Technique for simultaneous particle size and velocity measurement

• US 4,251,733 A
• Filed: 06/29/1978
• Issued: 02/17/1981
• Est. Priority Date: 06/29/1978
• Status: Expired due to Term

• Current Assignee: Edwin D. Hirleman Jr
• Original Assignee: Edwin D. Hirleman Jr
• Inventors: Hirleman, Edwin D. Jr.
• Primary Examiner(s): Nelms, David C.
• Application Number:
  US05/920,550
• Time in Patent Office: 964 Days
• Field of Search: 250/573, 250/574, 250/575, 250/223 R, 250/222 PC, 356/335, 356/336
• US Class Current: 250/575
• CPC Class Codes: G01N 15/0205 by optical means
• CPC Class Codes: G01P 5/20 using particles entrained by a fluid stream G01P5/22 takes precedence

Abstract

Two beams of electromagnetic radiation with symmetric radial intensity distributions are directed through space. A particle sampling volume is defined by those portions of the two beams within the field of view of one or more radiation sensitive detectors. The detectors respond to scattered radiation or fluorescence from particles passing through the beams in the sampling volume. The detector output for a single particle indicates two signal pulses corresponding to those times when the particle was in one of the beams. The speed of the particle in the plane perpendicular to the beams is determined from the transit time or width of the signal pulses, and the angle of the particle traverse in that plane determined from the time-of-flight between the signal pulses. The speed and angle thereby determine two velocity components in the perpendicular plane. Then the exact particle trajectory is specified by the angle and one point on the trajectory which is determined from relative magnitudes of the signal pulses. This allows calculation of the radiation intensity incident on the particle throughout the trajectory from known radiation beam properties. A device then responds to the signal pulses to indicate the size or other physical properities of the particle without the ambiguity present if the incident radiation intensity is unknown.

Claims

1. In a system for determining two velocity components and at least one of the physical properties of a particle passing through a particle sampling zone and including:

means for generating two beams of electromagnetic radiation with radially symmetric intensity distributions and for passing said beams of radiation through said zone whereby a portion of said radiation is incident on and is scattered by said particle;

detective means responsive to said scattered radiation for developing a signal indicative of the temporal history of the magnitude or intensity of said radiation incident on said particle during the traverse through said sampling zone where said signal contains two signal pulses separated in time resulting from said particle passing through each of the two said beams in said sampling zone in succession;

means responsive to said signal to determine the speed or velocity magnitude of said particle in the geometric plane normal to said beams from the shape of at least one of the two signal pulses;

means responsive to the time between said two signal pulses in conjunction with said speed measurement to determine the two velocity components in said plane;

means responsive to said two signal pulses in conjunction with said two velocity component measurement to determine an absolute measure of said radiation intensity incident on said particle during passage through said sampling zone; and

means responsive to said signal pulses in conjunction with said measure of said incident radiation intensity to determine a measure of at least one of the physical properties of said particle.

2. The system set forth in claim 1 wherein said beams of radiation are generated by a laser operating in the TEM_OO or fundamental mode whereby said radially symmetric intensity distributions will be gaussian and therefore said two signal pulses from said particle will also be of gaussian shape.

3. The system set forth in claim 2 wherein said means to determine said particle speed comprise measurement of the transit-time or width of said gaussian signal pulses at some constant fraction of the peak signal level and including means for measuring the actual spatial width of said gaussian laser beams at said constant fraction of the peak beam intensity and means for determining said particle speed from said spatial width traveled in said measured transit-time.

4. The system set forth in claim 2 including means for measuring the spacing between said beams and wherein the time-of-flight or time between the peaks of said signal pulses from said two beams in conjunction with said measured particle speed and spacing determines said angle of said particle traverse and thereby determines said two velocity components in said plane.

5. The system set forth in claim 2 wherein the ratio of said peaks of said signal pulses in conjunction with said measured particle speed and angle determines the position at which the particle traversed said sampling volume, and wherein said determined position and angle are used to calculate the maximum intensity of said incident laser radiation on said particle, and including means for determining a measure of the size of said particle from said peaks of said signal pulses normalized by said calculated maximum intensity incident on said particle.

6. The system set forth in claim 5 including means for determining a measure of the refractive index and therefore composition of said particle in conjunction with said measure of particle size and peaks of signal pulses normalized by said calculated maximum incident intensity from an additional detector sensitive to the refractive index of said particle.

7. The system set forth in claim 1 wherein said detective means are two detectors used with each of said detectors receiving said scattered radiation from said particle only when said particle is in one of said beams in the sampling zone and including means responsive to signals from both of said detectors for determining which of said beams said particle passed through first and thereby for determining the direction of the velocity of said particle.

8. The system set forth in claim 7 wherein said two beams are of different color and said detectors are selectively color sensitive for both velocity and particle property measurement.

9. The system set forth in claim 1 wherein said signal from a particle which passes through only one of said beams in said sampling volume can be identified as a partial or incomplete signal and said partial signal eliminated from further consideration by resetting said means responsive to the time between the two said signal pulses.

10. The system set forth in claim 1 wherein said means responsive to said shape of either of said signal pulses includes means for comparing said speeds calculated from the shape of both of said signal pulses and means for eliminating said particle signal from further consideration if said speeds do not agree to within some acceptable error band.

11. The system set forth in claim 1 wherein a portion of said radiation incident on said particle is partially absorbed and re-emitted as fluorescence by said particle and said signal is developed by detective means responsive to said fluorensence.

12. The system set forth in claim 11 wherein said detective means are two detectors used with each of said detectors receiving said fluorescent radiation only when said particle is in one of said beams in the sampling zone and including means responsive to signals from both of said detectors for determining which of said beams said particle passed through first and thereby for determining the direction of the velocity of said particle.

13. The system set forth in claim 11 wherein fluorescent radiation signal pulses determine said velocity components and said absolute measure of incident radiation intensity and said measure of particle size is indicative of the volume of the particle.

14. The system set forth in claim 1 wherein said measured physical particle property is particle size.