Brief introduction to Partial Differential Equations (PDEs)

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Presentation transcript:

Brief introduction to Partial Differential Equations (PDEs) G P Raja Sekhar Department of Mathematics IIT Kharagpur rajas@iitkgp.ac.in

First-Order PDEs Propagation of wave with speed c First-order linear wave equation (advection eq.) Propagation of wave with speed c Advection of passive scalar with speed c

Second-Order PDEs Advection-diffusion equation (linear)

Popular PDEs Laplace and Poisson’s equations Helmholtz equation Time-dependent harmonic waves Propagation of acoustic waves

Popular PDEs Wave equation Fourier equation (Heat equation)

Classification Linear second-order PDE in two independent variables (x,y), (x,t), etc. A, B, C, …, G are constant coefficients (may be generalized) (discriminant)

Well-Posed Problem (1) the solution exists (existence) (2) the solution is unique (uniqueness) (3) the solution depends continuously on the auxiliary data Mathematical - Computational

Boundary and Initial Conditions Initial conditions: starting point for propagation problems Boundary conditions: specified on domain boundaries to provide the interior solution in computational domain R R s n

Hyperbolic PDEs Two real roots, two characteristic directions Two propagation (marching) directions Domain of dependence Domain of influence (ux,uy,vx,vy) are not uniquely defined along the characteristic lines, discontinuity may occur Boundary conditions must be specified according to the characteristics

Parabolic PDEs One real (double) root, one characteristic direction (typically time is const) The solution is marching in time (or spatially) with given initial conditions The solution will be modified by the boundary conditions (time-dependent, in general) during the propagation Any change in boundary conditions at t1 will not affect solution at t < t1, but will change the solution after t = t1

Elliptic PDEs The derivatives (ux,uy,vx,vy) can always be uniquely determined at every point in the solution domain No marching or propagation direction ! Boundary conditions needed on all boundaries The solution will be continuous (smooth) in the entire solution domain