Instrument responsive to back-scattered or back-reflected radiation having passive system for range correction

• US 3,998,552 A
• Filed: 08/19/1974
• Issued: 12/21/1976
• Est. Priority Date: 08/19/1974
• Status: Expired due to Term

• Current Assignee: HSS Incorporated (UnitedHealth Group Incorporated)
• Original Assignee: HSS Incorporated (UnitedHealth Group Incorporated)
• Inventors: Brouwer, Willem, Stewart, Harold S., Shuler, Marion P. Jr.
• Primary Examiner(s): Corbin, John K.
• Assistant Examiner(s): Clark, Conrad
• Application Number:
  US05/498,372
• Time in Patent Office: 855 Days
• Field of Search: 356/103, 356/104, 356/225, 356/28, 350/206, 250/237 R, 250/574, 354/59
• US Class Current: 356/342
• CPC Class Codes: G01N 21/53 within a flowing fluid, e.g. smoke
• CPC Class Codes: G01S 7/4812 transmitted and received beams following a coaxial path

Abstract

An instrument for responding to backscattered or backreflected radiation from a path through a medium in which a beam of electromagnetic radiation is transmitted along the path, and a receiver system is arranged to receive backscattered radiation returning along the path substantially coaxially with the beam, the receiver system including detection means for the backscattered radiation and equalizing means for producing a substantially equal response regardless of the point of backscatter along the path. The equalizing means comprises a passive radiation transmission structure interposed in the path of return prior to the detection means, the passive structure having a substantially constant acceptance solid-angle for the returning radiation from points over the range of the path whereby radiation reaching the detection means from various points along the path does not vary in intensity due to the different distances of the points from the detection means. The passive structure is shown in the form of a full circular hole and a doughnut-shaped hole in an opaque plate, with the return beam focused to fill the hole out to a range of interest. Other passive structures are illustrated by a Fabry-Perot filter combined with a telescope and a bundle of opaque walled tubes. Transmissivity of a medium out to a point r is determined by the ratio of the integral of power from r to an outer limit range L in which the passive structure is still functional, as numerator, over the integral from the instrument to limit L as denominator. The coaxial array is shown achieved by use of a beam splitter, the beam from the source proceeding via the beam-splitter outwardly, the beamsplitter sized so that all return signal reaching the detector is treated equally by the beam-splitter. A multiple beam-splitter is shown by which multiple beams from a single source are produced, with the respective returns concentrated on a single detector.

Claims

1. In a radiometric instrument for responding to the intensity of backscattered including backreflected radiation from a path through a medium over a given desired detection range comprising means for transmitting a beam of electromagnetic radiation along said path, and a receiver system arranged to receive backscattered radiation returning along said path substantially coaxially with said beam, the receiver system including detection means for the backscattered radiation and equalizing means for producing a substantially equal receiver sensitivity regardless of the distance of the point of backscatter along the path, the improvement wherein said equalizing means comprises a passive radiation transmission structure interposed in the path of return prior to said detection means, said passive structure defining a substantially constant acceptance solid-angle for said returning radiation from points extending over said range of said path, and means defining the diameter of said beam to lie throughout said range substantially within the bounds defined by said solid angle whereby radiation reaching said detection means from various points spaced apart along said path over said range does not vary in intensity due to different sensitivity of said receiver system for different distances of said points from said detection means.

2. The instrument of claim 1 wherein said passive equalizing structure comprises an opaque plate having a transmission hole in it, said hole aligned with said path, and means to focus said backscatter into a return beam of diameter varying with the inverse of the distance of the point of origin of the backscatter relative to said detection means, said return beam striking said plate in alignment with said hole, said hole having a sufficiently small size such that, for backscatter returning from all points over said range of said path, said return beam is larger at said aperture than said hole, peripheral portions of said beam being intercepted by said plate and thereby prevented from reaching said detection means, more of said return beam reaching said detector means the further the point of backscatter is from said detection means.

3. The instrument of claim 2 wherein said equalizing means comprises a lens forming a convergent beam at said hole.

4. The instrument of claim 2 wherein said hole is provided with an opaque center and said lens is provided with a central obscuration, the optics system thus defined constructed and arranged to establish a minimum range for detection of backscattered radiation.

5. The instrument of claim 1 wherein said means for transmitting said beam of radiation comprises a source of said radiation, a partially silvered mirror positioned to receive radiation from said source and to reflect said radiation outwardly toward said path, said receiver means including said passive structure and said detection means positioned behind said partially silvered mirror in alignment with the axis of the initial beam reflected by said mirror whereby backscattered radiation passes through said partially silvered mirror thence through said passive structure to said detection means.

6. The instrument of claim 5 including a second mirror positioned to receive source radiation which passes through said partially silvered mirror and to reflect said radiation outwardly in a beam substantially parallel to that of said partially silvered mirror, said second mirror serving also to receive backscattered radiation and directing it to reflect off of the back side of said partially silvered mirror thence to said passive structure and said detection means.

7. The instrument of claim 6 wherein said passive equalizing structure comprises an opaque plate having a transmission hole in it, said hole aligned with said path, and means to focus said backscatter into a return beam of diameter varying with the inverse of the distance of the point of origin of the backscatter relative to said detection means, said return beam striking said plate in alignment with said hole, said hole having a sufficiently small size such that, for backscatter returning from all points over the range of said path, said return beam is larger at said aperture than said hole, peripheral portions of said beam being intercepted by said plate and thereby prevented from reaching said detection means, more of said return beam reaching said detector means the further the point of backscatter is from said detection means.

8. The instrument of claim 7 wherein said equalizing means comprises a lens forming a convergent beam at said hole.

9. The instrument of claim 1 wherein said means for transmitting said beam of radiation, said detection means and said passive structure having a substantially constant acceptance solid angle are mounted in close proximity to one another.

10. The instrument of claim 1 including means to determine effectively the integrals ∫

_r^L P_x dx and ∫

_o^L P_x dx, thus to enable the transmission of the medium to be determined from the relationship. ##EQU8## where T_r is the transmission from the instrument to selected range r, P_x dx is the detected power resulting from scattering from the beam in range element dx at range x and L is the limit of the range, greater than r, in which the constant solid acceptance angle is maintained, this formula effective when all or substantially all of the detected power is received from scatter points within limit L.

11. The instrument of claim 10 wherein the beam is continuous, the detected power represents scattering from all points out to L, and the means to effectively obtain the integral ∫

_r^L P_x dx includes means for preventing certain backscatter of the continuous beam from reaching the detector.

12. The instrument of claim 11 wherein a black absorber is caused to intercept and absorb all radiation beyond r to enable formation of the integral ∫

_o^r P_x dx whereby the integral ∫

_r L P_r^L P_x dx can be effectively obtained by the relationship ∫

_r^L P_x dx = ∫

_o^L P_x dx - ∫

_o^r P_x dx.

13. The instrument of claim 10 wherein the beam is continuous, two return paths are employed, one with a passive structure transmitting radiation to the detector from all points out to L while the other passive structure transmits radiation to the detector from all points from r to L only.

14. The instrument of claim 1 wherein said equalizing means comprises a packed side-by-side array of transmissive filaments having radiation absorptive side walls, said array of filaments arranged to receive backscattered radiation and direct it to said detecting means in accordance with said acceptance solid-angle.

15. The instrument of claim 1 wherein said equalizing means comprises a filter and lens system.

16. The instrument of claim 15 wherein said filter comprises a Fabry-Perot interference filter and a magnifying telescope focuses the return radiation thereon.

17. The instrument of claim 1 including a beam splitter means constructed to merge first and second optical axes with the axis of said path, said means for transmitting said beam of radiation comprising a source aligned with said first optical axis to transmit via said beam splitter outwardly along said path and said receiver means including said passive structure and said detector means aligned with said second axis to receive return radiation from said path via said beam splitter, said beam splitter sized sufficiently large that all return radiation passing through said passive structure and reaching said detector passes via and receives equal attenuation by said beam splitter.

18. The instrument of claim 13 wherein each of said passive structures comprises a hole in an opaque plate, both having an opaque center, lens means for focusing a return beam onto the respective holes, the lens means for the second mentioned passive structure having a central obscuration preventing return radiation from points closer than a given point from reaching the hole of the respective passive structure.