Not applicable.
1. Field of the Invention
The invention relates generally to the field of rotating wing aircraft (e.g. helicopter) position and orientation determination using radar. More specifically, the invention relates to devices and methods applied to enhance safety of helicopter landing under brownout (sand and/or dust) or whiteout (snow and/or fog) conditions created by the aircraft's main-rotor down-wash, under which near-ground flight is particularly perilous due to the sudden loss of visual cues on which the pilot depends.
2. Background Art
United States Defense Advanced Research Projects Agency (DARPA) Broad Agency Announcement No. BAA 06-45 requests solicitations for proposals to deal with affordable solutions to the problem of helicopter landing in brownout as well as other degraded visual environments (DVEs) such as whiteouts caused by snow and/or fog. Solutions are needed for the brownout phenomenon, which causes deadly accidents during helicopter landing and take-off operations in arid desert terrain. Intense, blinding dust clouds, which may be stirred up by the aircraft's main-rotor down-wash during near-ground flight can cause helicopter pilots to suddenly lose all visual cues. This creates significant flight safety risks from aircraft and ground obstacle collisions, rollover due to sloped and uneven terrain, etc.
What is needed is a sensor/visualization-display system that will effectively provide an affordable, landing capability in brownout/DVE conditions where the visibility is temporarily as low as zero with zero landing-zone infrastructure and limited knowledge of the terrain comprising the landing area. The invention may also be permanently deployed as an integral safety feature for landing areas experiencing frequent degradation of visibility such as offshore oil rigs (e.g. fog), desert installations (e.g. sand and dust) and Arctic/Antarctic installations (e.g. snow).
A method for determining position of an aircraft with respect to a ground station according to one aspect of the invention includes transmitting an electromagnetic signal from the aircraft. The signal includes a plurality of electromagnetic signals, each signal having a different selected frequency. The signal is detected at an array of sensors disposed on the ground surface in a selected pattern. The array includes at least one reference sensor and at least three spaced apart time difference determination sensors. A difference in arrival time of the signals between the reference sensor and each of the time difference determination sensors is determined and a spatial position of the aircraft is determined from the time differences.
Other aspects and advantages of the invention will be apparent from the following description and the appended claims.
The invention generally includes electromagnetic signal sensors disposed in a selected pattern on or about a helicopter landing pad which are able to provide with high accuracy the spatial (e.g., Cartesian x, y, z) positions of an electromagnetic signal (e.g., radio frequency) transmitter disposed on a helicopter. In this embodiment, the position and velocity vector of the helicopter may be determined to high precision relative to the coordinate system of the landing pad (with no loss of generality the landing pad may be assumed to be stationary) due to the long baselines available between the sensors.
An alternative embodiment of the invention would see the invention deployed as an integral part of the airframe of the helicopter and one or more radio beacons deployed in the reference frame of the landing pad. (See
It is straightforward to combine these two embodiments and include the invention deployed both on the landing pad and in the helicopter. This could be envisaged for the case where both the landing pad reference system X, Y, Z and the helicopter reference system X′, Y′, Z′ are moving; the application being landing a helicopter on board a water borne ship under low visibility conditions.
The height of the helicopter (Z) also may be obtained using an altimeter disposed at each of the forward and aft ends of the helicopter to provide greater confidence in the position information. As described above, it is possible to obtain height using the electromagnetic signal sensors, but the use of more sensors (e.g. altimeters, compasses, accelerometers, etc., individually or in combination) deployed as explained above also enables another means of determining the helicopter attitude (pitch) as well as (with additional sensors) yaw and roll. The alternate embodiment described above that allows both position and orientation of the helicopter to be measured reduces the need for additional sensors. One example of an altimeter suitable for use with the invention is a miniature radar altimeter. Commercially available altimeters of this type provide height determination accuracy of 2 cm.
In principle, an electromagnetic signal transmitter disposed on the helicopter transmits a frequency hopping signal, to be explained further below. The sensors deployed on or about the landing pad measure the phase difference between the signals received by three or more such sensors, distributed spatially, and a reference sensor. The phase difference is measured as a function of the hop frequency of the signal. The relationship of the phase difference with respect to the hop frequency of the signal enables determining the signal travel time delay between the arrivals of the electromagnetic signals at each sensor without ambiguity. This technique is known in the art as the “frequency hopping spread spectrum” technique for measuring time delays. Such time delays may be used to calculate the spatial position of the transmitter, and thus the helicopter, in three dimensions as a function of time delay. Such position information may easily be displayed as position, drift velocity and drift direction with respect to height. In some examples, the ground-deployed sensors can be moved onto the landing pad on a prepared frame for use, for example, only when adverse visibility conditions exist. The sensors do not need to be permanently mounted or affixed to the landing platform or pad.
A possible advantage of a method according to the invention is in its use of the slope of the phase difference with respect to the signal hop frequency to determine the time delay between the signal arrivals without ambiguity. The output position information can provide the helicopter pilot with the helicopter's rate of descent, absolute height above the ground with accuracies better than 30 cm, drift velocity with accuracy of better than 2 m/s and drift direction accuracy of better than 1 degree. The applications for this invention include, as non-limiting examples, landing pads on buildings, oil rigs and ships, lighthouses and sites of tactical military importance. That is, the invention may be used on any landing pad that is prepared and in ordinary use and which may be impacted by extreme weather conditions such as zero visibility by white-out, brownout of other low visibility conditions (including, e.g., degraded visibility environments (DVEs)). The invention may also be used on unprepared landing sites.
In some examples, e.g., “brownouts” due to dust raised by the helicopter itself, determining position may be of military importance when landing on unprepared sites. In such cases the pilot can select the landing site from above a height where the brownout exists. In one example, the pilot can lower a rope or cable C with the sensor array R coupled on the bottom end thereof (See
In one example, the position determination device can include a transmitter operating at 2.4 GHz carrier frequency located on the helicopter which transmits a specific sequence of electromagnetic signal pulses. Each signal pulse in the pulse sequence can be a modulation of the carrier frequency at a different “hop” frequency, with hop frequencies being, for example, integral multiples of 1 MHz difference from the carrier frequency. Each pulse in the pulse sequence can be separated from the next pulse by a preselected time interval, for example a selected number of carrier frequency cycles (e.g., 6000 cycles) during which no signal transmission takes place. In the array of receivers or sensors deployed on the ground, one receiver acts as a reference sensor and may be located at the center of the device. The other three sensors or receivers may be, for example located on the circumference of a circle of predetermined radius (e.g., about 2 meters).
Simulations of operation of a system made according to the above general parameters indicate that the position location system should provide positional (e.g., in Cartesian x, y, z coordinates) accuracies of a few centimeters for all helicopter heights down to about 1 m when the spacing between each of the outer positioned sensors and the reference sensor, represented by s, greater than about 15 wavelengths of the electromagnetic signal carrier. That is, s≧15λ(=1.9 m at 2.4 GHz), wherein λ represents the wavelength, the number of hop frequencies nhop≧50, a hop frequency interval of Δfhop=1 MHz, and standard error in measuring the phase differences of about 0.1 degrees.
Typical values of the size of the landing pad and a safety circle surrounding the pad are that the pad has dimensions of approximately 10 m diameter and the safety circle has a diameter of about 35 m.
The example geometry of the sensor array shown in
where c=3 108 meters per second. If, for example, Δfhop is chosen as 1 MHz and the number of hops is nhop=50, then the maximum value of s=3 m. In such case any choice of s<3 m that will provide sufficiently accurate time delay measurement will be acceptable. The shorter the sensor spacing, s, the greater the fractional time error will be due to uncertainties in the phase centers of the sensors. The ultimate system accuracy will depend on the accuracy of the phase difference measurements, the hop frequency interval, the carrier frequency and the sensor spacing s. From simulations it appears to be the case that spacings of 10 wavelengths or greater would be appropriate. At 2.4 GHz this would be about 1.25 m.
It is important to avoid the complications of multiple reflections of the transmitter signals. The system of the invention overcomes such complications by suitably selecting the position and size of the sensor array on the ground, the number of carrier frequency cycles used for each hop frequency and having a transmission break between each hop frequency transmission, and the number of sensors in the array. The array is shown as having four sensors in the various examples shown in the figures. It should be understood that more than four sensors may be used in other examples advantageously. Referring to
Locating the sensor array to be near the center of the landing pad it appears that for helicopter heights greater than 10 m the minimum extra distance traveled by an indirect signal path is about 18 meters as shown in
As previously explained, the accuracy with which the time delays can be measured depends on the of the sensor spacing, the number of hop frequencies, the hop frequency increment and the number of cycles available over which phase differences are measured. The larger each of these quantities is, the greater the accuracy of the time-delay estimate and thus the transmitter position. Simulations of operation of the above described system indicate positional accuracies of a few cm are obtained for all helicopter heights down to about 1 m for sensor spacing of s≧15λ(=1.9 m at 2.4 GHz), the number of hop frequencies nhop≧50, a hop frequency interval of Δfhop=1 MHz, and standard error in measuring the phase differences of better than 0.1 degrees of phase.
A first factor which affects the choice of frequency is the number of cycles available over which the phase differences can be measured. Thus, a higher frequency can provide better accuracy. A suggested frequency is one used widely in Bluetooth devices. This frequency is 2.4 GHz, which has a wavelength of 12.5 cm. For helicopter altitudes above 10 meters, the duration over which the phase can be measured will be about 10 meters/0.125 meter wavelength or 80 cycles. Below 10 meters altitude, the duration over which the phase can be measured will reduce to about 2.5 meters/0.125 meter wavelength or 20 cycles. The accuracy obtained by measuring over this varying number of cycles can be increased by increasing suitably the number of hop frequencies, the size of the frequency hop interval and the separation of the sensors.
Interference with the operation of other radio frequency devices is expected to be small as the signal will be low power, low duty cycle and will be frequency hopping.
The transmitted signal may consist of, for example, a first 20 cycle pulse at frequency f0 followed by a time interval during which no transmission takes place, followed by 20 cycles at f0+Δfhop until the required number of hop frequencies have been used, as an example, of the order of 50. The no-transmission breaks may be about 6000 cycles between 20 cycle pulses. The hop frequency sequencing need not be linear, but could follow a predetermined protocol defined for security/interference reasons.
The reason for the break in transmission is that following the 20 cycles of the one hop frequency there will be multiple arrivals of that hop frequency as described before. The break in transmission should be long enough for the multiple arrivals to have reduced in amplitude by about 60 dB before the next hop frequency is transmitted. The example number of cycles for the transmission breaks as indicated above is based on such attenuation of multiple travel path signals.
As the free-time reduces with reducing height below 10 meters altitude, there is no need to adjust the transmitted signal. The adaptation to the reduced free-time is that the processing only uses the maximum number of cycles for that altitude in which multiple travel path signals are substantially attenuated.
A sequence of 50 hop frequencies with 20 cycle duration at each hop frequency at a frequency of say 2.4 GHz with transmission breaks of 6000 cycles would last for about 0.125 msec. During this time the actual position of the transmitter on the helicopter will not have moved by more than 3 mm, even at speeds of up to 50 mph (22.5 m/s). Thus it is to be expected that the time to provide the coordinate position of the transmitter on the helicopter (H in
An example electromagnetic signal pulsing sequence is shown in
The foregoing description of the invention includes having the receiving sensors deployed on the ground and locating one transmitter on the helicopter with at least one, and preferably two or more, altimeters to provide measures of pitch, yaw and roll. The minimum additions to the helicopter would be the transmitter and an accurate altimeter. If the transmitter were disposed on the ground then the helicopter would need the receiving sensors plus at least one accurate altimeter. Again, the ground transmitter could be deployed when LVE conditions occur. The positional data obtained from the three sensors would already be on the helicopter. The main unknown is the multiple signal travel path effects of the helicopter itself. Therefore, it is advantageous in implementing the invention that the receiving sensors are deployed on the ground and the transmitter is deployed aboard the helicopter.
The description and equations below are for the example arrangement of the sensors shown in
D=√{square root over ((x2+y2+z2))}
The distances from the transmitter position (x, y, z) to the other sensors R2, R3, R4 are given by the equations:
dR2=sqrt((x−s)^2+y^2+z^2);
dR3=sqrt((x+sa)^2+(y−sb)^2+z^2);
dR4=sqrt((x+sa)^2+(y−sb)^2+(z)^2);
where each sensor R2, R3, R4 is located at a distance s from the reference sensor R1 and a=cos(30°) and b=cos(60°. The time delays, expressed as distances, may be calculated by the expressions:
mR2=(D−dR2)
mR3=(D−dR3)
mR4=(D−dR4)
Using the equations:
mR2=D−√{square root over (((x−s)2+y2+z2))}
mR3=D−√{square root over (((x+sa)2+(y−sb)2+z2))}{square root over (((x+sa)2+(y−sb)2+z2))}
mR4=D−√{square root over (((x+sa)2+(y+sb)2+z2))}{square root over (((x+sa)2+(y+sb)2+z2))}
the following 3 equations can be constructed where the αi and βi can be expressed in terms of the above three distances mi, a and b and s:
x=αa1D+β1
y=α2D+β2
y=α3D+β3
Thus a linear equation for D can be found as:
The above equation can be used directly for an estimate of D, and then x and y are obtained from the above equations. z may be obtained from the equation:
z=√{square root over ((D2−x2−y2))}
In the present example it is expected that the altimeter will also provide z so it may only be necessary to solve a quadratic equation to obtain D where z is otherwise obtained.
D2(α12+α22−1)+3D(α1β1+α2β2)+β12+β22+Z2=0
and then use the expressions:
x=α1D+β1
y=α2D+β2
It has been determined that the preferred technique for determining z above a certain helicopter altitude is to use the altimeter measurement and the quadratic equation above to obtain D with the value of D from the sensor array used to select the correct solution. Below this height the value of D can be obtained as explained above from the sensor array. Essentially, if the phase difference between two sensors as a function of frequency is known then the slope of the relationship gives the time delay between the sensors. If the phase difference between sensors separated by a baseline of N wavelengths becomes greater than 2π as the frequency varies then an unwrapping of the phase difference would be necessary. Phase unwrapping can be implemented, but it is preferable to be avoid phase unwrapping by limiting the distance between the reference sensor and the outer sensors.
To establish whether the phase difference for a baseline of N wavelengths is less than 2π as the hop frequency runs through its range. Let the baseline be N wavelengths. Then the phase difference can be calculated by the expression:
Then the change in the phase difference for a fractional frequency change is determined by the expression.
There are nhop frequencies at Δfhop intervals from the central frequency f0, po the maximum shift in phase difference for a fixed baseline due to change in frequency is
If the phase difference is Δφ then the resulting extent of the phase difference is due to frequency changes is thus given by the expression:
If the phase difference for one frequency is close to 2π, then this is the only boundary it can cross. So as the phase difference with respect to frequency is calculated to obtain the time delay it may occasionally have to make a single adjustment of 2π, but never more than one such adjustment.
The slope of a straight line through the phase difference versus hop frequency data is calculated in a least squares manner and provides the estimate of the time delay. If each point on the phase difference versus frequency plot has a standard error of a, then the standard error of the time delay estimate is:
where nh is the number of hop frequencies used and Δfhop is the increment between hop frequencies.
If more than four difference determination sensors are used, such sensors can be arranged in a regular, irregular or random array geometry.
In still other examples, and with reference to
The invention may enable a helicopter pilot to approach a landing pad in DVEs safely.
While the invention has been described with respect to a limited number of embodiments, those skilled in the art, having benefit of this disclosure, will appreciate that other embodiments can be devised which do not depart from the scope of the invention as disclosed herein. Accordingly, the scope of the invention should be limited only by the attached claims.
Priority is claimed from U.S. Patent Application No. 61/176,360 filed on May 7, 2009
Number | Name | Date | Kind |
---|---|---|---|
2437695 | Jansky | Mar 1948 | A |
3659085 | Potter et al. | Apr 1972 | A |
4232313 | Fleishman | Nov 1980 | A |
4740792 | Sagey et al. | Apr 1988 | A |
5099245 | Sagey | Mar 1992 | A |
5191342 | Alsup et al. | Mar 1993 | A |
5200748 | Attfield | Apr 1993 | A |
5534876 | Erickson et al. | Jul 1996 | A |
5583517 | Yokev et al. | Dec 1996 | A |
5596330 | Yokev et al. | Jan 1997 | A |
5724047 | Lioio et al. | Mar 1998 | A |
5999116 | Evers | Dec 1999 | A |
5999131 | Sullivan | Dec 1999 | A |
6094169 | Smith et al. | Jul 2000 | A |
6211811 | Evers | Apr 2001 | B1 |
6243587 | Dent et al. | Jun 2001 | B1 |
6366240 | Timothy et al. | Apr 2002 | B1 |
6407703 | Minter et al. | Jun 2002 | B1 |
6477163 | Miller | Nov 2002 | B1 |
6816105 | Winner et al. | Nov 2004 | B2 |
7019682 | Louberg et al. | Mar 2006 | B1 |
7170441 | Perl et al. | Jan 2007 | B2 |
7313143 | Bruno | Dec 2007 | B1 |
7365652 | Scherbarth | Apr 2008 | B2 |
7541968 | Hall et al. | Jun 2009 | B2 |
7570194 | Galati | Aug 2009 | B2 |
7642929 | Pinkus et al. | Jan 2010 | B1 |
8019360 | Qahwash | Sep 2011 | B2 |
8026850 | Seong et al. | Sep 2011 | B2 |
8138967 | Weedon | Mar 2012 | B2 |
20030142002 | Winner et al. | Jul 2003 | A1 |
20040032363 | Schantz et al. | Feb 2004 | A1 |
20050206555 | Bridgelall et al. | Sep 2005 | A1 |
20080231494 | Galati | Sep 2008 | A1 |
20080291089 | Seong et al. | Nov 2008 | A1 |
20090002220 | Lovberg et al. | Jan 2009 | A1 |
20090138138 | Ferren et al. | May 2009 | A1 |
20120075138 | Stayton et al. | Mar 2012 | A1 |
Number | Date | Country | |
---|---|---|---|
20100328138 A1 | Dec 2010 | US |
Number | Date | Country | |
---|---|---|---|
61176360 | May 2009 | US |