SYSTEM FOR DETECTION AND MEASUREMENT OF ATMOSPHERIC MOVEMENT

Abstract: A system for the detection and measurement of atmospheric air movement irregularities such as wind velocity vector, wind shear, downdraft, clear air turbulence, aircraft induced vorteces and turbulence, in particular along a glidepath near airports, whereby an air volume under investigation is illuminated by a radio wave transmitter with a beam of coherent electromagnetic energy and a resulting wave field is received and processed in processor means to derive information on the existence of said atmospheric irregularities and furthermore to give specific measurements of related parameters, comprising at least one receiver for said resulting wave field, which is due to scattering in said air volume, positioned at a bistatic location having a selected distance from said transmitter, characterized by acoustic transmitter means located between said transmitter and said at least one receiver, and adapted to emit acoustic waves into said air volume, with frequency and beamwidth of the acoustic waves chosen such that a resulting disturbance of the dielectric constant of air in said air volume, contributes to said scattering.

Description: SYSTEM FOR DETECTION AND MEASUREMENT OF ATMOSPHERIC MOVEMENT. This invention relates to a system for measuring and detecting of velocity, turbulence, vorteces and similar irregularities and phenomena in air, including classifi¬ cation of such phenomena. These may comprise the wind velocity, clear air turbulence as well as aircraft induced vortices and turbulence. Detection and measurement as contemplated takes place by combining electromagnetic and acoustic waves. The invention comprises a system of transmitter and receiver means for electromagnetic waves and transmitter means for acoustic waves, as well as an associated method. The invention is primarily directed to the measurement of the mentioned phenomena affecting air traffic safety, but may easily be adapted to other fields of use. This kind of phenomena have been measured before by measuring the scattering and Doppler-shift of electromagnetic beams when affected by the disturbances in the air. An example of this is given in the international patent application WO 93/19383 using electromagnetic transmitter and receiver means. The electromagnetic beam is transmitted at a microwave frequency and is scattered by disturbances in the air. The receiver means are positioned at a bistatic location and directed so as to cover a volume of air also covered by the transmitter, and to receive signals with a (preferrably low) scattering angle. Scattering of electromagnetic waves by acoustic waves is discussed in Appl. Sci. Res. Section B, Vol. 6, 1957 by A. Tonning: "Scattering of electromagnetic waves by an acoustic disturbance in the atmosphere". The publication discusses the cases of spherical and plane acoustic waves. This invention is based on the fact that acoustic waves generate disturbances in the dielectric constant in the air by changing its density. These disturbances are affected by wind and other phenomena in the air, and also scatter the electromagnetic energy. By controlling the acoustic signal and/or the electromagnetic energy the scattering may be controlled, and the received signal may then be use to meas¬ ure the other disturbances in the air. A system similar to this is described in US patent 4,351,188 in which radio waves are transmitted towards a spherical acoustic wavefront. The electromagnetic wave is reflected and focused by the acoustic wavefront towards electromagnetic receivers on the ground. A two-dimensional array of receivers is used to measure the position to which the electromagnetic wave is focused. This position and the time delay give an indication of the wind velocity at a given altitude. A disadvantage in this system is the limitations in the wind directions that can be measured. To get a reflection focused inside the receiver array the wind must blow along the direction from the electromagnetic trans¬ mitter, across the acoustic transmitter towards the electro¬ magnetic receivers. To get a compute? wind profile four electromagnetic and acoustic transmitters are used. Another disadvantage with this solution is that the transmitters and receivers need to be positioned close to each other, which limits the possibility for using existing components at the site in which the measuring is to be performed. The present invention avoids this problem by generating a grating in the dielectric constant of the air and measu- ring the fluctuations and movements of this grating to get a complete wind profile in a chosen air volume. The novel and specific features according to the invention are set out more completely in the claims. According to the invention the acoustic signal is essentially periodic. This will generate a generally periodic disturbance in the dielectric constant of the air. In this way a grating may be generated, moving at the speed of sound, with a spatial wavelength depending on the wavelength (and thereby frequency) of the acoustic energy. The grating will satisfy the Bragg conditions for certain combinations of acoustic and electromagnetic frequencies and thereby reflect part of the electromagnetic energy towards the receivers. The different movements in the air will affect the grating in different ways. Air moving parallel to the dire¬ ction of propagating acoustic energy will change the density of the grating, and air moving perpendicular to the acoustic energy will displace the grating. By measuring parameters like the acoustic or electromagnetic frequencies, or dis¬ placement or angle of arrival of the received electromagn¬ etic wavefronts the air velocity and direction may be found. The invention as well as the resulting advantages will be explained more in detail in the following description, referring also to the drawings in which: Fig. 1 schematically illustrates a system according to the invention, with electromagnetic and acoustic transmitters, and receiver means for electromagnetic energy. Fig. 2a illustrates the acoustic frequency range satisfying the Bragg conditions in a no wind situation. Fig. 2b illustrates the shift in the acoustic frequency satisfying the Bragg conditions when the grating is influenced by wind parallel to the acoustic beam. Fig. 3 shows the system and method of invention using two receivers to detect the angle of arrival of the electromagnetic beam. Fig. 4 shows the system/method invention using at least 3 receivers to measure the shape of the received wavefront. Fig. 5 illustrates the geometry in measuring the time delay of the electromagnetic signal. Fig. 6 illustrates the displacement of the grating due to wind moving perpendicular to the acoustic beam. Fig. 7 shows a complete setup for measuring wind moving across the acoustic beam, using more than one rec- eiver to measure the displacement of the received bea . Figure 1 illustrates the general setup of the invention, with a transmitter 1 for electromagnetic waves, transmitter means 2 for emitting acoustic waves, receiver means 3 for receiving the scattered electromagnetic waves. The receiver and transmitter means all point towards the same volume of air 4. The electromagnetic waves are sent in the direction of the selected volume of air 4, where they interact with the acoustic waves preferrably making a grating which, by Bragg reflection, reflects at least part of the electromagnetic energy towards the receiver(s) 3. Typically the elevation angles of the electromagnetic transmitter 1 and receiver(s) 3 is smaller than illustrated in the figur. The distance between the electromagnetic 1 and acoustic 2 transmitters is preferrably essentially sim- ilar to the distance between the acoustic transmitter 2 and the receiver(s) 3, and the elevation of acoustic transmit¬ ter(s) 2 is close to 90°. Ideally the beams from the trans¬ mitters 1,2 and the coverage of the receiver(s) span essen¬ tially in the same plane. The grating generated by the acoustic transmitter essentially consists of surfaces having different dielectric proporties. According to this invention the electromagnetic waves meets this grating at a relatively small angle and is partially reflected at each surface. If the frequencies of the waves are chosen according to the invention satisfy the Bragg conditiones the reflected electromagnetic beams reflected from each surface interfer making an interference pattern with a main reflection towards the receivers. To obtain this the distance between the acoustic transmitter and the air volume to be measured is preferrably less than the distance between the electromagnetic and the acoustic transmitters. In a first embodiment of the invention a change in the density of the grating due to movement in the air changes the condition for reflection, and the signal is lost from the receiver 3. This change is compensated for by varying the emitted acoustic frequency until the electromagnetic signal is again received by the receiver. The air velocity corresponding to this change in frequency is found by studying the equation describing the Bragg conditions: where F aco is the acoustic frequency, F rf is the electromagn¬ etic frequency, c aco is the speed of sound, c rf is the speed of light, and θ is the angle between the transmitted and the reflected electromagnetic beam. With wind affecting the grating we have: F Ω F aco=2— - (c aco+V)sin- o where V is that component of velocity of the air in the acoustic propagation direction. The electromagnetic beam has a beamwidth β, and the receiver covers an angle of about the same size. Together they select a specific volume of air 4 to be measured. Since the electromagnetic energy is reflected within this volume the angles of reflection are limited by the maximum θ max and minimum θ 0 angles between the transmitted and received electromagnetic waves. This in turn limits the range acoustic frequencies usable. In order to measure wind moving parallel to the acou¬ stic energy, by the use of the coupling of electromagnetic and acoustic waves, the atmospheric volume illuminated by the RF transmitter and seen by the RF receiver should be modulated by acoustic waves in the frequency range from F θ ( F aco ) nu . n =2 — „ - c aco sin— (3 •» )# rf • * ( κ F a;o' ) max =2 — - ( c aco +V) sin ( — 2 + β ) (4) 'rf where θ 0 is the minimum angle between the electromagnetic beam, and the sector covered by the receiver as shown in figure 1. Figure 2a illustrates the range of acoustic freq¬ uencies giving reflection when no wind is present. The difference in acoustic frequency due to the change in the grating caused by the wind may then be expressed as: This shift in acoustic frequency is illustrated in figure 2b. By emitting acoustic "chirps", preferrably starting at the highest frequency, and correlating the received signal with the emitted acoustic signal, the wind velocity at a specific height may be found. By integrating this over the frequencies of the acoustic signal the wind as a function of height may be found. A similar method may be used by varying the electromagnetic frequency. The change in the grating may of course also be measured by detecting the change in angle by which the electromagnetic energy is received. Using receiver means being able to detect the angle of arrival of the electromagnetic energy will then be another possible variant within the scope of the invention. Consider, as illustrated in figure 3, a case where the acoustic frequency for zero wind is matched with a RF freq¬ uency for scattering angle θ 0 =2α 0 . This requires an acoustic frequency given by If we have a wind velocity V for a fixed acoustic freq- uency, the matching scattering angle becomes and from these equations the change in angle of arrival is found to be The angle of arrival may be measured by measuring the difference in phase of the output of two receiving antennas and using this in the following equation: Δ ΛΩ θ= c Δφ— to ) FD 360 " } where ΔΘ=2Δ , F is the radio frequency, D is the antenna spacing, Δφ is the phase resolution and c is the phase velocity of the radio wave. Figure 4 illustrates an embodiment of the invention for measuring shape of the received wavefront by using three or more receivers positioned in a vertical array. An electro- magnetic wave is scattered towards the receiver at the scat¬ tering angle θ 0 , and a wave scattered at the angle Θ 0 +ΔΘ C is anti-matched with the first, which means that the wavenumber in the second case is changed by a factor 2. This may be expressed as: Thus the difference in scattering angle required for dest¬ ructive coupling is: Q Δθ =2sin '1 (2sin^) -θ n (11) c 2 ° Using equation (8) and the fact that Δθ 0 v=2Δα 0 v+θ 0 is the minimum angle of arrival with a vertical wind velocity V we find that: Substituting θ ov for θ 0 in equation (11) gives the width of the angle of arrival spectrum as a funtion of wind velocity. The spatial correlation of the field strength at the receiver is the Fourier transform of the angular power spectrum. Assuming that this may be expressed as a sine function, the spatial autocorrelation of the field strength is a rectangular function, the width L of which is given as: _rr~ = ^c <") λ rf Δθ. (14) From the equations above the vertical correlation distance may be measured in wavelength as a function of vertical wind velocity. Measuring the time delay of the transmitted signal and thereby the distance of travel to find the wind velocity is another technique within the scope of this invention. Referring to figure 5 we find the following relationship: 1 H ( H 2 (15) where d is the distance between the transmitter and the receiver and 1 is the length of the path of the electromagn¬ etic energy. Knowing that the delay time τ may be expressed as τ 0 =l 0 /c we get the following equation for the minimum time delay: τ "" ~c \ , +1 (16) From equation (8) we know that an increase in wind gives an increase in scattering angle. The corresponding increase in time delay may then be expressed as: (Δτ) - (17) w c 2 J civ 2 / J where Δθ w may be found from equation 8, since Δθ w =2Δ +θ 0 . It may also be of interest to calculate the broadening Δτ=— (θβ 2c EFF μ EFF' (18) of the delay spectrum. This is given by: where β EFF is the effective beamwidth of the electromagnetic beam. This scintillation bandwidth and the spectral shape og the received electromagnetic beam indicates the amount distortion in the acoustic grating. This indicates the degree of turbulence and other small scale disturbances in the air affecting the acoustic beam from the transmitter upwards to the interaction area. By varying the acoustic and electromagnetic frequencies selectively it is possible to make a profile of the turbulence from the acoustic transmitter to a selected height. Air movements essentially perpendicular to both the acoustic and the electromagnetic beam may also be measured with this invention. The grating will be affected by the air movements by shifting sidewards and will behave like the acoustic source was moved, as seen in Figure 6, a distance Δx horisontally where V Δx=H- (19) and H is the height at which the measurement is taken. The electromagnetic energy is reflected in a different direction, and may be received at a new location moved a distance Δx 2 : where R x is the horisontal distance from the transmitter to the measuring area, and R 2 is the horisontal distance from this area to the receivers, as shown in figure 7. By using an array of acoustic transmitters and adjusting their frequency and/or phase until the electromagnetic energy is received by the receiver. This way the air move- ments perpendicular to the acoustic energy may be measured. Alternatively an array of receivers may be used to measure the displacement of the received energy. In case of a vertical gradient of the cross-wind the system will measure the integrated influence of the wind from height zero to the measured volume. If more than one acoustic frequency is used each freguency of the acoustic stimulation will measure at a height H such that it satisfy the Bragg condition. Thus by transmitting several acoustic frequencies in parallel and sequence information is retrieved on the horisontal wind profile. In a similar way wind essentially parallel with the electromagnetic beam will move the grating a distance δD. This may be measured by observing the fact that if the acou¬ stic waves use a time time t to reach a heigth h s satisfying the Bragg conditions in a no-wind situation, the waves will use more time to reach the same height if the grating is moved by the wind. This delay may be measured be measuring the phase of the acoustic signal in the scattering volume. Geometries give the following expression: S 21 F_ c aco ) For a homogeneous wind profile the scattering volume has been shifted a distance where c a is the mean horisontal wind from the ground to the scattering volume. The distance travelled by the acoustic signal is and the acoustic phase φ=K aco h v , where K aco is the wavenumber. Using this and equation 21 and 22 the equation for finding the phase of the acoustic signal is: From this equation the horizontal wind velocity V y may be found by measuring the phase of the scattering acoustic waves. To measure the acoustic phase the electromagnetic receiver receiver means may be syncronized with the acoustic source. The speed of sound being a factor in many of the above mentioned equations, is dependant on the temperature in the air. It may therefore be necessary to measure the tempe¬ rature in the air above the acoustic transmitter. This is preferrably done using standard RASS technology measuring acoustic signal scattered back towards the acoustic transmitter. A possible problem in receiving the electromagnetic signal is to eliminate noise from transmitted electro¬ magnetic signals that have not been scattered in the mentioned air volume. This may be electromagnetic waves received directly from the transmitter, or waves scattered by other prosesses. To avoid this the receiver may be phaselocked to the transmitted electromagnetic frequency minus the transmitted acoustic frequency. By using more than one electromagnetic frequency simultaneously spatial information may be retreived. If the information, such as frequency or phase, in the emitted electromagnetic beam varies in the direction perpendicular to its direction of propation, it will be possible to ident¬ ify the part of the beam reflected from the different parts of the measured volume. When using this invention in connection to air traffic control an already existing ILS transmitter may be employed. Another possibility within the scope of this invention is the use of more than one set of electromagnetic trans¬ mitters and receivers, using the same acoustic transmit¬ ter(s) and measuring the same air volume from a different direction. This gives an abundance of data and more precise measurements. Using more than one electromagnetic and acoustic beams directed in different directions at the same time is also within the scope of the invention. If more than two acoustic transmitters are used in the system they may be positioned in groups separated with a distance larger than the distance between the transmitters within each group.

Claims: C L A I M S 1. A system for the detection and measurement of atmos¬ pheric air movement irregularities such as wind velocity vector, wind shear, downdraft, clear air turbulence, air¬ craft induced vorteces and turbulence, in particular along a glidepath near airports, whereby an air volume under investigation is illuminated by a radio wave transmitter with a beam of essentially coherent electromagnetic energy and a resulting wave field is received and processed in processor means to derive information on the existence of said atmospheric irregularities and furthermore to give specific measurements of related parameters, comprising at least one receiver for said resulting wave field, which is due to scattering in said air volume, positioned at a bistatic location having a selected distance from said transmitter, and also comprising acoustic transmitter means located between said transmitter and said at least one receiver, and adapted to emit acoustic waves into said air volume, c h a r a c t e r i z e d in that the frequency and beamwidth of the acoustic waves is chosen such that a disturbance of the dielectric constant of air in said air volume is created which contributes to said scattering, and that the frequency is chosen such that the disturbance of the dielectric constant formes an essentially periodic gra¬ ting which satisfies the Bragg conditions for the trans¬ mitted electromagnetic energy and thereby reflects the electromagnetic energy in the direction of said at least one receivers, and in that the distance between the acoustic trans¬ mitter and said air volume is less than the distance between said electromagnetic transmitter and the acoustic transmit¬ ter. 2. A system according to claim 1, c h a r a c t e r i z e d in that said acoustic transmitter means are located close to the axis between said electro- magnetic wave transmitter and receiver(s), and that the emitted electromagnetic beam, the emitted acoustic beam and the reflected electromagnetic beam generally define a plane. 3. A system according to claim 1 or 2, c h a r a c t e r i z e d in that the frequency of the acoustic signal is variable. 4. A system according to claim 3, c h a r a c t e r i z e d in that the acoustic signal con¬ sists of frequency chirps, preferrably starting at the high¬ est frequency, each chirp comprising frequencies satisfying the Bragg conditions at a range of height intervals. 5. A system according to any one of claim 1-4, c h a r a c t e r i z e d in that said acoustic transmitter means consists of two or more acoustic transmitters in a one or two-dimensional array, each being capable of transmitting at different variable frequencies. 6. A system according to any one of the preceding claims, c h a r a c t e r i z e d in that said electromagnetic wave transmitter is adapted for emitting electromagnetic waves at one or more variable frequencies, and that said at least one receiver is adapted for detecting the frequency or frequen¬ cies of the received signal. 7. A system according to claim 6, c h a r a c t e r i z e d in that the electromagnetic trans¬ mitter is an ILS transmitter. 8. A system according to any one of the preceding claims, c h a r a c t e r i z e d in comprising at least two recei¬ vers adapted for detecting the frequency, phase and/or ar¬ rival angle of said reflected electromagnetic signal, and thereby being able to locate the measured air movement within said investigated air volume. 9. A system according to claim 8, c h a r a c t e r i z e d by comprising at least three receivers, whereby the shape of the wavefield may be measured, and the degree of small scale disturbance and turbulence in said air volume may be measured. 10. A system according to any one of the preceding claims, c h a r a c t e r i z e d by comprising means for measuring the propagation time used by the electromagnetic energy from said transmitter to said receiver(s). 11. A system according to any one of the preceding claims, c h a r a c t e r i z e d by comprising means for measuring the spectral beamwidth and spectral shape of the received electromagnetic energy at one or more acoustic frequencies in order to measure and classify turbulence and other disturbances between said acoustic transmitter (2) means and the scattering volume (4) . 12. A system according to any one of the preceding claims, c h a r a c t e r i z e d in that the electromagnetic rece¬ iver means are phaselocked to the transmitted electromagnetic frequency minus the transmitted acoustic frequency. 13. A method for measuring wind components along the direction of said electromagnetic beam using a system according to one or more of the claims 1-12, c h a r a c t e r i z e d by measuring the mean acoustic phaseshift of said transmitted acoustic signal due to the displacement of said air volume, using said received, scat¬ tered electromagnetic waves, and thereby calculating the wind velocity. 14. A method for measuring the wind profile using a system according to one or more of the claims 1-12, c h a r a c t e r i z e d in that the air movements in said air volume having components parallel to the progating acoustic energy are measured by one or more of the following techniques: i) measuring the angle of arrival of the scattered electromagnetic energy as a function of the emitted acoustic frequency, ii) detecting the acoustic frequencies resulting in disturbances contributing to said scattering of the electromagnetic energy towards said receiver means, and calculating the velocities and height of said air movements on on the basis of the detected acoustic frequencies and the time distribution of the emitted and received acoustic frequencies, iii) measuring the time delay of the electromagnetic energy scattered in said air volume as a function of acoustic frequency, and iv) measuring the correlation distance of the received wavefield and calculating the vertical dimensions of said scattering volume. 15. A method for measuring wind profile using a system according to claims 1-12, c h a r a c t e r i z e d in that air movements having components prependicular to the emitted acoustic energy are measured by measuring the displacement of said disturbance in the dielectric constant in the air due to the movements in the air by using one of the following techniques: i) by measuring the displacement of the emitted acoustic signal by emitting different frequencies at different locations in an acoustic array and correlating the angle of arrival of the electromagnetic signal with the displaced scattering acoustic frequency, or ii) by measuring the displacement of the received electro¬ magnetic energy as a function of angles of arrival and/or variabel emitted acoustic frequencies.

Inventors: GJESSING DAG T, HJELMSTAD JENS, TONNING ANDREAS, GJESSING, DAG, T., HJELMSTAD, JENS, TONNING, ANDREAS
Applicants: GJESSING DAG T, HJELMSTAD JENS, TONNING ANDREAS, TRIAD A S, GJESSING, DAG, T., HJELMSTAD, JENS, TONNING, ANDREAS, TRIAD A.S
Application year: 1996
Main classification: G01S13
IPC codes: G01S13