Fundamentals of Heat and Mass Transfer, 6...

download Fundamentals of Heat and Mass Transfer, 6 editioncourse.sdu.edu.cn/download/174fae3e-0ab9-41ab-a152... · Fundamentals of Heat and Mass Transfer, 6e 1 ... then solution of the differential

If you can't read please download the document

Transcript of Fundamentals of Heat and Mass Transfer, 6...

  • 1Fundamentals of Heat and Mass Transfer, 6e

    Fundamentals of Heat and Mass

    Transfer, 6th edition

    Presented E-mail: [email protected]

    Telephone: 88399000-2511

    mailto:[email protected]

  • 2Fundamentals of Heat and Mass Transfer, 6e

    Chapter 6 Introduction to convection

    Convection: energy transfer between a surface and a fluid moving over the surface

    ObjectivesUnderstand the physical mechanism of convection;

    Develop means to perform convection transfer calculation

    Contents:Basic contents on convection heat transfer and convection

    mass transfer

    physical origin, dimensionless parameters, analogies

  • 3Fundamentals of Heat and Mass Transfer, 6e

    Chapter 6 Introduction to convection

    Convection: energy transfer between a surface and a fluid moving over the surface()

    the bulk fluid motion (advection)

    the random motion of fluid molecules (conduction or diffusion)

    The determination of convection transfer coefficient and related heat transfer

    enhancement method are the central problems in the study of convection issue.

  • 4Fundamentals of Heat and Mass Transfer, 6e

    Chapter 7 External flow

    Chapter 8 Internal flow

    Chapter 9 Free convection

    Chapter 10 Boiling and condensation

    Chapter 11 Heat exchangers

  • 5Fundamentals of Heat and Mass Transfer, 6e

    6.1 the convection boundary layer

    Boundary layers: velocity, thermal , concentration,

    Friction coefficient

    Convection heat transfer coefficient

    Convection mass transfer coefficient

  • 6Fundamentals of Heat and Mass Transfer, 6e

    6.1 the convection boundary layer

    The velocity boundary layer Fluid velocity=0 at the surface

    Velocity grow Velocity u

    Shear stress (), parallel to fluid velocity

    In boundary layer ( a thin layer): velocity gradients and shear stresses are large

    Region outside the boundary layer: velocity gradients and shear stresses are

    negligible

    uu 99.0Velocity boundary layer thickness

  • 7Fundamentals of Heat and Mass Transfer, 6e

    6.1 the convection boundary layer

    Velocity boundary layer: developed whenever there is fluid flow over a surface

    For a Newtonian fluid

    dynamic viscosity

    kg/m S

    u velocity along the x direction

    m/s

    surface shear stressN/m2

    Cf: the local friction coefficient,

    to determine the friction drag a dimensionless parameter

    sx

    y

    u

    Cf

  • 8Fundamentals of Heat and Mass Transfer, 6e

    6.1 the thermal boundary layer

    99.0)/()( TTTT sst Thermal boundary layer thickness when

    Developed when the flow free stream and the surface temperatures differ

    x y

    T

    h

  • 9Fundamentals of Heat and Mass Transfer, 6e

    6.1 the concentration boundary layer

    Example: air past the surface of a pool of water evaporation a binary mixture of chemical species A and B,

    Sublimation

    CA: molar concentration , kmol/m3

  • 10Fundamentals of Heat and Mass Transfer, 6e

    Concentration boundary layer:

    concentration gradients exist()

    :thickness is defined asc 99.0)(

    )(

    ,,

    ,

    AsA

    AsA

    CCCC

    Molar flux of species A , NA (kmol / s m2)A

    Binary diffusion coefficient, DAB

    Fick s law Diffusion mass transfer,y

    CDN AABA

    ''

    At the surface y=0,

    diffusion mass transfer 0''

    ,

    y

    AABsA

    y

    CDN

    6.1 the concentration boundary layer

  • 11Fundamentals of Heat and Mass Transfer, 6e

    Analogous to Newtons law of cooling

    6.1 the concentration boundary layer

    )( ,.,''

    AsAmsA CChN

    ,,

    0

    AsA

    AAB

    mCC

    yy

    CD

    h

    hm, convection mass transfer

    coefficient, m/s,

    y

    CDN AABA

    ''

  • 12Fundamentals of Heat and Mass Transfer, 6e

    6.1 significance of the boundary layer

    Flow over a surface velocity boundary layer surface friction

    Flow over a surface with temp difference thermal boundary

    layer convection heat transfer

    Flow over a surface with concentration difference concentration

    boundary layer convection mass transfer

    items Characteristics Key parameters

    Velocity gradient,

    shear stresses

    Friction coefficient Cf

    Temp gradient,

    heat transfer

    Heat transfer coefficient,

    h

    Concentration gradient,

    species transfer

    Mass transfer coefficient,

    hm

    t

    t

    c

  • 13Fundamentals of Heat and Mass Transfer, 6e

    6.2 local and average convection

    coefficients

    Heat transfer

    The local heat flux , q

    The total heat rate , q

    Average convection heat transfer coefficient, h

  • 14Fundamentals of Heat and Mass Transfer, 6e

    6.2 local and average convection

    coefficients

    Mass transfer

    NA: molar transfer rate kmol/s

  • 15Fundamentals of Heat and Mass Transfer, 6e

    6.2 local and average convection

    coefficients

    Molar flux mass flux

    Molar transfer rate mass transfer rate

    0

    ''

    ,

    y

    AABsA

    yDn

    Molecular weight (kg/kmol)

    Molecular weight (kg/kmol)

    ,,

    0

    AsA

    AAB

    m

    yy

    Dh

    AAA CM

  • 16Fundamentals of Heat and Mass Transfer, 6e

    Example 6.1

  • 17Fundamentals of Heat and Mass Transfer, 6e

  • 18Fundamentals of Heat and Mass Transfer, 6e

    6.3 laminar and turbulent flow

    Flow condition: laminar flow() turbulent flow

  • 19Fundamentals of Heat and Mass Transfer, 6e

    6.3 laminar and turbulent flow

    Boundary layer development on a flat plat

    Laminar flow: fluid flow is highly ordered, streamline

    Transition zone: laminar or turbulent

    Turbulent flow: flow is highly irregular, random, 3-D motion, chaotic flow

    3 regions in the turbulent boundary layer: viscous sublayer ()buffer layer ()turbulent zone ()

  • 20Fundamentals of Heat and Mass Transfer, 6e

    5105Re

    xux

    Critical Reynolds number, ranging in 105~3X106

    xucx

    ,Re

    Determination parameter for the onset of turbulent flow :

    Reynolds number =the ratio of inertia to viscous forces

    = /

    x, characteristic length

  • 21Fundamentals of Heat and Mass Transfer, 6e

    Laminar and turbulent thermal

    boundary layer

    Laminar region :streamline, temperature gradient is decreased in the streamline direction heat transfer

    coefficient is decreased

    Transition region:

    Turbulent region: local convection heat transfer

    coefficient is decreased

    along the flow direction.

  • 22Fundamentals of Heat and Mass Transfer, 6e

  • 23Fundamentals of Heat and Mass Transfer, 6e

  • 24Fundamentals of Heat and Mass Transfer, 6e

  • 25Fundamentals of Heat and Mass Transfer, 6e

  • 26Fundamentals of Heat and Mass Transfer, 6e

    Thermal and species concentration

    boundary layer

    Laminar region :streamline, temp and concentration gradient decrease in the streamline direction heat and

    mass transfer coefficient decrease

    Transition region:

    Turbulent region: local convection heat and mass

    transfer increased

  • 27Fundamentals of Heat and Mass Transfer, 6e

    Example 6.4 p362

    For concentration boundary layer

  • 28Fundamentals of Heat and Mass Transfer, 6e

    6.4 the boundary layer equation

  • 29Fundamentals of Heat and Mass Transfer, 6e

    6.4 the boundary layer equation

    Boundary layer equations for laminar flowComply with fundamental laws of nature:

    Including conservation of mass, energy and chemical species, Newtons second law of motion

    Assumption

    In the Cartesian coordinate, equations for the steady, 2D flow of an incompressible fluid with constant properties are summarized in Appendix D the convection Transfer Equations.

    ( Appendix E gives the corresponding equations for the boundary layer in turbulent flow.)

  • 30Fundamentals of Heat and Mass Transfer, 6e

    6.4 the boundary layer equation

    The continuity equation

  • 31Fundamentals of Heat and Mass Transfer, 6e

    6.4 the boundary layer equation

    The x momentum equation x

    The net pressure

    force

    The net rate

    force due to

    viscous shear

    stresses

    The net rate due

    to fluid motion

    across boundary

  • 32Fundamentals of Heat and Mass Transfer, 6e

    6.4 the boundary layer equation

    The energy equation,

    The net

    conduction rate

    in the y direction

    The net rate due

    to fluid advection

    Viscous dissipation

    Neglect in some cases

  • 33Fundamentals of Heat and Mass Transfer, 6e

    6.4 the boundary layer equation

    The species concentration equation

    The net transport

    of species A due

    to advection

    The net transport

    of species A due

    to y-direction

    diffusion

  • 34Fundamentals of Heat and Mass Transfer, 6e

    6.4 the boundary layer equation

    Laminar boundary layer equations

    Right side: diffusion terms

    If neglect

    Left side: advection terms

    44

  • 35Fundamentals of Heat and Mass Transfer, 6e

    6.5 boundary layer similarity

    Nondimensionalizing the governing equations:

    L: characteristic length of the surface of interest,

    V: velocity of the upstream

    Viscous dissipation is neglected

  • 36Fundamentals of Heat and Mass Transfer, 6e

    Nondimensional form of the

    boundary layer equation

  • 37Fundamentals of Heat and Mass Transfer, 6e

    6.5 boundary layer similarity

    Similarity parameters (important, apply results for a surface to geometrically similar surfaces)

    Reynolds number Re

    Prandtl number, Pr,

    If both the boundary conditions and similarity parameters

    are same for two different conditions (that is geometrically

    similar ), then solution of the differential equations for the

    nondimensional velocity and temperature will be same.

    VLRe

    Dynamic viscosity, kg/s m

    Kinetic viscosity, m2/s

  • 38Fundamentals of Heat and Mass Transfer, 6e

    6.5 boundary layer similarity

    Functional form of the solutions

    Local

    Nusselt Number

    Average

  • 39Fundamentals of Heat and Mass Transfer, 6e

    6.5 boundary layer similarity

    Functional form of the solutions

  • 40Fundamentals of Heat and Mass Transfer, 6e

  • 41Fundamentals of Heat and Mass Transfer, 6e

    6.6 physical significance of the

    dimensionless parameters

    Reynolds number: the ratio of inertia to viscous forces

    Grashof number: the ratio of the buoyancy forces to

    viscous forces

    Prandtl number: the relative effectiveness of momentum

    and energy transfer by diffusion in the velocity and

    thermal boundary layer, the relative thickness of velocity

    and thermal boundary layer.

    For gas Pr=1, For liquid metal Pr1

    n is a positive component

  • 42Fundamentals of Heat and Mass Transfer, 6e

    6.6 physical significance of the

    dimensionless parameters

  • 43Fundamentals of Heat and Mass Transfer, 6e

  • 44Fundamentals of Heat and Mass Transfer, 6e

  • 45Fundamentals of Heat and Mass Transfer, 6e

    6.7 boundary layer analogies

    Analogy

    Analogy between momentum-energy-mass

  • 46Fundamentals of Heat and Mass Transfer, 6e

    6.7 boundary layer analogies

  • 47Fundamentals of Heat and Mass Transfer, 6e

    6.7 boundary layer analogies

    Analogy between two convection coefficient

    In general, n=1/3

    OK for both

    turbulent and laminar

    Example 6.6 p379

  • 48Fundamentals of Heat and Mass Transfer, 6e

    6.7 boundary layer analogies

    The Reynolds analogy

  • 49Fundamentals of Heat and Mass Transfer, 6e

    6.7 boundary layer analogies

    The Chilton-Colburn analogies ()

    jh: Colburn j factor for heat transfer, j

    jm: Colburn j factor for mass transfer j

    Valid In laminar flow when

    Approximately valid in turbulent flow condition

  • 50Fundamentals of Heat and Mass Transfer, 6e

    6.8 the convection coefficients

    The primary objective on the problem of

    convection is to develop means to

    determine the convection coefficient h.

    6.9 summary

  • 51Fundamentals of Heat and Mass Transfer, 6e

    Homework Assignment

    Boundary layer profiles

    6.1

    6.3

    Heat transfer coefficients

    6.5

    Similarity and dimensionless parameters

    6.20

    Reynolds analogy

    6.34

    Mass transfer

    6.41

    Example 6.3