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Lecture24 Navier Stokes

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Mecanica de Fluidos - Ecuaciones de Navier Stokes

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  • FC-CIV MECAFLUI: Fluid Mechanics Session 24:

    Navier-Stokes Equation

    Eusebio Ingol Blanco, Ph.D.

    Civil Engineering Program, San Ignacio de Loyola University

  • Objective

    Universidad San Ignacio de Loyola Eusebio Ingol Blanco, Ph.D.

    Understand the meaning of Navier-Stokes (N-S) equation and its derivation.

    Apply the N-S equation to fluid mechanics problems

  • Navier-Stokes Equation

    Universidad San Ignacio de Loyola Eusebio Ingol Blanco, Ph.D.

    For fluids at rest, the only stress on a fluid element is

    the hydrostatic pressure, which always acts inward and

    normal to any surface.

    ij, called the viscous stress tensor or the

    deviatoric stress tensor

    Mechanical pressure is the mean normal

    stress acting inwardly on a fluid element.

  • Newtonian versus Non-Newtonian Fluids

    Universidad San Ignacio de Loyola Eusebio Ingol Blanco, Ph.D.

    Rheology: The study of the deformation of

    flowing fluids.

    Newtonian fluids: Fluids for which the shear

    stress is linearly proportional to the shear

    strain rate.

    Non-Newtonian fluids: Fluids for which the

    shear stress is not linearly related to the shear

    strain rate.

    Viscoelastic: A fluid that returns (either fully

    or partially) to its original shape after the

    applied stress is released.

    Some non-Newtonian fluids are called shear

    thinning fluids or pseudoplastic fluids,

    because the more the fluid is sheared, the less

    viscous it becomes.

    Plastic fluids are those in which the shear

    thinning effect is extreme.

    Rheological behavior of fluids

    shear stress as a function of shear

    strain rate.

  • Derivation of the NavierStokes Equation for Incompressible, Isothermal Flow

    Universidad San Ignacio de Loyola Eusebio Ingol Blanco, Ph.D.

    The incompressible flow approximation implies constant density,

    and the isothermal approximation implies constant

    viscosity.

    ij is the strain rate tensor

  • Derivation of the NavierStokes Equation for Incompressible, Isothermal Flow

    Universidad San Ignacio de Loyola Eusebio Ingol Blanco, Ph.D.

    In Cartesian coordinates the stress tensor becomes:

    We substitute the previous equation into the three Cartesian components of Cauchys

    equation. For the x-component

    This is the continuity equation = 0

    The Laplacian of

    Velocity component u

  • Derivation of the NavierStokes Equation for Incompressible, Isothermal Flow

    Universidad San Ignacio de Loyola Eusebio Ingol Blanco, Ph.D.

    The Laplacian operator, shown here in both Cartesian and

    cylindrical coordinates, appears in the viscous term of the

    incompressible NavierStokes equation.

  • Derivation of the NavierStokes Equation for Incompressible, Isothermal Flow

    Universidad San Ignacio de Loyola Eusebio Ingol Blanco, Ph.D.

    We combine the last three components into one vector equation, to get

    the Navier-Stokes equation for incompressible flow with constant

    viscosity

  • Continuity and NavierStokes Equations in Cartesian Coordinates

    Universidad San Ignacio de Loyola Eusebio Ingol Blanco, Ph.D.

  • Continuity and NavierStokes Equations in Cylindrical Coordinates

    Universidad San Ignacio de Loyola Eusebio Ingol Blanco, Ph.D.

  • Continuity and NavierStokes Equations in Cylindrical Coordinates

    Universidad San Ignacio de Loyola Eusebio Ingol Blanco, Ph.D.

    The six independent components of the viscous stress tensor in cylindrical coordinates:

  • Differential Analysis of Fluid Flow Problems

    Universidad San Ignacio de Loyola Eusebio Ingol Blanco, Ph.D.

    There are two types of problems for which the differential equations (continuity and

    NavierStokes) are useful:

    Calculating the pressure field for a known velocity field

    Calculating both the velocity and pressure fields for a flow of known geometry and known boundary conditions

  • Example 9-13

    Universidad San Ignacio de Loyola Eusebio Ingol Blanco, Ph.D.

  • Example 9-13

    Universidad San Ignacio de Loyola Eusebio Ingol Blanco, Ph.D.

  • Example 9-13

    Universidad San Ignacio de Loyola Eusebio Ingol Blanco, Ph.D.

  • Example 9-14

    Universidad San Ignacio de Loyola Eusebio Ingol Blanco, Ph.D.

  • Example 9-14

    Universidad San Ignacio de Loyola Eusebio Ingol Blanco, Ph.D.

  • Example 9-14

    Universidad San Ignacio de Loyola Eusebio Ingol Blanco, Ph.D.

  • Example 9-14

    Universidad San Ignacio de Loyola Eusebio Ingol Blanco, Ph.D.

  • Example 9-14

    Universidad San Ignacio de Loyola Eusebio Ingol Blanco, Ph.D.

    The two-dimensional line

    vortex is a simple

    approximation of a tornado; the

    lowest pressure is at the center

    of the vortex.

  • Exact Solutions of the Continuity and NavierStokes Equations

    Universidad San Ignacio de Loyola Eusebio Ingol Blanco, Ph.D.

    Boundary Conditions

    A piston moving at speed VP in a cylinder. A thin film of oil is sheared between the piston and the cylinder; a

    magnified view of the oil film is shown. The no-slip boundary condition requires that the velocity of fluid

    adjacent to a wall equal that of the wall.

  • Exact Solutions of the Continuity and NavierStokes Equations

    Universidad San Ignacio de Loyola Eusebio Ingol Blanco, Ph.D.

    At an interface between two fluids,

    the velocity of the two fluids must

    be equal. In addition, the shear

    stress parallel to the interface must

    be the same in both fluids.

    Along a horizontal free surface of

    water and air, the water and air

    velocities must be equal and the shear

    stresses must match. However, since

    air

  • Exact Solutions of the Continuity and NavierStokes Equations

    Universidad San Ignacio de Loyola Eusebio Ingol Blanco, Ph.D.

    Boundary conditions along a plane of symmetry are defined so as to ensure that

    the flow field on one side of the symmetry plane is a mirror image of that on the

    other side, as shown here for a horizontal symmetry plane.

  • Problems 9-90 and 9-91

    Universidad San Ignacio de Loyola Eusebio Ingol Blanco, Ph.D.

    Review solved examples, 9-16, 9-17, 9-18

    Problem 9-90

    Problem 9-91

  • Problem 9-106

    Universidad San Ignacio de Loyola Eusebio Ingol Blanco, Ph.D.

  • Summary

    Universidad San Ignacio de Loyola Eusebio Ingol Blanco, Ph.D.

    Navier-Stokes Equation and Derivation

    Navier-Stokes equation in Cartesian and cylindrical coordinates

    Differential analysis of fluid flow problems

    Applications

  • Homework

    Universidad San Ignacio de Loyola Eusebio Ingol Blanco, Ph.D.

    Study sections: 9-5 and 9-6

    Hw8 is going to be posted soon.


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