Fundamentals of Heat and Mass Transfer, 6...
Transcript of Fundamentals of Heat and Mass Transfer, 6...
-
1Fundamentals of Heat and Mass Transfer, 6e
Fundamentals of Heat and Mass
Transfer, 6th edition
Presented E-mail: [email protected]
Telephone: 88399000-2511
mailto:[email protected]
-
2Fundamentals of Heat and Mass Transfer, 6e
Chapter 6 Introduction to convection
Convection: energy transfer between a surface and a fluid moving over the surface
ObjectivesUnderstand the physical mechanism of convection;
Develop means to perform convection transfer calculation
Contents:Basic contents on convection heat transfer and convection
mass transfer
physical origin, dimensionless parameters, analogies
-
3Fundamentals of Heat and Mass Transfer, 6e
Chapter 6 Introduction to convection
Convection: energy transfer between a surface and a fluid moving over the surface()
the bulk fluid motion (advection)
the random motion of fluid molecules (conduction or diffusion)
The determination of convection transfer coefficient and related heat transfer
enhancement method are the central problems in the study of convection issue.
-
4Fundamentals of Heat and Mass Transfer, 6e
Chapter 7 External flow
Chapter 8 Internal flow
Chapter 9 Free convection
Chapter 10 Boiling and condensation
Chapter 11 Heat exchangers
-
5Fundamentals of Heat and Mass Transfer, 6e
6.1 the convection boundary layer
Boundary layers: velocity, thermal , concentration,
Friction coefficient
Convection heat transfer coefficient
Convection mass transfer coefficient
-
6Fundamentals of Heat and Mass Transfer, 6e
6.1 the convection boundary layer
The velocity boundary layer Fluid velocity=0 at the surface
Velocity grow Velocity u
Shear stress (), parallel to fluid velocity
In boundary layer ( a thin layer): velocity gradients and shear stresses are large
Region outside the boundary layer: velocity gradients and shear stresses are
negligible
uu 99.0Velocity boundary layer thickness
-
7Fundamentals of Heat and Mass Transfer, 6e
6.1 the convection boundary layer
Velocity boundary layer: developed whenever there is fluid flow over a surface
For a Newtonian fluid
dynamic viscosity
kg/m S
u velocity along the x direction
m/s
surface shear stressN/m2
Cf: the local friction coefficient,
to determine the friction drag a dimensionless parameter
sx
y
u
Cf
-
8Fundamentals of Heat and Mass Transfer, 6e
6.1 the thermal boundary layer
99.0)/()( TTTT sst Thermal boundary layer thickness when
Developed when the flow free stream and the surface temperatures differ
x y
T
h
-
9Fundamentals of Heat and Mass Transfer, 6e
6.1 the concentration boundary layer
Example: air past the surface of a pool of water evaporation a binary mixture of chemical species A and B,
Sublimation
CA: molar concentration , kmol/m3
-
10Fundamentals of Heat and Mass Transfer, 6e
Concentration boundary layer:
concentration gradients exist()
:thickness is defined asc 99.0)(
)(
,,
,
AsA
AsA
CCCC
Molar flux of species A , NA (kmol / s m2)A
Binary diffusion coefficient, DAB
Fick s law Diffusion mass transfer,y
CDN AABA
''
At the surface y=0,
diffusion mass transfer 0''
,
y
AABsA
y
CDN
6.1 the concentration boundary layer
-
11Fundamentals of Heat and Mass Transfer, 6e
Analogous to Newtons law of cooling
6.1 the concentration boundary layer
)( ,.,''
AsAmsA CChN
,,
0
AsA
AAB
mCC
yy
CD
h
hm, convection mass transfer
coefficient, m/s,
y
CDN AABA
''
-
12Fundamentals of Heat and Mass Transfer, 6e
6.1 significance of the boundary layer
Flow over a surface velocity boundary layer surface friction
Flow over a surface with temp difference thermal boundary
layer convection heat transfer
Flow over a surface with concentration difference concentration
boundary layer convection mass transfer
items Characteristics Key parameters
Velocity gradient,
shear stresses
Friction coefficient Cf
Temp gradient,
heat transfer
Heat transfer coefficient,
h
Concentration gradient,
species transfer
Mass transfer coefficient,
hm
t
t
c
-
13Fundamentals of Heat and Mass Transfer, 6e
6.2 local and average convection
coefficients
Heat transfer
The local heat flux , q
The total heat rate , q
Average convection heat transfer coefficient, h
-
14Fundamentals of Heat and Mass Transfer, 6e
6.2 local and average convection
coefficients
Mass transfer
NA: molar transfer rate kmol/s
-
15Fundamentals of Heat and Mass Transfer, 6e
6.2 local and average convection
coefficients
Molar flux mass flux
Molar transfer rate mass transfer rate
0
''
,
y
AABsA
yDn
Molecular weight (kg/kmol)
Molecular weight (kg/kmol)
,,
0
AsA
AAB
m
yy
Dh
AAA CM
-
16Fundamentals of Heat and Mass Transfer, 6e
Example 6.1
-
17Fundamentals of Heat and Mass Transfer, 6e
-
18Fundamentals of Heat and Mass Transfer, 6e
6.3 laminar and turbulent flow
Flow condition: laminar flow() turbulent flow
-
19Fundamentals of Heat and Mass Transfer, 6e
6.3 laminar and turbulent flow
Boundary layer development on a flat plat
Laminar flow: fluid flow is highly ordered, streamline
Transition zone: laminar or turbulent
Turbulent flow: flow is highly irregular, random, 3-D motion, chaotic flow
3 regions in the turbulent boundary layer: viscous sublayer ()buffer layer ()turbulent zone ()
-
20Fundamentals of Heat and Mass Transfer, 6e
5105Re
xux
Critical Reynolds number, ranging in 105~3X106
xucx
,Re
Determination parameter for the onset of turbulent flow :
Reynolds number =the ratio of inertia to viscous forces
= /
x, characteristic length
-
21Fundamentals of Heat and Mass Transfer, 6e
Laminar and turbulent thermal
boundary layer
Laminar region :streamline, temperature gradient is decreased in the streamline direction heat transfer
coefficient is decreased
Transition region:
Turbulent region: local convection heat transfer
coefficient is decreased
along the flow direction.
-
22Fundamentals of Heat and Mass Transfer, 6e
-
23Fundamentals of Heat and Mass Transfer, 6e
-
24Fundamentals of Heat and Mass Transfer, 6e
-
25Fundamentals of Heat and Mass Transfer, 6e
-
26Fundamentals of Heat and Mass Transfer, 6e
Thermal and species concentration
boundary layer
Laminar region :streamline, temp and concentration gradient decrease in the streamline direction heat and
mass transfer coefficient decrease
Transition region:
Turbulent region: local convection heat and mass
transfer increased
-
27Fundamentals of Heat and Mass Transfer, 6e
Example 6.4 p362
For concentration boundary layer
-
28Fundamentals of Heat and Mass Transfer, 6e
6.4 the boundary layer equation
-
29Fundamentals of Heat and Mass Transfer, 6e
6.4 the boundary layer equation
Boundary layer equations for laminar flowComply with fundamental laws of nature:
Including conservation of mass, energy and chemical species, Newtons second law of motion
Assumption
In the Cartesian coordinate, equations for the steady, 2D flow of an incompressible fluid with constant properties are summarized in Appendix D the convection Transfer Equations.
( Appendix E gives the corresponding equations for the boundary layer in turbulent flow.)
-
30Fundamentals of Heat and Mass Transfer, 6e
6.4 the boundary layer equation
The continuity equation
-
31Fundamentals of Heat and Mass Transfer, 6e
6.4 the boundary layer equation
The x momentum equation x
The net pressure
force
The net rate
force due to
viscous shear
stresses
The net rate due
to fluid motion
across boundary
-
32Fundamentals of Heat and Mass Transfer, 6e
6.4 the boundary layer equation
The energy equation,
The net
conduction rate
in the y direction
The net rate due
to fluid advection
Viscous dissipation
Neglect in some cases
-
33Fundamentals of Heat and Mass Transfer, 6e
6.4 the boundary layer equation
The species concentration equation
The net transport
of species A due
to advection
The net transport
of species A due
to y-direction
diffusion
-
34Fundamentals of Heat and Mass Transfer, 6e
6.4 the boundary layer equation
Laminar boundary layer equations
Right side: diffusion terms
If neglect
Left side: advection terms
44
-
35Fundamentals of Heat and Mass Transfer, 6e
6.5 boundary layer similarity
Nondimensionalizing the governing equations:
L: characteristic length of the surface of interest,
V: velocity of the upstream
Viscous dissipation is neglected
-
36Fundamentals of Heat and Mass Transfer, 6e
Nondimensional form of the
boundary layer equation
-
37Fundamentals of Heat and Mass Transfer, 6e
6.5 boundary layer similarity
Similarity parameters (important, apply results for a surface to geometrically similar surfaces)
Reynolds number Re
Prandtl number, Pr,
If both the boundary conditions and similarity parameters
are same for two different conditions (that is geometrically
similar ), then solution of the differential equations for the
nondimensional velocity and temperature will be same.
VLRe
Dynamic viscosity, kg/s m
Kinetic viscosity, m2/s
-
38Fundamentals of Heat and Mass Transfer, 6e
6.5 boundary layer similarity
Functional form of the solutions
Local
Nusselt Number
Average
-
39Fundamentals of Heat and Mass Transfer, 6e
6.5 boundary layer similarity
Functional form of the solutions
-
40Fundamentals of Heat and Mass Transfer, 6e
-
41Fundamentals of Heat and Mass Transfer, 6e
6.6 physical significance of the
dimensionless parameters
Reynolds number: the ratio of inertia to viscous forces
Grashof number: the ratio of the buoyancy forces to
viscous forces
Prandtl number: the relative effectiveness of momentum
and energy transfer by diffusion in the velocity and
thermal boundary layer, the relative thickness of velocity
and thermal boundary layer.
For gas Pr=1, For liquid metal Pr1
n is a positive component
-
42Fundamentals of Heat and Mass Transfer, 6e
6.6 physical significance of the
dimensionless parameters
-
43Fundamentals of Heat and Mass Transfer, 6e
-
44Fundamentals of Heat and Mass Transfer, 6e
-
45Fundamentals of Heat and Mass Transfer, 6e
6.7 boundary layer analogies
Analogy
Analogy between momentum-energy-mass
-
46Fundamentals of Heat and Mass Transfer, 6e
6.7 boundary layer analogies
-
47Fundamentals of Heat and Mass Transfer, 6e
6.7 boundary layer analogies
Analogy between two convection coefficient
In general, n=1/3
OK for both
turbulent and laminar
Example 6.6 p379
-
48Fundamentals of Heat and Mass Transfer, 6e
6.7 boundary layer analogies
The Reynolds analogy
-
49Fundamentals of Heat and Mass Transfer, 6e
6.7 boundary layer analogies
The Chilton-Colburn analogies ()
jh: Colburn j factor for heat transfer, j
jm: Colburn j factor for mass transfer j
Valid In laminar flow when
Approximately valid in turbulent flow condition
-
50Fundamentals of Heat and Mass Transfer, 6e
6.8 the convection coefficients
The primary objective on the problem of
convection is to develop means to
determine the convection coefficient h.
6.9 summary
-
51Fundamentals of Heat and Mass Transfer, 6e
Homework Assignment
Boundary layer profiles
6.1
6.3
Heat transfer coefficients
6.5
Similarity and dimensionless parameters
6.20
Reynolds analogy
6.34
Mass transfer
6.41
Example 6.3