Abstract:
A sensor system includes an enclosure mounted externally on an aerial vehicle and a sensor chamber mounted internally within the aerial vehicle. The enclosure receives and converges air particles to cause inertial separation that transfers a first portion of the air particles to a first air transfer path and that causes a second portion of the air particles to bypass the first air transfer path. The first air transfer path transfers the first portion of the air particles from the enclosure to the sensor chamber. The sensor chamber includes at least one sensor that produces sensor data for the first portion of the air particles. A second air transfer path transfers the first portion of the air particles from the sampling chamber to the enclosure. The enclosure transfers the first portion of the air particles and the second portion of the air particles to the atmosphere.

Description:
RELATED APPLICATIONS  
       [0001]     This patent application is a continuation of patent application Ser. No. 10/304,577; that is entitled “An Aerial Sampler System”; that was filed on Nov. 26, 2002; and that is hereby incorporated by reference into this patent application. 
     
    
     FEDERALLY SPONSORED RESEARCH OR DEVELOPMENT  
       [[0002]]     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  
       [0003]     Not applicable  
       BACKGROUND OF THE INVENTION  
       [0004]     1. Field of the Invention  
         [0005]     The invention is related to the fields of aviation and sensors, and in particular, to sensor systems for aerial vehicles.  
         [0006]     2. Description of the Prior Art  
         [0007]     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&#39;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.        
 
         [0011]     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.  
         [0012]     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&#39;s equation: 
 
 V   2 =2( P   T   −P   S )/ρ
 
 where V is velocity; 
        P T  is total pressure;     P S  is static pressure; and     ρ is the density of air, which is a function of atmospheric pressure and temperature.        
 
         [0017]     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&#39;s skin. One problem with these two probes is the frictional drag from the extension of both probe from the aircraft&#39;s skin. The TAT probe has a frictional drag that is an effective 2.5 Ibs. 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.  
         [0018]     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.  
         [0019]     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.  
         [0020]     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  
       [0021]     Examples of the invention include a sensor system and its method of operation. The sensor system includes an enclosure mounted externally on an aerial vehicle and a sensor chamber mounted internally within the aerial vehicle. The enclosure receives and converges air particles to cause inertial separation that transfers a first portion of the air particles to a first air transfer path and that causes a second portion of the air particles to bypass the first air transfer path. The first air transfer path transfers the first portion of the air particles from the enclosure to the sensor chamber. The sensor chamber includes at least one sensor that produces sensor data for the first portion of the air particles. A second air transfer path transfers the first portion of the air particles from the sampling chamber to the enclosure. The enclosure transfers the first portion of the air particles and the second portion of the air particles to the atmosphere. 
     
    
     BRIEF DESCRIPTION OF THE DRAWINGS  
       [0022]     The same reference number represents the same element on all drawings.  
         [0023]      FIG. 1  is an illustration of a prior system with a total air temperature probe and a water vapor sensing system in the prior art.  
         [0024]      FIG. 2  is an illustration of an aerial sampler system in an example of the invention.  
         [0025]      FIG. 3  is a flow chart of an aerial sampler system in an example of the invention.  
         [0026]      FIG. 4  is an illustration of a top view of an enclosure in the Fleming Sampler (FS) system in an example of the invention.  
         [0027]      FIG. 5  is an illustration of a cross section view of an enclosure in the FS system in an example of the invention.  
         [0028]      FIG. 6  is an illustration of a side view of the FS system in an example of the invention.  
         [0029]      FIG. 7  is an illustration of a detailed side view of the rib of the enclosure, an incoming coupling pipe, and an outgoing coupling pipe in an example of the invention.  
         [0030]      FIG. 8  is an illustration of a cylindrical sampling tube in an example of the invention. 
     
    
     DETAILED DESCRIPTION OF THE PREFERRED EMBODIMENT  
       [0031]      FIGS. 2-8  and the following description depict specific examples to teach those skilled in the art how to make and use the best mode of the invention. For the purpose of teaching inventive principles, some conventional aspects have been simplified or omitted. Those skilled in the art will appreciate variations from these examples that fall within the scope of the invention. Those skilled in the art will appreciate that the features described below can be combined in various ways to form multiple variations of the invention. As a result, the invention is not limited to the specific examples described below, but only by the claims and their equivalents.  
         [heading-0032]     Aerial Sampler System— FIGS. 2-3   
         [0033]      FIG. 2  depicts an aerial sampler system  200  in an example of the invention. The aerial sampler system  200  includes an enclosure  220 , an external surface  230  of an aerial vehicle, a transfer system  240 , and a measurement system  250 . The enclosure  220  is located on the external surface  230  of the aerial vehicle. The external surface  230  has an aperture  260 . At the aperture  260 , the transfer system  240  is connected to the enclosure  220  and the external surface  230  to allow atmospheric flow  210  to enter the transfer system  240 . The transfer system  240  is also connected to the measurement system  250 .  
         [0034]     The atmospheric flow  210  is any flow of trace gases and/or particles that are in a planetary atmosphere. The atmospheric flow  210  typically contains water vapor, which is a trace gas and can vary from 3 to over 40,000 parts per million by volume (ppmv). In one example of the earth&#39;s atmosphere, the atmospheric flow contains nitrogen and oxygen gas, water vapor, other trace gases, and particles including aerosols, possible liquid water droplets, and ice crystals. The external surface  230  of an aerial vehicle is the outer layer of an aerial vehicle. In one example, the external surface  230  is the “skin” of a commercial jet aircraft. An aerial vehicle is any object that flies. Some example of aerial vehicles are commercial and military jet aircraft, special purpose manned aircraft, and unmanned aerial vehicles (UAVs).  
         [0035]     An enclosure  220  is any configuration of materials that is configured to receive the atmospheric flow  210  from an external surface  230  of an aerial vehicle and direct at least some of the atmospheric flow  210  into an aperture  260  in the external surface  230 . One embodiment of the enclosure  220  forms a rib that is shown in  FIGS. 4, 5 ,  6 , and  7 , which are described below. The transfer system  240  is any device, group of devices, or material that is configured to transfer some of the atmospheric flow  210  from the aperture  260  of an external surface of an aerial vehicle to a measurement system  250 . One example of the transfer system  240  is a coupling pipe, which is described below in  FIG. 6, 7 , and  8 .  
         [0036]     The measurement system  250  is any device, group of devices, or material configured to measure atmospheric trace gases of the atmospheric flow and is internal to an external surface of an aerial vehicle. One example of the measurement system  250  is a cylindrical sampling tube which is shown in  FIGS. 6 and 8 , which are described below. An example of measuring atmospheric water vapor is described below.  
         [0037]      FIG. 3  depicts a flow chart of the aerial sampler system  200  in an example of the invention.  FIG. 3  begins in step  300 . In step  302 , the enclosure  220  receives the atmospheric flow  210  from the external surface  230  of an aerial vehicle. In step  304 , the enclosure  220  directs some of the atmospheric flow  210  into the aperture  260  in the external surface  230 . In step  306 , the transfer system  240  transfers some of the atmospheric flow  210  from the aperture  260  to the measurement system  250  that is internal to the external surface  230  of the aerial vehicle. In step  308 , the measurement system  250  measures the atmospheric trace gases of the atmospheric flow  210 .  FIG. 3  ends in step  310 .  
         [0038]     The aerial sampler system  200  advantageously measures atmospheric flow from the skin of the aerial vehicle. The aerial sampler system  200  has minimal frictional drag as compared with the TAT probe and the pitot probe. Also, the aerial sampler system  200  does not include any heater as in the TAT probe, which reduces cost, weight, energy consumed, and maintenance for failures. Further advantages for other embodiments are discussed below.  
         [heading-0039]     Fleming Sampler System— FIGS. 4-8   
         [0040]      FIG. 4  depicts a top view of an enclosure in a Fleming Sampler (FS) system  400  in an example of the invention. The FS system  400  includes an enclosure  410  that forms a rib  420  on the bottom side of the enclosure. Typically, the rib  420  is not seen from the top view but is shown in  FIG. 4  to show the placement of the rib  420  within the enclosure  410 . In this embodiment, the enclosure  410  is attached on top of an external plate that has a diameter of approximately 9 cm and the external plate is not shown in  FIG. 4 . In this embodiment, the enclosure  410  and the external plate are circular. In other embodiments, the enclosure  410  and the external plate could have another shape. The external plate is a metal doubler plate of standard thickness conventionally attached to an airframe. The external plate has two 0.635 cm holes [¼ inch] leading to the interior of the aircraft. The rib  420  has a width of 6.35 mm and a length of approximately 9 cm. The rib  420  extends from left to right across the center of the external plate. In this example, the aircraft is assumed to be moving from right to left. Thus, the air is entering the left side of the rib  420  and exiting the right side or tail of the rib  420 . The direction of the air is shown by the arrow  430 .  
         [0041]      FIG. 5  depicts a cross section view of the enclosure  410  of the FS system  400  in an example of the invention.  FIG. 5  depicts the rib  420  located within the enclosure  410 , which is attached on top of the external plate  510 . In this embodiment, the diameter of the rib  420  is slightly tapered to achieve inertial separation of particles (liquid water droplets, ice crystals, aerosols, etc.) out the tail of the rib  420 . The rib  420  has a height of approximately 6.35 mm.  
         [0042]      FIG. 6  depicts a side view of FS system  400  in an example of the invention. The FS system  400  includes a rib  420 , an external surface  510  of the aircraft, an incoming coupling pipe  610 , a cylindrical sampling tube  630 , and an outgoing coupling pipe  640 . The external plate is not depicted in  FIG. 6  for the sake of simplicity and to focus on the flow of atmospheric trace gases to be measured. The rib  420  is attached to the external surface  510  of the aircraft via the external plate. The rib  420 , the external plate, and the external surface  510  of the aircraft has an incoming hole  602  and an outgoing hole  604  for air flow. The incoming coupling pipe  610  is connected to the rib  420 , the external plate, and the external surface  510  through the incoming hole  602 . The opposite end of the incoming coupling pipe  610  is connected to the cylindrical sampling tube  630 . The cylindrical sampling tube  630  is also connected to the outgoing coupling tube  640 . The outgoing coupling tube  640  is connected to the rib  420 , the external plate, and the external surface  510  of the aircraft through the outgoing hole  604 .  
         [0043]     In this embodiment, the incoming coupling pipe  610  and the outgoing coupling pipe  640  are stainless steel, flexible Kevlar hoses or other hoses of similar material whether fixed or flexible that direct air flow into and out of the cylindrical sampling tube  630 . In some embodiments, the incoming coupling pipe  610  and the outgoing coupling pipe  640  may be heated or non-heated. In this embodiment, the cylindrical sampling tube  630  is a stainless steel tube that is 24 cm long. In this embodiment, the cylindrical sampling tube  630  is optimized for an existing diode laser for water vapor measurement, which is described in further detail below in  FIG. 8 . In another embodiment, the cylindrical sampling tube  630  is 12 cm long with a sapphire-coated mirror at the end that keeps the effective path length 24 cm long. In other embodiments, other reflective material could be in the cylindrical sampling tube  630  to decrease the path length. The diameter of the inlets of the rib  420 , the location of the apertures, and the diameter of the cylindrical sampling tube  630  can be altered for other embodiments and optimized for a particular aerial application.  
         [0044]      FIG. 7  depicts a detailed side view of the rib  420 , the incoming coupling pipe  610 , and the outgoing coupling pipe  640  in an example of the invention. The rib  420  includes an inertial separator  710 . The inertial separator  710  is attached to the top of the rib  420 . The inertial separator  710  is a converging metal shape with an approximately 1-2 mm rise. Once again, in this example, the air flows left to right in the rib  420 . The inertial separator  710  is configured to converge air flow. The air flow then diverges after the inertial separator  710 . The inertial separator  710  forces most particles out the back exit of the rib  420  because of the momentum of the particles (the combination of their density and the fast flow). In other embodiments, there are numerous variations in the height, shape, and position of the inertial separator  710  to converge and then diverge air flow. Also, in other embodiments, the outgoing coupling pipe  640  is attached in various configurations in the aerial vehicle to remove the sampled atmospheric flow from the cylindrical sampling tube  630 .  
         [0045]     In some embodiments, the rib  420  may include an incoming flow enhancer  720 , an outgoing flow enhancer  730 , and a base flow enhancer  725 . The incoming flow enhancer  720  on top of the base flow enhancer  725  is adjacent to the incoming hole  602 . The incoming flow enhancer  720  and the base flow enhancer  725  assist in directing air flow in the incoming hole  602  to the incoming coupling pipe  610 . The outgoing flow enhancer  730  on top of the base flow enhancer  725  is adjacent to the outgoing hole  604 . The outgoing flow enhancer  730  and the base flow enhancer  725  assist in directing air flow out of the outgoing hole  604  from the outgoing coupling pipe  640 . The outgoing flow enhancer  730  and the base flow enhancer  725  prevent the air flow from outgoing hole  604  from going right to left in the opposite direction of the original air flow.  
         [0046]      FIG. 8  depicts an illustration of the cylindrical sampling tube  630  in an example of the invention. As discussed above, the cylindrical sampling tube  630  is connected to the incoming coupling pipe  610  and the outgoing coupling pipe  640 . The cylindrical tube  630  comprises a laser transmitter  810 , a temperature sensor  820 , a pressure sensor  830 , and a receiver  840 .  
         [0047]     The cylindrical sampling tube  630  is 24 cm long. This length is sufficiently long for extremely accurate water vapor mixing ratios such as measurements of equivalent relative humidity (RH) as dry as 5% at 40,000 feet. The length is also sufficiently short for the fast-moving air to provide a new sampling volume in a small to large fraction of a second depending upon the aircraft speed. The cylindrical sampling tube  630  also comprises a temperature sensor  820  and a pressure sensor  830  for measuring temperature and pressure, respectively. The temperature sensor  820  and the pressure sensor  830  are mounted on the chamber walls of the cylindrical sampling tube  630 . The laser transmitter  810  is a conventional diode laser transmitter configured to transmit laser signals. The receiver  840  is a conventional receiver configured to receive laser signals. In other embodiments, the laser transmitter  810  can be a quantum cascade laser. Measurements of water vapor by diode lasers is disclosed in a publication entitled “Open-Path, Near-Infrared Tunable Diode Laser Spectrometer for Atmospheric Measurement for H 2 0,” by May, R. D., in  the Journal for Geophysical Research,  vol. 103, p. 19,161-19,172 (1998), which is hereby incorporated by reference.  
         [0048]     The links  812 ,  822 ,  832 , and  842  are connected to the laser transmitter  810 , the temperature sensor  820 , the pressure sensor  830 , and the laser receiver  840 , respectively. In some embodiments, the links  812 ,  822 ,  832 , and  842  are connected through a multi-pin connector. In some embodiments, the links  812 ,  822 ,  832 , and  842  are connected to electronic circuitry, computers, or other processing systems that control, manage and/or process the measurements from the laser transmitter  810 , the temperature sensor  820 , the pressure sensor  830 , and the laser receiver  840 . These electronic circuitry, computers, or other processing systems could be located anywhere within the aerial vehicle. Processed information can then be sent to the cockpit and/or to the ground via wireless communications. The measurements could be used in a variety of applications including weather related applications and navigation.  
         [0049]     The mixing ratio of atmospheric trace gases may be sampled from the boundary layer of the aircraft because the ultimate intended measurement is unaffected. The laser signal is at a chosen frequency that matches the absorption cross section frequency of the trace gas being measured. Thus, the mixing ratio of water vapor or of some other trace gas can be accurately determined from the lasers, the use of Beer&#39;s Law, and measurement of pressure and temperature. It is the measurement of the actual temperature and pressure near the laser light path that makes Beer&#39;s law useful. The mixing ratios are conserved properties whether they be determined in static conditions, in fully dynamic or total conditions, or in conditions between the two extremes. Beer&#39;s law is: 
 
 I=I   O    exp (−σ n l ) 
 
 where I is light intensity at the detector (receiver); 
        I O  is the light source intensity; and     (σn l)=absorbance 
            where σ is the molecular absorption cross section (a function of frequency, pressure, and temperature);     n is the number density of the absorbing species to be measured such as H 2 O, CO, CH 4 , N 2 O, NO, SOx, 0 3 ; and    
            l is the path length.        
 
         [0056]     Aerial vehicles may encounter rain, snow, or dense cloud events (water droplets, ice crystals, or a mixture of both) that lead to sensor “wetting.” This FS system  400  and the use of a specific laser frequency have a distinct advantage in not being affected by the liquid and solid water elements as such elements do not absorb the laser light at the selected frequency. Only if there were significant amounts of such elements in the cylindrical sampling tube  630  (a situation avoided by the use of the inertial separator  710  in the rib  420  of the FS system  400 ) would they affect the laser light scattering (not the light absorption) and reduce the sensitivity of the measurement.  
         [0057]     In other embodiments, other sampling tubes are added in series to the cylindrical sampling tube  630  so that quantum cascade laser simultaneously measures various chemical or biological species with a different path length that is optimized to match the desired measurement range and consistent with the quantum cascade laser frequency and efficiency.  
         [0058]     In one embodiment for an unmanned aerial vehicle such as the large RQ-4A Global Hawk that flies up to 65,000 ft, the FS system  400  measures the water vapor in the stratosphere to a minimum value of 3 ppmv. The usual range in the driest part of the tropical lower stratosphere is typically 3-5 ppmv. In this embodiment, the cylindrical sampling tube  630  is extended to 40 cm.  
         [0059]     In another embodiment on the opposite end of the current spectrum of unmanned aerial vehicles such as the small GNAT 750 that has an altitude flight limit of 25,000 feet, the FS system  400  includes the cylindrical sampling tube that is 10 cm. This embodiment accurately measures the full range of expected water vapor mixing ratio values or equivalent RH encountered in the troposphere below 25,000 feet.  
         [0060]     In other embodiments, the aircraft could be any unmanned aerial vehicle that operates below 18,000 ft. In this embodiment, the dimensions of the FS system  400  is scaled down by a factor of two except for the length of the cylindrical sampling tube, which is scaled down by a factor of five to ten such as with a path length of 4 to 2 cm. This embodiment achieves a minimum measurement of 1% RH at 18,000 ft. and lower minimum values yet at lower levels of the troposphere.  
         [0061]     The FS system  400  has the following advantages. First, the FS system  400  does not include the heater from the TAT probe, which eliminates the costs, weight, energy consumption, and failures associated with the TAT probe. The FS system  400  also has reduced frictional drag as compared with the TAT probe and pitot tube. This may save $1-$2 per pound per week per aircraft, which is a significant cost.  
         [0062]     The FS system  400  is also lightweight and efficient as compared to the “open path” prior system. The FS system  400  provides an environment for more accurate measurements of atmospheric trace gases. Also, the FS system  400  does not have the problems of solar interference as in the “open path” prior system. Also, the FS system  400  has less frictional drag than the “open path” prior system.  
         [0063]     The FS system  400  also has more sensitivity than the prior system with the TAT probe and the water vapor sensing system by a factor of more than six. This occurs because of the added width and length of the cylindrical sampling tube  630 . This eliminates the need for fiber optic laser connections and thus fringes. The measured minimum absorbance improves from 1×10 −4  to 3.75×10 −5 —a factor of 2.67 improvement in sensitivity. The added length of the cylindrical sampling tube  630  to 24 cm from 10.2 cm increases the path length by a factor of 2.35. Together, these factors multiply to an improved sensitivity of a factor of 6.2.  
         [0064]     The FR system  400  and the use of lasers allows a highly effective water vapor measurement system that can have a significant impact on improving aviation safety, efficiency, and capacity. The FS system  400  and the use of lasers allows water vapor and other trace gas measurements that can contribute to atmospheric science across a spectrum of atmospheric science application ranging from short-term weather predictions to climate change assessments.  
         [0065]     The laser light produces accurate water vapor answers even in the presence of aerosols unless the density and number of such aerosols is exceedingly large. If this occurs, the laser intensity (a separate measurement) drops and the software can use information from a second cross cell laser to verify such a condition. These and similar procedures can be shown to lead to further benefits of the FS system  400  in providing an early warning system for volcanic ash (a serious concern for engine performance and hence, safety).  
         [0066]     Another application for the FS system  400  is for nuclear-biological-chemical (NBC) terrorism. Mesoscale information from commercial aircraft as part of a composite environmental observing system help mitigate the effects of NBC terrorism. Diode and QC lasers in the FS system  400  provide valuable information for the strategic mesoscale observing system that is now unavailable, and on the tactical observing system that is brought to ground zero should an NBC terrorism event occur. Accurate analysis of atmospheric stability (temperature and water vapor) are required to properly drive plume models. The commercial aircraft can help provide 100 times more stability profiles per day than obtainable from today&#39;s balloon-borne radiosonde system. This is the strategic observing system prior to an event. The nature of the tactical observing system is driven by the form of the NBC terrorism event. The identification of the contaminated plume and the environment surrounding it at ground zero can be obtained with special manned aircraft and UAVs with the FS system  400 . This would be an important part of the tactical observing system.  
         [0067]     In one embodiment for an icing detector, the inlet to the enclosure is made sufficiently small that an icing situation would immediately block the flow into the enclosure. The inertial separator in the enclosure is not needed and is replaced with a pressure sensor. The pressure sensor (which normally would detect full dynamic pressure) would only detect the much weaker static pressure if the hole was blocked by ice build-up. Thus, the detection of ice is performed instantaneously.  
         [0068]     The second function of a successful icing detector is to remove the ice extremely rapidly in order to again serve as an icing detector. The time required to remove the ice is what determines the sensor&#39;s response time. Of the two known types of icing sensors in use or being developed today, this response time is exceedingly slow (20 or more seconds). The area of ice capture is too large in these sensors and it takes too long to remove the ice through electrical resistance heating. Thus, these sensors have little value in ascent/descent of an aircraft where one would like to know the vertical levels of icing more precisely.  
         [0069]     In this embodiment, the enclosure inlet has a thin ring of electrically heated metal surrounding the inlet orifice. This large heat source confined to the miniature ringlet provides a response time of less than 1-2 seconds or a factor of 10 faster than current icing sensors. The sensor information would pass from the enclosure via a multiple pin connector to an external processing system. The processing system includes the heating circuit logic. Heating begins upon ice detection and an immediate cease of heating upon ice removal (pressure back to full dynamic pressure). From the processing system, the information is relayed to the cockpit and to the ground-based personnel in real time like the other application embodiments.  
         [0070]     In one embodiment for volcanic ash, the cylindrical sampling tube  630  includes a laser detecting gas from a volcanic eruption and another simple optical laser looking across the cylindrical sampling tube that would confirm that the volcanic aerosol content was sufficiently high. Normally, the inertial separator would remove most aerosol particles-but in a volcanic eruption incident the aircraft may come close enough to the volcanic plume, or to the plume in its subsequently dispersed form, such that the concentration of aerosol particles would be sufficiently dense to override the effects of the inertial separator-leaving a detectable signal. The sensor information would pass from the cylindrical sampling tube  630  via a multiple pin connector and go to an external processing system. From the processing system, the information is relayed to the cockpit and to the ground-based personnel in real-time like the other application embodiments of the invention.