US3603689A - Scanning scattered light photometer - Google Patents

Scanning scattered light photometer Download PDF

Info

Publication number
US3603689A
US3603689A US865899A US3603689DA US3603689A US 3603689 A US3603689 A US 3603689A US 865899 A US865899 A US 865899A US 3603689D A US3603689D A US 3603689DA US 3603689 A US3603689 A US 3603689A
Authority
US
United States
Prior art keywords
output
light
polarizer
rotor
signal
Prior art date
Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
Expired - Lifetime
Application number
US865899A
Inventor
James William Shelnutt
Current Assignee (The listed assignees may be inaccurate. Google has not performed a legal analysis and makes no representation or warranty as to the accuracy of the list.)
US Air Force
Original Assignee
US Air Force
Priority date (The priority date is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the date listed.)
Filing date
Publication date
Application filed by US Air Force filed Critical US Air Force
Application granted granted Critical
Publication of US3603689A publication Critical patent/US3603689A/en
Anticipated expiration legal-status Critical
Expired - Lifetime legal-status Critical Current

Links

Images

Classifications

    • G—PHYSICS
    • G01—MEASURING; TESTING
    • G01N—INVESTIGATING OR ANALYSING MATERIALS BY DETERMINING THEIR CHEMICAL OR PHYSICAL PROPERTIES
    • G01N21/00—Investigating or analysing materials by the use of optical means, i.e. using sub-millimetre waves, infrared, visible or ultraviolet light
    • G01N21/17—Systems in which incident light is modified in accordance with the properties of the material investigated
    • G01N21/21—Polarisation-affecting properties
    • G—PHYSICS
    • G01—MEASURING; TESTING
    • G01N—INVESTIGATING OR ANALYSING MATERIALS BY DETERMINING THEIR CHEMICAL OR PHYSICAL PROPERTIES
    • G01N15/00—Investigating characteristics of particles; Investigating permeability, pore-volume, or surface-area of porous materials
    • G01N15/02—Investigating particle size or size distribution
    • G01N15/0205—Investigating particle size or size distribution by optical means, e.g. by light scattering, diffraction, holography or imaging
    • G—PHYSICS
    • G01—MEASURING; TESTING
    • G01N—INVESTIGATING OR ANALYSING MATERIALS BY DETERMINING THEIR CHEMICAL OR PHYSICAL PROPERTIES
    • G01N21/00—Investigating or analysing materials by the use of optical means, i.e. using sub-millimetre waves, infrared, visible or ultraviolet light
    • G01N21/17—Systems in which incident light is modified in accordance with the properties of the material investigated
    • G01N21/47—Scattering, i.e. diffuse reflection
    • G01N21/49—Scattering, i.e. diffuse reflection within a body or fluid
    • G01N21/53—Scattering, i.e. diffuse reflection within a body or fluid within a flowing fluid, e.g. smoke
    • G—PHYSICS
    • G01—MEASURING; TESTING
    • G01N—INVESTIGATING OR ANALYSING MATERIALS BY DETERMINING THEIR CHEMICAL OR PHYSICAL PROPERTIES
    • G01N21/00—Investigating or analysing materials by the use of optical means, i.e. using sub-millimetre waves, infrared, visible or ultraviolet light
    • G01N21/17—Systems in which incident light is modified in accordance with the properties of the material investigated
    • G01N21/47—Scattering, i.e. diffuse reflection
    • G01N2021/4792—Polarisation of scatter light

Definitions

  • a polarizing beamsplitter on the rotor separates the scattered light into two perpendicular components.
  • a first mirror on the rotor directs a first polarized component of light in the plane of rotation of the rotor toward a first photomultiplier.
  • a second mirror on the rotor directs light polarized perpendicular to the plane of rotation toward a second photomultiplier.
  • a fixed mirror directs undispersed light toward a photoconductive device to provide a synchronizing output pulse when the polarizer beamsplitter passes through the beam between the light source and the aerosol flow.
  • the outputs of the photomultipliers and photoconductive device are fed to a ratio and averaging circuit and then to a recorder.
  • an apparatus that substantially reduces the time required to obtain data from a sample and which provides more complete data than could be obtained with prior art methods.
  • a collimated, monochromatic unpolarized light source is positioned to impinge a beam of light on an aerosol sample in a space between an entrance nozzle and a vacuum exhaust outlet.
  • the sample flows through the center of a hub around which a scanner rotates.
  • a polarizing prism and two mirrors are mounted on the scanner. The mirrors direct the two polarized components of the light scattered by the sample to two photomultipliers positioned above the center of the scanner.
  • the outputs of the photomultipliers are fed to an analog divider circuit and signal averaging circuit with the output of the signal averaging circuit being applied to a display device and a recorder.
  • a sync signal for the signal averager may be provided if needed.
  • FIG. 1 is a schematic diagram partially in block form of a scanning scattered light photometer system according to the invention
  • FIG. 2 is a partially cutaway front elevation of the scanning apparatus for the device of FIG. 1;
  • FIG. 3 is a sectional view of the device of FIG. 2 along the line 33;
  • FIG. 4 is a top view of the rotor assembly for the device of FIG. 2.
  • FIG. 1 of the drawing shows a scattered light photometric system including a scanning apparatus 12 shown in greater detail in FIGS. 2-4.
  • the scanning apparatus 12 includes a chamber 14.
  • a sample to be tested is supplied to a nozzle in the center of chamber 14 from sample supply 16.
  • the flow leaving nozzle 15 is directed toward an exhaust outlet 17 which leads to a vacuum source, not shown.
  • a beam of collimated, monochromatic un polarized light is directed toward the sample from a light source 19.
  • the light is scattered by the particles of the sample leaving the nozzle 15.
  • a rotor 20 has a hub 22 surrounding the exhaust outlet 17.
  • the rotor 20 is driven by a motor 24 through a gear train 25.
  • a polarizing beamsplitter 27 is mounted on the rotor 20. As the scanner is rotated, the light scattered at any particular angle is received by a slot 30 in a mask 31 positioned in front of the polarizing beamsplitter 27. Light polarized in the plane of rotation of the polarizer on the scanner is reflected by a precision front surface mirror 32 toward photomultiplier 33. Light polarized in the plane perpendicular to the plane of rotation is reflected by a precision front surface mirror through a slot 34 in rotor 20 toward a photomultiplier 36. A counterbalance 37 for the beamsplitter 27 and mirrors 32 and 35 is provided on rotor 20. A
  • beamsplitter 27 may be a Spectra Physics Model 5115 polarizing beamsplitter and the mirrors 32 and 35 may be Spectra Physics Model 576-4l front surface mirrors.
  • the light source 19 may be a Spectra Physics Model 132 l-milliwatt heliumneon laser.
  • the output of photomultipliers 33 and 36 are passed through preamplifiers 40 and 42 and then to an analog divider 46 which provides an output A/B.
  • the analog divider as may be, for example, a Princeton Applied Research Co. Model 230.
  • the output of the analog divider 46 is then supplied to a signal averaging circuit ltl which may be, for example, the Princeton Applied Research Co. Model TDH-9 Waveform Eductor.
  • the signal averaging circuit divides the signal waveform into segments continuously samples and averages each segment and provides in the output a smooth waveform based on these averages which is substantially free of noise.
  • a device which performs the function of both the analog divider 46 and the signal averaging circuit 48 is the Fabri-Telc I070 signal averaging computer.
  • the output of the signal averaging circuit 48 is applied to either a recorder such as an oscillograph 51 or to a display device such as an oscil loscope 52.
  • the output of the photomultipliers 33 and 36 may be used in other circuits than that described, for example, they could be supplied to a circuit to provide an output A-B/A+B or other outputs as may be desired.
  • this signal may be obtained by providing a stationary mirror 55 mounted on flange 18 on outlet 17 which directs unscattered light to a photoconductor 56. This light is blocked from the mirror and photoconductor whenever the polarizer 47 and mirrors 32 and 35 pass the side of the chamber I4 ad jacent the light source 19 and thus provides a synchronizing pulse to the averaging circuit 48. Since light scattered by the sample is the same on both sides of the beam, an output is needed for only of the rotation of the rotor.
  • a shield 53 having a semicircular opening 59 blocks light from mirrors 32 and 35 to photomultipliers 33 and 36 during half of the rotation. This could also be accomplished electronically by means of a gate circuit which provides a gate pulse for the desired period to be observed by the waveform averages in response to the output from the photoconductor 56. Power is supplied to the various devices from a power supply 60.
  • a device for providing an output signal proportional to the two polarized components of light scattered by a flowing aerosol for all angular positions in a predetermined 180 region around the flowing aerosol comprising: means for providing a sample flow; means for directing a beam of collimated monochromatic unpolarized light toward said flow; a beamsplitter polarizer; an apertured mask between said beamsplitter polarizer and said sample flow; means for moving said mask and said polarizer in a circular path around said sample flow; a first photomultiplier tube; means for directing a first polarized component of light scattered by the flowing aerosol, in the plane of said circular path, toward said first photomultiplier tube; a second photomultiplier scattered by the flowing aerosol, perpendicular to the plane of said circular path, toward said second photomultiplier tube; means responsive to the output of said photomultipliers for providing an output signal proportional to the output of the first photomultiplier tube and the second photomultiplier tube.
  • said means for providing an output signal includes an analog divider means for providing a signal proportional to the ratio of the output of said first photomultiplier and the output of said second photomultiplier; a signal averaging circuit connected to the output of said analog divider means; means for supplying a signal to said signal averaging circuit for synchronizing the the polarizer includes a photovoltaic cell; a stationary mirror positioned in line with the beam of collimated monochromatic unpolarizcd light; said means for moving said polarizer in a circular path being a rotor for moving the polarizer into the light beam path once during each revolution of the rotor to block light to said stationary mirror and photovoltaic cell to thereby provide a synchronizing signal for said averaging circuit.

Abstract

A scanning scattered light photometer system having a rotor with a beamsplitter-polarizer and a nozzle for directing an aerosol flow along the axis of the rotor toward an exhaust outlet. The aerosol flow is illuminated by a collimated monochromatic unpolarized light. A polarizing beamsplitter on the rotor separates the scattered light into two perpendicular components. A first mirror on the rotor directs a first polarized component of light in the plane of rotation of the rotor toward a first photomultiplier. A second mirror on the rotor directs light polarized perpendicular to the plane of rotation toward a second photomultiplier. A fixed mirror directs undispersed light toward a photoconductive device to provide a synchronizing output pulse when the polarizer beamsplitter passes through the beam between the light source and the aerosol flow. The outputs of the photomultipliers and photoconductive device are fed to a ratio and averaging circuit and then to a recorder.

Description

United States Patent lnventor James William Shelnutt, 111
Dayton, Ohio [21 1 Appl. No. 865,899 [22] Filed Oct. 13, 1969 [45] Patented Sept. 7, 1971 [73] Assignee The United States of America as represented by the Secretary of the Air Force I E [54] SCANNING SCATTERED LIGHT PHOTOMETER 5 Claims, 4 Drawing Figs.
[52] US. Cl. 356/103, 356/1 14 [51] Int. Cl G0ln21/00, G0 1 n 21/40 [50] Field oiSearch 356/103, 104, 1 l4, 1 15 [56] References Cited UNITED STATES PATENTS 3,334,537 8/1967 Beattie 3,420,609 1/1969 Kozawa ABSTRACT: A scanning scattered light photometer system having a rotor with a beamsplitter-polarizer and a nozzle for directing an aerosol flow along the axis of the rotor toward an exhaust outlet. The aerosol flow is illuminated by a collimated monochromatic unpolarized light. A polarizing beamsplitter on the rotor separates the scattered light into two perpendicular components. A first mirror on the rotor directs a first polarized component of light in the plane of rotation of the rotor toward a first photomultiplier. A second mirror on the rotor directs light polarized perpendicular to the plane of rotation toward a second photomultiplier. A fixed mirror directs undispersed light toward a photoconductive device to provide a synchronizing output pulse when the polarizer beamsplitter passes through the beam between the light source and the aerosol flow. The outputs of the photomultipliers and photoconductive device are fed to a ratio and averaging circuit and then to a recorder.
PATENTEDSEP m 33,603,689
SHEET 2 [IF 4 PATENIEDSEP 71971 $603,689
sum 3 BF 4 PATENTEDSEP mm SHEET t 0F 4 INVENTOR.
SCANNING SCATTERED LIGI-IT PlIIOTOME'IER BACKGROUND OF THE INVENTION In the study of aerosols, colloidal dispersions, and other particulate suspensions the particle size distribution is obtained by the polarization ratio method as is described in the article "Aerosol Studies by Light Scattering" in The Journal of Colloid Science, Vol. 19, 1964, pp. 21 3-222.
In the prior art, data is obtained in a point-by-point system. This is very time consuming and limits the type of samples from which data may be obtained. Since data must be obtained by moving from point to point to different angular positions around the sample there is a considerable time lag between the obtaining of the initial and the final data. In samples wherein changes are occurring, such as coagulation, this time lag seriously limits the data obtainable from the sample.
SUMMARY OF THE INVENTION According to this invention, an apparatus is provided that substantially reduces the time required to obtain data from a sample and which provides more complete data than could be obtained with prior art methods. A collimated, monochromatic unpolarized light source is positioned to impinge a beam of light on an aerosol sample in a space between an entrance nozzle and a vacuum exhaust outlet. The sample flows through the center of a hub around which a scanner rotates. A polarizing prism and two mirrors are mounted on the scanner. The mirrors direct the two polarized components of the light scattered by the sample to two photomultipliers positioned above the center of the scanner. The outputs of the photomultipliers are fed to an analog divider circuit and signal averaging circuit with the output of the signal averaging circuit being applied to a display device and a recorder. A sync signal for the signal averager may be provided if needed.
IN THE DRAWING FIG. 1 is a schematic diagram partially in block form of a scanning scattered light photometer system according to the invention;
FIG. 2 is a partially cutaway front elevation of the scanning apparatus for the device of FIG. 1;
FIG. 3 is a sectional view of the device of FIG. 2 along the line 33; and
FIG. 4 is a top view of the rotor assembly for the device of FIG. 2.
DETAILED DESCRIPTION OF THE INVENTION Reference is now made to FIG. 1 of the drawing which shows a scattered light photometric system including a scanning apparatus 12 shown in greater detail in FIGS. 2-4. The scanning apparatus 12 includes a chamber 14. A sample to be tested is supplied to a nozzle in the center of chamber 14 from sample supply 16. The flow leaving nozzle 15 is directed toward an exhaust outlet 17 which leads to a vacuum source, not shown. A beam of collimated, monochromatic un polarized light is directed toward the sample from a light source 19. The light is scattered by the particles of the sample leaving the nozzle 15. A rotor 20 has a hub 22 surrounding the exhaust outlet 17. The rotor 20 is driven by a motor 24 through a gear train 25. A polarizing beamsplitter 27 is mounted on the rotor 20. As the scanner is rotated, the light scattered at any particular angle is received by a slot 30 in a mask 31 positioned in front of the polarizing beamsplitter 27. Light polarized in the plane of rotation of the polarizer on the scanner is reflected by a precision front surface mirror 32 toward photomultiplier 33. Light polarized in the plane perpendicular to the plane of rotation is reflected by a precision front surface mirror through a slot 34 in rotor 20 toward a photomultiplier 36. A counterbalance 37 for the beamsplitter 27 and mirrors 32 and 35 is provided on rotor 20. A
beamsplitter 27 may be a Spectra Physics Model 5115 polarizing beamsplitter and the mirrors 32 and 35 may be Spectra Physics Model 576-4l front surface mirrors. The light source 19 may be a Spectra Physics Model 132 l-milliwatt heliumneon laser.
The output of photomultipliers 33 and 36 are passed through preamplifiers 40 and 42 and then to an analog divider 46 which provides an output A/B. The analog divider as may be, for example, a Princeton Applied Research Co. Model 230. The output of the analog divider 46 is then supplied to a signal averaging circuit ltl which may be, for example, the Princeton Applied Research Co. Model TDH-9 Waveform Eductor. The signal averaging circuit divides the signal waveform into segments continuously samples and averages each segment and provides in the output a smooth waveform based on these averages which is substantially free of noise. A device which performs the function of both the analog divider 46 and the signal averaging circuit 48 is the Fabri-Telc I070 signal averaging computer. The output of the signal averaging circuit 48 is applied to either a recorder such as an oscillograph 51 or to a display device such as an oscil loscope 52.
The output of the photomultipliers 33 and 36 may be used in other circuits than that described, for example, they could be supplied to a circuit to provide an output A-B/A+B or other outputs as may be desired.
When a synchronizing signal is needed such as in averaging corresponding parts of a signal, as in signal averaging circuit 48, this signal may be obtained by providing a stationary mirror 55 mounted on flange 18 on outlet 17 which directs unscattered light to a photoconductor 56. This light is blocked from the mirror and photoconductor whenever the polarizer 47 and mirrors 32 and 35 pass the side of the chamber I4 ad jacent the light source 19 and thus provides a synchronizing pulse to the averaging circuit 48. Since light scattered by the sample is the same on both sides of the beam, an output is needed for only of the rotation of the rotor. A shield 53 having a semicircular opening 59 blocks light from mirrors 32 and 35 to photomultipliers 33 and 36 during half of the rotation. This could also be accomplished electronically by means of a gate circuit which provides a gate pulse for the desired period to be observed by the waveform averages in response to the output from the photoconductor 56. Power is supplied to the various devices from a power supply 60.
There is thus provided a scanning scattered light photometer system which provides more complete data and substantially reduces the time required to obtain data.
I claim:
I. A device for providing an output signal proportional to the two polarized components of light scattered by a flowing aerosol for all angular positions in a predetermined 180 region around the flowing aerosol comprising: means for providing a sample flow; means for directing a beam of collimated monochromatic unpolarized light toward said flow; a beamsplitter polarizer; an apertured mask between said beamsplitter polarizer and said sample flow; means for moving said mask and said polarizer in a circular path around said sample flow; a first photomultiplier tube; means for directing a first polarized component of light scattered by the flowing aerosol, in the plane of said circular path, toward said first photomultiplier tube; a second photomultiplier scattered by the flowing aerosol, perpendicular to the plane of said circular path, toward said second photomultiplier tube; means responsive to the output of said photomultipliers for providing an output signal proportional to the output of the first photomultiplier tube and the second photomultiplier tube.
2. The device as recited in claim I wherein said means for providing an output signal includes an analog divider means for providing a signal proportional to the ratio of the output of said first photomultiplier and the output of said second photomultiplier; a signal averaging circuit connected to the output of said analog divider means; means for supplying a signal to said signal averaging circuit for synchronizing the the polarizer includes a photovoltaic cell; a stationary mirror positioned in line with the beam of collimated monochromatic unpolarizcd light; said means for moving said polarizer in a circular path being a rotor for moving the polarizer into the light beam path once during each revolution of the rotor to block light to said stationary mirror and photovoltaic cell to thereby provide a synchronizing signal for said averaging circuit.

Claims (5)

1. A device for providing an output signal proportional to the two polarized components of light scattered by a flowing aerosol for all angular positions in a predetermined 180* region around the flowing aerosol comprising: means for providing a sample flow; means for directing a beam of collimated monochromatic unpolarized light toward said flow; a beamsplitter polarizer; an apertured mask between said beamsplitter polarizer and said sample flow; means for moving said mask and said polarizer in a circular path around said sample flow; a first photomultiplier tube; means for directing a first polarized component of light scattered by the flowing aerosol, in the plane of said circular path, toward said first photomultiplier tube; a second photomultiplier scattered by the flowing aerosol, perpendicular to the plane of said circular path, toward said second photomultiplier tube; means responsive to the output of said photomultipliers for providing an output signal proportional to the output of the first photomultiplier tube and the second photomultiplier tube.
2. The device as recited in claim 1 wherein said means for providing an output signal includes an analog divider means for providing a signal proportional to the ratio of the output of said first photomultiplier and the output of said second photomultiplier; a signal averaging circuit connected to the output of said analog divider means; means for supplying a signal to said signal averaging circuit for synchronizing the signal averaging circuit with the rotation of the polarizer in said circular path; an output circuit connected to said signal averaging circuit.
3. The device as recited in claim 2 wherein said output circuit includes a recorder.
4. The device as recited in claim 2 wherein said output circuit includes a visual display device.
5. The device as recited in claim 2 wherein said means for synchronizing the signal averaging circuit with the rotation of the polarizer includes a photovoltaic cell; a stationary mirror positioned in line with the beam of collimated monochromatic unpolarized light; said means for moving said polarizer in a circular path being a rotor for moving the polarizer into the light beam path once during each revolution of the rotor to block light to said stationary mirror and photovoltaic cell to thereby provide a synchronizing signal for said averaging circuit.
US865899A 1969-10-13 1969-10-13 Scanning scattered light photometer Expired - Lifetime US3603689A (en)

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
US86589969A 1969-10-13 1969-10-13

Publications (1)

Publication Number Publication Date
US3603689A true US3603689A (en) 1971-09-07

Family

ID=25346484

Family Applications (1)

Application Number Title Priority Date Filing Date
US865899A Expired - Lifetime US3603689A (en) 1969-10-13 1969-10-13 Scanning scattered light photometer

Country Status (1)

Country Link
US (1) US3603689A (en)

Cited By (7)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US3724951A (en) * 1971-08-31 1973-04-03 Eastman Kodak Co Method and apparatus for determining radiation transmission characteristics of a generally transparent medium
US3879615A (en) * 1972-11-09 1975-04-22 Kernforschung Gmbh Ges Fuer Method and apparatus for the rapid measuring of the angular dependence of scattered light
US4134679A (en) * 1976-11-05 1979-01-16 Leeds & Northrup Company Determining the volume and the volume distribution of suspended small particles
US4362387A (en) * 1980-08-22 1982-12-07 Rockwell International Corporation Method and apparatus for measuring visibility from the polarization properties of the daylight sky
US4662742A (en) * 1985-05-10 1987-05-05 Becton, Dickinson And Company Scatter/fluorescene beam splitter in a flow cytometry apparatus
US4885473A (en) * 1988-04-29 1989-12-05 Shofner Engineering Associates, Inc. Method and apparatus for detecting particles in a fluid using a scanning beam
EP1588147A2 (en) * 2003-01-24 2005-10-26 Beckman Coulter, Inc. Extracted polarization intensity differential scattering for particle characterization

Citations (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US3283644A (en) * 1962-11-27 1966-11-08 Du Pont Apparatus for determining the concentration of dispersed particulate solids in liquids
US3334537A (en) * 1963-04-29 1967-08-08 Beckman Instruments Inc Light scattering attachment
US3420609A (en) * 1964-08-27 1969-01-07 Shimadzu Corp Photometer for comparing scattered with transmitted light

Patent Citations (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US3283644A (en) * 1962-11-27 1966-11-08 Du Pont Apparatus for determining the concentration of dispersed particulate solids in liquids
US3334537A (en) * 1963-04-29 1967-08-08 Beckman Instruments Inc Light scattering attachment
US3420609A (en) * 1964-08-27 1969-01-07 Shimadzu Corp Photometer for comparing scattered with transmitted light

Cited By (8)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US3724951A (en) * 1971-08-31 1973-04-03 Eastman Kodak Co Method and apparatus for determining radiation transmission characteristics of a generally transparent medium
US3879615A (en) * 1972-11-09 1975-04-22 Kernforschung Gmbh Ges Fuer Method and apparatus for the rapid measuring of the angular dependence of scattered light
US4134679A (en) * 1976-11-05 1979-01-16 Leeds & Northrup Company Determining the volume and the volume distribution of suspended small particles
US4362387A (en) * 1980-08-22 1982-12-07 Rockwell International Corporation Method and apparatus for measuring visibility from the polarization properties of the daylight sky
US4662742A (en) * 1985-05-10 1987-05-05 Becton, Dickinson And Company Scatter/fluorescene beam splitter in a flow cytometry apparatus
US4885473A (en) * 1988-04-29 1989-12-05 Shofner Engineering Associates, Inc. Method and apparatus for detecting particles in a fluid using a scanning beam
EP1588147A2 (en) * 2003-01-24 2005-10-26 Beckman Coulter, Inc. Extracted polarization intensity differential scattering for particle characterization
EP1588147A4 (en) * 2003-01-24 2011-09-28 Beckman Coulter Inc Extracted polarization intensity differential scattering for particle characterization

Similar Documents

Publication Publication Date Title
US4919536A (en) System for measuring velocity field of fluid flow utilizing a laser-doppler spectral image converter
US3866055A (en) Laser doppler velocimetry
US3835315A (en) System for determining parameters of a particle by radiant energy scattering techniques
US3941477A (en) Measuring device for the measurement of fluid flow rates
GB1284199A (en) Photoanalysis apparatus
US3603689A (en) Scanning scattered light photometer
SE7905294L (en) STOFTMETNING
US4097153A (en) Method and apparatus for measuring the electrophoretic mobility of suspended particles
GB1168005A (en) A Method of and Apparatus for Determining Geometrical Deviations from a Desired Surface by Optical Means
DE69920312T2 (en) Detection of air flow velocity and flow direction
GB1242574A (en) A method of, and apparatus for, inspecting the shape of small objects
US4140902A (en) Device for measurement of hair-like particulate material
US4068122A (en) Isotope analysis
Gucker et al. Rapid measurement of light-scattering diagrams from single particles in an aerosol stream and determination of latex particle size
US3832059A (en) Flow velocity measuring arrangement utilizing laser doppler probe
US2817769A (en) Radiation comparison systems
GB1000286A (en) Light scattering measuring apparatus
JPS58153107A (en) Device for measuring diameter and speed of particle simultaneously
US3488122A (en) Process for determining the spectral composition of luminous radiation diffused by a colored surface,and apparatus for carrying out said process
Karns Development of a laser doppler velocimetry system for supersonic jet turbulence measurements
Sauer Molecular Orientation in Quantasomes: III. A Flow Dichroism Apparatus and Its Application to the Study of the Structure of Spinach Quantasomes
US3667851A (en) Measuring system for an analytical centrifuge
Kabardin et al. Kinematic characteristics investigation in a transparent swirler of a vortex tube with square cross-section
Shaughnessy et al. GaAlAs diode sources for laser‐Doppler anemometry
GB1019540A (en) A method and apparatus for determining the difference in area of an article from an article of known area