heat transfer booklet

Upload: dhilee

Post on 02-Mar-2018

217 views

Category:

Documents


0 download

TRANSCRIPT

  • 7/26/2019 Heat Transfer Booklet

    1/10

    1

    HEAT TRANSFER EQUATION SHEETHeat ConductionRate Equations (Fourier's Law)

    Heat Flux : = k:Thermal Conductivity Heat Rate :

    =

    Ac:Cross-Sectional Area

    Heat ConvectionRate Equations (Newton's Law of Cooling)

    Heat Flux: =( ) h:Convection Heat Transfer Coefficient Heat Rate: =( ) As:Surface Area 2

    Heat Radiationemitted ideally by a blackbody surface has a surface emissive power: = 4

    Heat Flux emitted : = 4 where is the emissivitywith range of 0 1and = 5.67 108 is the Stefan-Boltzmann constant

    Irradiation:

    =

    but we assume small body in a large enclosure with

    =

    so that

    =

    4

    Net Radiation heat flux from surface: = = () = (4 4 ) Net radiation heat exchange rate: = (4 4 ) where for a real surface 0 1This can ALSO be expressed as: = ( )depending on the application

    where is the radiation heat transfer coefficient which is: = ( + )(2 + 2 ) TOTAL heat transfer from a surface: = + =( ) + (4 4 )

    Conservation of Energy (Energy Balance)

    +

    =

    (Control Volume Balance) ;

    = 0 (Control Surface Balance)

    where is the conversion of internal energy (chemical, nuclear, electrical) to thermal or mechanical energy, and = 0for steady-state conditions. If not steady-state (i.e., transient) then = Heat Equation(used to find the temperature distribution)

    Heat Equation (Cartesian): + + + =

    If is constant then the above simplifies to: + + + = 1 where = is the thermal diffusivityHeat Equation (Cylindrical): 1 + 1 + + = Heat Eqn. (Spherical):

    1 2 + 1 sin + 1 sin sin + = Thermal Circuits

    Plane Wall: , = Cylinder: , = ln2 Sphere: , = (r r)4

  • 7/26/2019 Heat Transfer Booklet

    2/10

    2, = 1 , = 1_____________________________________________________________________________________________________________

    General Lumped Capacitance Analysis

    , +

    [

    (

    ) +

    (

    4

    4 )]

    (,) =

    Radiation Only Equation

    = 4, ln + ln + + 2 tan1 tan1 Heat Flux, Energy Generation, Convection, and No Radiation Equation

    = exp() ; where =, and = ,+

    Convection Only Equation = = exp = 1 () = ; = 1 exp ; =

    = If there is an additional resistance either in series or in parallel, then replace

    with

    in all the above lumped capacitance

    equations, where = 1 ; = overall heat transfer coefficient, = total resistance,= surface area.Convection Heat Transfer = = [Reynolds Number] ; = [Average Nusselt Number]

    where is the density, is the velocity, is the characteristic length, is the dynamic viscosity, is the kinematic viscosity, is the mass flowrate, is the average convection coefficient, and is the fluid thermal conductivity.

  • 7/26/2019 Heat Transfer Booklet

    3/10

    3

    Internal Flow = 4 [For Internal Flow in a Pipe of Diameter D]For Constant Heat Flux [ =]: =( ) ; where P = Perimeter, L = Length

    (

    ) =

    ,

    +

    For Constant Surface Temperature [ =]:If there is only convection between the surface temperature, , and the mean fluid temperature, , use

    (), = If there are multiple resistances between the outermost temperature, ,and the mean fluid temperature, , use ()

    ,

    =

    =

    1

    Total heat transfer rate over the entire tube length: = , , = ; =Log mean temperature difference: = ln ; = , ; = ,

    Free Convection Heat Transfer

    = () [Grashof Number] = () [Rayleigh Number]

    Vertical Plates: =0.825 + 0.387/1+. //2

    ;[Entire range of RaL; properties evaluated at T

    f]

    -For better accuracy for Laminar Flow: = 0.68 + 0.670/1+. // ; 109 [Properties evaluated at Tf]Inclined Plates:for the topand bottomsurfaces of cooledand heatedinclined plates, respectively, the equations of the vertical

    plate can be used by replacing (g) with ( cos ) in RaLfor 0 60.Horizontal Plates: use the following correlations with = whereAs= Surface Area and P= Perimeter

    -Upper surface of Hot Plate or Lower Surface of Cold Plate: = 0.54 1/4 (104 107); = 0.15 1/3 (107 1011)-Lower Surface of Hot Plate or Upper Surface of Cold Plate: = 0.27 1/4 (105 1010)

  • 7/26/2019 Heat Transfer Booklet

    4/10

    4

    Vertical Cylinders:the equations for the Vertical Platecan be applied to vertical cylinders of height Lif the following criterion is

    met: 35/

    Long Horizontal Cylinders: =0.60 + 0.387/1+

    .

    /

    /2

    ; 1012 [Properties evaluated at Tf]Spheres: = 2 + 0.589/1+. // ; 1011; 0.7 [Properties evaluated at Tf]

    Heat Exchangers

    Heat Gain/Loss Equations: =( ) =; where is the overall heat transfer coefficientLog-Mean Temperature Difference:

    , = ,,,,

    ln ,

    ,

    ,, [Parallel-Flow Heat Exchanger]

    Log-Mean Temperature Difference: , = ,,,,ln,,,, [Counter-Flow Heat Exchanger]For Cross-Flow and Shell-and-Tube Heat Exchangers: = , ; where is a correction factorNumber of Transfer Units (NTU): = ; where is the minimum heat capacity rate in [W/K]Heat Capacity Rates: = , [Cold Fluid] ; = , [Hot Fluid] ; = [Heat Capacity Ratio]Note:The condensation or evaporation side of the heat exchanger is associated with =

  • 7/26/2019 Heat Transfer Booklet

    5/10

    5

    If Pr 10 n = 0.37

    If Pr 10 n = 0.36

  • 7/26/2019 Heat Transfer Booklet

    6/10

    6

  • 7/26/2019 Heat Transfer Booklet

    7/10

    7

  • 7/26/2019 Heat Transfer Booklet

    8/10

    8

  • 7/26/2019 Heat Transfer Booklet

    9/10

    9

  • 7/26/2019 Heat Transfer Booklet

    10/10

    10