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CP502 Advanced Fluid Mechanics

CP502 Advanced Fluid Mechanics. Incompressible Flow of Viscous Fluids. Set 01. υ. ρ. Equations describing incompressible flow of viscous fluid: We will learn: Physical meaning of each term How to derive How to solve. What do we mean by ‘Fluid’?. Physically: liquids or gases

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CP502 Advanced Fluid Mechanics

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  1. CP502 Advanced Fluid Mechanics Incompressible Flow of Viscous Fluids Set 01

  2. υ ρ Equations describing incompressible flow of viscous fluid: We will learn: • Physical meaning of each term • How to derive • How to solve

  3. What do we mean by ‘Fluid’? • Physically: liquids or gases • Mathematically: • A vector field u(represents the fluid velocity) • A scalar field p (represents the fluid pressure) • fluid density (ρ) and fluid viscosity (μ)

  4. Recalling vector operations • Del Operator: • Laplacian Operator: • Gradient: • Vector Gradient: • Divergence: • Directional Derivative:

  5. Continuity equationfor incompressible (constant density) flow - derived from conservation of mass where u is the velocity vector ux, uy & uz are velocity components in x, y & z directions

  6. Continuity equationderivation Mass flux on left face Mass flux on right face Inflow at left face = Outflow at right face = Difference between inflow and outflow in the x direction per unit volume

  7. Continuity equationderivation Mass flux on left face Mass flux on right face Difference between inflow and outflow in the y direction per unit volume Difference between inflow and outflow in the z direction per unit volume Thus net rate of inflow/outflow per unit volume

  8. Continuity equationderivation Mass flux on left face Mass flux on right face Net rate of inflow/outflow per unit volume = rate of increase in mass per unit volume = rate of change of density Continuity equation in general form

  9. Continuity equationfor incompressible flow Density is constant for incompressible flow: Divergence of u or

  10. υ ρ Navier-Stokes equationfor incompressible flow of Newtonian (constant viscosity) fluid - derived from conservation of momentum kinematic viscosity (constant) density (constant) pressure external force (such as gravity)

  11. υ υ ρ ρ Navier-Stokes equationfor incompressible flow of Newtonian (constant viscosity) fluid - derived from conservation of momentum

  12. υ ρ Navier-Stokes equationfor incompressible flow of Newtonian (constant viscosity) fluid - derived from conservation of momentum Acceleration term: change of velocity with time

  13. υ ρ Navier-Stokes equationfor incompressible flow of Newtonian (constant viscosity) fluid - derived from conservation of momentum Convection term

  14. υ ρ Navier-Stokes equationfor incompressible flow of Newtonian (constant viscosity) fluid - derived from conservation of momentum Viscous forces term

  15. υ ρ Navier-Stokes equationfor incompressible flow of Newtonian (constant viscosity) fluid - derived from conservation of momentum Pressure term: Fluid flows in the direction of largest change in pressure

  16. υ ρ Navier-Stokes equationfor incompressible flow of Newtonian (constant viscosity) fluid - derived from conservation of momentum Body force term: external forces that act on the fluid (such as gravity, electromagnetic, etc.)

  17. υ ρ Navier-Stokes equationfor incompressible flow of Newtonian (constant viscosity) fluid - derived from conservation of momentum

  18. υ ρ Continuity and Navier-Stokes equationsfor incompressible flow of Newtonian fluid

  19. Continuity and Navier-Stokes equationsfor incompressible flow of Newtonian fluid in Cartesian coordinates Continuity: Navier-Stokes: x - component: y - component: z - component:

  20. Moving plate Fixed plate h h Fluid flow direction Fluid flow direction y y x x Fixed plate Fixed plate Steady, incompressible flow of Newtonian fluid in an infinite channel with stationery plates- fully developed plane Poiseuille flow Steady, incompressible flow of Newtonian fluid in an infinite channel with one plate moving at uniform velocity - fully developed plane Couette flow

  21. Continuity and Navier-Stokes equationsfor incompressible flow of Newtonian fluid in cylindrical coordinates Continuity: Navier-Stokes: Radial component: See the handout Tangential component: Axial component:

  22. φ 2a Steady, incompressible flow of Newtonian fluid in a pipe- fully developed pipe Poisuille flow Fixed pipe r z Fluid flow direction 2a

  23. φ a r b aΩ Steady, incompressible flow of Newtonian fluid between a stationary outer cylinder and a rotating inner cylinder- fully developed pipe Couette flow

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