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Radar Polarization (Harrisburg, PA)

Radar image tones may also vary in another systematic and controllable way. When a pulse of photon energy is sent from the transmitter, its electrical field vector can be made to vibrate in either a horizontal (H) or a vertical (V) direction depending on antenna design. Most reflected pulses are parallel-polarized, i.e., return with the same direction of electric field vibration as the transmitted pulse. Thus, either a HH or VV polarization pairing of the transmitted and returned signals will ensue. However, upon striking the target, the pulses can undergo depolarization to some extent so that reflections with different directions of vibration may be returned. A second antenna will pick up cross-polarization that is orthogonal to the transmitted direction, leading to either a VH or HV mode (first letter refers to transmitted signal). Some ground features appear about the same in either parallel or cross-polarized images. But, vegetation, in particular, tends to show different degrees of image brightness in HV or VH modes, owing to depolarization by multiple reflecting branches and leaves. Compare the HV image of Harrisburg shown below with the previous image of that area, obtained simultaneouly in the HH mode.

Other factors contribute to the brightness or intensity of the returned signal. Two properties of materials provide clues about composition and surface state by the manner in which these attributes interact with the incoming pulses. One is the dielectric constant (Symbol is the small Greek letter k, a dimensionless number determined as the ratio of the capacitance of a material to that of a vacuum [set at 1.00]; this is an electrical property that relates to a material's capability [capacity] to hold a charge), which is a measure of the degree of polarizability of a material subjected to an applied electric field. Radar waves penetrate deeper into materials with low dielectric constants and reflect more efficiently from those with high constants. Values for k range from 3 to 16 for most dry rocks and soils up to 80 for water with impurities. Moist soils have values typically between 30 and 60. Thus, variation in intensities of reflected pulses may, other factors being held constant, indicate differences in soil moisture. Variations among rocks is generally too small to distinguish most types by this property alone.

Second, surfaces representing various kinds of materials differ from one another in their natural or cultivated state of roughness. Roughness, in this sense, refers to irregularities of dimensions that relate either to textures of the surfaces or of objects on them (such as close-spaced vegetation which may assume a variety of shapes). Examples include the surficial character of pitted materials, granular soils, gravel, grass blades, and other covering objects whose surfaces have dimensional variability of the order of millimeters to centimenters. The height of an irregularity, together with radar wavelength and grazing angle at point of contact, determines the behavior of a surface as smooth (specular reflector), intermediate, or rough (diffuse reflector). A surface with an irregularity height averaging 0.5 cm will respond to K band ( = 0.85 cm), X band ( = 3 cm), and L band ( = 25 cm) radar waves in the reflection sequence of smooth, intermediate, and rough respectively. Other average heights produce different responses, from combinations of "all smooth" to "all rough" for the several bands used. This opens the possibility of a radar broadcasting three bands simultaneously in a quasi-multispectral mode, from which color composites can be produced by assigning a color to each band (see below). Patterns of relative intensities (as gray levels) for images made from different bands may serve as diagnostic tonal signatures for diverse materials whose surfaces show contrasted roughness.

Radar Penetration

The particular radar wavelength also influences penetrability below target tops to ground surfaces. Depth of penetration increases with : L and P band radar penetrates deeper than K or X bands. Shorter wavelengths, such as C-band, reflect largely from forest canopy tops. At longer wavelengths, tree leaves are too small to have much influence on backscatter, although branches will interact, so that canopies are penetrated to varying degrees. The image below, acquired by the SAR on the SIR-C spacecraft, shows how L-band radar has penetrated through the dense, continuous tropical vegetation cover of the Amazon Basin in Brazil to image the gently rolling terrain beneath.

Signals for all common radar bands pass through the fine droplets of moisture making up clouds, so that this condensation is effectively transparent or invisible to the beam. However, large ice crystals or raindrops do backscatter K band radiation. Weather radar relies on this band interval to "picture" clouds and determine their movement using the Doppler effect (frequencies will shift depending on motion toward or away from the receiver).


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Code 935, Goddard Space Flight Center, NASA
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