US4986656A
Expired / Lapsed
US
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Method of remotely measuring diffuse attenuation coefficient of sea water
Assignee: General Dynamics Government Systems Corp
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Filing: 1989-11-30
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Granted: 1991-01-22
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Expires: 2009-11-30
Abstract
Abstract A method of remotely measuring the diffuse attenuation coefficient K of ocean water from an airborne platform such as an aircraft. By directing a pulsed laser beam having a wavelength λ 0 from the platform into the water, the beam interacts therewith to produce inelastic Brillouin backscatter signals at the wavelength λ 1 , where λ 1 ≠λ 0 . The desired backscatter propagate generally oppositely to the direction of propagation of the pulsed laser beam so that the backscatter can be received and collected at the platform. The upwelling optical energy includes the desired backscatter signals, which are separated out from the remainder of the upwelling optical energy. The separated backscatter signals are converted to equivalent electrical signals and periodically analyzed to generate therefrom the diffuse attenuation coefficient of the ocean water at the λ 1 wavelength at periodic depths beneath the water surface. In another aspect of this invention both the Brillouin backscatter signals and the Raman backscatteer signals are separately filtered out to simultaneously measure the diffuse attenuation coefficient of the water at two distinct wavelengths. In another aspect of this invention the diffused attenation coefficient K is measured from a submerged platform, such as a submarine. This has the advantage of allowing deep ocean layers to be measured along with ocean water beneath the polar ice cap.
Inventors
- 👤 Harold E. Sweeney
- 👤 Paul J. Titterton
- 👤 Donald A. Leonard
Bibliographic Details
Application Number
—
Jurisdiction
US
Data Source
google_patents
Last Synchronized
2026-11-09 21:10
CPC Classifications
G; G01; G01J; G01J3/00; G01J3/28; G01J3/44; G01N; G01N21/00; G01N21/17; G01N21/47; G01N21/49; G01N21/53; G01J3/12; G01J2003/1226; G01J2003/1252; G01J3/26; G01N2021/1793; G01N2201/00; G01N2201/02; G01N2201/021; G01N2201/0214
Claims Analysis
Total Claims: 13
Claim 1
Independent Claim
126 words
A remote method of measuring the diffuse attenuation coefficient of ocean water comprising of the steps of: from an airborne platform over said water generating a pulsed laser probe beam having a wavelength λ o ; directing said probe beam downwardly into said water thereby causing said probe beam to interact with said water and producing at least backscatter signals at the wavelength λ 1 , where λ 1 ≠λ o , and propagating generally oppositely to the direction of propagation of said probe beam; receiving at said airborne platform upwelling optical energy including said backscatter signals; separating out said backscatter signals from said upwelling optical energy; and analyzing said backscatter signals and generating therefrom the diffuse attenuation coefficient of said ocean water at said wavelength.
Claim 2
Dependent Claim
126 words
A remote method of measuring the diffuse attenuation coefficient of ocean water comprising of the steps of: from an airborne platform over said water generating a pulsed laser probe beam having a wavelength λ o ; directing said probe beam downwardly into said water thereby causing said probe beam to interact with said water and producing at least backscatter signals at the wavelength λ 1 , where λ 1 ≠λ o , and propagating generally oppositely to the direction of propagation of said probe beam; receiving at said airborne platform upwelling optical energy including said backscatter signals; separating out said backscatter signals from said upwelling optical energy; and analyzing said backscatter signals and generating therefrom the diffuse attenuation coefficient of said ocean water at said wavelength.
Claim 3
Dependent Claim
14 words
The method according to claim 1 wherein said backscatter signals further comprise inelastic backscatter.
Claim 4
Dependent Claim
16 words
The method according to claim 2 wherein said backscatter signals further comprise Brillouin and Raman backscatter.
Claim 5
Dependent Claim
39 words
The method according to claim 2 wherein said analyzing step further comprises: analyzing said backscatter signals at periodic intervals of time and generating therefrom the diffuse attenuation coefficient of said ocean water at periodic depths beneath the ocean surface.
Claim 6
Independent Claim
128 words
A method of measuring the diffuse attenuation coefficient of ocean water from beneath the ocean surface comprising the steps of: from a submerged platform generating a pulsed laser probe beam having a wavelength λ o ; directing said probe beam away from said platform into said water thereby causing said probe beam to interact with said water and producing at least backscatter signals at the wavelength λ 1 , where λ 1 ≠λ o , and propagating generally oppositely to the direction of propagation of said probe beam; receiving at said submerged platform optical energy including said backscatter signals; and periodically analyzing said backscatter signals and generating therefrom the diffuse attenuation coefficient of said ocean water at said λ 1 wavelength at periodic distances from said submerged platform.
Claim 7
Independent Claim
128 words
A method of measuring the diffuse attenuation coefficient of ocean water from beneath the ocean surface comprising the steps of: from a submerged platform generating a pulsed laser probe beam having a wavelength λ o ; directing said probe beam away from said platform into said water thereby causing said probe beam to interact with said water and producing at least backscatter signals at the wavelength λ 1 , where λ 1 ≠λ o , and propagating generally oppositely to the direction of propagation of said probe beam; receiving at said submerged platform optical energy including said backscatter signals; and periodically analyzing said backscatter signals and generating therefrom the diffuse attenuation coefficient of said ocean water at said λ 1 wavelength at periodic distances from said submerged platform.
Claim 8
Independent Claim
115 words
A method of measuring the diffuse attenuation coefficient of ocean water consisting of the steps of: from an aircraft travelling over said ocean water, generating a pulsed laser probe beam and directing said probe beam downwardly into said water thereby causing said probe beam to interact with said water to produce Brillouin and Raman backscatter signals, at least a portion of said signals propagating upwardly toward said aircraft; receiving at aircraft upwelling optical energy including said backscatter signals; separating said Brillouin and Raman signals from said upwelling optical energy; and generating from the Brillouin and Raman signals the diffuse attenuation coefficient of the ocean water at the respective wavelengths of said Brillouin and Raman backscatter.
Claim 9
Independent Claim
115 words
A method of measuring the diffuse attenuation coefficient of ocean water consisting of the steps of: from an aircraft travelling over said ocean water, generating a pulsed laser probe beam and directing said probe beam downwardly into said water thereby causing said probe beam to interact with said water to produce Brillouin and Raman backscatter signals, at least a portion of said signals propagating upwardly toward said aircraft; receiving at aircraft upwelling optical energy including said backscatter signals; separating said Brillouin and Raman signals from said upwelling optical energy; and generating from the Brillouin and Raman signals the diffuse attenuation coefficient of the ocean water at the respective wavelengths of said Brillouin and Raman backscatter.
Claim 10
Dependent Claim
73 words
The method according to claim 6 wherein said last mentioned generating step further comprises: converting said Brillouin and Raman backscatter signals respectively, from optical signals into Brillouin electrical signals and Raman electrical signals., periodically digitizing said respective electrical signals; and processing said digitized Brillouin electrical signals and said digitized Raman electrical signals, and producing therefrom the diffuse attenuation coefficients of said ocean water at the Brillouin and Raman wavelengths, respectively, at periodic depths.
Claim 11
Dependent Claim
24 words
The method according to claim 6 wherein said separating step further comprises: filtering said Brillouin and Raman signals with respective narrowband optical bandpass filters.
Claim 12
Dependent Claim
262 words
A remote method of measuring the diffuse attenuation coefficient of ocean water comprising of the steps of: from an airborne platform over said water generating a pulsed laser probe beam having a wavelength λ o ; directing said pulsed laser probe beam into said water, said beam interacting with said water and producing at least a pulsed backscatter signal at the wavelength λ 1 , where λ 1 ≠λ o , and generally propagating oppositely to the direction of propagation of said probe beam; receiving at said airborne platform upwelling optical energy including said pulsed backscatter signal; filtering said upwelling optical energy to pass only said pulsed backscatter signal; converting said pulsed backscatter signal into a corresponding pulsed electrical signal; measuring the time differential between each pulse of said pulsed laser probe beam and each corresponding pulse of said pulsed backscatter signal for computing the altitude H of said airborne platform, periodically digitizing at predetermined time intervals each pulse of said pulsed electrical signal, for generating I B (D n ) where I B (D n ) represents the signal intensity of the n th sample of each pulse, D o corresponding to the water surface; and calculating the diffuse attenuation coefficient of said ocean water at the wavelength λ 1 by making the following computations: ##EQU5## where, I B (D n )=intensity at depth D n ; I B (D n+1 )=intensity at depth D n+1 ; ΔD=D n+1 -D n ; ln=natural log; and K B =diffuse attenuation coefficient over the depth interval between D n and D n+1 :
Claim 13
Dependent Claim
262 words
A remote method of measuring the diffuse attenuation coefficient of ocean water comprising of the steps of: from an airborne platform over said water generating a pulsed laser probe beam having a wavelength λ o ; directing said pulsed laser probe beam into said water, said beam interacting with said water and producing at least a pulsed backscatter signal at the wavelength λ 1 , where λ 1 ≠λ o , and generally propagating oppositely to the direction of propagation of said probe beam; receiving at said airborne platform upwelling optical energy including said pulsed backscatter signal; filtering said upwelling optical energy to pass only said pulsed backscatter signal; converting said pulsed backscatter signal into a corresponding pulsed electrical signal; measuring the time differential between each pulse of said pulsed laser probe beam and each corresponding pulse of said pulsed backscatter signal for computing the altitude H of said airborne platform, periodically digitizing at predetermined time intervals each pulse of said pulsed electrical signal, for generating I B (D n ) where I B (D n ) represents the signal intensity of the n th sample of each pulse, D o corresponding to the water surface; and calculating the diffuse attenuation coefficient of said ocean water at the wavelength λ 1 by making the following computations: ##EQU5## where, I B (D n )=intensity at depth D n ; I B (D n+1 )=intensity at depth D n+1 ; ΔD=D n+1 -D n ; ln=natural log; and K B =diffuse attenuation coefficient over the depth interval between D n and D n+1 :
References Cited (Backward Citations)
USPTO Annuity & Maintenance Windows
| Annuity Stage | Window Opens | Payment Deadline | Surcharge Period Until | Estimated Fee | Status |
|---|---|---|---|---|---|
| 3.5 Years (Year 4) | 1994-01-21 | 1994-07-23 | 1995-01-22 | $2000.00 | Window Closed / Lapsed |
| 7.5 Years (Year 8) | 1998-01-21 | 1998-07-23 | 1999-01-22 | $3760.00 | Window Closed / Lapsed |
| 11.5 Years (Year 12) | 2002-01-21 | 2002-07-23 | 2003-01-22 | $7700.00 | Window Closed / Lapsed |