AEME 339 Computational Fluid Dynamics CFD K M
- Slides: 27
AE/ME 339 Computational Fluid Dynamics (CFD) K. M. Isaac 12/19/2021 topic 20_Burger's_Equation 1
Computational Fluid Dynamics (AE/ME 339) K. M. Isaac MAEEM Dept. , UMR Burger’s Equation (Ref. Tannehill, Anderson and Pletcher, Computational Fluid Mechanics and Heat Transfer, 1997) It is a model equation used to test finite difference techniques Inviscid and viscous forms can be used Has a time dependent term, non-linear term similar to the convection term, and a viscous dissipation term 12/19/2021 topic 20_Burger's_Equation 2
Computational Fluid Dynamics (AE/ME 339) K. M. Isaac MAEEM Dept. , UMR Equation (1) is parabolic when the viscous dissipation term is included. With only the terms on the LHS, the equation is hyperbolic. Equation 2 can be thought of as the non-linear wave equation, where each point on the wave can propagate with a different speed. 12/19/2021 topic 20_Burger's_Equation 3
Computational Fluid Dynamics (AE/ME 339) 12/19/2021 topic 20_Burger's_Equation K. M. Isaac MAEEM Dept. , UMR 4
Computational Fluid Dynamics (AE/ME 339) 12/19/2021 topic 20_Burger's_Equation K. M. Isaac MAEEM Dept. , UMR 5
Computational Fluid Dynamics (AE/ME 339) K. M. Isaac MAEEM Dept. , UMR Tranveling Discontinuity Problem for Burger’s Equation 12/19/2021 topic 20_Burger's_Equation 6
Computational Fluid Dynamics (AE/ME 339) 12/19/2021 topic 20_Burger's_Equation K. M. Isaac MAEEM Dept. , UMR 7
Computational Fluid Dynamics (AE/ME 339) 12/19/2021 topic 20_Burger's_Equation K. M. Isaac MAEEM Dept. , UMR 8
Computational Fluid Dynamics (AE/ME 339) K. M. Isaac MAEEM Dept. , UMR Figure 2. Characteristics for Centered Expansion 12/19/2021 topic 20_Burger's_Equation 9
Computational Fluid Dynamics (AE/ME 339) 12/19/2021 topic 20_Burger's_Equation K. M. Isaac MAEEM Dept. , UMR 10
Computational Fluid Dynamics (AE/ME 339) K. M. Isaac MAEEM Dept. , UMR The initial distribution of u results in a centered expansion where the width of the expansion grows linearly with time. The above solutions can now be used to evaluate finite difference algorithms. 12/19/2021 topic 20_Burger's_Equation 11
Computational Fluid Dynamics (AE/ME 339) 12/19/2021 topic 20_Burger's_Equation K. M. Isaac MAEEM Dept. , UMR 12
Computational Fluid Dynamics (AE/ME 339) 12/19/2021 topic 20_Burger's_Equation K. M. Isaac MAEEM Dept. , UMR 13
Computational Fluid Dynamics (AE/ME 339) 12/19/2021 topic 20_Burger's_Equation K. M. Isaac MAEEM Dept. , UMR 14
Computational Fluid Dynamics (AE/ME 339) 12/19/2021 topic 20_Burger's_Equation K. M. Isaac MAEEM Dept. , UMR 15
Computational Fluid Dynamics (AE/ME 339) K. M. Isaac MAEEM Dept. , UMR The method is 2 nd order accurate (e = O[(Dt)2, (Dx)2]) and unconditionally stable for all time steps. A tridiagonal system must be solved for each time step. 12/19/2021 topic 20_Burger's_Equation 16
Beam and Warming method Summary 12/19/2021 topic 20_Burger's_Equation 17
Computational Fluid Dynamics (AE/ME 339) K. M. Isaac MAEEM Dept. , UMR The Beam-Warming method can now be applied to the inviscid Burger’s equation 12/19/2021 topic 20_Burger's_Equation 18
Computational Fluid Dynamics (AE/ME 339) 12/19/2021 topic 20_Burger's_Equation K. M. Isaac MAEEM Dept. , UMR 19
Computational Fluid Dynamics (AE/ME 339) 12/19/2021 topic 20_Burger's_Equation K. M. Isaac MAEEM Dept. , UMR 20
Computational Fluid Dynamics (AE/ME 339) 12/19/2021 topic 20_Burger's_Equation K. M. Isaac MAEEM Dept. , UMR 21
Computational Fluid Dynamics (AE/ME 339) 12/19/2021 topic 20_Burger's_Equation K. M. Isaac MAEEM Dept. , UMR 22
Computational Fluid Dynamics (AE/ME 339) 12/19/2021 topic 20_Burger's_Equation K. M. Isaac MAEEM Dept. , UMR 23
Computational Fluid Dynamics (AE/ME 339) K. M. Isaac MAEEM Dept. , UMR Some Examples 12/19/2021 topic 20_Burger's_Equation 24
Computational Fluid Dynamics (AE/ME 339) K. M. Isaac MAEEM Dept. , UMR Solution of Burger’s equation Use Mac. Cormack’s method to solve inviscid Burger’s equation using a mesh with 51 points in the x-direction. Solve the equation for a right propagating discontinuity with u = 1 at the first 11 nodes and u = 0 at the rest of the nodes. Use Courant number = 1. Solution 12/19/2021 topic 20_Burger's_Equation 25
Computational Fluid Dynamics (AE/ME 339) 12/19/2021 topic 20_Burger's_Equation K. M. Isaac MAEEM Dept. , UMR 26
Program Completed University of Missouri-Rolla Copyright 2002 Curators of University of Missouri 12/19/2021 topic 20_Burger's_Equation 27
- Computational fluid dynamics
- Sutherland's law
- Cern alice
- Computational fluid dynamics
- Fluid dynamics
- Computational fluid dynamics
- 8883396469
- Lesson 8 quadratic functions page 339
- Computational fluid dynamic
- Fluid compartments in the body
- Shifting dullness vs fluid thrill
- Synovial membrane
- Bioimpedância
- P1-p2
- Define fluid kinematics
- Interstitial vs intracellular
- Fluid statics deals with
- Movement of body fluids
- Fluid dynamics
- Fluid dynamics definition
- Fluid dynamics
- Fluid dynamics notes
- Fluid dynamics
- Fluid power dynamics
- Real-time fluid dynamics for games
- Geophysical fluid dynamics
- Euler equation
- Colloid osmotic pressure