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Chapter 3

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Title: Chapter 3


1
Chapter 3Part 2
  • Blackbody Radiation/
  • Planetary Energy Balance

2
Solar Spectrum The sun emits radiation at all
wavelengths Most of its energy is in the
IR-VIS-UV portions of the spectrum 50 of the
energy is in the visible region 40 in the
near-IR 10 in the UV
3
Wavelength (m)
4
Blackbody Radiation
Planck function
Blackbody radiationradiation emitted by a body
that emits (or absorbs) equally well at all
wavelengths
5
Wikipedia Commons http//en.wikipedia.org/wiki/Im
ageBbs.jpg
6
  • Basic Laws of Radiation
  • All objects emit radiant energy.

7
  • Basic Laws of Radiation
  • All objects emit radiant energy.
  • Hotter objects emit more energy than colder
    objects.

8
  • Basic Laws of Radiation
  • All objects emit radiant energy.
  • Hotter objects emit more energy than colder
    objects. The amount of energy radiated is
    proportional to the temperature of the object
    raised to the fourth power.

9
  • Basic Laws of Radiation
  • All objects emit radiant energy.
  • Hotter objects emit more energy than colder
    objects. The amount of energy radiated is
    proportional to the temperature of the object
    raised to the fourth power.
  • ? This is the Stefan Boltzmann Law
  • F ? T4
  • F flux of energy (W/m2)
  • T temperature (K)
  • ? 5.67 x 10-8 W/m2K4 (a constant)

10
Wikipedia Commons http//en.wikipedia.org/wiki/Im
ageBbs.jpg
11
  • Basic Laws of Radiation
  • All objects emit radiant energy.
  • Hotter objects emit more energy than colder
    objects (per unit area). The amount of energy
    radiated is proportional to the temperature of
    the object.
  • The hotter the object, the shorter the wavelength
    (?) of emitted energy.

12
  • Basic Laws of Radiation
  • All objects emit radiant energy.
  • Hotter objects emit more energy than colder
    objects (per unit area). The amount of energy
    radiated is proportional to the temperature of
    the object.
  • The hotter the object, the shorter the wavelength
    (?) of the peak in emitted energy.
  • ?This is Wiens Law

13
Wikipedia Commons http//en.wikipedia.org/wiki/Im
ageBbs.jpg
14
? Stefan-Boltzmann law F ? T4 F flux
of energy (W/m2) T temperature (K) ? 5.67
x 10-8 W/m2K4 (a constant) ? Wiens law
15
We can use these equations to calculate
properties of energy radiating from the Sun and
the Earth.
6,000 K
300 K
16
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17
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18
Electromagnetic Spectrum
visible light
ultraviolet
infrared
x-rays
microwaves
High Energy
Low Energy
? (?m)
19
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20
  • Blue light from the Sun is removed from the beam
  • by Rayleigh scattering, so the Sun appears
    yellow
  • when viewed from Earths surface even though
    its
  • radiation peaks in the green

21
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22
? Stefan-Boltzman law F ? T4 F flux of
energy (W/m2) T temperature (K) ? 5.67 x
10-8 W/m2/K4 (a constant)
23
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24
Solar Radiation and Earths Energy Balance
25
Planetary Energy Balance
  • We can use the concepts learned so far to
    calculate the radiation balance of the Earth

26
Some Basic Information Area of a circle ?
r2 Area of a sphere 4 ? r2
27
Energy Balance The amount of energy delivered
to the Earth is equal to the energy lost from the
Earth. Otherwise, the Earths temperature would
continually rise (or fall).
28
Energy Balance Incoming energy outgoing
energy Ein Eout
Eout
Ein
29
How much solar energy reaches the Earth?
30
How much solar energy reaches the Earth? As
energy moves away from the sun, it is spread over
a greater and greater area.
31
How much solar energy reaches the Earth? As
energy moves away from the sun, it is spread over
a greater and greater area. ? This is the
Inverse Square Law
32
Define So as the energy flux reaching the Earth
from the Sun. We can calculate So So L /
A, where L The Suns luminosity and A area
of a sphere with a radius equal to Earths
orbital distance
33
So is the solar constant for Earth
34
So is the solar constant for Earth It is
determined by the distance between Earth (rs-e)
and the Sun and the Sun luminosity.
35
Each planet has its own solar constant
36
How much solar energy reaches the
Earth? Assuming solar radiation covers the area
of a circle defined by the radius of the Earth
(re)
Ein
re
37
How much solar energy reaches the
Earth? Assuming solar radiation covers the area
of a circle defined by the radius of the Earth
(re) Ein So (W/m2) x ? re2 (m2)
Ein
re
38
How much energy does the Earth emit?
300 K
39
How much energy does the Earth emit? Eout F x
(area of the Earth)
40
How much energy does the Earth emit? Eout F x
(area of the Earth) F ? T4 Area 4 ? re2
41
How much energy does the Earth emit? Eout F x
(area of the Earth) F ? T4 Area 4 ? re2
Eout (? T4) x (4 ? re2)
42
Sun
Earth
Hotter objects emit more energy than colder
objects
? (?m)
43
Sun
Earth
Hotter objects emit more energy than colder
objects F ? T4
? (?m)
44
Hotter objects emit at shorter wavelengths. ?max
3000/T
Sun
Earth
Hotter objects emit more energy than colder
objects F ? T4
? (?m)
45
How much energy does the Earth emit? Eout F x
(area of the Earth)
46
How much energy does the Earth emit? Eout F x
(area of the Earth) F ? T4 Area 4 ? re2
Eout (? T4) x (4 ? re2)
47
How much solar energy reaches the Earth?
Ein
48
How much solar energy reaches the Earth? We can
assume solar radiation covers the area of a
circle defined by the radius of the Earth (re).
Ein
re
49
How much solar energy reaches the Earth? We can
assume solar radiation covers the area of a
circle defined by the radius of the Earth
(re). Ein So x (area of circle)
Ein
re
50
Remember
So is the solar constant for Earth It is
determined by the distance between Earth and the
Sun (R) and the Suns luminosity (L).
51
How much solar energy reaches the Earth? We can
assume solar radiation covers the area of a
circle defined by the radius of the Earth
(re). Ein So x (area of circle) Ein So
(W/m2) x ? re2 (m2)
Ein
re
52
How much solar energy reaches the Earth? Ein
So ? re2 BUT THIS IS NOT QUITE
CORRECT! Some energy is reflected away
Ein
re
53
How much solar energy reaches the Earth? Albedo
(A) energy reflected away Ein So ? re2
(1-A)
Ein
re
54
How much solar energy reaches the Earth? Albedo
(A) energy reflected away A 0.3 today Ein
So ? re2 (1-A) Ein So ? re2 (0.7)
re
Ein
55
Energy Balance Incoming energy outgoing
energy Ein Eout
Eout
Ein
56
Energy Balance Ein Eout Ein So ? re2 (1-A)
Ein
57
Energy Balance Ein Eout Ein So ? re2
(1-A) Eout ? T4(4 ? re2)
Ein
58
Energy Balance Ein Eout So ? re2 (1-A) ?
T4 (4 ? re2)
Ein
59
Energy Balance Ein Eout So ? re2 (1-A) ?
T4 (4 ? re2)
Ein
60
Energy Balance Ein Eout So (1-A) ? T4 (4)
Ein
61
Energy Balance Ein Eout So (1-A) ? T4
(4) T4 So(1-A) 4?
Ein
62
T4 So(1-A) 4?
If we know So and A, we can calculate the
temperature of the Earth. We call this the
expected temperature (Texp). It is the
temperature we would expect if Earth behaves like
a blackbody. This calculation can be done for
any planet, provided we know its solar constant
and albedo.
63
T4 So(1-A) 4?
For Earth So 1370 W/m2 A 0.3 ? 5.67 x
10-8 W/m2K4
64
T4 So(1-A) 4?
For Earth So 1370 W/m2 A 0.3 ? 5.67 x
10-8 T4 (1370 W/m2)(1-0.3) 4
(5.67 x 10-8 W/m2K4)
65
T4 So(1-A) 4?
For Earth So 1370 W/m2 A 0.3 ? 5.67 x
10-8 T4 (1370 W/m2)(1-0.3) 4
(5.67 x 10-8 W/m2K4) T4 4.23 x 109 (K4) T
255 K
66
Expected Temperature Texp 255 K (oC) (K) -
273
67
Expected Temperature Texp 255 K (oC) (K) -
273 So. Texp (255 - 273) -18 oC (which is
about 0 oF)
68
Is the Earths surface really -18 oC?
69
Is the Earths surface really -18 oC? NO. The
actual temperature is warmer! The observed
temperature (Tobs) is 15 oC, or about 59 oF.
70
Is the Earths surface really -18 oC? NO. The
actual temperature is warmer! The observed
temperature (Tobs) is 15 oC, or about 59 oF. The
difference between observed and expected
temperatures (?T) ?T Tobs - Texp ?T 15 -
(-18) ?T 33 oC
71
?T 33 oC In other words, the Earth is 33 oC
warmer than expected based on black body
calculations and the known input of solar energy.
72
?T 33 oC In other words, the Earth is 33 oC
warmer than expected based on black body
calculations and the known input of solar
energy. This extra warmth is what we call the
GREENHOUSE EFFECT.
73
?T 33 oC In other words, the Earth is 33 oC
warmer than expected based on black body
calculations and the known input of solar
energy. This extra warmth is what we call the
GREENHOUSE EFFECT. It is a result of warming
of the Earths surface by the absorption of
radiation by molecules in the atmosphere.
74
The greenhouse effect Heat is absorbed or
trapped by gases in the atmosphere. Earth
naturally has a greenhouse effect of 33 oC.
75
The concern is that the amount of greenhouse
warming will increase with the rise of CO2 due to
human activity.
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