Laplacian: Nonlinear Function
Created: June 08, 2024
Modified: June 08, 2024

Laplacian

This page is from my personal notes, and has not been specifically reviewed for public consumption. It might be incomplete, wrong, outdated, or stupid. Caveat lector.

The Laplacian or Laplace operator 2\nabla^2 computes the vector divergence of the gradient of a function f(x)f(\mathbf{x}),

2f(x)=div  f(x)=2f(x)x12+2f(x)x22+,\nabla^2 f(\mathbf{x}) = \text{div} \;\nabla f(\mathbf{x}) = \frac{\partial^2 f(\mathbf{x})}{\partial x_1^2} + \frac{\partial^2 f(\mathbf{x})}{\partial x_2^2} + \ldots,

given by the sum of 'unmixed' second derivatives, or equivalently the trace of the Hessian matrix H(f(x))H(f(\mathbf{x})).

It is proportional to the difference between the average value of ff in a small ball around x\mathbf{x}, and the value at x\mathbf{x} itself. When 2f\nabla^2 f is positive, then ff is concave up (smaller than the local average), and when 2f\nabla^2 f is negative then ff is concave down (larger than its local average). The Laplacian therefore shows up in diffusion processes (such as the heat equation), where the function value at each point is continuously updated towards the average of its neighbors.