Smaller-radius quantitative bounds for the constructed common pressure and the actual first time derivative of the correction.
Scaling a small error and its first derivatives leaves a linear smallness factor in the actual quadratic source bound.
The explicit raw-source bound before using the target-error smallness.
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The factor in the correction bound after removing the common delta.
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An explicit source constant involving only the prescribed norm budgets and the reciprocal initial radius; it is independent of delta.
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Pressure cost, given by 2*(B.spatial q hq).full.M*B.sourceCost period q hq.
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- EulerAllOrderDriftCorrection.Budget.pressureCost period B q hq = 2 * (B.spatial q hq).full.M * EulerAllOrderDriftCorrection.Budget.sourceCost period B q hq
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Time derivative cost, given by (1+2*(B.spatial q hq).full.M*(448*(B.spatial q hq).full.B+1))*B.sourceCost period q hq.
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The common raw source is bounded at the fixed smaller radius, using only the actual correction and derivative bounds already proved.
The pressure is the actual common signed pressure obtained from the coercive elliptic inverse, with an explicit smaller-radius bound.
The actual continuous time-derivative field has the bound obtained from its literal raw-source and signed-pressure equation.
The actual pressure-gradient norm is linear in the target error.
The actual first time derivative has the same linear target-error factor, at the same fixed radius and every finite external cutoff.