How statement and proof provenance work
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A planar discontinuity and the space--time normal form of Rankine--Hugoniot
Example
Let , , , , a unit vector , and distinct states . Prescribe the Riemann datum for and for , and for set when and when . This bounded piecewise-constant function has strong local initial trace and is a distributional weak solution of exactly when The plane interface has unit normal from the left side to the right side ; hence the equivalent space--time normal equation is where and . This direct plane calculation uses no division by the jump.
Facts & Assumptions
Given: , , , a unit vector , , distinct , the piecewise constant function above, and a test function .
The Cauchy weak identity is the integral over with its initial term (Distributional weak solutions of the Cauchy problem). For this profile the interior equation and the strong trace established in step 1.1 give that identity by a time cutoff and passage to (Scalar conservation laws, fluxes and Cauchy data).
On the graph , Fubini's theorem reduces the space--time integral to iterated integrals, the one-dimensional fundamental theorem of calculus evaluates the -integral against at the moving endpoint, differentiation under the integral sign with the chain rule differentiates the endpoint in the remaining variables (the compactly supported smooth test supplies a uniform integrable majorant), and products of smooth functions are smooth (Fubini's theorem for L^1 functions on a sigma-finite product, The second fundamental theorem: if is differentiable on with and is integrable, then , Differentiation under the integral sign, The chain rule, in one line from Carathéodory: if is differentiable at and is differentiable at , then is differentiable at with , Sums, scalar multiples, products and quotients: , , , and when ).
For every point of an open set and every neighbourhood of it there is a nonnegative smooth compactly supported test function, supported in that neighbourhood and positive at the point: take a finite product of rescaled translated copies of the bump of Explicit compactly supported smooth cutoffs.
Proof
The initial trace. For a compact and , the two definitions of and differ exactly on , a set of measure at most ; hence as . So has the strong local trace .
The interface computation. Choose with , and put . For a test supported in , integrate first in on each side of . FTC and the moving-endpoint rule give the weak pairing For the lower side is the left state; for the lower side is the right state, which reverses the jump and converts to . The endpoint derivatives are and .
The initial boundary. For a test meeting , perform the same integration on . The bottom term is . By step 1.1 it converges to , cancelling the prescribed initial term. Thus the full Cauchy residual is the interface integral of step 1.2 over .
Necessity. If , then it is nonzero on a small interface patch; by [F3] there is a nonnegative smooth compactly supported test function supported in a small space--time neighbourhood of a point of that patch and positive on the patch, and step 2.1 makes the weak residual for this test nonzero, contradicting the weak identity.
Sufficiency and normal form. Conversely, if , the interface bracket vanishes identically and step 2.1 shows that the weak identity holds for every test function; the trace was verified in step 1.1, so is a distributional weak solution. Since is a unit vector, has length , so the unit normal from the minus side is and the condition becomes . No division by the jump was used at any point.
Depends on
- Scalar conservation laws, fluxes and Cauchy data
- Distributional weak solutions of the Cauchy problem
- Fubini's theorem for L^1 functions on a sigma-finite product
- The second fundamental theorem: if $G$ is differentiable on $[a,b]$ with $G' = f$ and $f$ is integrable, then $\int_a^b f = G(b)-G(a)$
- Differentiation under the integral sign
- The chain rule, in one line from Carathéodory: if $g$ is differentiable at $c$ and $f$ is differentiable at $g(c)$, then $f \circ g$ is differentiable at $c$ with $(f \circ g)'(c) = f'(g(c))\,g'(c)$
- Sums, scalar multiples, products and quotients: $(f+g)'(c) = f'(c) + g'(c)$, $(\alpha f)'(c) = \alpha f'(c)$, $(fg)'(c) = f'(c)g(c) + f(c)g'(c)$, and $(f/g)'(c) = \bigl(f'(c)g(c) - f(c)g'(c)\bigr)/g(c)^{2}$ when $g(c) \ne 0$
- Explicit compactly supported smooth cutoffs
Used by
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Sources
- G. A. Chechkin and A. Yu. Goritsky (translated by B. Andreianov), “S. N. Kruzhkov’s lectures on first-order quasilinear PDEs,” in Analytical and Numerical Aspects of PDEs, de Gruyter 2009, complete lecture-notes text (standard reference, not scraped)
- Alberto Bressan, “Hyperbolic Conservation Laws: An Illustrated Tutorial,” 2009, complete lecture notes (standard reference, not scraped)