GB2031146A - Creación de Inventos y Patentes con Inteligencia Artificial

GB2031146A – Gasanalyzer
– Google Patents

GB2031146A – Gasanalyzer
– Google Patents
Gasanalyzer

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Publication number
GB2031146A

GB2031146A
GB7930187A
GB7930187A
GB2031146A
GB 2031146 A
GB2031146 A
GB 2031146A
GB 7930187 A
GB7930187 A
GB 7930187A
GB 7930187 A
GB7930187 A
GB 7930187A
GB 2031146 A
GB2031146 A
GB 2031146A
Authority
GB
United Kingdom
Prior art keywords
attenuation
gas
analyzer
measuring
chamber
Prior art date
1978-09-01
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.)

Granted

Application number
GB7930187A
Other versions

GB2031146B
(en

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.)

INSTRUMENTATION Oy

Original Assignee
INSTRUMENTATION Oy
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.)
1978-09-01
Filing date
1979-08-31
Publication date
1980-04-16

1979-08-31
Application filed by INSTRUMENTATION Oy
filed
Critical
INSTRUMENTATION Oy

1980-04-16
Publication of GB2031146A
publication
Critical
patent/GB2031146A/en

1983-01-06
Application granted
granted
Critical

1983-01-06
Publication of GB2031146B
publication
Critical
patent/GB2031146B/en

Status
Expired
legal-status
Critical
Current

Links

Espacenet

Global Dossier

Discuss

238000010521
absorption reaction
Methods

0.000
claims
description
15

239000007789
gas
Substances

0.000
description
19

230000000694
effects
Effects

0.000
description
5

238000005259
measurement
Methods

0.000
description
3

230000005855
radiation
Effects

0.000
description
3

238000002474
experimental method
Methods

0.000
description
2

230000001154
acute effect
Effects

0.000
description
1

239000012080
ambient air
Substances

0.000
description
1

QVGXLLKOCUKJST-UHFFFAOYSA-N
atomic oxygen
Chemical compound

[O]
QVGXLLKOCUKJST-UHFFFAOYSA-N
0.000
description
1

230000001419
dependent effect
Effects

0.000
description
1

238000010586
diagram
Methods

0.000
description
1

238000000034
method
Methods

0.000
description
1

239000001301
oxygen
Substances

0.000
description
1

229910052760
oxygen
Inorganic materials

0.000
description
1

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

G01N21/25—Colour; Spectral properties, i.e. comparison of effect of material on the light at two or more different wavelengths or wavelength bands

G01N21/31—Investigating relative effect of material at wavelengths characteristic of specific elements or molecules, e.g. atomic absorption spectrometry

G01N21/35—Investigating relative effect of material at wavelengths characteristic of specific elements or molecules, e.g. atomic absorption spectrometry using infrared light

G01N21/37—Investigating relative effect of material at wavelengths characteristic of specific elements or molecules, e.g. atomic absorption spectrometry using infrared light using pneumatic detection

Description

1 GB 2 031 146A 1
SPECIFICATION
Gas analyzer The present invention relates to a gas analyzer, for instance aC02 analyzer, comprising a 5 measuring chamber for the gas to be examined, a reference chamber from which the gas to be measured has been drawn off, a light source, a chopper disc which chops the light beam to make it pass alternatingly through the measuring and reference chambers and so that in between there is a period during which no light is passed through at all, and an automatic gain control which maintains a constant difference between the «dark» signal and the signal 10 delivered by the reference chamber.
The problem in known gas analyzers of this type is that as the light has to travel a certain distance through ambient gas an error is introduced by variations of the content of the gas under measurement in the ambient gas. The magnitude of this error is dependent on the ambient content, on the distance which the light beam travels in the ambient space and the 15 content of the gas under measurement. In a CO, analyzer, for instance, where the measuring light beam travels parts of its path in the ambient CO, content, the varying ambient CO, content introduces an error. This problem is particularly acute in CO, analyzers because the absorption of infra-red radiation as a function of CO, content is strongly non-linear. The ambient C02, causes equal attenuation both of the measuring and the reference beam. Since in the case of increasing 20 CO,, content the absorption caused by it increases at a relatively slower rate, that is, the absorption curve plotted as a function of content becomes less steep at the upper end, even a minor additional absorption causes a major error. This is only minimally corrected by the change in gain which is caused by the attenuation of the reference beam due to the ambient environment.
An object of the invention is to provide a gas analyzer of the type mentioned above, in which the error effect referred to can be substantially reduced.
According to the invention there is provided a gas analyzer comprising a measuring chamber for the gas to be examined, a reference chamber from which the gas to be measured has been drawn off, a light source for emitting a light beam, a chopper disc for chopping the light beam 30 so that the beam alternatingly passes through the measuring and reference chambers, an automatic gain control adapted to maintain constant the difference between a dark signal and a signal from the reference chamber, and an attenuation member located in the path of the light beam passing through the reference chamber, which member in the wavelength range employed has a high enough attenuation capacity to cause a shift of the operating point of the 35 gain control circuit to a gently sloping part of the absorption versus concentration curve.
In use of the invention the additional attenuation caused by the ambient environment in the reference beam results in a change of gain which compensates for the ambient attenuation of the measuring beam.
It is advantageous in the measuring ranges normally involved in CO,, analyzers if the attenuation of the attenuation disc is of the order of 8%.
In the accompanying drawings:
Figure 1 shows an embodiment of a gas analyzer of the invention, partly as a block diagram and partly in structural cross section; and Figure 2 shows the absorption curve for infra-red radiation plotted against the CO,, content.
Fig. 1 shows a frame plate 1 having a motor 2 attached thereto which rotates a chopper disc 3 provided with a sequence of holes 5 for chopping a measuring beam 7 and a sequence of holes 6 for chopping a reference beam 8 in such manner that the beams 7 and 8 will alternately pass the disc. The beams 7 and 8 are transmitted from an infra-red light source 9, and the measuring beam 7 passes through a measuring chamber 10 and the reference beam 8 through 50 a reference chamber 11. In the present exemplary case the analyzer is a C02, analyzer. The gas of which the C02, content is to be measured is conducted through the measuring chamber 10.
In the reference chamber 11 a gas is enclosed from which the C02, has been drawn off. The filter 12 is employed to filter out of the radiation all but that wavelength range in whichC02, displays the strongest absorption. After the measuring and reference beams 7 and 8 have in 55 succession arrived at the detector 14, there follows a dark period, which is used for the automatic gain control to be described later on, by keeping constant the difference between the dark signal and the signal 8 produced by the reference chamber 11. The tripartite signal (measuring signal plus reference signal plus dark signal) thus formed at the detector is conducted through a pre-amplifier 15 to an AC amplifier 16, the operating point of the latter 60 being governed by an automatic gain control circuit 22.
In order to render the said three signals (measuring, reference and dark signal) identifiable and distinguishable from each other, the chopper disc 3 is provided with three sequences of synchronizing holes 4, through which synchronizing light pulses are transmitted from a LED unit 16, these pulses being received in the light receiver and synchronizing signal transmitter unit 65 2 GB 2 031 146A 2 18. The positions of the holes 4 in the chopper disc 3 is so chosen that a signal A coincides with the measuring signal received by the detector 14, a signal B with the reference signal and a signal C with the dark signal. With the aid of these synchronizing signals A, B and C the synchronizing and measuring difference signal forming unit 20 is controlled by the timing 5 control unit 19. I The unit 20 has the task of forming the analog and difference signals between the three different phases of the signal coming from the unit 16. Firstly, there is generated therein a reference voltage by measuring the difference between the reference signal and the dark signal. This difference voltage is monitored by an automatic gain control circuit 22 to keep it at a predetermined constant value. The control circuit 22 governs the AC amplifier 16 for maintaining the said predetermined reference voltage. Secondly, the measuring signal proper is formed in the unit 20. This signal is obtained as the difference between the signal received through the measuring chamber 10 and that received through the reference chamber 11. This analog difference signal is conducted to a DC amplifier 23 and thence via linearizing and measuring circuits 24 to a display instrument 25 on which the C02, content can be read. The 15 linearizing process taking place in the circuit 24 serves to compensate for the non-linear relationship between the absorption and the C02, content in the measuring chamber 10, displayed in Fig. 2.
The above-described principle of design and operation of the analyzer is known in the art. It is inevitable that the measuring beam 7 travels part of its path through the ambient gas. The non- 20 linear relationship between absorption and C02, content, shown in Fig. 2, has the effect that an additional absorption is caused by the ambient C02, content variations, even at comparatively low concentrations, and in the gently sloping portion of the curve the additional absorption is large enough to cause an appreciable error in the content that is being measured.
The apparatus of the invention compensates for this to a substantial extent, by placing in front 25 of the reference chamber 11 an attenuation plate 13, which within the wavelength range selected by the filter 12 has a large enough attenuating capacity to cause the result that the automatic gain control circuit 22 shifts the operating point of the AC amplifier 16 to the shallow part of the curve reproduced in Fig. 2. As can be seen in Fig. 2, a suitable absorption for the attenuation disc in a C02, analyzer, is about 8%. In that case the additional attenuation due to 30 the ambient environment is sufficient at the reference level too, to cause such a change of the gain that this change will compensate for a substantial part of that interference attenuation which the measuring beam suffers due to the environment.
This compensating effect is illustrated by the aid of two experiments set out below. In both experiments which were carried out, the ambient C02, content was first 0. 0 and, next 0.3% by 35 volume. The length of the light beam path through ambient air was 4 mm and the path within the measuring chamber was also 4 mm. The gas which was measured had in both instances a content of 8% C02, by volume.
1. Without attenuation disc Total Total Measuring atten- atten Ambient chamber Ambient uation uation Total content attenua- attenu- in ref. in meas. Equivalent error 45 % CO, tion ation chamber chamber to CO,-% C02_% at 4 0 9.2 0 0 9.2 8 0 0.3 9.2 0.5 0.5 9.65 9.2 1.2 50 2. With attenuation disc Absorption of the attenuation disc is 8% Total Total Measuring attenatten- Equi- Ambient chamber Ambient Atten- uation uation valent content attenua- attenua- uation in ref. in meas. to C02 Error % C02 tion tion % disc % chamber chamber % C02% 60 0 9.2 0 8 8.0 9.2 8 0 0.3 9.2′ 0.5 8 8.46 9.65 8.2 0.2 3 GB 2 031 146A 3 1.
From the foregoing it will be seen that by using an attenuation disc 13 it is possible in a simple and inexpensive way to improve substantially the accuracy of measurement of the analyzer by causing a shift of the reference level to move. the operation of the analyzer into the gently sloping part of the absorption curve, whereby the effect of the incremental attenuation due to the ambient environment will produce an adequate change in the amplifier gain for 5 substantial compensation of the incremental attenuation of the measuring beam due to ambience.
Although in the foregoing the invention has been described in connection with a C02 analyzer, it will be obvious that it is applicable in other types of gas analyzers. For example, the invention has been tried out in an oxygen analyzer, and there too it has been found to eliminate 10 the ambient interference effects to a remarkable extent.

Claims (5)

1. A gas analyzer comprising a measuring chamber for the gas to be examined, a reference chamber from which the gas to be measured has been drawn off, a light source for emitting a light beam, a chopper disc for chopping the light beam so that the beam alternatingly passes through the measuring and reference chambers, an automatic gain control adapted to maintain constant the difference between a dark signal and a signal from the reference chamber, and an attenuation member located in the path of the light beam passing through the reference chamber, which member in the wavelength range employed has a high enough attenuation capacity to cause a shift of the operating point of the gain control circuit to a gently sloping part of the absorption versus concentration curve.

2. An analyzer according to claim 1, adapted for use as a C02 analyzer, wherein the attenuation by the attenuation member is of the order of 8%.

3. An analyzer according to claim 1 or 2, wherein the attenuation member is disposed 25 between the reference chamber and the chopper disc.

4. An analyzer according to claim 3, wherein the attenuation member is an attenuation plate affixed to the surface of the reference chamber.

5. A gas analyzer substantially as herein described with reference to the accompanying drawings.
Printed for Her Majesty’s Stationery Office by Burgess & Son (Abingdon) Ltd.-1 980. Published at The Patent Office, 25 Southampton Buildings, London, WC2A 1AY, from which copies may be obtained.

GB7930187A
1978-09-01
1979-08-31
Gasanalyzer

Expired

GB2031146B
(en)

Applications Claiming Priority (1)

Application Number
Priority Date
Filing Date
Title

FI782692A

FI56902C
(en)

1978-09-01
1978-09-01

a gas analyzer

Publications (2)

Publication Number
Publication Date

GB2031146A
true

GB2031146A
(en)

1980-04-16

GB2031146B

GB2031146B
(en)

1983-01-06

Family
ID=8511976
Family Applications (1)

Application Number
Title
Priority Date
Filing Date

GB7930187A
Expired

GB2031146B
(en)

1978-09-01
1979-08-31
Gasanalyzer

Country Status (8)

Country
Link

US
(1)

US4266131A
(en)

JP
(1)

JPS5554432A
(en)

DE
(1)

DE2935509A1
(en)

FI
(1)

FI56902C
(en)

FR
(1)

FR2435030A1
(en)

GB
(1)

GB2031146B
(en)

NL
(1)

NL7906551A
(en)

SE
(1)

SE440407B
(en)

Cited By (1)

* Cited by examiner, † Cited by third party

Publication number
Priority date
Publication date
Assignee
Title

US5510269A
(en)

1992-11-20
1996-04-23
Sensors, Inc.
Infrared method and apparatus for measuring gas concentration including electronic calibration

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Assignee
Title

US4370553A
(en)

1980-07-02
1983-01-25
Sensors, Inc.
Contaminated sample gas analyzer and gas cell therefor

US4413427A
(en)

1981-07-29
1983-11-08
Aer Corporation
Fuel control system for dryer

US4499377A
(en)

1982-09-29
1985-02-12
Acme Engineering Products Ltd.
Detection and control system based on ambient air quality

FI67625C
(en)

1983-04-06
1985-04-10
Instrumentarium Oy

FOERFARANDE FOER ELIMINERING AV MAETNINGSFEL VID FOTOMETERANALYS

JPH0432601Y2
(en)

1985-12-20
1992-08-05

DE3627232C2
(en)

1986-08-11
1995-11-16
Leybold Ag

Photometer

US4907166A
(en)

1986-10-17
1990-03-06
Nellcor, Inc.
Multichannel gas analyzer and method of use

US4817013A
(en)

1986-10-17
1989-03-28
Nellcor, Inc.
Multichannel gas analyzer and method of use

DE4342246C2
(en)

1993-12-10
1997-03-20
Karl Stefan Riener

Characteristic absorption

US5464983A
(en)

1994-04-05
1995-11-07
Industrial Scientific Corporation
Method and apparatus for determining the concentration of a gas

US5870185A
(en)

1996-10-21
1999-02-09
C.F.C. Technology, Inc.
Apparatus and method for fluid analysis

US5925831A
(en)

1997-10-18
1999-07-20
Cardiopulmonary Technologies, Inc.
Respiratory air flow sensor

US6809807B1
(en)

1999-03-09
2004-10-26
Integ, Inc.
Body fluid analyte measurement

US7321424B2
(en)

2004-08-05
2008-01-22
Acton Research Corp.
Self-referencing instrument and method thereof for measuring electromagnetic properties

US11204378B2
(en)

2019-12-30
2021-12-21
Texas Instruments Incorporated
Background suppression for MM-wave spectroscopy

US11652455B2
(en)

2021-02-11
2023-05-16
Cirrus Logic, Inc.
Chop tone management for a current sensor or a voltage sensor

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Priority date
Publication date
Assignee
Title

US3116413A
(en)

1959-07-04
1963-12-31
Hartmann & Braun Ag
Apparatus for the analysis of gas mixtures by absorption of radiation

US3193676A
(en)

1961-12-15
1965-07-06
Parsons & Co Sir Howard G
Infra-red gas analysers

US3560736A
(en)

1968-10-09
1971-02-02
Mine Safety Appliances Co
Non-dispersive infrared gas analyzer with unbalanced operation

US3790797A
(en)

1971-09-07
1974-02-05
S Sternberg
Method and system for the infrared analysis of gases

US4008394A
(en)

1973-06-28
1977-02-15
Sensors, Inc.
Gas analyzing

US4087690A
(en)

1976-06-22
1978-05-02
E. I. Du Pont De Nemours And Company
Spurious radiation compensation in infrared analyzers

GB1560613A
(en)

1977-03-24
1980-02-06
Yokogawa Electric Works Ltd
Infrared gas analyzer

1978

1978-09-01
FI
FI782692A
patent/FI56902C/en
not_active
IP Right Cessation

1979

1979-08-31
GB
GB7930187A
patent/GB2031146B/en
not_active
Expired

1979-08-31
FR
FR7921949A
patent/FR2435030A1/en
active
Granted

1979-08-31
SE
SE7907265A
patent/SE440407B/en
not_active
IP Right Cessation

1979-08-31
NL
NL7906551A
patent/NL7906551A/en
active
Search and Examination

1979-08-31
US
US06/071,564
patent/US4266131A/en
not_active
Expired – Lifetime

1979-09-01
JP
JP11233779A
patent/JPS5554432A/en
active
Pending

1979-09-03
DE
DE19792935509
patent/DE2935509A1/en
not_active
Ceased

Cited By (3)

* Cited by examiner, † Cited by third party

Publication number
Priority date
Publication date
Assignee
Title

US5510269A
(en)

1992-11-20
1996-04-23
Sensors, Inc.
Infrared method and apparatus for measuring gas concentration including electronic calibration

US5583339A
(en)

1992-11-20
1996-12-10
Sensors, Inc.
Infrared method and apparatus for measuring gas concentration of a plurality of component gases in a sample

USRE36277E
(en)

1992-11-20
1999-08-24
Sensors, Inc.
Infrared method and apparatus for measuring gas concentration of a plurality of component gases in a sample

Also Published As

Publication number
Publication date

DE2935509A1
(en)

1980-03-13

GB2031146B
(en)

1983-01-06

SE440407B
(en)

1985-07-29

NL7906551A
(en)

1980-03-04

FR2435030A1
(en)

1980-03-28

US4266131A
(en)

1981-05-05

FI56902C
(en)

1980-04-10

JPS5554432A
(en)

1980-04-21

SE7907265L
(en)

1980-03-02

FI56902B
(en)

1979-12-31

FR2435030B1
(en)

1984-06-29

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