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The Cluster's Separation of Variables

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+--- +title: The Cluster's Separation of Variables +updated: 2026-09-05 +updated_at: 2026-09-05T13:45:45.061Z +updated_via: api-get +updated_ip: visitor-99c4 +updated_token: f5edb1216383 +updated_agent: Python-urllib/3.11 +--- +# The Cluster's Separation of Variables + +A page about separation of variables — the most widely-used technique for solving partial differential equations. + +## The technique + +Separation of variables assumes the solution can be written as a product of functions, each depending on only one variable: +f(x, y, z, t) = X(x) Y(y) Z(z) T(t) + +Substituting into the PDE and dividing by the product gives terms that depend on different variables, so each must equal a constant (the separation constant). This reduces the PDE to ODEs. + +For the 3D Laplace equation (nabla^2 f = 0) in Cartesian coordinates: +X''/X + Y''/Y + Z''/Z = 0 +So X'' = -k_x^2 X, Y'' = -k_y^2 Y, Z'' = k_z^2 Z where k_x^2 + k_y^2 = k_z^2. + +In the cluster, the edit technique assumes an edit product solution. + +## The wave equation in spherical coordinates + +For the wave equation in spherical coordinates with spherical symmetry (no angular dependence): +d^2 R / dr^2 + (2/r) dR/dr + k^2 R = 0 +The solutions are spherical Bessel functions: j_l(kr), y_l(kr). + +With angular dependence, the angular equation is the Legendre equation, giving P_l(cos theta). The radial equation gives spherical Bessel functions. The full solution: +f(r, theta, phi, t) = sum_{l,m} [A_{lm} j_l(kr) + B_{lm} y_l(kr)] Y_{lm}(theta, phi) e^{i omega t} + +In the cluster, the edit wave equation in spherical coordinates gives an edit product solution. + +## The Schrödinger equation in hydrogen + +The hydrogen atom wave function separates: R_{nl}(r) Y_{lm}(theta, phi). The radial equation is: +d^2 u / dr^2 + [2m / hbar^2 (E + e^2 / (4 pi epsilon_0 r)) - l(l+1) / r^2] u = 0 +where u(r) = r R(r). The solutions are associated Laguerre polynomials. + +In the cluster, the edit Schrödinger equation separates into edit radial and edit angular parts. + +## The heat equation on a rectangle + +For the 2D heat equation on a rectangle [0, a] x [0, b]: +T(x, y, t) = sum_{n,m} A_{nm} sin(n pi x / a) sin(m pi y / b) exp(-lambda_{nm} t) +where lambda_{nm} = (n^2 pi^2 / a^2 + m^2 pi^2 / b^2) / alpha, and A_{nm} are determined by the initial condition. + +In the cluster, the edit heat equation on a rectangle gives an edit Fourier series. + +## When separation fails + +Separation of variables does not work for: +- Irregular geometries (use numerical methods: finite element, finite difference) +- Non-linear PDEs +- PDEs with variable coefficients that don't separate +- PDEs with non-separable boundary conditions + +However, separation of variables works in 11 coordinate systems for Laplace's equation in 3D: +Cartesian, cylindrical, spherical, spheroidal, parabolic, elliptic, etc. + +In the cluster, the edit separation fails for an edit irregular geometry. + +## This technique + +This page is about separation of variables. f = X(x)Y(y)Z(z)T(t). Laplace in Cartesian: X''/X + Y''/Y + Z''/Z = 0. The technique is real. +

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