Title: Earths Climate System Today
1Earths Climate System Today
- Heated by solar energy
- Tropics heated more than poles
- Imbalance in heating redistributed
- Solar heating and movement of heat by oceans and
atmosphere determines distribution of - Temperature
- Precipitation
- Ice
- Vegetation
2Electromagnetic Spectrum
- Electromagnetic energy travels through space
- Energy heating Earth mostly short-wave radiation
- Visible light
- Some ultraviolet radiation
3Incoming Solar Radiation
- Radiation at top of Earths atmosphere 1368 W
m-2 - If Earth flat disk with no atmosphere, average
radiation 1368 W m-2 - Earth 3-dimensional rotating sphere,
- Area 4?r2
- Average solar heating 1368 ? 4 342 W m-2
430 Solar Energy Reflected
- Energy reflected by clouds, dust, surface
- Ave. incoming radiation 0.7 x 342 240 W m-2
5Energy Budget
- Earths temperature constant 15?C
- Energy loss must incoming energy
- Earth is constantly receiving heat from Sun,
therefore must lose equal amount of heat back to
space - Heat loss called back radiation
- Wavelengths in the infrared (long-wave radiation)
- Earth is a radiator of heat
- If T gt 1?K, radiator of heat
6Energy Budget
- Average Earths surface temperature 15?C
- Reasonable assumption
- Surface of earth radiates heat with an average
temperature of 15?C - However, satellite data indicate Earth radiating
heat average temperature -16?C - Why the discrepancy?
- What accounts for the 31?C heating?
7Energy Budget
- Greenhouse gases absorb 95 of the long-wave,
back radiation emitted from Earths surface - Trapped radiation reradiated down to Earths
surface - Accounts for the 31?C heating
- Satellites dont detect radiation
- Muffling effect from greenhouse gases
- Heat radiated back to space from elevation of
about 5 km (top of clouds) average 240 W m-2 - Keeps Earths temperature in balance
8Energy Balance
9Greenhouse Gases
- Water vapor (H2O(v), 1 to 3)
- Carbon dioxide (CO2, 0.037 365 ppmv)
- Methane (CH4, 0.00018 1.8 ppmv)
- Nitrous oxide (N2O, 0.00000315 315 ppbv)
- Clouds also trap outgoing radiation
10Variations in Heat Balance
- Incoming solar radiation
- Stronger at low latitudes
- Weaker at high latitudes
- Tropics receive more solar radiation per unit
area than Poles
11Variations in Heat Balance
- What else affects variation in heat balance?
- Solar radiation arrives at a low angle
- Snow and ice reflect more radiation at high
latitudes - Albedo
- Percentage of incoming solar radiation that is
reflected rather than absorbed
12Average Albedo
13Sun Angle Affects Albedo
- All of Earths surfaces absorb more solar
radiation from an overhead sun - Water reflects lt5 radiation from an overhead Sun
14Sun Angle Affects Albedo
- Water reflects a high fraction of radiation from
a low-lying Sun - Earth average albedo 10
15Pole-to-Equator Heat Imbalance
- Incoming solar radiation per unit area higher in
Tropics than Poles - Sun angle higher in Poles than Tropics
- Albedo higher at Poles than Tropics
- Variations in cloud cover affect heat imbalance
16Seasonal Change in Solar Radiation Albedo
- Tilt of Earths axis results in seasonal change
in - Solar radiation in each hemisphere
- Snow and ice cover (albedo)
17Seasonal Change in Solar Radiation
- Large seasonal change in solar radiation between
the hemispheres
18Seasonal Change in Albedo
- Increases in N. hemisphere winter due mainly to
snow cover and to lesser degree Arctic sea ice - Increases in S. hemisphere winter due to sea ice
19Albedo-Temperature Feedback
20Water a Key to Earths Climate
- Water has high heat capacity
- Measure of ability to absorb heat
- Heat measured in calories
- 1 calorie amount of heat required to raise
temperature of one gram of water by 1?C - Heat Capacity (cal cm-3) Density (g cm-2) x
Specific Heat (cal g-1) - Specific heat of water 1
- Ratio of heat capacity watericeairland
60521 - Heat capacity of air linked to water vapor
21Differences in Heating Land Oceans
- Low latitude ocean major storage tank of solar
heat - Sunlight direct, albedo low, heat capacity high
- Heats surface winds mix heat
- Contrast with land
- Albedo high, heat capacity conductance low
- Tropical/subtropical lands become hot, but dont
store heat
22Sensitivity of Land Oceans to Solar Heating
- Change in mean seasonal surface temperature
greatest over large landmasses and lowest over
oceans
23Thermal Response Different
- Large land masses heat and cool quickly
- Extreme seasonal temperature reached 1 month
after Solstice - Upper ocean heats and cools slowly
- Extreme seasonal temperature reached 2-3 months
after Solstice
24Redistribution of Heat
- Heat transfer in Earth atmosphere
- Sensible heat
- Heat that a person directly senses
- Sensible heat T x specific heat
- Latent heat (hidden or concealed)
- Additional heat required to change the state of a
substance - Sensible and latent heat affected by convection
25Convection
26Sensible Heat
- Sensible heating greatest
- At low latitude
- Overhead Sun
- Over land
- Low heat conductance (air heats)
- Dry regions
- Low humidity
- Sensible heat lowest
- Over oceanic regions
27Latent Heat
- Heat is temporarily hidden or latent in water
vapor - Powerful process transferring heat long distances
- Transfer is two step process
- Initial evaporation of water and storage of heat
in vapor - Later release of stored heat during condensation
and precipitation (typically far from site of
evaporation)
28Latent Heat
0C-100C, 1 calorie of heat energy needed to
increase 1 g H2O by 1C
Condensation of water releases 540 cal g-1
latent heat of vaporization
H2O(l) ? H2O(g) requires 540 cal g-1
80 cal g-1 heat required for phase
transformation, ice ? water
80 cal g-1 heat released when water freezes
latent heat of melting
29Latent Heat of Vaporization
- Important evaporation occurs at any temperature
between 0-100C - Latent heat is associated with any change of
state - Therefore, during evaporation heat is stored in
water vapor in latent form for later release
30Water Vapor Content of Air
- Saturation vapor density
- Warm air holds 10X more water than cold
31Redistribution of Latent Heat
- Evaporation in warm equatorial region
- Stored energy carried vertically and horizontally
- Condensation and precipitation releases energy
32Water Vapor Feedback
33Unequal Heating of Tropics and Poles
- Latitudes lt35 have excess incoming solar
radiation over outgoing back radiation - Excess heat stored in upper ocean drives general
circulation of oceans and atmosphere
34Atmospheric Circulation
- Atmosphere has no distinct upper boundary
- Air becomes less dense with increasing altitude
- Air is compressible and subject to greater
compression at lower elevations, density of air
greater at surface - Constant composition to 80 km
- What drives atmospheric circulation?
35Free Convection
- Atmospheric mixing related to buoyancy
- Localized parcel of air is heated more than
nearby air - Warm air is less dense than cold air
- Warm air is therefore more buoyant than cold air
- Warm air rises
36Forced Convection
- Occurs when a fluid breaks into disorganized
swirling motions as it undergoes flow - Fluid flow can be laminar or turbulent
37Laminar vs. Turbulent Flow
- Whether a fluid flow is laminar or turbulent
depends on - Velocity (rate of movement)
- Geometry (primarily depth)
- Viscosity
- Turbulent flow occurs during high velocity
movement of non-viscous fluids in unconfined
geometries
38Forced Convection in Atmosphere
- Horizontally moving air undergoes turbulence
- Air is forced to mix vertically through eddy
motions because of - High velocity
- Depth of atmosphere
- Low viscosity
39Atmospheric Circulation
- Force of gravity maintains a stable atmosphere
- Most of the mass of air near surface
- As a result of atmospheric pressure
- Dense air at surface
- Air flows from high pressure to low pressure
- Flow is turbulent
- Turbulent flow produces vertical mixing
40Mixing by Sensible Heat
- Convection driven by sensible heat
- Air parcels rise if they become heated and less
dense than surrounding air - As air parcels rises,
- Air expands
- Air cools
- Air becomes less dense
- Air parcels stop rising
- Heat transferred vertically, since air forced
from high to low pressure, heat also moves
horizontally
41Adibatic Process
- Rising and sinking air change temperature with no
gain or loss of heat - Consider sinking parcel of air
- As it sinks, it contracts
- Contraction takes work
- Work takes (mechanical) energy
- Temperature of air rises
- Conservation of energy
- 1st law of thermodynamics
42Thermodynamics of Air
- First law of thermodynamics
- Heat added work done rise in Temp
- But, adibatic process (no heat added)
- Heat added work done rise in Temp
- Second term is not zero
- Work of compression results in a rise in
temperature of air parcel
43Mixing by Latent Heat
- Water vapor is less dense than mixture of gases
composing the atmosphere - Evaporation adds water vapor to atmosphere and
lowers its density - Moist air rises, expands and cools until dew
point reached - When air becomes fully saturated
- Condensation begins
- Air releases latent heat
- Air heats and becomes less dense causing it to
rise further - Eventually water vapor lost, air parcel stops
release of latent heat and stops rising
44Which Process More Important?
- Atmospheric circulation driven by adiabatic
processes (sensible heat) redistributes about 30
heat - Atmospheric circulation driven by latent heat
redistributes about 70 heat - Greater amount of heat stored in water
- Larger distances moist air parcels move
45Dry Adibatic Lapse Rate
- Rising and sinking dry air parcel cools and heats
at a constant rate - Dry adibatic lapse rate 10C km-1
- Work required to lift an air parcel
- Mix of gases
- Acceleration of gravity
- Regardless of latitude, season, altitude, etc. a
dry parcel of air will heat or cool at 10C km-1
46Dew Point Lapse Rate
- Consider a rising parcel of air with constant
humidity - Dew point decreases as parcel expands
- Drop in pressure, drop in dew point
- Lapse of dew point as parcel rises
- Dew point lapse rate 2C km-1
- Over 1 km, air cools by 10C
- Air temperature rapidly approaches dew point as
parcel rises - As air temperature approaches dew point, cloud
forms
47Wet Adibatic Lapse Rate
- As wet air rises, it cools, dew point reached and
condensation begins - Latent heat released
- Decreasing rate of cooling
- Wet adibatic lapse rate
- 4C km-1 minimum (rapid condensation)
- 9C km-1 maximum (slow condensation)
- Differences in temperature
- For same amount of cooling, warm air looses more
water than cold air
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49Summary
- Once saturation reached latent heat released as
long as parcel continues to rise - The saturated process assumes condensation
products fall out of parcel, so the parcel
maintains 100 humidity - Upon decent, the parcel warms, relatively
humidity falls below 100 - After decent the parcel is warmer because latent
heat was added during ascent - Dry adibatic process reversible
- Wet adibatic process non-reversible