heat transfer introduction and conduction. conduction if a temperature gradient exits in a...
DESCRIPTION
Convection When a current or macroscopic particle of fluid crosses a specific surface, such as the boundary of a control volume, it carries with it a definite quantity of enthalpy Occurs only when forces act on the particle or stream of fluid and maintain motion against forces of friction Thermodynamically, convection is not heat flow, but flux Closely associated with fluid mechanics Examples – transfer of enthalpy by eddies of turbulent flow, current of warm air from a furnace flowing across a roomTRANSCRIPT
Heat Transfer IntroductionHeat Transfer Introductionand Conductionand Conduction
ConductionConduction If a temperature gradient exits in a continuous If a temperature gradient exits in a continuous
substance, heat can flow unaccompanied by any substance, heat can flow unaccompanied by any observable motion of matterobservable motion of matter
Metallic solids – conduction occurs from the Metallic solids – conduction occurs from the motion of unbound electronsmotion of unbound electrons
Other solids and liquids – conduction results Other solids and liquids – conduction results from the transport of momentum of individual from the transport of momentum of individual molecules along the temperature gradientmolecules along the temperature gradient
Gases – conduction occurs by random motion of Gases – conduction occurs by random motion of molecules; heat is “diffused” from hotter regions molecules; heat is “diffused” from hotter regions to colder onesto colder ones
Examples – heat flow in opaque solids, ie., brick Examples – heat flow in opaque solids, ie., brick wall of furnace or metal wall of a tubewall of furnace or metal wall of a tube
ConvectionConvection When a current or macroscopic particle of fluid When a current or macroscopic particle of fluid
crosses a specific surface, such as the boundary crosses a specific surface, such as the boundary of a control volume, it carries with it a definite of a control volume, it carries with it a definite quantity of enthalpyquantity of enthalpy
Occurs only when forces act on the particle or Occurs only when forces act on the particle or stream of fluid and maintain motion against stream of fluid and maintain motion against forces of frictionforces of friction
Thermodynamically, convection is not heat flow, Thermodynamically, convection is not heat flow, but fluxbut flux Closely associated with fluid mechanicsClosely associated with fluid mechanics
Examples – transfer of enthalpy by eddies of Examples – transfer of enthalpy by eddies of turbulent flow, current of warm air from a furnace turbulent flow, current of warm air from a furnace flowing across a roomflowing across a room
Natural and Forced ConvectionNatural and Forced Convection Natural convection – currents are the result of Natural convection – currents are the result of
buoyancy forces generated by differences in buoyancy forces generated by differences in density and differences in density are in caused density and differences in density are in caused by temperature gradients in fluid massby temperature gradients in fluid mass Flow of air across a heated radiatorFlow of air across a heated radiator
Forced convection – currents are set in motion Forced convection – currents are set in motion by action of a mechanical device such a pump or by action of a mechanical device such a pump or agitator, flow is independent of density gradientsagitator, flow is independent of density gradients Heat flow to a fluid pumped through a heated pipeHeat flow to a fluid pumped through a heated pipe
RadiationRadiation
Transfer of energy through space by Transfer of energy through space by electromagnetic waveselectromagnetic waves
If matter appears in the path, radiation will If matter appears in the path, radiation will be transmitted, reflected, or absorbedbe transmitted, reflected, or absorbed
Only absorbed energy appears as heatOnly absorbed energy appears as heat Examples – loss of heat from a radiator or Examples – loss of heat from a radiator or
uninsulated stream pipe; heat transfer in uninsulated stream pipe; heat transfer in furnacesfurnaces
Heat Transfer by ConductionHeat Transfer by Conduction Fourier’s lawFourier’s law
Temperature can vary with both location and timeTemperature can vary with both location and time Heat flow occurs from hot to coldHeat flow occurs from hot to cold
ntk
dAdq
Where A = area of isothermal surface n = distance measured normally to surface q = rate of heat flow across surface in direction normal to surface T = temperature k = proportionality constant
One-Dimensional Heat FlowOne-Dimensional Heat Flow
Hot Gas
B
Water
Tem
pera
ture
700 C
25 Cc
III
II
I
I – at instant of exposure of wall to high temperature
II – during heating at time t
III – at steady state
For Steady One-Dimensional FlowFor Steady One-Dimensional Flow
Thermal conductivity, kThermal conductivity, k Proportionality factor that represents a Proportionality factor that represents a
physical property of a substancephysical property of a substance q/A – rate of heat flow per unit areaq/A – rate of heat flow per unit area dT/dn – temperature gradientdT/dn – temperature gradient q – watts or Btu/hq – watts or Btu/h dt/dn - dt/dn - C/m or C/m or F/ftF/ft k – W/m-k – W/m-C or Btu-ft-h-C or Btu-ft-h-FF
dndTk
Aq
For small temperature ranges, k is constantFor small temperature ranges, k is constant For larger temperature ranges,For larger temperature ranges,
k = a + bTk = a + bTWhere a and b are empirical constantsWhere a and b are empirical constants
k for metalsk for metals Stainless – 17 W/m-Stainless – 17 W/m-CC Silver – 415 W/m-Silver – 415 W/m-CC
k for liquidsk for liquids Water - 0.5 – 0.7 W/m-Water - 0.5 – 0.7 W/m-CC
k for gasesk for gases Air – 0.024 W/m-Air – 0.024 W/m-CC
Solids with low k values are often used as Solids with low k values are often used as insulatorsinsulators
Steady State ConductionSteady State Conduction For a flat slab of thickness, BFor a flat slab of thickness, B
R is the thermal resistance of the solid R is the thermal resistance of the solid between two pointsbetween two points
RT
BTk
xxTTk
Aq
dxkAqdT
dxdTk
Aq
12
21
Resistances in SeriesResistances in SeriesT
TCTBTA
RA RB RC
BA BB BC
T
TC
TB
TA
RT
RRRT
kBkBkBT
Aq
TkABq
kABq
kABqTTT
CBACCBBAA
C
CC
B
BB
A
AACBA
///
Heat Flow through a Cylinder Heat Flow through a Cylinder
To Ti
dr
ri
rro
)/ln(
)/ln()(2
)(
)/ln())(2(
2
2
io
ioL
io
ioL
io
oiL
io
oi
r
r
T
T
rrrrr
rrrrLA
rrTTAkq
rrTTLkq
dTqLk
rdr
rLdrdTkq
o
i
i
o
Heat Flow in FluidsHeat Flow in Fluids Typical equipment Typical equipment
consists of a bundle consists of a bundle of parallel tube of parallel tube encased in a encased in a cylindrical shellcylindrical shell