HeatTransfer Power Point

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Transcript of HeatTransfer Power Point

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    Energy Transfer

    ! When two objects of differenttemperatures are placed in thermalcontact, the temperature of the warmerdecreases and the temperature of thecooler increases

    ! The energy exchange ceases when theobjects reach thermal equilibrium

    ! The concept of energy was broadenedfrom just mechanical to include internal! Made Conservation of Energy a universal

    law of nature

    Methods of Heat Transfer

    ! Need to know the rate at whichenergy is transferred

    ! Need to know the mechanismsresponsible for the transfer

    ! Methods include! Conduction

    ! Convection

    ! Radiation

    Conduction

    ! The transfer can be viewed on anatomic scale

    ! It is an exchange of energy between

    microscopic particles by collisions! Less energetic particles gain energy during

    collisions with more energetic particles

    ! Rate of conduction depends upon thecharacteristics of the substance

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    Conduction example

    ! The molecules vibrateabout their equilibriumpositions

    ! Particles near the stovecoil vibrate with largeramplitudes

    ! These collide withadjacent molecules andtransfer some energy

    ! Eventually, the energytravels entirely throughthe pan and its handle

    Conduction, cont.

    ! In general, metals are good conductors

    ! They contain large numbers of electronsthat are relatively free to move through themetal

    ! They can transport energy from one region

    to another

    ! Conduction can occur only if there is adifference in temperature between twoparts of the conducting medium

    Conduction, equation

    ! The slab allowsenergy to transferfrom the region of

    highertemperature tothe region oflowertemperature

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    Conduction, equationexplanation

    ! A is the cross-sectional area

    ! L = !x is the thickness of the slab orthe length of a rod

    ! P is in Watts when Q is in Joules and t isin seconds

    ! k is the thermal conductivityof thematerial! See table 11.3 for some conductivities

    ! Good conductors have high k values andgood insulators have low k values

    Home Insulation

    ! Substances are rated by their Rvalues! R = L / k

    ! See table 11.4 for some R values

    ! For multiple layers, the total Rvalue is the sum of the R values ofeach layer

    ! Wind increases the energy loss by

    conduction in a home

    Conduction and Insulationwith Multiple Materials

    ! Each portion will have a specificthickness and a specific thermalconductivity

    ! The rate of conduction througheach portion is equal

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    Multiple Materials, cont.

    ! The rate through the multiplematerials will be

    ! THand TCare the temperatures atthe outer extremities of thecompound material

    Convection

    ! Energy transferred by themovement of a substance

    ! When the movement results fromdifferences in density, it is callednatural conduction

    ! When the movement is forced by afan or a pump, it is called forcedconvection

    Convection example

    ! Air directly abovethe flame iswarmed andexpands

    ! The density of theair decreases, andit rises

    ! The mass of airwarms the handas it moves by

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    Convection applications

    ! Boiling water

    ! Radiators

    ! Upwelling

    ! Cooling automobile engines

    ! Algal blooms in ponds and lakes

    Convection CurrentExample

    ! The radiator warmsthe air in the lowerregion of the room

    ! The warm air is lessdense, so it rises tothe ceiling

    ! The denser, coolerair sinks

    ! A continuous aircurrent pattern is setup as shown

    Radiation

    ! Radiation does not require physicalcontact

    ! All objects radiate energy

    continuously in the form ofelectromagnetic waves due tothermal vibrations of the molecules

    ! Rate of radiation is given byStefans Law

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    Radiation example

    ! The electromagnetic waves carry theenergy from the fire to the hands

    ! No physical contact is necessary

    ! Cannot be accounted for by conductionor convection

    Radiation equation

    !

    ! The power is the rate of energytransfer, in Watts

    ! != 5.6696 x 10-8W/m2.K4

    ! A is the surface area of the object

    ! e is a constant called the emissivity

    ! e varies from 0 to 1

    ! T is the temperature in Kelvins

    Energy Absorption andEmission by Radiation

    ! With its surroundings, the rate atwhich the object at temperature Twith surroundings at Toradiates is

    !

    ! When an object is in equilibrium withits surroundings, it radiates andabsorbs at the same rate

    ! Its temperature will not change

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    Ideal Absorbers

    ! An ideal absorberis defined as anobject that absorbs all of theenergy incident on it! e = 1

    ! This type of object is called a blackbody

    ! An ideal absorber is also an idealradiator of energy

    Ideal Reflector

    ! An ideal reflector absorbs none ofthe energy incident on it

    ! e = 0

    Applications of Radiation

    ! Clothing! Black fabric acts as a good absorber

    ! White fabric is a better reflector

    !

    Thermography! The amount of energy radiated by an object

    can be measured with a thermograph

    ! Body temperature! Radiation thermometer measures the

    intensity of the infrared radiation from theeardrum

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    Resisting Energy Transfer

    ! Dewar flask/thermos bottle

    ! Designed to minimizeenergy transfer tosurroundings

    ! Space between walls is

    evacuated to minimizeconduction and convection

    ! Silvered surface minimizesradiation

    ! Neck size is reduced

    Global Warming

    ! Greenhouse example

    ! Visible light is absorbed and re-emitted as infrared radiation

    ! Convection currents are inhibited bythe glass

    ! Earths atmosphere is also a goodtransmitter of visible light and agood absorber of infrared radiation