One-dimensional wave equation with non-constant speed

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Homework Help Overview

The problem involves analyzing wave propagation along a string with a sinusoidally varying cross-section, where the wave speed is not constant. The original poster seeks to explore how a wave generated by a small perturbation spreads through this non-uniform medium.

Discussion Character

  • Exploratory, Conceptual clarification, Mathematical reasoning, Assumption checking

Approaches and Questions Raised

  • Participants discuss the wave equation and its application to the problem, with some suggesting the use of Laplace transformations and separation of variables. Questions arise regarding the interpretation of initial conditions and the implications of a non-constant wave speed on the application of d'Alembert's formula.

Discussion Status

The discussion is ongoing, with participants providing insights into the wave equation and raising questions about the initial conditions and methods applicable to the problem. There is no explicit consensus, but several lines of reasoning are being explored.

Contextual Notes

Participants note the ambiguity surrounding the term "short stroke" and its implications for the initial conditions, as well as the challenges posed by the infinite nature of the string in relation to boundary conditions.

j5rp
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Homework Statement



The cross-section of a long string (string along the x axis) is not constant, but it changes wit the coordinate x sinusoidally. Explore how a wave, caused with a short stroke, spreads through the string.


Homework Equations



Relevant is the one-dimensional wave equation, where the wave speed c is not a constant (i.e. c=√T/ρS, where T is the string tension, ρ is the density of the string, and S is the cross-section).

The cross-section:
S=S1+S2*Sin[x]


The Attempt at a Solution



I thought about using Laplace transformation so that I get an ordinary differential equation. I also have trouble with the initial conditions, I don't know what is meant by short stroke, or if it really matters.
 
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I interpret 'short stroke' as simply meaning it is a small perturbation.
Can you write down the wave equation?
 
The wave equation:

(∂^2 u)/(∂t)^2 = c^2 (∂^2 u)/(∂x)^2,

where u is displacement of the string and c is the wave speed. c is not a constant, because c^2 = T/S, where T is the string tension and S is the cross-sectional area and is dependent on x. S[x]=S1+S2*Sin[x].

(Sorry about the formatting. The ∂ stands for derivative.)
 
j5rp said:
The wave equation:

(∂^2 u)/(∂t)^2 = c^2 (∂^2 u)/(∂x)^2,

where u is displacement of the string and c is the wave speed. c is not a constant, because c^2 = T/S, where T is the string tension and S is the cross-sectional area and is dependent on x. S[x]=S1+S2*Sin[x].

(Sorry about the formatting. The ∂ stands for derivative.)

In LaTeX: ##\frac{\partial^2 u}{\partial t^2} = c^2\frac{\partial^2 u}{\partial x^2}##.
So, plugging in the expression for c(x), can you apply e.g. separation of variables?
 
So, plugging in the expression for c(x), can you apply e.g. separation of variables?

I think not, because the initial conditions are probably going to be in the form u(t=0,x)=f(x) and [itex]\frac{∂u}{∂t}[/itex](t=0,x)=g(x), because it is an infinite string (no boundary conditions). But if I we separate variables (i.e. u(x,t)=X(x)*T(t)), we have to put a single value and not a function for initial conditions (example: X(0)=value, instead of u(t=0,x)= function).

I was wandering if d'Alembert's formula applies if speed of propagation (also c in the link) is not constant?
 

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