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We discuss the impact of a covolume mesh based filter on the CFL number for these methods and present an algorithm which has a CFL number independent of the spatial order of approximation. We present computational results for the advection equation and the wave equation on one-dimensional meshes using up to tenth order in space and time.<\/jats:p>","DOI":"10.1137\/060672601","type":"journal-article","created":{"date-parts":[[2008,9,18]],"date-time":"2008-09-18T10:32:23Z","timestamp":1221733943000},"page":"3151-3180","source":"Crossref","is-referenced-by-count":48,"title":["Taming the CFL Number for Discontinuous Galerkin Methods on Structured Meshes"],"prefix":"10.1137","volume":"46","author":[{"given":"T.","family":"Warburton","sequence":"first","affiliation":[],"role":[{"vocabulary":"crossref","role":"author"}]},{"given":"T.","family":"Hagstrom","sequence":"additional","affiliation":[],"role":[{"vocabulary":"crossref","role":"author"}]}],"member":"351","published-online":{"date-parts":[[2008,9,17]]},"reference":[{"key":"R1","doi-asserted-by":"publisher","DOI":"10.1016\/j.jcp.2004.01.004"},{"key":"R2","doi-asserted-by":"publisher","DOI":"10.1016\/0168-9274(94)90029-9"},{"key":"R3","doi-asserted-by":"crossref","unstructured":"P. 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