Isotope Analysis

In the accompanying drawing,

FIG. 1 is a schematic representation of an embodiment of the apparatus of this invention.

FIGS. 2 and 3 illustrate disks which are rotated in the beams of materials being compared in the apparatus of FIG. 1.

FIG. 4 is a schematic circuit drawing of the electrical components associated with the apparatus of FIG. 1.

Referring now to the drawing in detail and to FIG. 1 in particular, there is shown a mass spectrometer 10, the inlet section of which is positioned within a housing 11. Mass spectrometer 10 is provided with two openings 12 and 13 which permit samples to be analyzed to be introduced into the inlet ionization chamber of the spectrometer. A first conduit 14 extends into housing 11 to deliver a first material to be analyzed. Conduit 14 is provided with suitable apertures to direct a narrow beam of the material toward inlet 12. This first beam passes through an aperture 15 in a direction toward inlet 12. A second conduit 16 extends into housing 11 to introduce a beam of a second material to be analyzed. This second beam passes through a second aperture 17 toward inlet 13. First and second disks 19 and 20 are mounted on a shaft 21 which is rotated by a motor 22. These disks are positioned in the paths of the beams from respective conduits 14 and 16. A conduit 23 extends from housing 11 to a vacuum pump, not shown, in order to maintain the interior of housing 11 at a low pressure, such as 10.sup.-3 to 10.sup.-7 Torr, for example.

As illustrated in FIG. 2, disk 19 is provided with openings 24, 25 and 26 which are located such that the first beam directed toward inlet 12 passes through these openings as disk 19 is rotated. As illustrated in FIG. 3, disk 20 is provided with corresponding openings 27 to 31 which permit passage of the second beam directed toward inlet 13. As will be discussed hereinafter in greater detail, the two disks are provided with a different number of openings.

Disk 19 is also provided with three openings 24a, 25a and 26a which are positioned so as to permit passage of a beam of light from a lamp 32 to a photocell 33. In a similar fashion, disk 20 is provided with openings 27 a to 31a which permit passage of a beam of light from a lamp 34 to a photocell 35.

As illustrated in FIG. 4, the output signal from mass spectrometer 10 is applied to first and second synchronous detectors which can be phase sensitive amplifiers 36 and 37. A suitable amplifier for this purpose is the Model 840 Autoloc Amplifier described in Keithley Engineering Notes, volume 19, No. 1, of Keithley Instruments, 28775 Auroro Road, Cleveland, Ohio 44139. Electrical signals derived from photocells 33 and 35 are also applied to respective phase sensitive amplifiers 36 and 37. The output signals from these two amplifiers are applied to the inputs of a differential amplifier 38. The output of amplifier 38 is applied to a recorder 39.

In one method of operation of this invention, a stream of a first gas to be analyzed is introduced through conduit 14. A sample of a reference gas, which has a composition closely approximating the first material, is introduced through conduit 16. Motor 22 is actuated to rotate disks 19 and 29 at a predetermined rate. Mass spectrometer 10 is set to measure a given mass number of a constituent of the two gases. In the method described in U.S. Pat. No. 3,649,201, for example, the ratio of carbon-13 to carbon-12 is measured in two carbon dioxide samples. In such a measurement, mass spectrometer is first set to measure mass 44, a representative of carbon-12. The apparatus is then adjusted so that the output signals from amplifiers 36 and 37 have the same amplitude. This adjustment can be made by manipulation of one or both of trimming devices 40 and 41 of FIG. 1 which can be rotated into and out of the respective beams to reduce or increase the magnitude of the beam reaching the inlet of the mass spectrometer. After this initial adjustment has been made, mass spectrometer 10 is set to measure a different mass number, such as 45 which is representative of carbon-13. The resulting output signal applied to recorder 39 can be utilized to measure the isotope ratio of carbon-13 in the two samples. The isotope ratio difference can readily be calculated by dividing the difference signal applied to recorder 39 by the output signal from detector 36 alone. To this end, recorder 39 can be a multi-channel recorder which also records the output signal from detector 39. As an alternative, a signal dividing circuit can be provided to divide the difference signal from the two detectors by the signal from detector 36 alone. The signals can be utilized in the manner described in U.S. Pat. No. 3,649,201, for example.

As previously mentioned, the two beams are delivered to the inlet of the mass spectrometer at different frequencies. This is readily accomplished by mounting the two chopping disks on a common shaft, and providing a different number of openings in the two disks. As an alternative, two disks with the same number of openings can be rotated in the respective beams at different rates. If the two beams are directed toward the inlet of the mass spectrometer from adjacent sources at a converging angle, a single disk with two sets of openings can be employed. In this case, one beam passes through one set of openings and the second beam passes through the second set of openings.

In another specific embodiment of this invention, the mass-3 to mass-2 ratio of a hydrogen sample is measured using apparatus of the type illustrated in the drawing. A typical composition of the reference hydrogen sample is 99.8 percent mass-2 and 0.2 percent mass-3. The sample to be analyzed may have a composition of 99.9 percent mass-2 and 0.1 percent mass-3. Disks 19 and 20 are rotated at 50 Hz. Mass spectrometer 10 first measures mass-2 for some 5 to 10 minutes, after which mass-3 is measured for some 2 to 15 minutes.

While this invention has been described in conjunction with presently preferred embodiments, it obviously is not limited thereto.