2 Electromagnetic Energy Flashcards
Basic requirement for Remote Sensing
Source of energy in the form of EM radiation
EM radiation emitted by the source (usually the sun) -> propagates through a material/vacuum -> Interacts with the Earth’s atmosphere -> interacts with the Earth’s surface -> Interacts with the Earth’s atmosphere again -> Reaches the sensor and being recorded by the detectors
EM radiation
a form of energy and has wave-like and particle-like properties.
can be modeled by Classic physics and modern quantum theory
– Classical physics (Electromagnetic wave theory)
• The flow of energy through a medium in the form of electric and magnetic fields
– Modern quantum theory (Planck’s quantum theory)
• Flow of photons, as small particles, at the speed of light through space
EM waves
- EM waves are created by the vibration of electric charges.
- EM waves are in the form of mutually linked electric (E) and magnetic (M) fields.
- Electric and magnetic fields change in magnitude in a direction perpendicular to the traveling direction of the radiation.
- The magnetic field is oriented at right angles to the electrical field.
Important characteristics of EM waves
# Frequency (f) • How often a wave passes a given point per second • Measured in hertz (Hz) or its factors such as MHz (106 Hz) or GHz (109 Hz). • 1 cycle per second = 1 Hz
Wavelength (lamda)
• The length of one cycle (distance between successive crests or troughs)
• Usually measured in m or its factors such as nm (10-9 m), μm (10-6metres) or cm (10-2 meters)
# Speed (c) • In vacuum, EM waves travel at the speed of light (c)
*note: lamda= c/f. Frequency and wavelength are inversely proportional
Planck’s quantum theory
- Planck’s quantum theory models some aspects that could not be rationalized by EM wave theory.
- Electromagnetic radiation exists in discrete quanta of energy, called photons.
- Photons are packets of energy that travel at the speed of light.
- Energy carried by a single photon is proportional to its frequency and inversely proportional to its wavelength
E = hf = hc/lamda where E = enrgy h = Planck's constant = 6.26 x 10^-34 f = wave frequency lamda = wavelength c = speed of light = 3 x 10^8 m/s
• EM radiation with shorter wavelength have higher level of quantum energy
– Gamma- and X-ray and Ultraviolet are dangerous to human body.
– longer wavelength (lower energy) like Microwaves or radio waves are not dangerous.
• Implication to remote sensing
– It is more difficult to detect the radiant energy at longer wavelength than shorter wavelength
Spectral density of EM radiation (1/3)
• Planck’s law describes the spectral density of EM radiation emitted by a black body
• A black body
– Absorbs all incident radiations
– Emits black body radiation at all frequencies
Spectral density of EM radiation (2/3)
• Planck’s law describes the electromagnetic radiation a black body emits at a certain wavelength as a function of its temperature
• Kelvin and Celsius have the same magnitude
– 1 K = 1 °C
– [K] = [°C] + 273.15
Spectral density of EM radiation (3/3)
• Materials at different temperature emit different magnitudes of EM radiations
• The sun
– Temperature of 5778 K
– Mostly emits in visible, infrared, and UV
• Our planet
– Average temperature of 288 K
– Emits mostly infrared radiation
Total EM radiation
• Stefan-Boltzmann’s law describes the total electromagnetic radiation emitted across all wavelengths by a black body
M=§T^4 where M = total radiant exitance [Wm^2] T = absolute temperature [K] § = Stefan-Boltzman constant [5.67 x 10^-8 W m^-2 K^-4]
• The total energy is directly proportional to the fourth power of the temperature
Maximum Spectral radiation
# The Wien's displacement law lamda max = A/T where lamda max = wavelength of maximum spectral radiant exitance [miu m] A = Wien's constant [2897.8 mium.K] T = absolute temperature [K]
– Increasing temperature maximum radiation shifts towards shorter wavelengths
– The temperature of the Sun is 5778 K corresponding to a peak emission at 502 nm
the implication of maximum spectral radiation in RS
– To measure human body at average temperature of 310 kelvin and a peak at 10 μm, we need a sensor at the range of 7-14 μm
– To measure earth surface at average temperature of 300 k, we should look at 8-14 μm
– To measure forest fire at 800 k we should look at 3-5 μm.
Radiation of gray body
- Real world materials are not ideal black bodies
- Gray bodies emit only a fraction of radiation emitted by black body.
- Effectiveness of an object in emitting EM radiation is defined by Emissivity
Emisivity= radiant exitance of an object at a given temp / radiant exitance of a blackbody at the same temp
–Emissivity values can range from 0 to 1 (dimensionless)
– A black body has an emissivity of 1
– A white body has an emissivity of 0
– A gray body has an emissivity between 0 and 1
Selective Radiators
• For many materials, the emissivity depends on the wavelength
– Such material is called selective radiator
- Most natural objects are selective radiators
- Emissivity depends on surface TEMPERATURE; WAVELENGTH; PHYSICAL PROPERTIES of the surface
- Objects with the same Temperature can have significantly different radiations.
Interaction between EM radiation and materials
# Absorption # Transmission # Reflection # Scattering
Interaction of EM energy with the atmosphere
1. ABSORPTION
- Transmission
- Scattering
- Reflection
– Some parts of EM radiation are absorbed by different gasses in the atmosphere
– Oxygen (O2), Ozone (O3), water vapor (H2O), and carbon dioxide (CO2) are the major absorbers.