Title: Moist Adiabatic Processes
1Moist Adiabatic Processes
2Moist Adiabatic Processes
- Parcel Theory
- Dry Adiabatic Process
- Moist Adiabatic Process
- Saturated Adiabatic Process
- Pseudo Adiabatic Process
3Moist Adiabatic Processes
- Reading
- Hess
- Section 4.6
- pp 51 - 58
- Equivalent Temp.
- pp 63
4Moist Adiabatic Processes
- Wallace Hobbs
- pp 84 87
- Tsonis
- pp 103 116
- Bohren Albrecht
- pp 287-291
5Moist Adiabatic Process
- Objectives
- Be able to identify parcel theory assumptions
- Be able to state the composition of air involved
in dry adiabatic processes - Be able to perform calculations using Poissons
Equation for dry air
6Moist Adiabatic Process
- Objectives
- Be able to state the composition of air involved
in moist adiabatic processes - Be able to perform calculations using the
equation for moist adiabatic processes
7Moist Adiabatic Process
- Objectives
- Be able to state the composition of an air parcel
involved in saturated adiabatic processes - Be able to describe the heat transfer in a parcel
of air during saturated adiabatic ascent
8Moist Adiabatic Process
- Objectives
- Be able to state the composition of an air parcel
involved in pseudo adiabatic processes - Be able to describe the heat transfer in an air
parcel during pseudo adiabatic ascent
9Moist Adiabatic Process
- Objectives
- Be able to state the definition of equivalent
potential temperature - Be able to identify conserved properties for dry
and pseudo adiabatic ascent - Be able to calculate equivalent potential
temperature
10Moist Adiabatic Process
- Lets review dry adiabatic processes
- Parcel Theory
- Poissons Equation
11Parcel Theory
- Assumptions
- Thermally insulated from its environment
- Temperature changes adiabatically
- Always at the same pressure as the environment at
that level
Tp,P
Te,P
w
12Parcel Theory
- Assumptions
- Hydrostatic equilibrium
- Moving slow enough that its kinetic energy is a
negligible
Tp,P
Te,P
w
13Parcel Theory
- Types of Processes
- Dry Adiabatic
- Moist Adiabatic
- Saturated Adiabatic
- Pseudo Adiabatic
14Dry Adiabatic Process
- First Law of Thermodynamic
pda
- Work of expansion results in a temperature change
of the parcel
15Dry Adiabatic Process
16Dry Adiabatic Process
17Dry Adiabatic Process
- Parcel Contains NO Moisture at All
- No Water Vapor
- No Liquid Water
Dry as a popcorn ......
18Dry Adiabatic Process
- Rising Parcel Cools at the Dry Adiabatic Lapse
Rate - Potential Temperature is Constant in the Parcel
q const
19Moist Adiabatic Process
- Moist Adiabatic Process?
- Dry adiabatic processes that involve water vapor
20Moist Adiabatic Process
- Air is a Mixture
- Dry Air
- Oxygen, Nitrogen, Argon, Carbon Dioxide, etc.
- Moisture
- Water Vapor
21Moist Adiabatic Process
- Lets look at a moist adiabatic process that
involves only water vapor - Parcel Remains Unsaturated
22Moist Adiabatic Process
- Moist Adiabatic (Unsaturated) Ascent
- Must include the contribution of water vapor to
mixture
- Adjust R/cp to account for water vapor
23Moist Adiabatic Process
md mass of dry air mv mass of water vapor m
total mass of air Rd Gas Constant of Dry
Air Rv Gas Constant of Water Vapor
24Moist Adiabatic Process
25Moist Adiabatic Process
q specific humidity
26Moist Adiabatic Process
27Moist Adiabatic Process
28Moist Adiabatic Process
- Similarly, evaluate cp for the mixture
- The heat absorbed to raise the temperature during
an isobaric process
Q total heat qd heat (per mass) of dry air md
mass of dry air qv heat (per mass) of water
vapor mv mass of water vapor
29Moist Adiabatic Process
30Moist Adiabatic Process
31Moist Adiabatic Process
32Moist Adiabatic Process
cp specific heat at constant pressure
33Moist Adiabatic Proces
34Moist Adiabatic Process
35Moist Adiabatic Process
36Moist Adiabatic Process
cpd specific heat of dry air at constant
pressure 1004 J kg-1 K-1
cpv specific heat of water vapor at constant
pressure 1870 J kg-1 K-1
37Moist Adiabatic Process
38Moist Adiabatic Process
- Now let look at Poissons Equation
39Moist Adiabatic Process
- Simplify using polynomial division
40Moist Adiabatic Process
- Poissons Equation for moist, unsaturated air
41Moist Adiabatic Process
- Potential Temperature for Moist, Unsaturated Air
- Use 1000 mb As Reference Pressure
42Moist Adiabatic Process
- Little difference between
- Dry adiabatic process
-
- Moist, unsaturated adiabatic process
43Moist Adiabatic Process
- Rising Air Expands and Cools Adiabatically
- Temperature Decreases
- Mixing Ratio (w) is Constant
- Only depends on mass
- At Saturation
- ws w
- Condensation
- Latent Heat Release
w ws
T decr. w const.
44Saturated Adiabatic Process
- Now lets consider condensation
45Saturated Adiabatic Process
- Two Methods to Describe the Ascent
- Saturated Adiabatic Process
- Pseudoadiabatic Process
46Saturated Adiabatic Process
- Latent Heat Release Will
- 1. Warm Air
- Heterogeneous System
- Dry Air
- Water Vapor
- Condensation Particles
47Saturated Adiabatic Process
- Latent Heat Release
- 2. Do Work
- Heating Causes Expansion
48Saturated Adiabatic Process
- Water Droplets Remain in Parcel
- Latent Heat Remains within Parcel
49Saturated Adiabatic Process
- Reversible
- Adiabatic
- Isentropic
50Saturated Adiabatic Process
- Mass of System
- Dry Air (md)
- Constant
- Total Water (mt)
- Vapor (mv)
- Liquid Water (mw)
md
mt mt mt
51Saturated Adiabatic Process
- Condensation
- Water Vapor to Liquid Water
dmv
52Saturated Adiabatic Process
- First Law of Thermodynamics
53Saturated Adiabatic Process
54Saturated Adiabatic Process
55Saturated Adiabatic Process
- Lets evaluate cp, R and p
- Latent Heat Warms
- Dry Air
- Water Vapor
- Liquid Water
56Saturated Adiabatic Process
57Saturated Adiabatic Process
58Saturated Adiabatic Process
- Yikes!
- Saturated Adiabatic Process
- Latent Heat of Condensation Warms
- Dry Air
- Water Vapor
- Liquid Water
59Saturated Adiabatic Process
- Assumptions
- Difference Between Moist Adabatic and Dry
Adiabatic Processes is Small
60Saturated Adiabatic Process
- Assumptions
- Can neglect heating of water vapor
- Pressure of dry air is the total pressure
61Saturated Adiabatic Process
- Equation for Saturated Adiabatic Process
- Ignore Heating of Water Vapor
- Small Error
- Liquid Water Remains with Rising Parcel
62Pseudoadiabatic Process
- Water Droplets Fall Out of Parcel
- Latent Heat Remains within Parcel
- Latent Heat Warms Only Dry Air
63Pseudoadiabatic Process
- Irreversible
- Pseudoadiabatic
- Change in Entropy
64Pseudoadiabatic Process
- What does that do to our equation?
65Pseudoadiabatic Process
- Divide both sides by mass of dry air
w mixing ratio
66Pseudoadiabatic Process
- Equation for pseudoadiabatic processes
- Neglects heating of water vapor
- Neglects heating of water mass
- Latent heat release only warms dry air
67Pseudoadiabatic Process
- Not a bad integration except for.
- Left hand side
- lv f(T)
- w f(T)
68Pseudoadiabatic Process
- Assumptions
- lv varies little with temperature (T)
- Valid assumption
69Pseudoadiabatic Process
- Assumptions
- Which varies more during a pseudoadiabatic
process? - dw or T?
- Lets evaluate!
70Pseudoadiabatic Process
71Pseudoadiabatic Process
- Which term is more important?
?
- Lets evaluate using a thermodynamic diagram
72Pseudoadiabatic Process
- Look at the change in w and T along a
pseudoadiabat
73Pseudoadiabatic Process
74Pseudoadiabatic Process
2.8
3.9
75Pseudoadiabatic Process
267
273
76Pseudoadiabatic Process
77Pseudoadiabatic Process
- Plug back into the pseudoadiabatic equation
78Pseudoadiabatic Process
79Pseudoadiabatic Process
80Pseudoadiabatic Process
ws mixing ratio at q qe potential
temperature after all water vapor has condensed
81Pseudoadiabatic Process
- Remember dT is smaller than dw
ws mixing ratio at q qe potential
temperature after all water vapor has condensed
82Pseudoadiabatic Process
- Integrate and evaluate the limits
83Pseudoadiabatic Process
- Take the inverse natural logarithm
84Pseudoadiabatic Process
85Equivalent Potential Temperature (qe )
- The potential temperature a parcel of air would
have if all of its water vapor were condensed and
the latent heat released warmed only the dry air.
86Equivalent Potential Temperature (qe )
ws mixing ratio at once air has become
saturated by adiabatic cooling or ... mixing
ratio at dew point
87Equivalent Potential Temperature (qe )
lv latent heat of vaporization cp
specific heat of dry air T temperature q
potential temperature of air with temperature T
and pressure p
88Equivalent Potential Temperature (qe )
- A measure of the total energy of a parcel of air
- Internal Energy
- Energy from Latent Heat
89Equivalent Potential Temperature (qe )
90Equivalent Potential Temperature (qe )
- Conserved for
- Dry Adiabatic Processes
- Pseudoadiabatic Processes
qe constant
q constant
91Equivalent Potential Temperature (qe )
- Conserved for
- Dry Adiabatic Processes
- Pseudoadiabatic Processes
qe constant
92Equivalent Potential Temperature (qe )
- As the air becomes drier (ws 0), qe approaches q
93Equivalent Potential Temperature (qe )
q
qe
94Review
- Potential Temperature (q )
- The temperature a parcel of air would have if it
were expanded or compressed adiabatically from
its existing pressure and temperature to a
standard pressure of 1000 mb.
95Review
- Wet-Bulb Temperature (Tw)
- The temperature to which air is cooled by
evaporating water into it at constant pressure
until the air is saturated
96Review
- Wet Bulb Potential Temperature (qw )
- The wet bulb temperature the air would have if it
were expanded or compressed adiabatically from
its existing pressure and wet bulb temperature to
a standard pressure of 1000 mb.
97Review
- Virtual Temperature (Tv)
- The temperature dry air must have in order to
have the same density as moist air at the same
pressure
98Review
- Virtual Potential Temperature (qv )
- The virtual temperature the air would have if it
were expanded or compressed adiabatically from
its existing pressure and virtual temperature to
a standard pressure of 1000 mb.
99Review
- Equivalent Temperature (Te )
- The temperature a parcel of air would have if all
of its water vapor were condensed and the latent
heat released warmed only the dry air.
100Review
- Equivalent Potential Temperature (qe )
- The potential temperature a parcel of air would
have if all of its water vapor were condensed and
the latent heat released warmed only the dry air.
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