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