Patent US4608147A successfully refreshed from Google Patents.
US4523841A
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US
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Radiant energy reradiating flow cell system and method
Assignee: Coulter Electronics Inc
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Filing: 1979-03-15
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Granted: 1985-06-18
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Expires: 1999-03-15
Abstract
Abstract In an apparatus in which particles which may include biological cells are passed through an optical sensing zone to measure their spatial radiant energy distribution for the purpose of identifying and/or characterizing the particles or cells, a structure and method are provided for increasing the usefulness of a geometric configuration of photovoltaic detectors such as a known assembly of generally concentric rings of such detectors usually including some wedge-shaped detectors. These are provided in a generally planar form and the invention provides structure which captures radiant energy in a flow cell of a particular type before projecting the energy to the detector. In particular an ellipsoid, paraboloid, hyperboloid or similar reflector which is symmetrical about its optical axis is utilized first to capture the radiant energy on angles which could include most forward and/or backward angles and all azimuthal angles and then deviating the same to the detector assembly mentioned. By moving the arrangement or assembly of detectors along the optical axis of the reflector the optimum distance is established for obtaining the greatest amount of information sought. Although the assembly of photovoltaic detectors may thereafter be left in place, it is preferred to substitute for said assembly a second highly economical deviating or reflecting device capable of capturing the radiant energy which would otherwise have fallen on the sensitive plane of the assembly of photovoltaic detectors and deviating the same along a plurality of different spaced paths to independent photodetecting devices.
Inventors
- 👤 Albert Brunsting
- 👤 Walter R. Hogg
Bibliographic Details
Application Number
—
Jurisdiction
US
Data Source
google_patents
Last Synchronized
2026-11-03 21:20
CPC Classifications
G; G01; G01N; G01N15/00; G01N15/10; G01N15/14; G01N15/1434; G01N15/1436; G01N21/00; G01N21/17; G01N21/47; G01N15/1456; G01N15/1459; G01N21/01; G01N21/03; G01N21/05; G01N2021/052; G01N2021/4704; G01N2021/4711; G01N2021/4716
Claims Analysis
Total Claims: 8
Claim 1
Independent Claim
247 words
A method of measuring the directional distributional properties of the radiant energy reradiated from a particle for characterization or the like of said particle and using a known integral configuration of photovoltaic detectors having a sensitive front planar surface which method comprises: A. Passing the particle through a sensing zone located on the interior of a concave reflector whose configuration is substantially defined by a geometric law, the reflector being symmetrical about an optical axis and having a first focal point also defined by said geometric law, the sensing zone being at said first focal point, B. directing a beam of incident radiant energy along said axis to said sensing zone, C. intercepting the radiant energy which has been reradiated by said particle and emerging from the front or said reflector at said planar surface, D. adjusting the integral configuration along said axis while maintaining its disposition relative to the axis in order to modify the response of said photovoltaic detectors due to said reradiated radiant energy from said particle, and thereafter E. removing the integral configuration and substituting therefor a composite optical member having the property of separating the received reradiated energy from said particles into plural individual ray groups and directing said ray groups along an equivalent plural number of respective paths, each group having a different direction relative to one another and a direction divergent from the said axis, and measuring the said individual ray groups separately by respective interception of said plural paths.
Claim 2
Independent Claim
247 words
A method of measuring the directional distributional properties of the radiant energy reradiated from a particle for characterization or the like of said particle and using a known integral configuration of photovoltaic detectors having a sensitive front planar surface which method comprises: A. Passing the particle through a sensing zone located on the interior of a concave reflector whose configuration is substantially defined by a geometric law, the reflector being symmetrical about an optical axis and having a first focal point also defined by said geometric law, the sensing zone being at said first focal point, B. directing a beam of incident radiant energy along said axis to said sensing zone, C. intercepting the radiant energy which has been reradiated by said particle and emerging from the front or said reflector at said planar surface, D. adjusting the integral configuration along said axis while maintaining its disposition relative to the axis in order to modify the response of said photovoltaic detectors due to said reradiated radiant energy from said particle, and thereafter E. removing the integral configuration and substituting therefor a composite optical member having the property of separating the received reradiated energy from said particles into plural individual ray groups and directing said ray groups along an equivalent plural number of respective paths, each group having a different direction relative to one another and a direction divergent from the said axis, and measuring the said individual ray groups separately by respective interception of said plural paths.
Claim 3
Dependent Claim
22 words
The method as claimed in claim 1 in which the separation is effected by deviation in transmission through said composite optical member.
Claim 4
Dependent Claim
20 words
The method as claimed in claim 1 in which the separation is effected by deviation from said composite optical member.
Claim 5
Independent Claim
277 words
A method of measuring the directional distributional properties of the radiant energy reradiated from a particle for characterization or the like of said particle and using a known integral configuration of photovoltaic detectors having a sensitive front planar surface which method comprises: A. Passing the particle through a sensing zone located on the interior of a concave reflector whose configuration is substantially defined by the geometric law for an ellipsoid, the reflector being symmetrical about an optical axis and having a first focal point also defined by said geometric law, the sensing zone being at said first focal point, B. directing a beam of incident radiant energy along said axis to said sensing zone, C. passing the reradiated radiant energy from said particles through an aperture for the suppression of stray light at the second focal point of said ellipsoid before intercepting the same, D. intercepting the radiant energy which has been reradiated by said particle and emerging from the front of said reflector at said planar surface, E. adjusting the integral configuration along the axis while maintaining its disposition relative to the axis in order to modify the response of said photovoltaic detectors due to said reradiant radiant energy from said particle, and thereafter F. removing the integral configuration and substituting therefor a composite optical member having the property of separating the received reradiated radiant energy into plural individual ray groups and directing said ray groups along an equivalent plural number of respective paths, each having a different direction relative to one another and a direction divergent from the said axis, and measuring the said individual ray groups separately by respective interception of said plural paths.
Claim 6
Independent Claim
277 words
A method of measuring the directional distributional properties of the radiant energy reradiated from a particle for characterization or the like of said particle and using a known integral configuration of photovoltaic detectors having a sensitive front planar surface which method comprises: A. Passing the particle through a sensing zone located on the interior of a concave reflector whose configuration is substantially defined by the geometric law for an ellipsoid, the reflector being symmetrical about an optical axis and having a first focal point also defined by said geometric law, the sensing zone being at said first focal point, B. directing a beam of incident radiant energy along said axis to said sensing zone, C. passing the reradiated radiant energy from said particles through an aperture for the suppression of stray light at the second focal point of said ellipsoid before intercepting the same, D. intercepting the radiant energy which has been reradiated by said particle and emerging from the front of said reflector at said planar surface, E. adjusting the integral configuration along the axis while maintaining its disposition relative to the axis in order to modify the response of said photovoltaic detectors due to said reradiant radiant energy from said particle, and thereafter F. removing the integral configuration and substituting therefor a composite optical member having the property of separating the received reradiated radiant energy into plural individual ray groups and directing said ray groups along an equivalent plural number of respective paths, each having a different direction relative to one another and a direction divergent from the said axis, and measuring the said individual ray groups separately by respective interception of said plural paths.
Claim 7
Dependent Claim
38 words
The method as claimed in claim 4 in which the beam of incident radiant energy is directed from the rear of the reflector to said sensing zone whereby to provide primarily information on reradiation directed initially mostly backwards.
Claim 8
Dependent Claim
37 words
The method as claimed in claim 4 in which the beam of incident radiant energy is directed from the front of the reflector to said sensing zone whereby to provide primarily information on reradiation directed initially forwards.
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USPTO Annuity & Maintenance Windows
| Annuity Stage | Window Opens | Payment Deadline | Surcharge Period Until | Estimated Fee | Status |
|---|---|---|---|---|---|
| 3.5 Years (Year 4) | 1988-06-17 | 1988-12-17 | 1989-06-18 | $2000.00 | Window Closed / Lapsed |
| 7.5 Years (Year 8) | 1992-06-17 | 1992-12-17 | 1993-06-18 | $3760.00 | Window Closed / Lapsed |
| 11.5 Years (Year 12) | 1996-06-17 | 1996-12-17 | 1997-06-18 | $7700.00 | Window Closed / Lapsed |