Title: Chapter 7: Conductances for Heat and Mass Transfer
1Chapter 7 Conductances for Heat and Mass
Transfer
- Continue with investigation of conductance
- Now consider methods for computing conductances
themselves - Return to two laws discussed in last chapter
- Ficks Law and Fouriers Law
- Need to manipulate equations to determine
conductances
2Four Processes for Conductances
- Molecular Diffusion
- Random molecular movement
- Forced Convection
- Fluid moved passed surface by external force
- Free Convection
- Fluid flow generated by temperature gradients
- Turbulent Transport or Eddy Diffusion
- Wind over rough surfaces
3Determining a Conductance
- Consider the process
- Decide what is moving in the system
- Heat? H2O? CO2?
- Determine the scale of the process
- Molecular diffusion happens on a VERY SMALL SCALE
- Forced and free convection are a leaf level
process - Turbulent transport is a field level process
- Select correct equation from Table 7.6
- If it is molecular diffusion, use equation for
specific movement (planar, cylindrical,
spherical)
4Process 1 Molecular Diffusion
- Occurs on a very small scale
- Molecules move along by random collisions along a
potential gradient - No Bulk Flow of Fluid
- Examples
- Air-filled pores in soils
- Stomatal cavities of leaves
- Animal coats
- Where hair/feathers makes up a small of total
volume
5Process 1 Molecular Diffusion
- Ficks Law for Steady State Diffusion
6Process 1 Molecular Diffusion
7Process 1 Molecular Diffusion
8Process 1 Molecular Diffusion
A(z)
A(zs)
zs
za
9Process 1 Molecular Diffusion
A(z)
A(zs)
zs
za
10Process 1 Molecular Diffusion
- Finding molar density and Diffusivity
- Temperature and pressure dependent
- Use Table A.1
- For the diffusivity of gas j in air
11- Example The finger of a wool glove has a
diameter of 3 cm. The diameter of a persons
finger inside the glove is 2 cm. If wool acts as
a layer of still air around the finger, what is
the conductance of the glove finger at 20o C and
100 kPa? What if it was a mitten instead?
12Process 2 Turbulent Transport
- Diffusion of eddy packets of air on a grand scale
- Similar to diffusion molecular diffusion because
- Packets are passively moving from one place to
another - The turbulent movement of heat and mass is a
topic for an entire course - We do not have time for that
- Read 7.4 to 7.6 on your own
13Stability in the Atmosphere
- Hear this term on the news
- Stable conditions
- Heat flux is negative
- Air temperature gt surface temperature
- Air is stratified
- We see this when smoke rises then seems to move
horizontally
14Instability in the Atmosphere
- Unstable conditions
- Heat flux, H, is positive
- Surface temperature gt Air temperature
- Heat moving from surface up into the atmosphere
- Creates thermal turbulence
- Packets rising because they have lower density
15Calculating Turbulent Transport Fluxes
- Combine mechanical and thermal turbulence into
one equation - When atmosphere is at neutral stability, in
between stable and unstable, ignore Ym and YH
16Using Stability Factors, Y
- Typically, when u gt 3 m/s, Y can be ignored
- Must use them when
- Wind speed is low
- Night time stable conditions
17- Example Consider a flat surface with snow on it
where air temperature is 10o C, hr is 100, u(2m)
10 m/s, and Pa 92 kPa. Find the water vapor
and heat flux from the surface. (zm comes from
Table 5.1, 0.002 m)
18Process 3 Forced Convection
- Intermediate scale
- ltmm to m/km for atmospheric fluxes
- Typically mm to m scale
- Leaf, flat plate, etc.
- Calculations involve empirical formulae
- Taken from Fluid Dynamics and Heat/Mass Transfer
- Use dimensionless numbers that relate relevant
numbers to each other - Reynolds number, Prandtl number, etc.
- Found in Table 7.3
19Dimensionless Numbers
- Reynolds number
- Relates inertial forces to viscous forces
- Determines laminar or turbulent conditions
- Value of 5 x 105 is typical difference between
laminar and turbulent flow for an average plate - Calculated
20Calculating Forced Convection Conductance
21Natural Turbulent Flow Correction Factor
22Free Convection
- Similar principle but uses different
dimensionless numbers - Laminar free convection for air
23Example Leaf in wind
24Forced vs. Free Convection
- Often you have both forces in the same problem
- How do you separate?
- If it gtgt than 1 then it is free convection
- If it is ltlt than 1 then it is forced
- In between Both must be considered
25Example Find Gr and ratio for the leaf
conductance example
26Evaluating Conductance 4 Basic Types
27Calculating Conductances
- Once you have determined the process
- Find Characteristic Dimension from Table 7.5
- Use equations for heat and mass transport in
Table 7.6