Title: The Greenhouse Effect
1The Greenhouse Effect
- Ananda Guneratne
- (Part A)
2Topics Covered in this Presentation
- Finding the Intensity of Radiation on a planet
- 8.5.1 - Calculate the intensity of the Sun's
radiation incident on a planet. -
- Albedo
- 8.5.2 - Define albedo.
- 8.5.3 - State factors that determine a planet's
albedo. -
- Black-Body Radiation
- 8.5.8 - Outline the nature of black-body
radiation. - 8.5.9 - Draw and annotate a grap of thee emission
spectra of black bodies at different temperatures - 8.5.10 - State the Stefan-Boltzmann Law and apply
it to compare emission rates from different
surfaces. - 8.5.11 - Apply the concept of emissivity to
compare the emission rates from the different
surfaces.
3Intensity of Solar Radiation
8.5.1
- How to calculate the solar radiation incident on
any planet -
- Imagine the planet as a disc
- The intensity of the radiation is measured in
watts per square meter. - Thus, the intensity of solar radiation incident
on a planet is
Fig. 0.0 - Discs and Spheres
4Example - Earth
8.5.1
Average energy of solar radiation entering
Earth's atmosphere Thus, The average
radiation incident at the surface of the Earth is
342 watts per meter squared.
5What is Albedo?
8.5.2
- Definition
-
- The albedo of a surface is the percentage of
incoming radiation that is reflected (rather than
absorbed) by that surface. - Albedo
-
Radiation reflected
Total incoming Radiation
Fig. 1.0 - Differences between albedos
6What Determines Albedo?
8.5.3
- Color
- Caused by reflection
- Angle
- Latitude
- Season
- Cloud cover
- Daily variance
Some Common Albedo Ranges Fresh Snow/Ice
0.60-0.90 Old melting snow
0.40-0.70 Clouds
0.40-0.90 Desert Sand
0.30-0.50 Soil
0.05-0.30 Tundra
0.15-0.35 Grasslands
0.18-0.25 Forest
0.05-0.20 Water
0.05-0.10 Global Annual Mean 0.30
7What Determines Albedo?
8.5.3
Fig. 1.1 - The Seasons
8What Determines Albedo?
8.5.3
Fig. 1.2 - Seasonal and Latitudinal Albedo Changes
9Albedo Loss - "The Slippery Slope to Hell"
Fig. 1.3 - Polar Icecaps and Albedo
10What is a black body?
8.5.8
- Hypothetical
- Perfect absorber
- Perfect emitter
- Produces black-body radiation
- Emitted from a black body
- Properties depend solely on temperature
Fig. 2.0 - Black Body
11The Ultraviolet Catastrophe
8.5.8
- Classical Physics
- (James Maxwell)
- Energy is proportional to frequency
- Quantum Physics
- (Max Planck)
- Ehf, energy emitted in quanta
Fig. 2.1 Black body raditation under classical
theory
12The Blackbody Spectrum
8.5.9
Fig. 2.2 - Blackbody spectra at various
temperatures
13The Stefan-Boltzmann Law
8.5.10
- The Stefan-Boltzmann Law states that the amount
of energy radiated per unit area per second is
proportional to the temperature of the object
raised to the fourth power. -
- General Formulation
- Q Energy transferred per unit time (W)
- b Constant
- A Area
- T1 Absolute temperature of radiating body
- T2 Absolute temperature of absorbing body
14Stefan-Boltzmann Constant
8.5.10
15Example
8.5.10
Surface A has a temperature of 50.0 K and a
constant b of 0.021. Surface B has a temperature
of 100. K and a constant b of 0.016. Assume both
surfaces have an equal area, and that the
surrounding temperature is 25.0 K, which surface
has a higher rate of emission? Since we do not
know area, we will be finding our answer in rate
of emission per unit area. Thus,
and We can thus see that
Surface B will emit electromagnetic radiation at
a higher rate.
16Emissivity
8.5.11
- Emissivity is the ratio of the radiation emitted
by a surface to the radiation of a blackbody at
the same temperature and under similar
conditions. - Kirchoff's law
- At a given temperature, the rate of emission
of electromagnetic energy by an object is equal
to the rate at which the object absorbs
electromagnetic energy of the same wavelength.
17Example
8.5.11
Surface A has an emissivity of 0.8. Surface B
has an emissivity of 0.2. If the rate of
emission of a black body under similar conditions
is 5 kJ per second, find the rates of emmission
of Surface A and Surface B. A 5(0.8) 4 kJ
per second B 5(0.2) 1 kJ per second
18Sources
- B.N. Taylor, P.J. Mohr, D.B. Newell,CODATA
Reccomended Values of the Fundemental Physical
Constants 2006,(National Institute of Standards
and Technology,Gaithersburg, Maryland, 2006). - J.R. Gribbin, Q is for Quantum Particle Physics
From A-Z, 1st ed. (Weidenfield Nicolson, Great
Britain, 1998), p. 44-45, 201, 286, 376. - Van Nostrand Reinhold Company, Van Nostrand's
Scientific Encyclopedia, 5th ed. (Van Nostrand
Reinhold Company, New York, 1976), p. 948, 1249. - W.F. Ruddiman, Earth's Climate Past and Future,
1st ed. (W.F. Freeman Co., New York, 2000), p.
19-20, 22-25.
19Picture Sources
- Fig. 0.0 http//www.windows.ucar.edu/earth/climat
e/images/earth_insolation_disk_sphere_big.jpg - Fig. 1.0 http//www.uwsp.edu/geo/faculty/ritter/i
mages/atmosphere/energy/albedo.gif - Fig. 1.1 http//www.dkimages.com/discover/preview
s/784/563581.JPG - Fig. 1.2 http//photojournal.jpl.nasa.gov/jpeg/PI
A04378.jpg - Fig. 1.3 http//www.zeeburgnieuws.nl/nieuws/image
s/albedo_effect_sea_ice_loss.jpg - http//www.zeeburgnieuws.nl/nieuws/
images/sea_ice_yearly_decline.jpg - Fig. 2.0 http//www.egglescliffe.org.uk/physics/a
stronomy/blackbody/animation.gif - Fig. 2.1 http//www.haverford.edu/physics/songs/c
avendish/uvcat.jpg - Fig. 2.2 http//rip.physics.unk.edu/Larsen/blackb
ody_spectra.jpg