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Publication numberUS3178930 A
Publication typeGrant
Publication dateApr 20, 1965
Filing dateApr 8, 1963
Priority dateApr 8, 1963
Publication numberUS 3178930 A, US 3178930A, US-A-3178930, US3178930 A, US3178930A
InventorsCharles B Moore, Vonnegut Bernard
Original AssigneeLittle Inc A
Export CitationBiBTeX, EndNote, RefMan
External Links: USPTO, USPTO Assignment, Espacenet
Monitor and spectrometer for atmospheric particulate matter
US 3178930 A
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Description  (OCR text may contain errors)

April 20, 1965 c. B. MOORE ETAL MONITOR AND SPECTROMETER FOR ATMOSPHERIC PARTICULATE MATTER Filed April 8, 1963 IIIIIIIIIIIIIIIIIIIIIIII'IIIIIIII'IIIIIIII Charles B. Moore Bernard Vonnegu1 INVENTORS United States Patent MONITOR AND SPECTROMETER FOR ATMOS- PHERIC PARTICULAT E MATTER Charles B. Moore, Lexington, and Bernard Vonnegut,

Weston, Mass., assignors to Arthur D. Little, Inc., Cambridge, Mass., 21 coiporation of Massachusetts Filed Apr. 8, 1963, Ser. No. 271,134

6 Claims. (Cl. 73-28) This invention relates to a monitor and spectrometer device for indicating the total concentration in the atmosphere of particles below any desired maximum mobility level. This monitor is for example particularly useful in the determination of concentrations and the distribution of sizes of suspended particles in the atmosphere.

US. Patent 2,986,923 of Bernard Vonnegut, one of the present applicants, describes an apparatus for detecting and measuring aerosols. In that apparatus, no special provision is made for the removal of the fast charging ions. In the apparatus of the present invention, however, an electric field is imposed in an ion filter that causes the charging ions to move in a controlled fashion. Movement of the fast ions is thus controlled independent- 1y. This apparatus therefore makes it possible to obtain the approximate spectra of particle size, in the sample of gaseous fluid being examined, from the mobility of the charged particles.

This device is furthermore very well suited for continuous measurement of the concentrations of atmospheric particles of any desired size range.

Ability to predict the incidence of fog is of particular importance in air navigation and operation. High humidity alone does. not necessarily bring about fog conditions. However, if high humidity--say 90%,is accompanied by a large concentration in the atmosphere of particles detectable by the apparatus of this invention, a high obscuring fog is very likely to follow. With such forecasting, suitable precautions can be taken, and preparations made, before the fog occurs.

The device of this invention operates by electrically charging incoming airborne particulate matter to the maximum that can be accepted (under the set conditions), removing all excess charging ions and then measuring the resulting charge concentrations. The apparatus consists of (1) a suction fan or other suitable means for introducing air into the intake, (2) a charging section in which large quantities of fast, gaseous ions are produced in a potential gradient so that passing particles acquire a net charge of one polarity, (3) an ion filter section where all fast ions and charged particles with mobilities greater than some preset value are removed by electrostatic precipitation and (4) a Faraday cage in which the potential produced by the net mean charge concentration on the remaining particles is measured continuously with an electrometer.

This invention will now be described in detail in connection with the accompanying drawing, which is a partially schematic side elevation of a typical form of the apparatus, and is to be considered as illustrative rather than limiting.

The apparatus shown in the drawing comprises a duct 11 for incoming air, or other gas, to be examined, a radioactive particle charging device 13 in duct 11, an ion filter 15 into which the duct discharges, an outlet duct 17 leading from filter 15, a Faraday cage 19 into which duct 6 17 discharges, and an exhaust fan 21 connected to cage 19 and arranged to move the air or gas through the system.

A suitable potential is applied to charging device 13 by battery or other power source 23 connected across charging device 13 and the walls of duct 11 through a protective resistance 25. The lead-in wire to charging device 13 is suitably insulated from the duct walls, as by insulator 27. Ion filter 15 comprises an outer electrode 31, an inner electrode 33 mounted concentrically therewith and providing space 32 therebetween, and supported in position by insulating spacers 35, and a battery or other power source 37 connected across the two electrodes through a variable resistance 39. An insulator 41 is provided in the wall of the outer electrode 31 where the electrical circuit passes through the latter.

Duct 17 leads to Faraday cage 19 which is provided with an outlet duct 43 leading to fan 21. The cage is grounded, as at 45. It contains an element 47 adapted to measure the electric charge concentration, e.g. a polonium particles source located in the center and supported on a conductive metal probe 49 mounted through insulator 51 and connected to an electrometer 53 which in turn operates a recording galvanometer 55 and is grounded as at 57.

Elbows making turns are placed in each of the ducts 11, 17 and 43, as shown, so as to eliminate electrostatic interactions between sections (i.e. between each of elements 13, 15, 19 and 21).

Large quantities of gaseous ions can be produced by applying high potentials to points, to flames and to radioactive sources. The latter method is chosen for the purposes of this invention, for reasons for stability and freedom from contamination after experiences with the first two. With a point at potentials greater than about 4 kv. large quantities of ions of one polarity can be produced; a supply of unipolar ions is very desirable for this instrument. The potentials necessary, however, are suflicient to precipitate some of the incoming particulate matter. The instrument response varies with any variation in potential on the point to some high power so that a closely regulated high voltage power supply is necessary. For these reasons, charging from point discharge is not suitable for use with the present apparatus.

Flames have been used for particle charging; however, the production of particulate matter by combustion is a drawback, unless hydrogen flames are used and the water produced is not allowed to condense. The difficulty and possible hazards with unattended flames can be appreciable. Hence, flames are unsuitable here also.

The technique of particle charging by the use of radioactive elements is as follows: three 500 microcurie polonium strips were mounted at 13 to form a triangular prism with the active sides facing outward. The prism was located in the center of a 10 cm. diameter metal duct 11 on Teflon insulator 27. Potentials from an external supply 23 could be placed on the prism relative to the duct wall by use of a Teflon insulated wire 24. The potential can be varied as desired by resistance 25 which may be of a predetermined value or may be a variable resistance.

The polonium strips (with a half life of days) emit (when new) about 5x10 alpha particles per second and each of these produces about 3 X10 ion pairs in a 5 cm. path of air (the range of the alpha particles). Under the influence of an applied potential difference between the source and the walls, the ions migrate perpendicularly to the axis of the duct. Particles in the air being drawn through the apparatus become charged as a result of the ion current and the potential diflFerance in a manner somewhat similar to Wilsons mechanism explaining the charging of raindrops. The can be demonstrated to be the case even though the ions of both polarities are initially produced in identical quantities (if we neglect the positively charged alpha particles).

Charging potentials may be as low as 80-90 volts, but we find that most satisfactory results are attained at 3 150200 volts. Much higher potentials can in fact be used, e.g. 500 to 1000 volts, but they give poorer results and obviously require more complex equipment.

The upper limit of mobility for a particle passing through the ion filter 15 can be determined by equating the time required for a particle to flow through the filter to the time required for an ion to drift across the annular space 32 to the collecting electrode under the infiuence of the potential applied across the two electrodes 31 and 33.

From this we find that the product of the upper limit of particle mobility and the potential diiference equals the ion filter figure of merit which is the product of the air flow rate times the natural logarithm of the ratio of the larger radius of the filter annulus to the smaller radius and this product divided by 21r times the length of the filter.

If for example ion filter 15 has an inner (collecting) electrode (33) length of one meter and outside radius of 15.3 cm., and the inside radius of the outer electrode 35 is 16.5 cm., with an air flow of 14 liters per second, the filter figure of merit equals 1.7 cm. seer- This means that if 100 volts potential diiference were placed across the ion filter, all ions with mobilities of greater than 1.7/ 100 or 0.017 cm. sec? per volt cm. would be removed from the gas. The maximum potential applicable across the filter is that value above which the electrodes produce spark discharges which create spurious ions. For the filter given in the example above, the maximum potential across space 32 is about kv. Above this value, spark discharges occur and spurious ions are produced.

When the ion filter is arranged to remove all ions with mobilities greater than 3 10- cm. sec? per volt GEL-1, then few charged particles produced in the charging section at 11 should pass into the Faraday cage 19 unless the particles are larger than 0.05 micron. We find that condensation nuclei and other particles in the normal clean atmosphere produce relatively small signals in the apparatus under these conditions, but when the air becomes hazy the electrometer response appears to vary directlywith the observed haze obstructions to visibility. The monitor of this invention gave indications that closely paralleled those of the condensation nuclei apparatus described in U.S. Patent 2,684,008 (issued to one of the present inventors) when the filterpass mobility upper limit was set at 5X10 cm. sec. per volt cmf Faraday cage 19 is an enclosure having electrically conductive walls and conveniently of cylindrical shape. Element 47 is for example a 500 microcurie polonium element, and is mounted and connected as already described. Other types of field-measuring such as a field mill, can be used alternatively, for measuring the field in the Faraday cage.

The space charge imposed upon atmospheric particulate matter by charging device 13 causes a potential to exist in the center of Faraday cage 19 relative to the Walls. This potential is measured by electrometer 53 and a record thereof is made by recording galvanometer 55. For most sensitive measurement, element 4'7 should be substantially centrally located in the cage 19, i.e. so that it is not appreciably nearer to any one conducting wall than to another.

The difference in the work functions of the conducting Walls of the Faraday cage and the probe at the center of the cage can give an appreciable but spurious signal indicating the presence of charged particles even in their absence; This effect is eliminated by a periodic grounding of the charging section by means of switch 59, a

single-pole, double-throw type inserted in electric circuit wire 24 so that incoming particles no longer acquire a net charge and thus the eifect of no particulate matter is simulated and shown on the recording as a zero indication.

Fan 21 or equivalent gas-impelling means should be located at the exhaust end of the system to avoid contamination of the gas under study. The gas may however be impelled in other Ways, such as by moving the apparatus with respect to the surrounding gaseous atmosphere. This may be accomplished, for example, by means of a rising balloon, or by use of a moving vehicle or ship, by which the apparatus is carried.

We claim:

1. A device for indicating the total concentration of particles in a gaseous fluid comprising:

(a) an ion filter comprising a pair of concentrically arranged electrically conductive walls between which said fluid flows,

([1) means for imposing an electric potential between said conductive walls,

(c) an inlet duct leading to said ion filter and arranged to receive said gaseous fluid for testing,

(0!) a radioactive particle charging element in said inlet duct,

(e) means comprising an electric circuit for imposing an electric potential between said element and the walls of said inlet duct,

( a Faraday cage containing means for measuring the electric charge concentration in the gaseous fluid flowing through said cage,

(g) a second duct leading from said ion filter to said Faraday cage, and

(h) an exhaust duct leading out of said Faraday cage;

(1') the electric potential between the walls of said ion filter being sufiicient to remove substantially all the fast charging ions in said gaseous fluid passing through said ion filter,

(j) each of said ducts being provided with turns whereby electrostatic interactions between any of said particle changing element, said ion filter, and said Faraday cage are prevented.

2. A device in accordance with claim 1 further characterized in that said radioactive particle-charging element is polonium. I

3. A device in accordance with claim 1 further characterized that said measuring means in said Faraday cage is a radioactive particle source and an electrometer connected thereto.

4. A device in accordance with claim 1 further characterized in that a fan is provided in said exhaust duct which impels the gaseous fiuid through said device. I

5. A device in accordance with claim 1 further characterized in that each of said ducts contains a 90 degree turn.

6. A device in accordance with claim 1 further characterized in that a switch is provided, adapted to ground said electric circuit periodically as desired.

OTHER REFERENCES Mack, Garrett, Haskins, Verhoek, Textbook of Chemistry, Ginn and Company, 1949 pages 451.

RICHARD C. QUEISSER, Primary Examiner.

Patent Citations
Cited PatentFiling datePublication dateApplicantTitle
US2986923 *Jun 18, 1954Jun 6, 1961Little Inc AMeans for detecting and measuring aerosols
US3114877 *Oct 30, 1956Dec 17, 1963Gen ElectricParticle detector having improved unipolar charging structure
Referenced by
Citing PatentFiling datePublication dateApplicantTitle
US3351759 *Aug 4, 1964Nov 7, 1967Gen ElectricApparatus for determining aerosol particle size comprising a combined diffuser-denuder
US3573460 *Sep 12, 1966Apr 6, 1971Gen ElectricIon chamber detector for submicron particles
US4055075 *Apr 8, 1976Oct 25, 1977Flanders Filters, Inc.Method and apparatus for the leak testing of filters
US4121458 *Feb 24, 1977Oct 24, 1978Westinghouse Electric Corp.Reliable dynamoelectric machine condition monitor
US4236900 *Mar 30, 1978Dec 2, 1980Maxwell Laboratories, Inc.Electrostatic precipitator apparatus having an improved ion generating means
US4349359 *Apr 14, 1980Sep 14, 1982Maxwell Laboratories, Inc.Electrostatic precipitator apparatus having an improved ion generating means
US4364752 *Mar 13, 1981Dec 21, 1982Fitch Richard AElectrostatic precipitator apparatus having an improved ion generating means
US4959010 *Aug 20, 1984Sep 25, 1990Matter & Siegmann AgAutomatically regulated combustion process
US6752003 *May 1, 2001Jun 22, 2004Dr. Foedisch Umweltmesstechnik GmbhMethod and device for the extractive triboelectric measurements of dust and aerosols in streaming gases
US7549318 *Jan 12, 2006Jun 23, 2009Matter EngineeringMethod and device for the measurement of the number concentration and of the average diameter of aerosol particles
US7836751Jun 26, 2006Nov 23, 2010Koninklijke Philips Electronics N.V.Ultra fine particle sensor
WO2007000710A2 *Jun 26, 2006Jan 4, 2007Koninkl Philips Electronics NvUltra fine particle sensor
Classifications
U.S. Classification73/28.2, 55/DIG.380, 340/601, 250/308, 324/464, 96/62
International ClassificationG01N15/06, G01N27/64, G01N33/00, G01N15/02
Cooperative ClassificationY10S55/38, G01N27/622, G01N15/0266, G01N33/0027, G01N15/0656
European ClassificationG01N27/62A, G01N15/06D, G01N33/00D2D, G01N15/02D