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How can we derive the wave speed formula for a rope wave by comparing coefficients of the wave equation?

By comparing the mathematical properties of the traveling-wave solution with the physical wave equation, we can derive the wave speed. The traveling wave f(x,t)=f(x−vt,0)f(x,t)=f(x-vt,0) satisfies ∂2f∂x2=1v2∂2f∂t2\frac{\partial^2 f}{\partial x^2} = \frac{1}{v^2} \frac{\partial^2 f}{\partial t^2}. The physical wave equation is ∂2f∂x2=μFT∂2f∂t2\frac{\partial^2 f}{\partial x^2} = \frac{\mu}{F_T} \frac{\partial^2 f}{\partial t^2}. Equating the coefficients of ∂2f∂t2\frac{\partial^2 f}{\partial t^2} gives 1v2=μFT\frac{1}{v^2} = \frac{\mu}{F_T}, which solves to v=FTμv = \sqrt{\frac{F_T}{\mu}}.

Conditions

  • The wave can be written in the traveling-wave form f(x−vt,0)f(x-vt,0).
  • The physical system is a string with tension FTF_T and linear density μ\mu.

Reasoning, step by step

  1. Compute the second-order partial derivatives of the traveling wave f(x−vt,0)f(x-vt,0) with respect to xx and tt using the chain rule.
  2. Establish the mathematical relationship ∂2f∂x2=1v2∂2f∂t2\frac{\partial^2 f}{\partial x^2} = \frac{1}{v^2} \frac{\partial^2 f}{\partial t^2}.
  3. Recall the physical wave equation derived from force analysis: ∂2f∂x2=μFT∂2f∂t2\frac{\partial^2 f}{\partial x^2} = \frac{\mu}{F_T} \frac{\partial^2 f}{\partial t^2}.
  4. Compare the coefficients of the second time derivative in both equations.
  5. Solve the resulting algebraic equation 1v2=μFT\frac{1}{v^2} = \frac{\mu}{F_T} for vv.

Example

The center of the screen highlights two second-order partial derivative expressions in a red box, with blue arrows pointing downward to the equation 1v2=μFT  ⟹  v=FTμ\frac{1}{v^2} = \frac{\mu}{F_T} \implies v = \sqrt{\frac{F_T}{\mu}}.

Common misconceptions

  • Assuming the wave speed depends on the amplitude of the wave.
  • Forgetting that the coefficient comparison relies on both equations describing the exact same physical phenomenon.

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