Transport Processes Lec

Embed Size (px)

Citation preview

  • 7/30/2019 Transport Processes Lec

    1/20

    Chapter 1. Viscosity and the Mechanisms ofMomentum Transport

    Newtons law of viscosity (molecular momentumtransport)

    Generalisation of Newtons law of viscosity

    Pressure and temperature dependence of viscosity Molecular theory of the viscosity of gases at lowdensity, of liquids, and of suspensions andemulsions

    Convective momentum transport

  • 7/30/2019 Transport Processes Lec

    2/20

    Newtons law of viscosity(molecular transport of momentum)

    At steady-state

    Newtons law ofviscosity

    F V

    A Y

    xyx

    dv

    dy

  • 7/30/2019 Transport Processes Lec

    3/20

    Newtons law of viscosity

    Molecular transport of momentum

    = Viscosity,yx = Shear stress in the x-direction at constant y

    Velocity gradient is the driving force formomentum transport

    xyx

    dv

    dy

  • 7/30/2019 Transport Processes Lec

    4/20

    Newtons law of viscosity

    Another interpretation x-momentum is transmitted through the fluid in

    the y-direction

    yx = viscous flux of x-momentum in thepositive ydirection.

  • 7/30/2019 Transport Processes Lec

    5/20

    Newtonian fluids

    All gases and most simple liquids Viscosity is independent of -> =(T) Units: Pa.s

    Non-Newtonian fluids Viscosity is dependent of Polymeric liquids, pastes, slurries

    Kinematic viscosity, Units: m2/s

  • 7/30/2019 Transport Processes Lec

    6/20

    Viscosity Definition: the measure of a fluids resistance to flow under applied

    stress

    Newtonian: origin, constant slope( = viscosity), not time dependent

    Non-Newtonian: all others

    The apparent viscosity is the ratio of the shearstress to the shear rate. It is not the slope.

  • 7/30/2019 Transport Processes Lec

    7/20

    Example: Calculation of momentum flux Fluid between two parallel plates

    Details: plate velocity V= 1 ft/s, fluid viscosity = 0.7 cP, Y=0.001 ft

    Required: calculate steady state momentum flux yx

    2

    5 2 2/ 0 1.0 /

    (0.7 )(2.0886 10 ) 1.46 10 /0.001 0

    fx xyx f

    lb s ftdv v ft scp lb ft

    dy y cp ft

    Solution

  • 7/30/2019 Transport Processes Lec

    8/20

    Generalization of Newtons lawof viscosity

    Velocity is a vector

    Stress is a tensor with 9 components

    , ,x y zv v v v

    xx xy xz

    yx yy yz

    zx zy zz

  • 7/30/2019 Transport Processes Lec

    9/20

    Generalization of Newtons lawof viscosity

    A half of the cube is removed. Forces onthe free surface:

    x x xx xy xzpe and

    Associated to the pressure(perpendicular to the surface)

    Associated to the viscous forces.For a plane perpendicularto x-direction

  • 7/30/2019 Transport Processes Lec

    10/20

    Generalization of Newtons lawof viscosity

    Pressure and viscous forces;

  • 7/30/2019 Transport Processes Lec

    11/20

    Molecular stress

    Molecular Stress : Normal stress :

    Shear stress :

    Interpretationsij force in the j-direction on a unit areaperpendicular to the i-direction or

    ij flux of j-momentum in the positive ofi-direction

    ij ij ijp ( )ij i j

    ( )ij i j

  • 7/30/2019 Transport Processes Lec

    12/20

    = viscosity

    = dilatational viscosity (commonly not used)

    Stress tensor

    2

    3

    2

    3

    j yi x zij ij

    i j

    T

    v vv v v

    x x x y z

    v v v

  • 7/30/2019 Transport Processes Lec

    13/20

    Viscosity of gases and liquids

    Viscosity is a function of =(T,p) Viscosity may be obtained from Molecular theories

    Empirical correlations

    Correlation based in molecular theories

    Reference The Properties of Gases and Liquids by Poling, Prausnitz,

    and OConnell, 5th Ed.

  • 7/30/2019 Transport Processes Lec

    14/20

    Pressure and temperaturedependence of viscosity

    Reduced viscosity infunction of thereduced temperatureand reduced pressure

  • 7/30/2019 Transport Processes Lec

    15/20

    Critical pressure andtemperature

    The critical temperatureof a liquid is thattemperature beyond which the liquid cannot exist,no matter how much pressure is placed on it.

    The pressure that is needed to cause the gas to

    condense at the critical temperature is thecritical pressure.

  • 7/30/2019 Transport Processes Lec

    16/20

    Pressure and temperaturedependence of viscosity

    Viscosity of a gas at low density increases withincreasing temperature

    Viscosity of a liquid decreases with increasingtemperature

  • 7/30/2019 Transport Processes Lec

    17/20

    Molecular theory of the viscosityof gases at low density

    At low pressure, average velocity (random) andmean free path

    Viscosity

    2

    8 1

    2

    Tu

    md n

    2

    2

    3

    m T

    d

  • 7/30/2019 Transport Processes Lec

    18/20

    Rigorous kinetic theory.Monoatomic gases Lennard-Jones potential

    Viscosity for a pure mono-atomic gas (it can be usedfor poly-atomic gases aswell) in term of Lennard-

    Jones parameters

    12 6

    ( ) 4rr r

    2

    5

    16

    m T

  • 7/30/2019 Transport Processes Lec

    19/20

    Convective momentumtransport

    Momentum may be transported by the bulk flow ofthe fluid. Convective transport Momentum flux across the shaded area are

    Convective momentum-flux tensor (2nd order)

    Combined momentum flux

    ( ) ( ) ( )x y zv v v v v v

    i j i ji j

    vv vv ee

    vv p vv

  • 7/30/2019 Transport Processes Lec

    20/20

    Convective momentum transport.Convective momentum flux tensor