Method for the continuous measurement of the mass of aerosol particles in gaseous samples and a device for the implementation of the method

• US 4,518,861 A
• Filed: 11/05/1982
• Issued: 05/21/1985
• Est. Priority Date: 11/09/1981
• Status: Expired due to Fees

• Current Assignee: Hans List
• Original Assignee: Hans List
• Inventors: Schindler, Wolfgang, Krempl, Peter W., Faschingleitner, Leopold
• Primary Examiner(s): Howell, Janice A.
• Application Number:
  US06/439,596
• Time in Patent Office: 928 Days
• Field of Search: 250/339, 250/341, 250/343, 356/437, 356/438, 356/439
• US Class Current: 250/339.09
• CPC Class Codes: G01N 21/21 Polarisation-affecting properties G01N21/19 takes precedence
• CPC Class Codes: G01N 21/314 with comparison of measurements at specific and non-specific wavelengths dual wavelength spectrometry G01J3/427
• CPC Class Codes: G01N 21/53 within a flowing fluid, e.g. smoke
• CPC Class Codes: G01N 21/534 by measuring transmission alone, i.e. determining opacity
• CPC Class Codes: G01N 2201/127 Calibration; base line adjustment; drift compensation

Abstract

For a continuous measurement of the mass of absorbing particles in a gaseous sample, the sample is traversed by electromagnetic radiation of a wavelength greater than the mean radius of the particles. The difference in absorption for at least two frequencies is determined and appointed to the particle mass sought after.

Claims

1. A method for the continuous measurement of the mass of aerosol particles in gaseous samples, wherein a sample being traversed by electromagnetic radiation of a wavelength greater than the mean radius of said aerosol particles, and the absorption caused being measured for at least two different frequencies, and wherein the difference of the signals which have been received for the different frequencies and which are proportional to the respective absorption is used as a measurement value corresponding to the total mass of said aerosol particles.

2. A method as in claim 1, wherein the difference in absorption at said different frequencies is directly measured.

3. A method as in claim 2, wherein a narrow-band radiation source is wobbled over a certain frequency range with a given period, and wherein that part of the signal detected after the radiation has passed the sample, which varies with the wobbling period, is taken as the measurement value.

4. A method as in claim 3, wherein the wobbling range of said narrow-band radiation source contains at least part of the resonance absorption band of the aerosol particles to be measured, and wherein that part of the detector signal is used as a measurement signal which correlates with the shape of a reference signal corresponding to said absorption band.

5. A method as in claim 1 or 2, wherein a narrow frequency band is selected between preselectable frequencies by means of a selector unit with a preset period, from the radiation of a radiation source with an at least partially continuous spectrum, after said radiation has passed said sample, and wherein the part of the radiation intensity varying with the given period behind said selector unit is used as measurement value.

6. A method as in claim 1 or 2, wherein a detector is exposed to the selected radiation frequencies in turn, with a given periodicity, and the radiation intensities arriving at said detector when no aerosol particles are contained in said sample, are adjusted to equal values for these frequencies.

7. A method as in claim 1, wherein said radiation of each of said frequencies used for the absorption measurement is detected separately after having passed said sample, and wherein preferably the difference of the radiation intensities at the different frequencies is registered only.

8. A method as in claim 7, wherein said radiation intensity is periodically modulated.

9. A method as in claim 1, wherein an absorber with a known absorption capacity is periodically introduced into the radiation path for the purpose of calibration during the measurement process.

10. A method as in claim 9, wherein said absorber is introduced into said radiation path with a period being an integral multiple of the period of frequency change of the incident radiation.

11. A method as in claim 1, wherein in addition to said radiation traversing said sample, which is attenuated by absorption, the radiation scattered by said sample is also measured in a solid angle greater than 10 degrees.

12. A device for the continuous measurement of the mass of aerosol particles in a gaseous sample which includes a sample chamber for containing said gaseous sample;

means for directing a beam of electromagnetic radiation through said sample chamber, said electromagnetic radiation having at least two different wavelengths which are longer than the expected means radius of the aerosol particles in the gaseous sample in said sample chamber;

a beam splitter for splitting said beam into partial beams after said beam has passed through said sample chamber;

means for inserting selectively transparent filters into the partial beams for selected frequencies;

a detector; and

a selector unit for enabling said detector to be exposed to said partial beams at a given periodicity.

13. A device as in claim 12, wherein said selector unit comprises a rotating disk which is placed in the radiation path in front of said detector and has openings for the partial beams opening a passage to said detector in turn.

14. A device as in claim 12, wherein said selector unit is provided with polarizers of different directions in said partial beams, and with an additional polarizer in front of said detector, which transmits the different polarization directions in turn, with the given periodicity.

15. A device as in claims 12, 13 or 14, wherein a lock-in amplifier is provided for the evaluation of the detector signals, which is connected to said detector and to a pulse generator attached to said selector unit, said pulse generator supplying clock signals with a preselected periodicity.

16. A method for the continuous measurement of the mass of aerosol particles in a gaseous sample, the aerosol particles having an expected mean radius, said method comprising the steps of

(a) passing a beam of electromagnetic radiation through said gaseous sample, said electromagnetic radiation having at least two different wavelengths which are longer than said expected mean radius,

(b) measuring the absorption by said mass of aerosol particles in said gaseous sample at at least two of said different wavelengths to obtain two measurement signals, and

(c) determining the difference between said two measurement signals so as to provide a measurement value which corresponds to the total mass of said aerosol particles in said gaseous sample.