Aerial sampler system

Communications: electrical – Condition responsive indicating system – Specific condition

Reexamination Certificate

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Details

C340S962000, C340S966000, C340S968000, C073S861070

Reexamination Certificate

active

06809648

ABSTRACT:

RELATED APPLICATIONS
Not applicable
FEDERALLY SPONSORED RESEARCH OR DEVELOPMENT
This invention was made with Government support under Contract number #DTFA01-97-C-00006 awarded by the Federal Aviation Administration. The Government has certain rights in this invention.
MICROFICHE APPENDIX
Not applicable
BACKGROUND OF THE INVENTION
1. Field of the Invention
The invention is related to the field of aviation and weather related applications, and in particular, to apparatuses and methods for an aerial sampler system.
2. Description of the Prior Art
Aircraft have typically used two fundamental types of air samplers. The first type is called a total air temperature (TAT) probe that obtains total (dynamic) air temperature and static (ambient) air temperature. This TAT probe extends from the aircraft skin about 3 inches, which is away from the friction-heated boundary layer of air next to the aircraft's metal surface. The TAT probe measures the dynamic (total) temperature and obtains the static temperature through the equation:
T
T
=T
S
(1+0.2
M
2
)
where T
T
is the total temperature;
T
S
is the static temperature; and
M is the Mach number which is the fractional speed of the aircraft relative to the speed of sound.
The TAT probe includes a probe heater, which is an FAA requirement due to icing concerns. One problem is the heater tends to fail, which is the highest failure mode of the probes.
The second type of probe is called a pitot tube and is used to measure differential pressure (total minus static) for subsequent calculation of aircraft velocity through Bernoulli's equation:
V
2
=2(
P
T
−P
S
)/&rgr;
where V is velocity;
P
T
is total pressure;
P
S
is static pressure; and
&rgr; is the density of air, which is a function of atmospheric pressure and temperature.
These two probes work together to provide the information needed for efficient flight. Both types of probes have the common feature of extending away from the airframe to avoid contaminated measurements induced by boundary layer effects near the aircraft's skin. One problem with these two probes is the frictional drag from the extension of both probe from the aircraft's skin. The TAT probe has a frictional drag that is an effective 2.5 lbs. Over time, the cost of additional fuel for such additional weight ranges from $1-$2 per pound per week per aircraft. Another problem arises when the probes are applied to stealth aircrafts. Both of the probes increase the radar cross section, which increases the radar visibility of the aircraft.
Another important measurement for aircraft is water vapor. Water vapor affects virtually all aspects of aviation weather and thus, the safety, efficiency, and capacity of an airspace system. For example, summertime convection is behind most traffic delays. Weather prediction in general, but especially precipitation and severe storm prediction, are crucially dependent upon accurate water vapor profiles in the lower troposphere. The commercial aircraft real-time ascent and descent reports can provide profiles of winds, temperature, and water vapor.
One prior system has used the TAT probe in combination with a water vapor sensing system.
FIG. 1
depicts a prior system with the TAT probe and a water vapor sensing system in the prior art. The prior system includes a standard TAT probe to measure total air temperature and static air temperature from the air flow. The water vapor sensing system includes a diode laser to measure the water vapor. This prior system was tested in a prototype mode but never built as a commercial product because of the limited space available within the TAT probe. This forced the use of fiber optic cables to carry the laser light and these induced optical “fringes” that reduced sensitivity of the diode laser measurement technique.
Another prior system uses an “open path” for diode lasers to measure water vapor. The laser transmitter and receiver are external to the aircraft. However, this prior system has accuracy and solar interference problems in addition to the drag concerns.
SUMMARY OF THE INVENTION
The inventions solve the above problems by using an aerial sampler system. The aerial sampler system includes an enclosure, a transfer system, and a measurement system. The enclosure is connected to an external surface of an aerial vehicle and receives atmospheric flow from the external surface of the aerial vehicle. The enclosure also directs at least some of the atmospheric flow into an aperture in the external surface. The transfer system transfers some of the atmospheric flow from the aperture to a measurement system. The measurement system is internal to the external surface of the aerial vehicle and measures atmospheric trace gases in the atmospheric flow.
In some embodiments, the measurement system measures water vapor in the atmospheric flow. In some embodiments, the measurement system includes a laser transmitter, a receiver, and a processing system that determines water vapor based on the received laser signals. In some embodiments, the laser transmitter is a diode laser transmitter. In other embodiments, the laser transmitter is a quantum cascade laser transmitter. In some embodiments, the measurement system includes a temperature sensor and a pressure sensor. In some embodiments, the enclosure includes an inertial separator that converges and diverges the atmospheric flow. In some embodiments, the enclosure includes a pressure sensor that determines pressure for ice detection. In some embodiments, the enclosure includes electrically heated metal that removes ice.


REFERENCES:
patent: 2970475 (1961-02-01), Werner
patent: 5302026 (1994-04-01), Phillips
patent: 5544526 (1996-08-01), Baltins et al.
patent: 5653538 (1997-08-01), Phillips
patent: 5731507 (1998-03-01), Hagen et al.
patent: 6070475 (2000-06-01), Muehlhauser et al.
patent: 6076963 (2000-06-01), Menzies et al.
patent: 6250149 (2001-06-01), Black
patent: 6269320 (2001-07-01), Otto
patent: 6609825 (2003-08-01), Ice et al.
patent: 6672152 (2004-01-01), Rouse et al.

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