Sketching wave equation solutions.

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SUMMARY

The discussion focuses on solving the wave equation for an infinite string, specifically analyzing the transverse displacement \( z \) and the velocity of transverse traveling waves. The velocity is determined as \( v = \sqrt{T/\rho} \), where \( T \) is tension and \( \rho \) is linear density. The initial displacement is defined piecewise, and the solution involves D'Alembert's formula. Participants clarify the implications of boundary conditions and the behavior of waves upon reflection.

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  • Understanding of wave equations and their mathematical formulations
  • Familiarity with D'Alembert's solution for wave equations
  • Knowledge of boundary conditions in wave mechanics
  • Basic concepts of tension and linear density in strings
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Students and educators in physics, particularly those studying wave mechanics, as well as engineers and researchers working with wave phenomena in strings and similar systems.

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Homework Statement



An infinite string obeys the wave equation (d2z/dx2)=(ρ/T)(d2z/dt2) where z is the transverse displacement, and T and ρ are the tension and the linear density of the string. What is the velocity of transverse traveling waves on the string?
The string has an initial displacement
z= (h/L)(L-x) for 0<x<L, (h/L)(L+x) for -L<x<0, 0 otherwise
where h is a constant. The string is initially at rest. Sketch z(x,t) at the times
t=αL√(ρ/T) for α=0, 1/4, 1/2, and 1.

Homework Equations





The Attempt at a Solution



v=√(T/ρ), from the wave equation.

Using D'Alembert's solution, I get z=(h/2L)(L-(x+ct))+(h/2L)(L-(x-ct)) for 0<x<L
and z=(h/2L)(L+(x+ct))+(h/2L)(L+(x-ct)) for -L<x<0 and 0 otherwise.

But the ct terms seem to cancel, so I'm guessing I've gone wrong somewhere. :-/

Thanks in advance for any help! :-)
 
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Lucy Yeats said:

Homework Statement



An infinite string obeys the wave equation (d2z/dx2)=(ρ/T)(d2z/dt2) where z is the transverse displacement, and T and ρ are the tension and the linear density of the string. What is the velocity of transverse traveling waves on the string?
The string has an initial displacement
z= (h/L)(L-x) for 0<x<L, (h/L)(L+x) for -L<x<0, 0 otherwise
where h is a constant. The string is initially at rest. Sketch z(x,t) at the times
t=αL√(ρ/T) for α=0, 1/4, 1/2, and 1.

Homework Equations


The Attempt at a Solution



v=√(T/ρ), from the wave equation.

Using D'Alembert's solution, I get z=(h/2L)(L-(x+ct))+(h/2L)(L-(x-ct)) for 0<x<L
and z=(h/2L)(L+(x+ct))+(h/2L)(L+(x-ct)) for -L<x<0 and 0 otherwise.

But the ct terms seem to cancel, so I'm guessing I've gone wrong somewhere. :-/

Thanks in advance for any help! :-)

I assume your boundary condition is z(x=±L, t)=0;
Now image what happens if both ends of the string are free, the initial triangular shaped wave would
separate into two half-amplitude triangles and travel toward ±∞, since the endpoints are fixed, these
two waves are immediately reflected, the reflected wave must be of the same shape, 180° out of phase
and travel in the opposite direction, so that the total displacement at the endpoints are always zero ...
Now you know how to figure out the rest.

Alternatively, if you like doing more math and less thinking, general solutions to the wave equation on
a string must be given by some cosine and sine waves of wavelengths 2L/n ...
 
Sorry to be slow, but why am I not allowed to cancel out the ct terms? :-/

Thanks for helping!
 

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