| The
GPM Microwave Imager (GMI) will now include four high frequency
channels that will be used to measure precipitation in the form
of falling snow and light rain. GMI, which will fly on the GPM Core
Spacecraft, is being built by Ball Aerospace and Technologies Corporation.
Due to great interest shown by the science community in the observations
these high frequency channels will enable, NASA Headquarters elected
to include the channels on GMI through a contract modification.
The new high frequency channels—known as channels 10-13—will
augment the original nine baseline channels on GMI. Channels 10
and 11 will be centered around 165.5 GHz, with a bandwidth of 3
GHz. Channel 10 will be vertically polarized and channel 11 horizontally
polarized. Channels 12 and 13 will be vertically polarized and centered
about the water vapor absorption line at 183.31 GHz. Channel 12
will receive energy on wings offset by 3.0 GHz on both sides of
the central frequency. Similarly, channel 13 will receive energy
on wings separated by 9.0 GHz from the central frequency. The bandwidths
of channels 12 and 13 are 7.0 GHz and 9.0 GHz respectively.
NASA selected 183.31 GHz as the central frequency for channels
12 and 13 specifically because the atmosphere is opaque at this
frequency. Observing at frequencies surrounding an atmospheric gas
resonance (in this case, the water vapor resonance) is often termed
"sounding," which implies probing to different depths
in the atmosphere. Furthermore, the frequencies surrounding 183.31
GHz are inherently sensitive to the ice particles in clouds because
ice particle sizes are on the order of the central channel wavelength
(about 0.16 cm). In addition, at these high frequencies, certain
radiative properties (such as scattering) differ for liquid and
solid water particles, making it easier to conclusively detect cloud-borne
ice. This ability to resolve ice particles in clouds will allow
scientists to obtain more accurate estimates of light rain and falling
snow.
GMI channels 10-13 will work in conjunction with channels 8 and
9 (which are centered at 89.0 GHz) for the retrieval of snow. For
this reason, channels 10-13 have the same spatial resolution as
channels 8 and 9 (i.e., all four channels have "instantaneous
fields of view" of approximately 4 km by 7 km and identical
sampling intervals).
Although instruments observing in these high frequencies have flown
on spacecraft before, this will be the first time an instrument
employing these frequencies has been designed to detect falling
snow and light rain from space. Remote measurements of these types
of precipitation are typically difficult to make because it is challenging
to discriminate between ground features and falling precipitation,
especially in places where the Earth’s surface and temperature
are not very uniform, as is the case over land. The opaque nature
of the 183.31 GHz channels will allow the surface features to be
screened, resulting in more accurate precipitation values.
To assist in resolving GPM's snow and light rain measurements,
scientists will utilize observations made by the Dual-frequency
Precipitation Radar (DPR), also carried on the GPM Core Spacecraft.
DPR will operate at both 13.6 GHz (Ku-band) and 35.55 GHz (Ka-band).
The higher frequency Ka-band radar will provide good sensitivity
to snow and light rain, furnishing a critical reference for GMI's
high frequency channel observations. The science community is excited
about GPM's unique combination of radar and high frequency channel
measurements because it will mark the first time this measurement
complement is used to quantify light rain and snow. Other spaceborne
radiometers carry high frequency channels, but none carry a radar
instrument as well.
For further information on GMI, contact Steve Bidwell/GPM
Instrument System Engineer (Steven.W.Bidwell@nasa.gov).
Back to top
|