Article ID Journal Published Year Pages File Type
1862553 Physics Letters A 2012 6 Pages PDF
Abstract

The Zhdanov–Trubnikov equation describing wrinkled premixed flames is studied, using pole decompositions as starting points. Its one-parameter (−1⩽c⩽+1−1⩽c⩽+1) nonlinearity generalises the Michelson–Sivashinsky equation (c=0c=0) to a stronger Darrieus–Landau instability. The shapes of steady flame crests (or periodic cells) are deduced from Laguerre (or Jacobi) polynomials when c≈−1c≈−1, which numerical resolutions confirm. Large wrinkles are analysed via   a pole density: adapting results of Dunkl relates their shapes to the generating function of Meixner–Pollaczek polynomials, which numerical results confirm for −10c>0 (over-stabilisation) such analytical solutions can yield accurate flame shapes for 0⩽c⩽0.60⩽c⩽0.6. Open problems are invoked.

► We study a 1-parameter (c  ) nonlinear integral equation and get flame-wrinkle shapes. ► Pole decompositions of the front slope (periodic or not) are used as a basis. ► In limiting cases we relate the flame shapes to Laguerre or Jacobi polynomials. ► Linear integral equations for pole densities give accurate large-wrinkle shapes if c<0c<0. ► Though locally singular the shapes so obtained for c>0c>0 can be fairly accurate.

Related Topics
Physical Sciences and Engineering Physics and Astronomy Physics and Astronomy (General)
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