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Solutions to the Partial Differential Equation of Standing Waves 📂Partial Differential Equations

Solutions to the Partial Differential Equation of Standing Waves

Definition

A wave that satisfies the following condition is referred to as a stationary wave.

{ut=0,t>0u(t,x)=f(x),t=0 \begin{cases} u_{t} = 0 & , t>0 \\ u(t,x) = f(x) & , t=0 \end{cases}

Explanation

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A stationary wave is a wave whose shape does not change over time. Here, tt represents time, xx represents position, and u(t,x)u(t,x) represents the waveform at position xx when the time is tt. ff represents an initial condition, specifically the waveform when t=0t=0.

f(x)=u(0,x) f(x) = u(0, x)

If a solution exists to the partial differential equation of a stationary wave, the solution is as follows.

Solution

Take the definite integral from 00 to tt on both sides.

0tut(s,x)ds=0t0ds \int_{0}^{t} {{\partial u} \over { \partial t }} ( s , x ) ds = \int_{0}^{t} 0 ds

    u(t,x)u(0,x)=0 \implies u(t,x) - u(0,x) = 0

Regardless of tt, u(t,x)=u(0,x)u(t,x) = u(0,x) always holds, therefore u(t,x)=f(x)u(t,x) = f(x) is the case given the initial condition.