Patent US1716096A successfully refreshed from Google Patents.
Patent US4329053A successfully refreshed from Google Patents.
US4329053A
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Frequency-scanning particle size spectrometer
Assignee: National Aeronautics and Space Administration
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Filing: 1979-08-10
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Granted: 1982-05-11
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Expires: 1999-08-10
Abstract
Abstract A particle size spectrometer having a fixed field of view within the forward light scattering cone at an angle θ s between approximately 100 and 200 minutes of arc (preferably at 150 minutes), a spectral range extending approximately from 0.2 to 4.0 inverse micrometers (μm -1 ), and a spectral resolution between about 0.1 and 0.2 μm -1 (preferably toward the lower end of this range of spectral resolution), is employed to determine the distribution of particle sizes, independently of the chemical composition of the particles, from measurements of incident light, I o , at each frequency, σ (=1/λ), and scattered light, I(σ), according to the equation: ##EQU1## where l=2πsinθ, θ being the fixed viewing angle θ s at which scattered light is measured, r is particle size, σ is the reciprocal of wavelength, J 1 is a Bessel function of first kind and order unity, Y 1 is a Bessel function of second kind and order unity. The quantity, I.sub.σ, is the ratio of scattered light to incident light at each frequency interval. The apparatus is a passive remote sensor that can be used in laboratories, field stations, flying aircrafts and airships, and on board an orbiting satellite.
Inventors
- 👤 with respect to an invention of Fletcher James C. Administrator of the National Aeronautics and Space Administration
- 👤 Alain L. Fymat
Bibliographic Details
Application Number
—
Jurisdiction
US
Data Source
google_patents
Last Synchronized
2026-11-06 17:50
CPC Classifications
G; G01; G01N; G01N15/00; G01N15/02; G01N15/0205
Claims Analysis
Total Claims: 12
Claim 1
Independent Claim
341 words
A method for producing data values from forward scattered light for determining the size distribution of particles dispersed in a volume of gas independently of the refractive indices of the particles so that their chemical composition need not be known, even with a number of different species of particles dispersed in the volume, and even with a number of different species of gas in the volume, said method comprising the steps of varying the wavelength of light incident on said particles in said volume in incremental steps within a total spectral range of about 0.20≦σ≦4.0 μm -1 , where σ is the wavenumber equal to the reciprocal of wavelength λ, and the steps over this total range are at intervals of wavenumber, Δσ, of less than about 0.2 μm -1 , and for each interval, producing a signal representative of the wavenumber σ, for each wavenumber, detecting at a fixed viewing angle the intensity of light forward scattered in a narrow cone by said particles in said volume, said fixed viewing angle being between 100 and 200 minutes of arc from the axis of the scattering cone which coincides with the direction of incident light, and from the intensity, I(σ), of scattered light detected, generating a first electrical signal representing the value of intensity of forward scattered light at the narrow angle of detection, for each wavenumber, detecting the intensity, I o , of incident light and generating a second electrical signal representative of the intensity of incident light at the time forward scattered light is detected for the wavenumber, dividing the signal representative of the intensity of forward scattered light, I(σ), for each wavenumber by the signal representative of the intensity of incident light, I o , for the same wavenumber to obtain a signal representative of normalized forward scattered light, I.sub.σ, thereby to provide a set of data for use in determining particle size distribution, n(r), for various values of radius, r, larger than approximately 1 μm as a function of the wavenumber σ and normalized scattered light, I.sub.σ.
Claim 2
Independent Claim
341 words
A method for producing data values from forward scattered light for determining the size distribution of particles dispersed in a volume of gas independently of the refractive indices of the particles so that their chemical composition need not be known, even with a number of different species of particles dispersed in the volume, and even with a number of different species of gas in the volume, said method comprising the steps of varying the wavelength of light incident on said particles in said volume in incremental steps within a total spectral range of about 0.20≦σ≦4.0 μm -1 , where σ is the wavenumber equal to the reciprocal of wavelength λ, and the steps over this total range are at intervals of wavenumber, Δσ, of less than about 0.2 μm -1 , and for each interval, producing a signal representative of the wavenumber σ, for each wavenumber, detecting at a fixed viewing angle the intensity of light forward scattered in a narrow cone by said particles in said volume, said fixed viewing angle being between 100 and 200 minutes of arc from the axis of the scattering cone which coincides with the direction of incident light, and from the intensity, I(σ), of scattered light detected, generating a first electrical signal representing the value of intensity of forward scattered light at the narrow angle of detection, for each wavenumber, detecting the intensity, I o , of incident light and generating a second electrical signal representative of the intensity of incident light at the time forward scattered light is detected for the wavenumber, dividing the signal representative of the intensity of forward scattered light, I(σ), for each wavenumber by the signal representative of the intensity of incident light, I o , for the same wavenumber to obtain a signal representative of normalized forward scattered light, I.sub.σ, thereby to provide a set of data for use in determining particle size distribution, n(r), for various values of radius, r, larger than approximately 1 μm as a function of the wavenumber σ and normalized scattered light, I.sub.σ.
Claim 3
Dependent Claim
16 words
The method as defined in claim 1 wherein said viewing angle is 150 minutes of arc.
Claim 4
Dependent Claim
16 words
The method of claim 1 or 2 wherein said spectral range is 0.198≦σ≦4.070 μm -1 .
Claim 5
Dependent Claim
26 words
The method of claim 1 or 2 wherein said incremental steps are at intervals of wavenumber, Δσ, selected to be less than 0.2 μm -1 .
Claim 6
Dependent Claim
36 words
A method as defined in claim 1 or 2 wherein said spectral range is 0.198≦σ4.070 μm -1 and said incremental steps are at intervals of wavenumber, Δσ, selected to be less than 0.2 μm -1 .
Claim 7
Dependent Claim
345 words
Apparatus for producing data values from forward scattered light for determining the size distribution of particles dispersed in a volume of gas independently of the refractive indices of the particles so that their chemical composition need not be known, even with a number of different species of particles dispersed in the volume, and even with a number of different species of gas in the volume, said apparatus comprising means for varying the wavelength of light incident on said particles in said volume in incremental steps within a total spectral range of about 0.20≦σ≦4.0 μm -1 , where σ is the wavenumber equal to the reciprocal of wavelength λ, and the steps over this total range are at intervals of wavenumber, Δσ, of less than about 0.2 μm -1 , and for each interval, producing a signal representative of the wavenumber, σ, means for detecting at a fixed viewing angle for each wavenumber the intensity of light forward scattered in a narrow cone by said particles in said volume, said fixed viewing angle being between 100 and 200 minutes of arc from the axis of the scattering cone which coincides with the direction of incident light, and from the intensity, I(σ), of scattered light detected, generating a first electrical signal representing the value of intensity of forward scattered light at the narrow angle of detection, means for detecting the intensity, I o , of incident light for each wavenumber and generating a second electrical signal representative of the intensity of incident light at the time forward scattered light is detected for the wavenumber. means for dividing the signal representative of the intensity of forward scattered light, I(σ), for each wavenumber by the signal representative of the intensity of incident light, I o , for the same wavenumber to obtain a signal representative of normalized forward scattered light, I.sub.σ, thereby to provide a set of data for use in determining particle size distribution, n(r), for various values of radius, r, larger than approximately 1 μm as a function of the wavenumber, σ, and normalized scattered light, I.sub.σ.
Claim 8
Dependent Claim
345 words
Apparatus for producing data values from forward scattered light for determining the size distribution of particles dispersed in a volume of gas independently of the refractive indices of the particles so that their chemical composition need not be known, even with a number of different species of particles dispersed in the volume, and even with a number of different species of gas in the volume, said apparatus comprising means for varying the wavelength of light incident on said particles in said volume in incremental steps within a total spectral range of about 0.20≦σ≦4.0 μm -1 , where σ is the wavenumber equal to the reciprocal of wavelength λ, and the steps over this total range are at intervals of wavenumber, Δσ, of less than about 0.2 μm -1 , and for each interval, producing a signal representative of the wavenumber, σ, means for detecting at a fixed viewing angle for each wavenumber the intensity of light forward scattered in a narrow cone by said particles in said volume, said fixed viewing angle being between 100 and 200 minutes of arc from the axis of the scattering cone which coincides with the direction of incident light, and from the intensity, I(σ), of scattered light detected, generating a first electrical signal representing the value of intensity of forward scattered light at the narrow angle of detection, means for detecting the intensity, I o , of incident light for each wavenumber and generating a second electrical signal representative of the intensity of incident light at the time forward scattered light is detected for the wavenumber. means for dividing the signal representative of the intensity of forward scattered light, I(σ), for each wavenumber by the signal representative of the intensity of incident light, I o , for the same wavenumber to obtain a signal representative of normalized forward scattered light, I.sub.σ, thereby to provide a set of data for use in determining particle size distribution, n(r), for various values of radius, r, larger than approximately 1 μm as a function of the wavenumber, σ, and normalized scattered light, I.sub.σ.
Claim 9
Dependent Claim
15 words
Apparatus as defined in claim 6 wherein said viewing angle is 150 minutes of arc.
Claim 10
Dependent Claim
17 words
Apparatus as defined in claim 6 or 7 wherein said spectral range is 0.198≦σ≦4.070 μm -1 .
Claim 11
Dependent Claim
27 words
Apparatus as defined in claim 6 or 7 wherein said incremental steps are at intervals of wavenumber Δσ selected to be less than 0.2 μm -1 .
Claim 12
Dependent Claim
35 words
Apparatus as defined in claim 6 or 7 wherein said spectral range is 0.198≦σ4.070 μm -1 and said incremental steps are at intervals of wavenumber, Δσ, selected to be less than 0.2 μm -1 .
References Cited (Backward Citations)
US2788702A
Cited
US3724951A
Cited
USPTO Annuity & Maintenance Windows
| Annuity Stage | Window Opens | Payment Deadline | Surcharge Period Until | Estimated Fee | Status |
|---|---|---|---|---|---|
| 3.5 Years (Year 4) | 1985-05-10 | 1985-11-09 | 1986-05-11 | $2000.00 | Window Closed / Lapsed |
| 7.5 Years (Year 8) | 1989-05-10 | 1989-11-09 | 1990-05-11 | $3760.00 | Window Closed / Lapsed |
| 11.5 Years (Year 12) | 1993-05-10 | 1993-11-09 | 1994-05-11 | $7700.00 | Window Closed / Lapsed |