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1 LECTURE 2 Fundamentals of Convection Flow Over Flat Plates

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    LECTURE 2 Fundamentals of Convection

    Flow Over Flat Plates

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    conv = hAs (Ts T) Watt

    Convection Heat Transfer

    By Newtons Law of Cooling, convection heat transfer is

    proportional to temperature different :

    2

    Q

    h = convection heat transfer coefficient (W/m2 C) As = heat transfer surface area (m

    2)

    Ts = temperature of surface (C)

    T = temperature of media far from surface (C)

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    Heat transfer by conduction,

    cond = kAs (T1T2) / L = kAs T/ L

    Heat transfer by convection,

    conv = hAs (T1T2) = hAs T

    By taking ratio heat transfer of convection to conduction

    gives :

    conv / cond =

    3

    Q

    Q

    QQ

    Nusselt Number

    TS = T1 T = T2

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    or

    Reynolds Number

    Reynolds Number (Re) gives relation between inertial force and viscous force of fluid flow.

    Re = inertial force / viscous force

    VL / VD /

    V = free stream velocity (m/s)

    L = characteristic length (m) for flat plate

    D = diameter (m) for tube/cylinder

    = kinematic viscosity (m2/s)

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    Prandtl Number

    The thickness of thermal boundary layer increases in the flow direction of liquid.

    The development of velocity boundary layer relative to

    thermal boundary layer will have strong effect on

    convection heat transfer

    The relative thickness of the velocity and thermal boundary

    layers are described by the dimensionless parameter called :

    Prandtl Number (Pr)

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    Prandtl Number

    Heat diffuses very quick in liquid metals and gaseous

    (Pr =1 and less) and very slow in water/oil (Pr > 1).

    Liquid metals 0.004 0.03

    Gaseous 0.7 1.0

    Water 1.7 13.7

    Oil 50 100,000

    Typical values Pr Number :

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    Properties of Air

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    Friction Force over Flat Plate

    Because of the friction between the layers, exerting a friction force on the plate.

    The friction force over the entire surface is determined as

    below, where Cf is friction coefficient

    Friction Force, Ff = Cf As V 2 / 2 (N)

    The friction force is important parameter in heat transfer

    studies since its is directly related to the heat transfer

    coefficient.

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    Laminar :

    Turbulent :

    21Re

    328.1fC

    51Re

    074.0fC

    Re

    1742

    Re

    074.051fC

    Laminar & Turbulent

    Friction Coefficient over Flat Plate

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    Friction and Pressure Drag

    When the flat plate is placed normal to the flow direction,

    however, the drag force depends on the pressure only and is

    independent of the wall shear since the shear stress in this case

    acts in the direction normal to flow.

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    Friction and Pressure Drag

    The drag force FD depends on the density of the fluid, the

    upstream velocity, and the size, shape, and orientation of the

    body, among other things.

    The drag characteristics of a body is represented by the

    dimensionless drag coefficient CD defined as

    where A is the frontal area that tends to block the flow. The

    frontal area of a cylinder of diameter D and length L, for

    example, is A = LD.

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    Flow Across Different Bodies

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    Plate [ AN = L x w ] Sphere [ AN = D ] Cylinder [ AN = L x D ]

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    Limitation of Re over Flat Plate

    The transition from laminar to turbulent flow depends on

    the surface geometry, surface roughness, surface

    temperature, velocity and type of fluid used.

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    Limitation of Re over Flat Plate

    For fluid flow over the flat surface, the limit of laminar and turbulent flows is given as :

    Laminar Flow : Re < 5 x 105

    Turbulent Flow : Re 5 x 105

    Re = 5 x 105

    Transition ?

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    Nu, Pr and Re Numbers

    Generally, heat transfer analysis on forced convection involves three major numbers : Nusselt number (Nu), Prantdl number (Pr) and Reynolds number (Re).

    To simplify the numbers :

    C, m and n are constant value that depends on geometry

    and flow type of the body (range of Re). The value of

    m and n are between 0 to 1.

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    Nu = C Rem Prn

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    Nusselt Number over Flat Plates

    Laminar : Re < 5 x 105 315.0 Pr Re 664.0 Nu

    k

    hL

    Turbulent : Re 5 x 105 318.0 Pr Re 037.0 Nu

    k

    hL

    Laminar & Turbulent : Re 5 x 105

    318.0 Pr )871 Re 037.0( Nu k

    hL

    Nu = C Rem Prn

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    The flat plate is assumed to be at uniform temperature during the entire flow.

    However, when a flat plate is subjected to uniform heat

    flux instead of uniform temperature, the Nu is given as :

    Laminar :

    Turbulent :

    315.0 Pr Re 453.0 Nu k

    hL

    318.0 Pr Re 0308.0 Nu k

    hL

    Uniform Temperature/Heat Flux

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    q

    Uniform temperature

    Uniform heat flux

    Ts

    =W/m2

    Uniform Temperature/Heat Flux

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    Fluid Properties

    The fluid temperature in the thermal boundary layer varies from Ts at the surface to T at the outer edge of boundary.

    Therefore, by taking the average, the fluid properties are

    usually evaluated at film temperature (Tf ) :

    The fluid properties are assumed to remain constant

    during the entire flow.

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    Tf = (Ts + T) / 2

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    Methodology for Solving Problem

    Find the fluid properties based on Tf

    Calculate the Reynolds Number (Re)

    Identify the type of flow, based on Re obtained

    Determine h from equation of Nu

    Use the right equations

    = hAs(TsT)

    Cf = Laminar or Turbulent

    Ff = Cf A V2 / 2

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    Q

  • Ts = 110 C T= 30 C V = 6 m/s

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    5 m

    1.5 m

    Q

    Example 1

    Air, at 30C flows with a velocity of 6 m/s over a 1.5 m x 5m

    flat plate whose temperature is 110 C. Determine the rate of

    heat transfer from the plate if the flows parallel to :

    a) 5 m long side b) 1.5 m side

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    Properties of Air

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    Assume air at 1 atm pressure Tf = (Ts+T)/2 = (110 + 30)/2 = 70C Properties of air at 70C k = 0.02881 W/m.C =1.995 x 10-5 m2/s Pr = 0.7177 Surface are of the flat plate As = W x L = 1.5 x 5 = 7.5 m

    2

    Example 1

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    (a) 5 m long side (L = 5 m) Re = 1503759, Re 5 x 105 - Turbulent Assume the entire flow is turbulent

    Nu = 2899 h = 16.7 W/m2 C = 10020 W b) 1.5 m long side (L = 1.5 m) Re = 451128, Re < 5 x 105 - Laminar Nu = 399 h = 7.67 W/m2 C = 4602 W

    Q

    Q

    Example 1

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    Forced Convection

    EXERCISE 1

    Consider a hot automotive engine, which can be approximated

    as a 0.5-m-high, 0.40-m-wide, and 0.8-m-long rectangular

    block. The bottom surface of the block is at a temperature of

    100C and the ambient air is at 20C.

    Determine the rate of heat transfer from the bottom surface of

    the engine block by convection as the car travels at a velocity

    of 80 km/h.

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    Properties of Air

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    EXERCISE 2

    A 15-cm x 15-cm circuit board dissipating 15 W of power

    uniformly is cooled by air, which approaches the circuit

    board at 20C with a velocity of 6 m/s. Disregarding any heat

    transfer from the back surface of the board, determine the

    surface temperature of the electronic component.

    Forced Convection

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    Properties of Air

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    EXERCISE 3

    Consider a case of air flows over hot plates with 20 cm x 50 cm

    surface area. The velocity of air is 5 m/s, the temperature of

    each plate is 120C and the surrounding air temperature is 60C.

    Determine the rate of heat transfer.

    Forced Convection

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    Properties of Air