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2.2 Hyperbolic PDEs

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2.2 Hyperbolic PDEs

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    1. 2.2 Hyperbolic PDEs Example: Wave Equation Exact solution Linear Hyperbolic PDE, no attenuation

    3. 2.2.1 Interpretation by Characteristics Consider the Wave equation Two real roots (two characteristics) Two characteristic lines

    4. Method of Characteristics Develop computational grid and numerical solutions along the characteristic directions (? = x ? ct, ? = x + ct) General solutions - preserve the functional forms (f and g) along the characteristic lines during propagation In (x,t) coordinates, ? is a function of space and time, propagation with finite speed u = dx /dt = ? c In (?,?) coordinates, the wave appears to be stationary No attenuation (diffusion/dissipation) or dispersion (distortion of wave shape) Discontinuity will propagate into the flow domain

    5. 2.2.2 Interpretation on a Physics Basis Hyperbolic equation propagation problem with no dissipation

    6. Hyperbolic PDEs Wave equation Canonical form Consider a pure initial value problem with ?(x,0) = S(x), ?t (x,0) = cT(x)

    7. Hyperbolic PDEs Initial wave forms Exact solution

    8. Method of characteristics The solution at P(xi,tn) is uniquely determined by the initial conditions S(x) and T(x) Hyperbolic PDEs

    9. 2.2.3 Appropriate Boundary (and Initial) Conditions General rule for hyperbolic PDEs The number of auxiliary conditions is equal to the number of characteristics pointing into the domain Case (A): Both auxiliary conditions given on a non-characteristic curve Case (B): One auxiliary condition on a characteristic curve Case (c): Both auxiliary conditions on characteristic curves

    10. Auxiliary conditions Case (A): Both auxiliary conditions on a non-characteristic curve

    11. Auxiliary conditions Case (B): One auxiliary conditions on a characteristic curve

    12. Auxiliary conditions Case (C): Both auxiliary conditions on characteristic curves

    13. Characteristics - Propagation Domain of Dependence

    14. Characteristics - Propagation Domain of Influence

    15. 2.3 Parabolic PDEs Both the hyperbolic and parabolic PDEs are associated with propagation problems Hyperbolic propagation problems without attenuation Parabolic include dissipative (diffusive) mechanisms

    16. 2.3.1 Interpretation by Characteristics Consider ut + uux = ? uxx B2 4AC = 0 : Parabolic One characteristic direction defined by dt/dx = 0 The characteristic dt/dx = 0 never advance the solution in time, no equivalence to the method of characteristics for parabolic equations Hyperbolic advance the solutions in (?,?) directions

    17. Parabolic PDEs Parabolic never advance the solution in time, disturbance propagates immediately (with infinite speed) to every part of the solution domain at any given time t

    18. 2.3.2 Interpretation on a Physical Basis Typical parabolic problems march forward in time, but diffusive in space Dissipative disturbance attenuates quickly away from point P e?kx decay exponentially, but non-zero in the entire domain

    19. 2.4 Elliptic PDEs Examples A=1, B=0, C=1, B2 4AC = 4 < 0 Elliptic no real characteristics Maximum principle: both the maximum and minimum values of ? must occur on boundary Mean Value Theorem:

    20. 2.4.1 Interpretation by Characteristics The characteristics cannot be displayed in the (real) computational domain Identification of characteristics serves no purpose (no propagation behavior) Every direction is equally important Equilibrium problems When ? is small, the first order terms exhibit propagation behavior along dy/dx = v/u

    21. 2.4.2 Interpretation on a Physics Basis Equilibrium (Jury) problems A disturbance introduced at P influences all other points in the domain The influence usually diminishes away from P It is necessary to consider global solution domain (rather than marching) Discontinuity in auxiliary data are smoothed out in the interior (smooth solution) Boundary conditions are required on all boundaries (may be any combinations of Dirichlet, Neumann or mixed conditions) However, if Neumann conditions are used on all boundaries, then the Greens theorem must be satisfied

    22. Elliptic PDEs Domain of Dependence coincides with the domain of influence

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