With the exception of objects at absolute zero, all...
Transcript of With the exception of objects at absolute zero, all...
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With the exception of objects at absolute zero, all
objects emit electromagnetic radiation (EMR).
Objects also reflect radiation that has been emitted
by other objects.
Electromagnetic energy is generated by several
mechanisms.
Remote sensing imagery is interpreted based on the
interaction of the EMR with the Earth’s objects and
the atmosphere.
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• It is a way to transfer energy through space, which has properties of wave and particle.
• Every object with a temperature higher than0 K (-273.15 oC / -459.67 oF) emits electromagnetic radiation.
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The fusion process: Nuclear reactions where lightweight
chemical elements (like hydrogen) form heavier elements
(such as helium and carbon). This process converts matter
(i.e. mass of an atom) to energy.
Albert Einstein in 1905 showed that: E = mc2
Where, E= Energy
m= mass
c=speed of light in a vacuum (3.0 x 108 m/s)
The Sun produces its energy by two fusion reactions:
1. Proton-Proton (PP) – 88%
2. Carbon-Nitrogen-Oxygen (CNO) – 12%
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• James Clerk Maxwell (1864): Theory of Electromagnetic Radiation
• This radiation is made of the electric and magnetic fields, that travel perpendicular to each other along the wave propagation.
• These waves can be described with wavelength and frequency.
• They vary proportional inverse and are related by the following equation:
𝐟 =𝐜
ℷwhere c = velocity of light (constant)
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0.03 300 400 700
Gamma
Ray
X-Ray UV Visible
106
(1 mm)
Infrared Microwave
(Radar)
Radio
3X108
(30 cm)
Wavelength (nm)
Blue Green Red
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This radiation can be described equally well in terms of waves or
in terms of packets of radiant energy called quanta or photons.
The relationship between these two "forms" of electromagnetic
radiation is:
E = hfWhere,
E = Energy of a photon (joules)
h = Planck's constant (joules * s)
f = frequency (hertz)
1 hertz=cycle/second
Therefore, the energy of a photon is directly proportional to
the frequency but indirectly proportional to the wavelength.
Remember!
= c/f
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What is the energy of a photon with a wavelength of 400 nm?
1. Get wavelength () in meters:
1 nm = 10-9 meters
? meters = 400 nm (10-9 m) = 4 x 10–7 meters
1 nm
2. Get the frequency: f = c
= 3 x 108 m/s = 7.5 x 1014 cycles/second (or Hz)
4 x 10-7 m
3. Get the energy: E = hf
= (6.63 x 10-34 J*s) (7.5 x 1014 /s)
= 4.97 x 10-19 J
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What is the energy of a photon with a wavelength of 500 nm?
1. Get wavelength () in meters:
1 nm = 10-9 meters
? meters = 500 nm (10-9 m) = 5 x 10–7 meters
1 nm
2. Get the frequency: f = c
= 3 x 108 m/s = 6 x 1014 cycles/second (or Hz)
5 x 10-7 m
3. Get the energy: E = hf
= (6.63 x 10-34 J*s) (6 x 1014 /s)
= 3.98 x 10-19 J
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What is the energy of a photon with a wavelength of 700 nm?
1. Get wavelength () in meters:
1 nm = 10-9 meters
? meters = 700 nm (10-9 m) = 7 x 10–7 meters
1 nm
2. Get the frequency: f = c
= 3 x 108 m/s = 4.28 x 1014 cycles/second (or Hz)
7 x 10-7 m
3. Get the energy: E = hf
= (6.63 x 10-34 J*s) (6 x 1014 /s)
= 2.84 x 10-19 J
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At 400 nm
E=4.97 x 10-19 J
At 500 nm
E=3.98 x 10-19 J
At 700 nm
E=2.84 x 10-19 J
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Reflected IR Emitted IR
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•Planck Law: Energy and Frequency
•Kirchhoff Law: Energy, Wavelength, and Temperature
•Stefan-Boltzmann Law: Emitted radiation and temperature
•Wien Displacement Law: Wavelength and temperature
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Planck discovered that electromagnetic energy is absorbed and
emitted in discrete units now called quanta or photons.
The size of each unit is directly proportional to the frequency of the
energy’s radiation.
Q = hυWhere,
Q = Energy of a photon (joules)
h = Planck's constant (joules * s)
υ = frequency (hertz)
1 hertz=cycle/second
His model explains the photoelectric effect, the generation of electric
currents by the exposure of certain substances to light.
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The amount of energy and the wavelengths at
which it is emitted depend upon the
temperature of the object.
The area under each curve may be summed to
compute the total radiant energy exiting each
object. Thus, the Sun produces more radiant
exitance (Me) than the Earth because its
temperature is greater. Me is the ability of a
surface to emit radiation.
As the temperature of an object increases, its
dominant wavelength (λmax ) shifts toward the
shorter wavelengths of the spectrum.
A blackbody is a hypothetical source of
energy. It absorbs all incident radiation and
none is reflected. It emits energy with perfect
efficiency.
Blackbody radiation curves for
several objects including the Sun and
the Earth which approximate 6,000 K
and 300 K blackbodies, respectively.
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This law states that the ratio of emitted radiation to absorbed radiation
flux is the same for all blackbodies at the same temperature.
It forms the basis for the definition of emissivity (ε):
ε = MMb
Where,
M = the emittance of a given object
Mb = the emittance of a blackbody at the same temperature
The emissivity of a true blackbody is 1, and that of a perfect reflector
(a whitebody) would be 0. In nature, all objects have emissivities that
fall between these extremes (graybodies).
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Defines the relationship
between the total emitted
radiation (W) and
temperature (T).
It states that total radiation
emitted from a blackbody
is proportional to the fourth
power of its absolute
temperature.
W = σT4
It states that hot blackbodies emit more energy per unit area
than do cool blackbodies.
where σ is the Stefan-Boltzmann constant, 5.6697 x 10 -8 W m-2 K -4.
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where k is a constant equaling 2898 μm K, and T is the absolute
temperature in kelvin.
Therefore, as the Sun approximates a 6000 K blackbody, its
dominant wavelength (λmax ) is:
T
kλ
mK
Km
483.0
6000
2898
This law specifies the relationship between the wavelength of
radiation emitted and the temperature of a blackbody.
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Compare with Figure 2.5
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VeryImp.
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Atmospheric Dust
Smoke
Atmospheric
Molecules
Large Water
Droplets
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Itotal = IS + IO + ID
Total = Ground + Atmosphere + Diffuse
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Most remote sensors for land studies havebands in the Visible, IR, and Microwaves.
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Polarization
Reflection
Transmission Fluorescence
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https://youtu.be/cfXzwh3KadE
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1. Read Chapter 2 and answer the
review questions 4, 8, and 9
(at the end of the chapter).
2. Read Chapters 3 and 4.