http://www.ces.fau.edu/nasa/mod
ule-2/how-greenhouse-effect-
works.php
This figure shows the blackbody spectra of Earth and sun. The incoming radiation from
the sun is much more intense (Y-axis) than that of outgoing radiation from the Earth
because the energy emitted from a blackbody is proportionate to its temperature to the
fourth (σT4) – i.e. the sun emits a far greater amount of energy than the Earth. Incoming
solar radiation is shortwave (X-axis, wavelength in microns) and in the wavelength range
of ultraviolet and visible radiation (shown as the rainbow spectrum of colors). Outgoing
Earth’s radiation is long wave and and is in the range of infrared radiation (shown in red).
Below the blackbody spectra, molecules in the atmosphere, known as greenhouse gases,
interfere with incoming and outgoing radiation. For instance, ozone (O3) in the
stratosphere absorbs some of incoming radiation and is known as the ozone layer. That
said, greenhouse gases (N2O, O3, CO2, and H2O) mainly interfere with outgoing radiation.
Let’s talk about the molecular motion of these greenhouse gases to understand the
greenhouse effect.
Molecular Motions and the Greenhouse Gases H2O and CO2
2349cm-1 667cm-1
Here are the physical causes (molecular motion) of the greenhouse effect. But first… it
may be a bit chunky, so sit back, take a deep breath!
Gas molecules can absorb or emit radiation in the infrared range in two different
ways. One way is by changing the rate at which the molecules rotate. The theory of
quantum mechanics describes the behavior of matter on a microscopic scale – that is,
the size of molecules and smaller. According to this theory, molecules can rotate only
at certain discrete frequencies as if vibrations of a piano string in that they tend to be
at specific “ringing” frequencies. (The rotation frequency is the number of revolutions
that a molecule completes per second.) The molecule can absorb incident wave
(energy), if this incident wave has just the right frequency.
This frequency of the radiation that can be absorbed or emitted depends on the
molecule’s structure. The H2O molecule is constructed in such a manner that it
absorbs infrared radiation of wavelengths of about 12 micrometers and longer. This
interaction gives rise to a very strong absorption feature in Earth’s atmosphere called
the H2O rotation band. As shown in the previous slide, virtually 100 % of infrared
radiation longer than 12 micrometers is absorbed with a combination of CO2 and H2O.
(By the way, the H2O rotation band extends all the way into the microwave region of
the electromagnetic spectrum, i.e. above a wavelength of 1000 micrometer, which is
why a microwave oven is able to heat up anything that contains water.)
Molecular Motions and the Greenhouse Gases H2O and CO2
2349cm-1 667cm-1
The second way in which molecules can absorb or emit infrared radiation is by changing
the amplitude at which they vibrate. Molecules ...
1. http://www.ces.fau.edu/nasa/mod
ule-2/how-greenhouse-effect-
works.php
This figure shows the blackbody spectra of Earth and sun. The
incoming radiation from
the sun is much more intense (Y-axis) than that of outgoing
radiation from the Earth
because the energy emitted from a blackbody is proportionate to
its temperature to the
fourth (σT4) – i.e. the sun emits a far greater amount of energy
than the Earth. Incoming
solar radiation is shortwave (X-axis, wavelength in microns)
and in the wavelength range
of ultraviolet and visible radiation (shown as the rainbow
spectrum of colors). Outgoing
Earth’s radiation is long wave and and is in the range of
infrared radiation (shown in red).
Below the blackbody spectra, molecules in the atmosphere,
known as greenhouse gases,
interfere with incoming and outgoing radiation. For instance,
ozone (O3) in the
stratosphere absorbs some of incoming radiation and is known
as the ozone layer. That
said, greenhouse gases (N2O, O3, CO2, and H2O) mainly
interfere with outgoing radiation.
Let’s talk about the molecular motion of these greenhouse gases
to understand the
2. greenhouse effect.
Molecular Motions and the Greenhouse Gases H2O and CO2
2349cm-1 667cm-1
Here are the physical causes (molecular motion) of the
greenhouse effect. But first… it
may be a bit chunky, so sit back, take a deep breath!
Gas molecules can absorb or emit radiation in the infrared range
in two different
ways. One way is by changing the rate at which the molecules
rotate. The theory of
quantum mechanics describes the behavior of matter on a
microscopic scale – that is,
the size of molecules and smaller. According to this theory,
molecules can rotate only
at certain discrete frequencies as if vibrations of a piano string
in that they tend to be
at specific “ringing” frequencies. (The rotation frequency is the
number of revolutions
that a molecule completes per second.) The molecule can absorb
incident wave
(energy), if this incident wave has just the right frequency.
This frequency of the radiation that can be absorbed or emitted
depends on the
molecule’s structure. The H2O molecule is constructed in such a
manner that it
absorbs infrared radiation of wavelengths of about 12
micrometers and longer. This
3. interaction gives rise to a very strong absorption feature in
Earth’s atmosphere called
the H2O rotation band. As shown in the previous slide, virtually
100 % of infrared
radiation longer than 12 micrometers is absorbed with a
combination of CO2 and H2O.
(By the way, the H2O rotation band extends all the way into the
microwave region of
the electromagnetic spectrum, i.e. above a wavelength of 1000
micrometer, which is
why a microwave oven is able to heat up anything that contains
water.)
Molecular Motions and the Greenhouse Gases H2O and CO2
2349cm-1 667cm-1
The second way in which molecules can absorb or emit infrared
radiation is by changing
the amplitude at which they vibrate. Molecules not only rotate,
they also vibrate – their
constituent atoms move toward and away from each other. As
shown in the lower figures,
The molecular structure of water is electrically lopsided; a
molecule is bent to its lowest
energy state. This is because oxygen has two pairs of electrons
hanging off it, which push
the hydrogen toward the other side (Mickey Mouse structure!).
Hydrogen atoms hold their
electrons more loosely than oxygen atoms in chemical bonds, so
each hydrogen has a
4. slightly positive charge. The oxygen end of the molecule has a
slight negative charge. Thus,
water has a dipole moment built into its resting structure.
Rotating an H2O molecule would
oscillate the electric field and generate light. Due to the
complex arrangement of the nuclei
in H2O, there are many modes of vibration for the water
molecule, including a symmetric
stretch and a bend.
The CO2 molecule can vibrate in three ways. The bending mode
of vibration (upper figure).
This vibration has a frequency that allows the molecule to
absorb infrared radiation at a
wavelength of about 15 micrometers, which gives rise to a
strong absorption feature in
Earth’s atmosphere called the 15-micrometer CO2 band. Also,
similar to a H2O molecule,
the oxygen of a CO2 molecule tends to pull on electrons more
tightly than carbon does, but
the oxygen atom on one side pulls the electrons just as tightly
as the other oxygen on the
other side. Therefore, the molecule has no permanent electrical
field asymmetry (dipole
moment). This imbalance makes CO2 an important one for our
climate. In fact, most gases
in the atmosphere do not absorb or emit infrared light at all
(e.g. N2). Why? Because
vibrations in their bonds do not create an imbalance in the
electrical field.
Molecular Motions and the Greenhouse Gases H2O and CO2
2349cm-1 667cm-1
5. What does all of this information mean? Your take home note
is…. in order for gas
molecules to interfere with electromagnetic energy (to emit or
absorb infrared
light);
1) frequency of the molecular vibration must be equal to the
frequency of the
light (only a specific frequency of light can cause a specific
molecular
vibration!), and
2) the molecule must be electronically lopsided.
I am sharing a Youtube video that is very well made and that
allows us to visually
perceive these molecular motions. Please see a following slide.
Youtube video - https://youtu.be/3ojaDMadZXU
Please view this Youtube video to further your understanding of
molecular motion.
Particularly, the part from 2:40 to 4:47 is relevant to this
lecture.
https://youtu.be/3ojaDMadZXU
NASA, Robert Rohde -
http://earthobservatory.nasa.gov/Features/EnergyBalance/page7.
php en:NASA Earth Observatory
6. Atmospheric gases only absorb some wavelengths of energy but
are transparent to
others. The absorption patterns of water vapor (blue peaks) and
carbon dioxide (pink
peaks) overlap in some wavelengths. Water vapor is naturally
electrically lopsided
and can absorb and emit lots of frequencies of infrared light.
Interesting about H2O
is that not only is it a greenhouse gas, when we increase the
surface temperature,
more water will evaporate, which significantly increase the
amount of water vapor in
the atmosphere. Interestingly, this then makes H2O the most
concerning greenhouse
gas with greater uncertainty.
Carbon dioxide is not as strong a greenhouse gas when
compared to water vapor,
but it absorbs energy in wavelengths (12-15 micrometers) that
water vapor does not.
This is an important wavelength range because it is close to the
peak intensity of
outgoing radiation (thus effectively absorbs outgoing energy).
(Illustration NASA, Robert Rohde)
https://cimss.ssec.wisc.edu/sage/meteorology/lesson1/AtmAbsor
btion.htm
Atmospheric Absorption of incoming shortwave and
outgoing longwave radiation
7. Total atmospheric absorption is indicated by the bottom row.
The white areas
indicate regions of the electromagnetic spectrum not affected
(low absorption) by
the atmosphere where solar radiation can reach the Earth's
surface and terrestrial
radiation can escape out to space. Note the prominent role that
water vapor has in
absorbing Earth's long wave radiation.
Outgoing spectrum of the Earth
With an atmosphere
Okay – this is the last figure of today’s lecture.
In this figure, smooth curves show blackbody spectra for
temperatures ranging
from 300 K, surface temperature on a hot summer day, down to
220 K, which is
about the coldest it gets in the atmosphere, up near the
troposphere at about 10-
km altitude. There is also a jagged-looking curve (denoted as
“Atmosphere”)
moving among the smooth ones. This is a model-generated
spectrum of the
infrared light escaping to space at the top of the atmosphere.
This is jagged-
looking because CO2, water vapor, ozone, and methane absorb
specific
8. wavelengths of outgoing energy emitted from the ground.
So, what would the Earth’s surface temperature look like from
space if the Earth
had no atmosphere? – Without an atmosphere, more energy will
be radiated due
to a lack in the greenhouse effect. In fact, the outgoing
spectrum will look like a
blackbody spectrum for 270 K (= -3 C�, 26.6 F), between the
260 K and 280 K
spectra shown in figure. Compare this with the mean surface
temperature
described in slide #12. Blackbody spectra of Earth temperature
is 255 K!
August, 2016
https://eos.org/research-
spotlights/which-greenhouse-gas-does-
the-most-damage-to-crops
Account for the Greenhouse Effect
(one layer atmosphere model)
σTs
4 =
S
4
1− Albedo( )+σTe
4
9. σTs
4 = 2σTe
4
σTe
4 =
S
4
1− Albedo( )
Ts = 2
1
4Te240 Wm-2 coming into surface
240 Wm-2 leaving into space
340 Wm-2 available before accounting for albedo
*Remember S is the solar constant 1365Wm2
Ts is earth surface temp.
Te is temp at the top of the
atmosphere where energy is
radiated back to space
1)
2)
3)
4)
10. Here is our one layer atmosphere model that we reviewed
previous week. Although this
is a great model to help us learn how a climate model works, it
is a little too simple to
represent our true atmosphere.
Can you think about what is unrealistic about this layer model?
Although there are a number of answers, what stands out most
in terms of the
greenhouse effect is that 1) not all atmospheric gases are
greenhouse gases; and 2) the
temperature of the atmosphere is not vertically homogenous.
1) Not all atmospheric gases are greenhouse gases.
This layer model is based upon a simple concept of “what goes
in, must come out”.
With this, in the second equation, the Earth’s back radiation is
completely absorbed by
the atmosphere (greenhouse gases) and radiated equally back to
the surface of Earth
and to space (equation 2, in slide). However, in reality, we all
know that greenhouse
gases are definitely not a major component of the atmosphere!
This week, let’s talk
about what make greenhouse gases – greenhouse gases! After
this week, you should
be able to explain “what are greenhouse gases” from a slightly
different perspective –
in a quantum mechanical way.
2) temperature of the atmosphere is not vertically homogenous.
Of course, when you are away from a heat source (in this case,
the surface of the Earth),
temperature decreases. However, such diffusion cannot be
11. expressed by a simple layer
model. Therefore, climate scientists combine multiple layer
models vertically and
horizontally to make a climate model close to reality.
Composition of the Atmosphere including
variable components (by volume)
As we learned in previous lectures, major composition of the
atmosphere is nitrogen,
oxygen, and argon. Very interestingly, greenhouse gases consist
of only a fraction of
the atmosphere, and are called trace gases.
Radiative forcings, IPCC 2013
That said, although small, these gases are important in altering
the Earth’s energy
budget. Based on the IPCC’s (Intergovernmental Panel on
Climate Change)
assessment report (IPCC 2007), greenhouse gases, such as CO2,
CH4, N2O, and
Halocarbons, show positive radiative forcing. This means that
these gases
contribute to warming of the atmosphere.
12. CO2 carbon dioxide CH4 methane
N2O nitrous oxide
Important to note that, although we are focusing on CO2 to
examine climate
sensitivity here, we all know that there are other molecules that
can absorb long
wave back radiation: water molecules (H2O), methane (CH4),
nitrous oxide (N2O),
etc.
Elements
Atoms
Nucleus
Protons (+)
Neutrons (o)
Electrons (-)
• All matter, including minerals, rocks, and gas
molecules, are made of atoms
The chemical composition
First, let’s review basic chemistry.
Atoms
• Smallest particle into which an element can be divided
13. while still retaining the chemical characteristics of that
element
Here is an example of an oxygen atom. This conceptualized
view is only an
approximation or model showing the nucleus of the atom
surrounded by
orbiting electrons (middle figure). A more realistic view
consists of electron
shells surrounding the nucleus. Electrons are in the probability
clouds (far right
figure). This expression is based on quantum mechanics.
Carbon atom
Electron cloud
Nucleus
Composed of a nucleus surrounded by electrons
Nucleus is composed of protons (+) and neutrons (0)
Carbon atom
Electron cloud
Nucleus
Carbon has 6
electrons…
14. Electron (–)
Proton (+)
Neutron
Number of neutron adds
mass to the atom.
Number of electrons (-)
orbiting nucleus
determined by the
number of positively
charged protons.
Negatively charged
electrons balance the
positive charges of the
protons.
Carbon atom
Electron cloud
Nucleus
Carbon has 6
electrons…
…and a nucleus
of 6 protons …
…and 6 neutrons.
15. Electron (–)
Proton (+)
Neutron
Number of protons
defines the chemical
element and atomic
number (e.g. atomic
number of hydrogen
(H) is 1, He is 2, Li is
3, …)
ION = Charged Particle
CATION = Positive Charge
(lose electrons, i.e., Fe+2)
ANION = Negative Charge
(gain electrons, i.e., O-2)
BONDING
Each atom may or may not be connected to other atoms
with different types of bonding. Here, we learn three
major bondings: ionic bond, covalent bond, and
hydrogen bond.
Sodium atom Chlorine atom
16. Ionic Bond
Here is an example of NaCl, also know as salt.
Sodium loses one electron… …and chlorine acquires it.
Electrical
attraction
Sodium atom Chlorine atom Cation (+) Anion (–)
Ionic Bond
Sodium and chlorine are attracted to each other and create ionic
bonding.
Carbon atoms
are arranged in
regular tetrahedra…
…that share electrons
with neighboring atoms.
Carbon
atoms Electrons
Nucleus
Covalent Bond
Covalent bond is one of the strongest bonds. In this type of
17. bonding, the atoms
share an electron with adjacent atoms, so they are not easily
separable.
Examples of covalent bonds are ozone (O3), hydrogen (H2),
water (H2O), methane
(CH4), ammonia (NH3), and CO2 (carbon dioxide).
The Hydrogen Bond
• Chemistry of water
– Atoms and molecules
– Two hydrogen and one oxygen molecule (H2O)
– Covalent bonds
– Electrical polarity
of water molecule
– Hydrogen bonds
The hydrogen bond is a unique and weak bond. It is the
electrostatic attraction
between two polarized groups of atoms/molecules. One most
famous example
is a water molecule. Although, as we saw in the previous slide
that a water
molecule is a covalent bond, the bonds connecting water
molecules are
hydrogen bonds. This occurs because the molecular structure of
water is
18. unique and naturally polarized (electronically imbalanced) – I
call this
molecular structure a Mickey Mouse structure! Because water
molecules are
polarized, each molecule is attracted electrostatically.
Therefore, water has a
wonderful surface tension. In our childhood, we all tried to put
as many water
drops as possible on a surface of the coin… We are able to do
this because of
the hydrogen bond.
Okay – let’s continue to learn about greenhouse gases in the
following lecture
slides.