First-Order PDEs: The Transport Equation

25 min
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The transport (advection) equation is the simplest first-order PDE:

ut+cux=0.u_t + c\,u_x = 0.

Its general solution is any function of the single combination xctx - ct:

u(x,t)=f(xct).u(x, t) = f(x - ct).

This describes the initial profile f(x)=u(x,0)f(x) = u(x,0) rigidly sliding to the right at speed cc, its shape unchanged. The lines xct=constx - ct = \text{const} along which uu stays constant are called characteristics.

Worked example. Solve ut+4ux=0u_t + 4u_x = 0 with u(x,0)=x2u(x, 0) = x^2. The solution is u(x,t)=(x4t)2u(x,t) = (x - 4t)^2 — replace xx by xct=x4tx - ct = x - 4t. Check: ut=2(x4t)(4)=8(x4t)u_t = 2(x-4t)(-4) = -8(x-4t) and 4ux=42(x4t)=8(x4t)4u_x = 4\cdot 2(x-4t) = 8(x-4t), so ut+4ux=0u_t + 4u_x = 0 ✓. At x=10,t=2x = 10, t = 2: u=(108)2=4u = (10 - 8)^2 = 4.