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  "body": "\n## Summary\n\nThe Fourier series method solves linear partial differential equations on bounded intervals or boxes by expanding the unknown in a [[Fourier series|G12KXDHPPS]].\nEach term of the series is a sine or cosine mode, and the equation acts on each mode separately.\nThe partial differential equation then becomes a family of ordinary differential equations for the coefficients.\nFourier introduced the method to solve the [[heat equation|VP2HN86VAG]], and it led to the theory of Fourier series.\nSee the [[definition|J0MHS4ZCKR]].\n\n## Explanations\n\n### L1 human\n\nA vibrating string or a heated rod can be described as a sum of simple waves, each with its own frequency.\nUnder the heat equation or the wave equation, each simple wave evolves on its own, in a way that is easy to compute.\nSo one splits the initial state into simple waves, lets each of them evolve, and adds them up again.\nFor the heat equation on $(0, \\pi)$ with zero boundary values, the mode $\\sin(kx)$ just decays like $e^{-k^2 t}$.\nHigh frequencies decay fastest, which is why heat smooths out sharp temperature differences.\n",
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