Prerequisites
Calculus, second derivatives, dimensional analysis, and physical units.
For u_t = D u_xx with constant positive D, set x = L xi and t = (L^2/D) tau. The equation becomes u_tau = u_xixi. The natural timescale L^2/D is not automatically the exact time to reach a specified tolerance.
Worked example
Tripling L at fixed D multiplies the characteristic time by nine. Boundary conditions and initial profiles still determine the actual solution and any numerical prefactor.
Model and Assumptions
Use a simplified one-dimensional diffusion model for a tracer in a rock. D has units length^2/time. Let L = 4 and D = 2 in compatible units. Assume constant D, no advection, and stated boundary conditions.
Further inquiry
Carry out both derivative substitutions explicitly. Add a constant advection speed v and derive the dimensionless equation. Identify the group vL/D and discuss when ignoring it is unjustified.
Review criteria
- Show the chain-rule factors for time and space.
- State a consistent sign convention for advection.
- Connect the dimensionless group to competing transport processes.