Terminology — Question 6

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Question 6

For ut+ux=0u_t+u_x=0 on ℝ2\mathbb R^2, a classical solution here means a C1C^1 field satisfying the PDE at every point. Compare u(x,t)=|x−t|,uε(x,t)=(x−t)2+ε2,ε>0.u(x,t)=|x-t|,\qquad u_\varepsilon(x,t)=\sqrt{(x-t)^2+\varepsilon^2},\quad\varepsilon>0. For this question only, an integral solution is a locally integrable field satisfying ∫ℝ2u(x,t)(ϕt+ϕx)(x,t)dxdt=0\int_{\mathbb R^2}u(x,t)\bigl(\phi_t+\phi_x\bigr)(x,t)\,dx\,dt=0 for every smooth compactly supported test function ϕ\phi.

Tasks

  1. Check the PDE for uu off x=tx=t, and decide whether uu is a classical solution on the whole plane.

  2. Verify that each uεu_\varepsilon is classical and prove a uniform error bound tending to zero as ε↓0\varepsilon\downarrow 0.

  3. Explain precisely why uniform convergence of these classical solutions does not establish that uu is classical. Inspect uε,xu_{\varepsilon,x} near the line x=tx=t.

  4. Verify that uu is an integral solution using s=x−ts=x-t, r=tr=t. State which conclusions about uu have and have not been proved.

Original worksheet page 1: question and worked solution for 9-3-006
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Question 6 – Solution

Strategy. A solution label includes a regularity requirement; checking a formula away from a singular line is not enough.

Step 1: Locate the failure of classical regularity. For x>tx>t, ux=1,ut=−1u_x=1,u_t=-1; for x<tx<t, ux=−1,ut=1u_x=-1,u_t=1. Thus the PDE holds on both open regions. At x=tx=t, the two one-sided spatial derivatives disagree. The field is not differentiable there, hence is .

Step 2: Verify the smooth approximations. Writing s=x−ts=x-t, one has uε,x=ss2+ε2,uε,t=−ss2+ε2.u_{\varepsilon,x}=\frac{s}{\sqrt{s^2+\varepsilon^2}},\qquad u_{\varepsilon,t}=-\frac{s}{\sqrt{s^2+\varepsilon^2}}. These are smooth and sum to zero. Also 0≤s2+ε2−|s|=ε2s2+ε2+|s|≤ε.0\le\sqrt{s^2+\varepsilon^2}-|s| =\frac{\varepsilon^2}{\sqrt{s^2+\varepsilon^2}+|s|}\le\varepsilon. Equality occurs at s=0s=0, so the uniform error on the whole plane is exactly ε\varepsilon.

Step 3: Separate convergence of values from derivatives. For s≠0s\ne 0, uε,x→sgn⁡(s)u_{\varepsilon,x}\to\operatorname{sgn}(s), while its value at s=0s=0 is always zero. This pointwise limit is discontinuous at zero. It cannot be a uniform limit on any closed interval about zero of these continuous derivatives. Uniform convergence of function values does not preserve differentiability, so it does not prove classical solvability.

Step 4: Check the stated integral formulation. Set ψ(s,r)=ϕ(s+r,r)\psi(s,r)=\phi(s+r,r). The change of variables has Jacobian one, and ψr=ϕx+ϕt\psi_r=\phi_x+\phi_t. Compact support and local integrability allow integration in either order. Therefore ∫ℝ2|x−t|(ϕt+ϕx)dxdt=∫ℝ|s|(∫ℝψr(s,r)dr)ds=0.\int_{\mathbb R^2}|x-t|(\phi_t+\phi_x)\,dx\,dt =\int_{\mathbb R}|s|\left(\int_{\mathbb R}\psi_r(s,r)\,dr\right)ds=0. The inner integral vanishes by compact support. Thus uu is an integral solution under the supplied definition, as well as a classical solution off the line. It remains nonclassical on the whole plane; no uniqueness assertion follows from this verification alone.

Original worksheet page 2: question and worked solution for 9-3-006

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