Wave equation, D'Alembert's Solution

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SUMMARY

The discussion focuses on the wave equation and D'Alembert's solution, highlighting the distinction between general and specific solutions. D'Alembert's solution is recognized as a general solution to the wave equation, represented as a function g(x-ct) rather than in terms of sines and cosines. This approach allows for the representation of non-periodic waveforms, such as a distorted rope, which can be modeled by arbitrary functions. The conversation emphasizes the nature of wave propagation and the role of initial conditions in shaping the solution.

PREREQUISITES
  • Understanding of partial differential equations (PDEs)
  • Familiarity with wave equations and their properties
  • Knowledge of D'Alembert's solution and its formulation
  • Concept of initial conditions in wave motion
NEXT STEPS
  • Study the derivation of D'Alembert's solution for the wave equation
  • Explore the implications of initial conditions on wave propagation
  • Investigate the characteristics of non-periodic waveforms in physics
  • Learn about the role of Fourier series in solving wave equations
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Students and professionals in mathematics and physics, particularly those studying wave phenomena, partial differential equations, and the applications of D'Alembert's solution in various contexts.

Tuneman
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I am having trouble understanding the solution to the wave equation:

735128d3de55366340a2e5fb647c470e.png


this is thought of as the final solution to the PDE:
img250.gif


but I see that:
img246.gif


is a solution to the function. But what I don't get is why D'Alembert's Solution isn't in terms of sines and cosines like that solution right above.

Is it because D'Albemerts is a gereneral solution, and the other is a specific solution? If so, still how come the general solution to the problem isn't expressed as a wave, and instead of some arbitrary function g(x-ct)?
 
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The general solution is a wave. But a wave is not necessarily periodic like sine or cosine. Imagine a taut rope that is distorted initially in a shape that consists of a bulge, say a triangle between x= -1 and x= 1, given by y= x+1 for x<0, y= 1-x for x>=0 and then released from rest at t=0. "g" splits into two parts which move right and left: that's what (1/2)g(x-ct) and (1/2)g(x+ct) are. The h integral allows non-zero speed at t= 0 also.
 

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