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6.1: The Wave Equation

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    34548
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    A wave can be described by a function \(f(x,t)\), called a wavefunction, which specifies the value of a measurable physical quantity at each position \(x\) and time \(t\). For simplicity, we will assume that space is one-dimensional, so \(x\) is a single real number. We will also assume that \(f(x,t)\) is a number, rather than a more complicated object such as a vector. For instance, a sound wave can be described by a wavefunction \(f(x,t)\) representing the air pressure at each point of space and time.

    The evolution of the wavefunction is described by a partial differential equation (PDE) called the time-dependent wave equation: \[\frac{\partial^2 f}{\partial x^2} = \frac{1}{v^2} \frac{\partial^2 f}{\partial t^2}, \;\;\; v \in\mathbb{R}^+.\] The parameter \(v\), which we take to be a positive real constant, is called the wave speed, for reasons that will shortly become clear.

    Sometimes, we re-arrange the wave equation into the following form, consisting of a linear differential operator acting on \(f(x,t)\): \[\left(\frac{\partial^2}{\partial x^2} - \frac{1}{v^2} \frac{\partial^2}{\partial t^2}\right) \; f(x,t) = 0.\] This way of writing the wave equation emphasizes that it is a linear PDE, meaning that any linear superposition of solutions is likewise a solution.


    This page titled 6.1: The Wave Equation is shared under a CC BY-SA 4.0 license and was authored, remixed, and/or curated by Y. D. Chong via source content that was edited to the style and standards of the LibreTexts platform; a detailed edit history is available upon request.

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