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The degree-two GLL mass matrix changes only its highest Legendre mode
Example
For , the one-dimensional Legendre basis has exact mass matrix , whereas the GLL quadrature mass matrix is . The only change is the top mode, with correction .
Facts & Assumptions
Given: , , , , and the GLL definition.
Legendre-Gauss-Lobatto nodes, weights, and tensor quadrature: the nodes are with weights defined by integrating their cardinal polynomials.
GLL quadrature changes only the top Legendre modes and is p-uniformly equivalent: for degree , the GLL squared-norm defect is times the squared top Legendre coefficient.
Verification
Since , its interior GLL node is , and the two endpoints complete the nodes. The cardinal polynomials are , , and . Integrating them gives weights .
Legendre orthogonality [F3] gives the exact diagonal entries , , and . The nodes and weights in step 1.1 give , , and . Every cross product has degree at most three, so exactness through degree makes the off-diagonal entries zero. The top correction is , which agrees with [F2] at and top coefficient .
Depends on
Used by
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Dependency tree · two levels
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Sources
- Lloyd N. Trefethen, Short note on the mass matrix for Gauss-Lobatto grid points (standard reference, not scraped)
- Lucas Johannes Petrus Timmermans, Analysis of Spectral Element Methods with Application to Incompressible Flow (standard reference, not scraped)