3. DESCRIPTION OF PROBLEM OR FUNCTION
2DEPEP solves the partial
differential equation system:
C1(X,Y,U,V,T)*DU/DT=D(OXX)/DX+D(OXY)/DY+F1(X,Y,U,V,T)
C2(X,Y,U,V,T)*DV/DT=D(OYX)/DX+D(OYY)/DY+F2(X,Y,U,V,T) in a
general two-dimensional region, R, with
U=FB1(S)
V=FB2(S) for S on BR1, and
OXX*NX+OXY*NY=GB1(S,U,V,T)
OYX*NX+OYY*NY=GB2(S,U,V,T) for S on BR2, where BR1 and BR2 are
distinct parts of the boundary. (NX,NY)= unit outward normal.
U=U0(X,Y)
V=V0(X,Y) for T=T0, and
OXX=OXX(X,Y,DU/DX,DU/DY,DV/DX,DV/DY,T)
OXY=OXY(X,Y,DU/DX,DU/DY,DV/DX,DV/DY,T)
OYX=OYX(X,Y,DU/DX,DU/DY,DV/DX,DV/DY,T)
OYY=OYY(X,Y,DU/DX,DU/DY,DV/DX,DV/DY,T).
The Jacobian matrices of derivatives of OXX,OXY,OYX,OYY with
respect to DU/DX,DU/DY,DV/DX,DV/DY and of F1,F2 with respect to
U,V and of GB1,GB2 with respect to U,V must be symmetric.
The related elliptic and eigenvalue problems are also solved by
2DEPEP and single equations can be handled efficiently. Examples
of applications of the program are elasticity, one- or two-
component diffusion, heat conduction, minimal surface, potential
problems and the time-independent and time-dependent Schrodinger
equations.