EX1-1 Flashcards
Active remote sensing
An active sensor system provides its own energy source. As an example, a radar sensor sends out radio waves and records the reflection waves coming back from the surface.
Radar; Lidar
Passive remote sensing
Passive systems are much more common than active systems
• A passive sensor system needs an external
energy source. In most cases this source is
the sun.
• These sensors generally detect reflected
and emitted energy wave lengths from a
phenomenon
Optical; air photos; multispectral; hyperspectral
Spatial Resolution
It is the size of the smallest area that can be separately recorded as an entity on the image.
Spatial resolution depends on:
Property of sensor (e.g. Focal length of camera)
Altitude of sensor (e.g. platform height and stability)
Temporal Resolution
minimum time period between two images exact same area same viewing angle same platforms using the same instruments comparable conditions
weather satellites have high temporal but low spatial resolution.
Spectral Resolution
observed spectral differences in the energy (wavelength) reflected or emitted from features of interest.
the ability of a sensor to detect small differences in wavelength. The narrower the wavelength range, the finer the spectral resolution.
Radiometric Resolution
sensitivity of the sensor to incoming radiance or the differences in the brightness of objects.
(How much change in radiance is required to result in a change in recorded brightness value?)
Electromagnetic Radiation (principal spectrums and those that are useful for remote sensing)
Panchromatic – 1 Band (B&W)
Color – 3 Bands (RGB)
Multispectral – 4+ Bands (RGBNIR)
Hyperspectral – 100s of Bands
Limits of the visible spectrum are defined by the sensitivity of the human visual system. It can be divided into 3 segments (“additive primaries”) – B, G and R
Very large spectrum; Categorized into NIR, MIR and Far IR (also known as thermal IR). Along with visible spectrum, NIR and MIR form the “reflective spectrum” (i.e., they are essentially solar radiation reflected from the Earth’s surface). Far IR / thermal IR is radiation emitted by the Earth.
Relationship between frequency, wavelength, energy and speed of light
speed of light - c
Frequency - ν
Wavelength – λ
c = λ ν
Frequency and wavelength are inversely proportional
Emissivity
ratio between the emittance of a given object and that of a blackbody at the same temperature
•Emissivity ranges from 0-1 and describes an object’s
ability to behave like a black body
Blackbody
A blackbody radiator is a hypothetical body
that absorbs and re-radiates all energy
incident upon it with no change in energy
A blackbody emits energy with perfect
efficiency
Whitebody
A whitebody is a hypothetical body that
reflects all energy incident upon it with no
absorption or re-radiation of energy.
Graybody
Many bodies have a constant emissivity regarding the wave length, but do emit far less radiation than black bodies. They are called grey bodies.
Selective radiator
Bodies whos emissivity depends on the temperature and the wave length, such as metals, are called selective radiator.
Kirchoff’s Law (understanding of law and its implications for remote sensing)
DEFINES BLACKBODIES:
Ratio of emitted radiation/absorbed radiation
is the same for all blackbodies at the
same temperature.
This law forms the basis for the definition of emissivity.
The emissivity of an object varies at different wavelengths. efficiency of absorption and emission of radiation are material properties.
Stefan – Boltzmann Law (understanding of law, the formula and its implications for remote sensing)
This law defines the relationship
between the total emitted radiation (W)
(often expressed in watts per unit area)
and temperature
Stefan - Boltzmann Law: Total emission radiated from a blackbody is proportional to the fourth power of its absolute temperature (T): W = σT4,
where: W is the total emission radiatied
T is the absolute temperature in (K)
σ is the Stefan – Boltzmann constant
(5.6697 X 10-8)
Hot blackbodies emit more
energy per unit area than do cool
blackbodies
Wien’s Displacement Law (understanding of law, the formula and its implications for remote sensing)
Wien’s Law: The wavelength of max radiation is a function of an object’s temperature (T): λ max = 2898 mm / T, where: λ max is the wavelength at which radiance is at a maximum T is the absolute temperature in (K) This law specifies the relationship between the wavelength of radiation emitted and the temperature of a blackbody As blackbodies become hotter, the wavelength of maximum emittance shifts to shorter wavelengths
Reflectance and emittance of electromagnetic radiation
-
Atmospheric interactions of EMR – transmission, scattering, absorption
Scattered (i.e. reflected or refracted by atmospheric particles) before it reaches the
Earth’s surface
• Absorbed by atmospheric particles before it reaches Earth’s surface
• Transmitted to the earth’s surface, where it is either reflected, transmitted or
absorbed
• Absorbed by an object on the Earth’s surface, and then emitted by that object
transmission (Atmospheric)
• Transmission is what we want the atmosphere to do when we are studying
the earth itself.
• Desirable, but even under the best of conditions, 100% transmission does
not occur
• This is because some radiation is scattered, absorbed or reflected by
atmospheric gases
scattering (Atmospheric)
- Scattering is the redirection of radiation by particles suspendedin the atmosphere or by large molecules of atmospheric gases.
The mount of scattering depends on:
Size of atmospheric particles (from molecules of gases to dust particles to larger ice and water droplets)
The wavelength of radiation
absorption (Atmospheric)
Absorption occurs when the atmosphere prevents, or strongly attenuates, transmission of radiation through the atmosphere. Characteristics of absorption: Energy absorbed by the atmosphere is subsequently reradiated / emitted at longer wavelengths Different gases absorb well at different λ O3 absorbs …… CO2 absorbs……. WV absorbs …….(role of WV varies greatly with time and location)
3 kinds of scattering
Rayleigh, Mie, and Non-selective
Rayleigh scattering
Occurs when λ (shorter) > particle size;
Occurs primarily due to molecules of atmospheric gases;
Scattering inversely proportional to fourth power of λ
A perfectly clean atmosphere, consisting only of atmospheric gases, causes
scattering such that the amount of scattering increases greatly as λ becomes
shorter
Violet light scattered 16X Red light; Blue light scattered 4X Red light