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The SBP inflow SAT produces the boundary energy term

Example

On the interval [0,1], use two endpoint nodes, H=12I, D=(−11−11), left and right selectors RL=(1,0) and RR=(0,1), and B=diag⁡(−1,1). For ut+aux=0 with a>0, inflow value g(t) at x=0, and upwind outflow at x=1, the SBP-SAT ODE is HU˙+aHD U+aeL(UL−g)=0.

Facts & Assumptions

Given: The two-node SBP data, the upwind inflow SAT sign, and the discrete energy E=12UTHU.

[F1]

Upwind SBP-SAT discretization of constant transport: the inflow SAT in the strong form is −aeL(g−UL)=aeL(UL−g) and the outflow SAT is zero.

[F2]

Upwind SBP-SAT transport satisfies the semidiscrete L2 energy identity: the SBP identity converts the volume derivative term into the signed endpoint quadratic boundary term.

Verification

1.1givenF2algebra

The matrices satisfy HD=(−1/21/2−1/21/2) and HD+DTH=B, so UTHDU=12(UR2−UL2).

2.1givenF1step 1.1algebra∎

Multiply the ODE in [F1] by UT. The inflow penalty contributes aUL(UL−g), and step 1.1 gives E˙+a2UR2+a2(UL−g)2=a2g2. Thus the penalty has the sign required by the upwind energy identity.

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