Applied/ACMS/Spring2025: Difference between revisions
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| Mar 28 | | Mar 28 | ||
|Spring break | |Spring break | ||
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| Apr 18 | |Apr 11 | ||
|[https://meche.mit.edu/people/faculty/pierrel@mit.edu Pierre Lermusiaux] (MIT) | |||
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|Chen | |||
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|Apr 18 | |||
|[https://www.math.uci.edu/~jxin/ Jack Xin] (UC Irvine) '''[Colloquium]''' | |||
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| Apr 25 | |||
|[https://www-users.cse.umn.edu/~bcockbur/ Bernardo Cockburn] (Minnesota) | |[https://www-users.cse.umn.edu/~bcockbur/ Bernardo Cockburn] (Minnesota) | ||
|''Transforming stabilization into spaces'' | |''Transforming stabilization into spaces'' |
Latest revision as of 22:43, 7 September 2024
Spring 2025
date | speaker | title | host(s) | |
---|---|---|---|---|
Mar 28 | Spring break | |||
Apr 11 | Pierre Lermusiaux (MIT) | Chen | ||
Apr 18 | Jack Xin (UC Irvine) [Colloquium] | |||
Apr 25 | Bernardo Cockburn (Minnesota) | Transforming stabilization into spaces | Stechmann, Fabien |
Abstracts
Bernardo Cockburn (Minnesota)
Title: Transforming stabilization into spaces
In the framework of finite element methods for ordinary differential equations, we consider the continuous Galerkin method (introduced in 72) and the discontinuous Galerkin method (introduced in 73/74). We uncover the fact that both methods discretize the time derivative in exactly the same form, and discuss a few of its consequences. We end by briefly describing our ongoing work on the extension of this result to some Galerkin methods for partial differential equations.