Article ID | Journal | Published Year | Pages | File Type |
---|---|---|---|---|
1862553 | Physics Letters A | 2012 | 6 Pages |
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 −1
► 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.