The Laplacian operator is a second-order differential operator denoted by the symbol $$\nabla^2$$ or $$\Delta$$, which calculates the divergence of the gradient of a scalar field. In simpler terms, it measures how a function diverges from its average value around a point. The Laplacian is fundamental in various physical contexts, particularly in describing phenomena such as heat conduction, wave propagation, and electrostatics, and is closely tied to harmonic functions which are solutions to Laplace's equation.
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