Chapter 2 Flashcards
ω λ wavelength f/v frequency μm micrometer τ transmissivity ξ absorptivity θ theta
EMR defined
- Form of energy transport in free space
* wave travel through space at speed of light
Maxwell equations
Esubx = Eomega cos (wt-kz)
Eomega = max electrical energy ω= angular freq (2 piv)
Electric and magnetic fields are ________ to each other
Orthagonal (perpendicular?)
Radiant energy (Q of a photon) is proportional to frequency
Q=hv
Q=radiant energy (J)
v=frequency
h=Plank’s constant (6.626 X 10^-34 Js
substituteQ=hc/wavelength
h is small number, so approx Q~ 1/wavelength
Radiation from the Sun is ________________ (re polarization)
un-polarized
Man-made sources (laser, radar) have ___________ radiation (re polarization)
polarized
Electromagnetic spectrum for remote sensing
UV, visible, near-ir, mid-ir, thermal, microwave bands (Ka, Ku, X, C, S, L, P)–LOOK AT GRAPH FROM LECTURE
shorthand ranges for RGB spectra
blue .4-.5 μm
green .5-.6 μm
red .6-.7 μm
Polarization
The orientation of the electric field
Vertical polarization: electric vector is PERPENDICULAR to the plane of incidence
Horizontal polarization: electric vector is PARALLEL to the plane of incidence
Sun=unpolarized
Man-made sources (laser, radar) have polarized radiation
Infrared
near and mid=reflective =short wave
far=emissive radiative thermal
Microwaves
letters come from military, don’t want enemy to know signal
The bulk of sun’s radient energy distribution is
visible (43.5%) and near infrared (36.8%). Also significant amts of near UV (5.32%) and Mid IR (12%)
Blackbody concept
Object that absorbs and emits 100% of radiation
Does not exist in nature
Emissivity would equal 1
Assumptions:
- Isotropic
- homegeneous
- unpolarized
2 objects with same temp would emit same E
Blackbody would emit more E than a comparable gray body (which has Emissivity is < 1)
MOST IMPORT. CONCEPT
Graybody
Object that reflects part of the incident radiant
Emissivity is < 1
M=emissivitysigma constantTemp4 (double check this)
Emissivity
the relative ability of a surface to emit radiation
- describes ACTUAL absorption and emission properties of real objects (gray bodies)
- Is wavelength dependent (usually use avg)
- Is equal to (graybody emittance)/(blackbody emittance)–of same temp
- Use it to calculate an object’s radiant temp, or brightness temp
The temp at which a blackbody would have to be to emit the same energy as emitted a graybody at some physical temp
T(rad) = e^(1/4)T(kin) e= [(T(rad) / T(kin)] ^4
kin=kinematic physical
Selective radiator
emits certain types of EMR (better)
Two objects can have the same ___________ temp but different _________ temperatures…Why?
kinematic, radiant
Because they have different emissitivities
Understand why mirror has no emissivity
gah
Planck’s law (Spectral radiance)
‘All bodies who temp are above absolute zero K (-273.2), emit radiation”
Heat transformed into radiant energy
(need formula)
L = amount of E per unit serface per unit time, per solid angle emitted at the wavelength λ
Maximum radiation of sun at what wavelength?
6000K (Kelvin) at ~.5 micrometer
Stefan-Bolzmann law (TIR)
The total emitted energy over the whole spectrum is proportional to the physical temperature.
The amount of energy emitted by an object such as the Sun or Earth is a function of its temperature. ^temp=^emitted energy
Wien’s law
That wavelength of peak emittance (max wavelength) is inversely proportional to an object’s kinematic temperature (derivative of Planck’s law)
λmax = a/T
a=2898 μm K
e.g. hotter the object, the shorter wavelength of maximum intensity
False color
Different channels represented with color not true to visible light. May more clearly delineate areas
Solid angle
imagine as angle with three dimensions (cone)