What are the assumptions made in the D'alembert solution?

The D'alembert solution assumes that the string is infinitely long, has a constant tension, and is initially at rest. It also assumes that the string has a uniform density and is perfectly flexible.

4. How does the D'alembert solution differ from other solutions for a semi-infinite string?

The D'alembert solution is unique because it takes into account the initial conditions of the string, while other solutions may only consider the wave equation. It also allows for a more general solution, as it can be applied to various boundary conditions.

5. What are some real-life applications of the D'alembert solution for a semi-infinite string?

The D'alembert solution has many practical applications, such as in acoustics, vibrations, and signal processing. It can be used to model the behavior of musical instruments, analyze the vibrations of structures, and understand the propagation of seismic waves. It is also used in the design of musical instruments, bridges, and other structures.

Similar threads

  • Calculus and Beyond Homework Help
Replies
5
Views
647
  • Calculus and Beyond Homework Help
Replies
1
Views
2K
  • Calculus and Beyond Homework Help
Replies
3
Views
608
  • Calculus and Beyond Homework Help
Replies
1
Views
2K
  • Calculus and Beyond Homework Help
Replies
20
Views
521
  • Calculus and Beyond Homework Help
Replies
4
Views
1K
  • Calculus and Beyond Homework Help
Replies
3
Views
532
Replies
4
Views
3K
  • Calculus and Beyond Homework Help
Replies
5
Views
347
  • Calculus and Beyond Homework Help
Replies
2
Views
1K
Back
Top