Numerical study on nonlinear burgers and modified burgers equations using b splines
Loading...
Date
item.page.authors
Journal Title
Journal ISSN
Volume Title
Publisher
Abstract
Nonlinear partial differential equations emerge very frequently while modelling physical processes and are
newlinehighly useful in simulating and understanding a vast majority of phenomena in science and engineering. They
newlineplay a prominent role in the modelling of almost every physical, biological or technical process ranging from
newline
newlineatomic interactions to celestial motion. However, they can exhibit very chaotic behaviours, and hence under-
newlinestanding their physical characteristics by solving them analytically tend to be very complicated. Studies on
newline
newlinedifferential equations indicate that solving a partial differential equation by explicit formulas may not always
newlinebe possible. In many cases, it is challenging to justify even the elementary properties of existence, uniqueness
newline
newlineand well-posedness of solutions of nonlinear partial differential equations. Extensive research has been car-
newlineried out in developing several numerical techniques for studying the nature and solutions of partial differential
newline
newlineequations. However, many of these methods fail when the equations involved are highly nonlinear or when
newlinethe nature of equations is extremely chaotic. Hence, there prevails a need for more studies and investigations
newlinein this area and also the construction of more efficient and accurate numerical methods.
newline
newlineOne of the most significant nonlinear partial differential equations, which is at the heart of fluid flow mod-
newlineelling, is the Navier-Stokes equation. The general flow of a Newtonian incompressible fluid may be repre-
newlinesented by Navier-Stokes equation in three dimensions as: and#8706;U
newlineand#8706;t
newline+Uand#57344;and#57350;U = and#8722; 1
newlineand#57358;
newlineand#57350;p+ and#956;
newlineand#57358;
newlineand#57350;2U,
newline
newlinewhere, U = U(x, y,z,t) and#8712; R3 is the velocity vector, and#57358; represents the density of fluid, p denotes the pressure
newlinevector, and and#956; is the viscosity. A closed form solution of the Navier-Stokes equation is unknown to date.
newlineJohannes Martinus Burger, a Dutch scientist, devised a simplified form of the Navier-Stokes equation by
newlinedropping the pressure term.
newline