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Hyperbolic PDEs Numerical Methods for PDEs Spring 2007PowerPoint Presentation

Hyperbolic PDEs Numerical Methods for PDEs Spring 2007

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### Hyperbolic PDEs Numerical Methods for PDEs Spring 2007

Jim E. Jones

Partial Differential Equations (PDEs) :2nd order model problems

- PDE classified by discriminant: b2-4ac.
- Negative discriminant = Elliptic PDE. Example Laplace’s equation
- Zero discriminant = Parabolic PDE. Example Heat equation
- Positive discriminant = Hyperbolic PDE. Example Wave equation

Example: Hyperbolic Equation (Infinite Domain)

x+ct=constant

x-ct=constant

t

The point (x,t) is influenced only by initial conditions bounded by characteristic curves.

(x,t)

x

Example: Hyperbolic Equation (Infinite Domain)

x+ct=constant

x-ct=constant

t

The region bounded by the characteristics is called the domain of dependence of the PDE.

(x,t)

x

Hyperbolic PDES

- Typically describe time evolution with no steady state.
- Model problem: Describe the time evolution of the wave produced by plucking a string.

- Initial conditions have only local effect
- The constant c determines the speed of wave propagation.

Finite difference method for wave equation

Wave equation

Choose step size h in space and k in time

k

t

x

h

Finite difference method for wave equation

Wave equation

Choose step size h in space and k in time

Solve for ui,j+1

Finite difference method for wave equation

Stencil involves u values at 3 different time levels

k

t

x

h

Finite difference method for wave equation

Can’t use this for first time step.

U at initial time given by initial condition.

ui,0 = f(xi)

k

t

x

h

Finite difference method for wave equation

Use initial derivative to make first time step.

U at initial time given by initial condition

k

t

x

h

Domain of dependence for finite difference method

Those discrete values influence ui,j+1 define the discrete domain of dependence

k

t

x

h

CFL (Courant, Friedrichs, Lewy) Condition

A necessary condition for an explicit finite difference scheme for a hyperbolic PDE to be stable is that for each mesh point the domain of dependence of the PDE must lie within the discrete domain of dependence.

CFL (Courant, Friedrichs, Lewy) Condition

Unstable: part of domain of dependence of PDE is outside discrete domain of dependence

x-ct=constant

x+ct=constant

k

t

x

h

CFL (Courant, Friedrichs, Lewy) Condition

Possibly stable: domain of dependence of PDE is inside discrete domain of dependence

x+ct=constant

x-ct=constant

k

t

x

h

CFL (Courant, Friedrichs, Lewy) Condition

Boundary of unstable: domain of dependence of PDE is discrete domain of dependence

x+ct=constant

x-ct=constant

k

t

x

h

CFL (Courant, Friedrichs, Lewy) Condition

Boundary of unstable: domain of dependence of PDE is discrete domain of dependence

x+ct=constant

x-ct=constant

k/h=1/c

k

t

x

h

CFL (Courant, Friedrichs, Lewy) Condition

A necessary condition for an explicit finite difference scheme for a hyperbolic PDE to be stable is that for each mesh point the domain of dependence of the PDE must lie within the discrete domain of dependence.

CFL (Courant, Friedrichs, Lewy) Condition

The constant c is the wave speed, CFL condition says that a wave cannot cross more than one grid cell in one time step.

Hyperbolic Equation: characteristic curves on finite domain

x+ct=constant

x-ct=constant

t

(x,t)

x

x=a

x=b

Hyperbolic Equation: characteristic curves on finite domain

x+ct=constant

x-ct=constant

t

Value is influenced by boundary values. Represents incoming waves

(x,t)

x

x=a

x=b

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