Title: Moisture and Atmospheric Stability
1Moisture and Atmospheric Stability
Discussion Leader Val
2Contouring Help
3Review
- Turn in hw 3
- Badger forecasts
- Why do you dry off faster in a desert climate?
4The biggest power plant on Earths surface-
http//www.srh.weather.gov/jetstream/atmos/hydro.h
tm
5Water can exist in all three phases in our
atmosphere
- What term do we seem to use to quantify the
amount of water in any given volume of air at one
time? - Answer Moisture
6 Ways to measure the moisture content of the
atmosphere (discussed in lec.)
- Absolute Humidity
- Specific Humidity
- Saturation Mixing Ratio
- Vapor Pressure
- Saturation Vapor Pressure
- Relative Humidity
- Dew Point Temperature
7 The variables we will refer to most
- Mixing Ratio- mass of water vapor/mass of dry air
(does not change). - Relative Humidity- Vapor Pressure/ Saturation
vapor pressure. - Dew Point Temperature- The temperature at which
air with the current amount of vapor in it will
become saturated.
8Two ways to saturate the air
(or raise the
relative humidity)
9Two ways to saturate the air
(or raise the
relative humidity)
- 1. Add more water vapor to it
- 2. Decrease the temperature
- This is because warm air is capable of holding
more water vapor molecules than cold air. - (Remember the water vapor molecules are moving
faster in warm air and less likely to stick and
condense)
10Moisture
- An air parcel with a large moisture content has
the potential for that parcel to produce a great
amount of precipitation. - - Air with a mixing ratio of 13 g/kg will likely
rain a greater amount of water than air with a
mixing ratio of 6 g/kg.
11Moisture
Two parcels of air PARCEL 1 Temperature 31
oF, Dewpoint 28 oF PARCEL 2 Temperature
89 oF, Dewpoint 43 oF
Parcel 2 contains more water vapor than Parcel 1,
because its dewpoint is higher. Parcel 1 has a
higher relative humidity, because it wouldnt
take much cooling for the temperature to equal
the dewpoint! Thus, Parcel 1 is more likely to
become saturated. But if it happened that both
parcels became saturated then Parcel 2 would have
the potential for more precipitation. RH is not
simply equal to the dewpoint divided by the temp.
but is a good representation.
12The other key component to the hydrologic cycle-
Stability
- What is stability?
- Stability refers to a condition of equilibrium
- If we apply some perturbation to a system, how
will that system be affected? - Stable System returns to original state
- Unstable System continues to move away from
original state - Neutral System remains steady after perturbed
13Stability Example
Stable Marble returns to its original position
Unstable Marble rapidly moves away from initial
position
14Stability
How does a bowl and marble relate to the
atmosphere??
- When the atmosphere is stable, a parcel of air
that is lifted will want to return back to its
original position
http//www.chitambo.com/clouds/cloudshtml/humilis.
html
15Stability Cont.
- When the atmosphere is unstable (with respect to
a lifted parcel of air), a parcel will want to
continue to rise if lifted
http//www.physicalgeography.net/fundamentals/imag
es/cumulonimbus.jpg
16What do we mean by an air parcel?
- Imaginary small body of air a few meters wide
- Can expand and contract freely
- Does not break apart
- Only considered with adiabatic processes -
External air and heat cannot mix with the air
inside the parcel - Parcel warms or cools purely due to pressure
changes (?U Q W)
17Buoyancy and Stability
- At same pressure if at same altitude!
- So if ?parcel lt ?env. Parcel is positively
buoyant - In terms of temperature that would mean
- T of parcel gt T of environment buoyant!
(unstable) - T of parcel lt T of environment sink! (stable)
- T of parcel T of environment stays put
(neutral)
18Atmospheric Stability (Review)
This is all well and good but what about day to
day applications almost there
19Vertical Profile of Atmospheric Temperature
20Lapse Rates
Lapse Rate The rate at which temperature
decreases with height (Remember the inherent
negative wording to it) Environmental Lapse
Rate Lapse rates associated with an observed
atmospheric sounding (negative for an inversion
layer) Parcel Lapse Rate Lapse rate of a
parcel of air as it rises or falls (either
saturated or not) MALR - Moist Adiabatic Lapse
Rate Saturated air parcel DALR - Dry Adiabatic
Lapse Rate Dry air parcel
21DALR
- Air in parcel must be unsaturated
- (RH lt 100)
- Rate of adiabatic heating or cooling 9.8C for
every 1000 meter (1 kilometer) change in
elevation - Parcel temperature decreases by about 10 if
parcel is raised by 1km, and increases about 10
if it is lowered by 1km
22MALR (or SALR)
- As rising air cools, its RH increases because the
temperature approaches the dew point temperature,
Td - If T Td at some elevation, the air in the
parcel will be saturated (RH 100) - If parcel is raised further, condensation will
occur and the temperature of the parcel will cool
at the rate of about 6C per 1km in the
mid-latitudes
23DALR vs. MALR
- The MALR is less than the DALR because of latent
heating - As water vapor condenses into liquid water for a
saturated parcel, LH is released, lessening the
adiabatic cooling
Remember no heat exchanged with environment
24DALR vs. MALR
25Absolute Stability
- The atmosphere is absolutely stable when the
environmental lapse rate (ELR) is less than the
MLR - ELR lt MALR lt DALR
- A saturated OR unsaturated parcel will be cooler
than the surrounding environment and will sink,
if raised
26Absolute Stability
- Inversion layers are always absolutely stable
- Temperature increases with height
- Warm air above cold air very stable
27Absolute Instability
- The atmosphere is absolutely unstable when the
ELR is greater than the DALR - ELR gt DALR gt MALR
- An unsaturated OR saturated parcel will always be
warmer than the surrounding environment and will
continue to ascend, if raised
28Conditional Instability
- The atmosphere is conditionally unstable when the
ELR is greater than the MALR but less than the
DALR - MALR lt ELR lt DALR
- An unsaturated parcel will be cooler and will
sink, if raised - A saturated parcel will be warmer and will
continue to ascend, if raised
29Conditional Instability
- Example parcel at surface
- T(p) 30C, Td(p) 14C (unsaturated)
- ELR 8C/km for first 8km
- Parcel is forced upward, following DALR
- Parcel saturated at 2km, begins to rise at MALR
- At 4km, T(p) T(e)this is the level of free
convection (LFC)
30Conditional Instability
- Example continued
- Now, parcel will rise on its own because T(p) gt
T(e) after 4km - The parcel will freely rise until T(p) T(e),
again - This is the equilibrium level (EL)
- In this case, this point is reached at 9km
- Thus, parcel is stable from 0 4km and unstable
from 4 9km
LCL
31Lifting due to Topography
32How does the parcel get a lift?
- Convection
- Convergence
- Topography
33Lifting due to Topography
- This type of lifting occurs when air is
confronted by a sudden increase in the vertical
topography of the Earth - When air comes across a mountain, it is lifted up
and over, cooling as it is rising - The type of cloud formed is dependent upon the
moisture content and stability of the air
34Lifting by Convection
- As the earth is heated by the sun, thermals
(bubbles of hot air) rise upward from the surface - The thermal cools as it rises, losing some of its
buoyancy (its ability to rise) - The vertical extent of the cloud is largely
determined by the stability of the environment
35Lifting by Convection
- A deep stable layer restricts continued vertical
growth - A deep unstable layer will likely lead to
development of rain-producing clouds - These clouds are more vertically developed than
clouds developed by convergence lifting
36Lifting by Convergence
- Convergence exists when there is a horizontal net
inflow into a region - When air converges along the surface, it is
forced to rise
37Lifting by Convergence
- Large scale convergence can lift air hundreds of
kilometers across - Vertical motions associated with convergence are
generally much weaker than ones due to convection - Generally, clouds developed by convergence are
less vertically developed