JPS5928855B2 - How to measure exhaust gas from internal combustion engines - Google Patents
How to measure exhaust gas from internal combustion enginesInfo
- Publication number
- JPS5928855B2 JPS5928855B2 JP1683579A JP1683579A JPS5928855B2 JP S5928855 B2 JPS5928855 B2 JP S5928855B2 JP 1683579 A JP1683579 A JP 1683579A JP 1683579 A JP1683579 A JP 1683579A JP S5928855 B2 JPS5928855 B2 JP S5928855B2
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- gas
- characteristic curve
- analyzer
- concentration
- voltage value
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- 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
- G01N21/27—Colour; Spectral properties, i.e. comparison of effect of material on the light at two or more different wavelengths or wavelength bands using photo-electric detection ; circuits for computing concentration
- G01N21/274—Calibration, base line adjustment, drift correction
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- Mathematical Physics (AREA)
- Theoretical Computer Science (AREA)
- Spectroscopy & Molecular Physics (AREA)
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- Life Sciences & Earth Sciences (AREA)
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- Investigating Or Analysing Materials By Optical Means (AREA)
Description
【発明の詳細な説明】
本発明は当初に求めた特性曲線を基準にして排ガスの測
定濃度の誤差を補正するようにした内燃機関の排ガス測
定方法に関する。DETAILED DESCRIPTION OF THE INVENTION The present invention relates to a method for measuring exhaust gas from an internal combustion engine, in which errors in the measured concentration of exhaust gas are corrected based on an initially determined characteristic curve.
現在、日本国内および外国とも自動車の排ガス規制がな
されておわ、メーカより市販される自動車はすべて、そ
のエンジンが排出する排ガスが上記の排ガス規制をクリ
アしていなければ市販することはできない。Currently, automobile exhaust gas regulations are in place both in Japan and abroad, and all automobiles sold by manufacturers cannot be put on the market unless the exhaust gases emitted by their engines meet the above exhaust gas regulations.
このため、認証用ないし一般市販用の自動車は、そのエ
ンジンが上記排ガス規制をクリアしているか否かを全数
チェックしなければならないが、従来、排ガス中のCo
、C02、HCおよびN0x等の濃度は、非分散形赤外
分析計等を使用して、次のような方法で測定するように
していた。For this reason, all vehicles for certification or general commercial use must be checked to see if their engines meet the above exhaust gas regulations.
, CO2, HC, NOx, etc., were measured by the following method using a non-dispersive infrared analyzer or the like.
例えば、Coの濃度を測定する場合、1COの濃度が零
のゼロガスを非分散形赤外分析計(図示せず。For example, when measuring the concentration of Co, zero gas with a zero concentration of 1CO is measured using a non-dispersive infrared analyzer (not shown).
以下、分析計と記す。)に流してその出力電圧を零に調
整した後、2Co濃度がS’pμmのスパンガスを分析
計に流してその出力電圧をSmV±0.3%となるよう
に調整する。3次いで、Co濃度がB’、C’、D’、
E’およびF’pμmの資料ガスを上記分析計に流し、
これら各Co濃度B’、C’、D’、E’およびF’p
μmに対する上記分析計の出力電圧B、C、D、Eおよ
びFを、第1図に示すように、夫々プロットして基準特
性曲線を求めるとともに該基準特性曲線をコンピュータ
に記憶させておき、4その後、初」l定排ガスを上記分
析器に流してその出力電圧を上記コンピュータに入・
力し、上記基準特性曲線から排ガス中のCo濃度を求め
る。Hereinafter, it will be referred to as an analyzer. ) to adjust its output voltage to zero, then flow a span gas with a 2Co concentration of S'pμm to the analyzer and adjust its output voltage to SmV±0.3%. 3 Next, the Co concentration is B', C', D',
Flow the sample gas of E' and F' pμm into the above analyzer,
Each of these Co concentrations B', C', D', E' and F'p
As shown in FIG. 1, the output voltages B, C, D, E, and F of the analyzer with respect to μm are plotted to obtain a reference characteristic curve, and the reference characteristic curve is stored in the computer. After that, the first constant exhaust gas is passed through the analyzer and its output voltage is input to the computer.
Then, the Co concentration in the exhaust gas is determined from the reference characteristic curve.
しかしながら、上記の分析計は、一般に非常に高感度の
ものであつて、外的温度条件の変化や自己発熱等により
、分析計の各種電子素子が使用中・ に温度変化し、分
析計の出力電圧がドリフトすることは避けることができ
ない。However, the above-mentioned analyzers are generally very sensitive, and the temperature of various electronic elements of the analyzer changes during use due to changes in external temperature conditions or self-heating, and the output of the analyzer changes. Voltage drift is unavoidable.
従つて、上記の1から4の方法で排ガス中のCO等の濃
度を測定した場合、上記分析計は、使用するたびに、充
分なウオームアツプを行つた後、改めて上記の1から3
の操作を行つて新たな基準特性曲線を求め直さなければ
ならず、上記操作を行うたびに厳密に検定された種々の
濃度を有する高価な基準ガスを多量に必要とし、測定コ
ストが高くなる一方、測定の過程が非常に煩雑で時間を
要するばかbでなく、精度の高い測定を行うには熟練を
要するといつた多くの問題があつた。Therefore, when measuring the concentration of CO, etc. in exhaust gas using methods 1 to 4 above, the analyzer should be warmed up sufficiently each time it is used, and then tested again using methods 1 to 3 above.
A new standard characteristic curve must be determined by performing the above operations, and each time the above operation is performed, a large amount of expensive reference gas with various concentrations that have been rigorously verified is required, which increases the measurement cost. However, there were many problems such as the fact that the measurement process was very complicated and time consuming, and required skill to perform highly accurate measurements.
一方、本願発明者は、多数の実測データを解析する過程
で、ゼロガスに対する上記分析計の出力電圧やスパンガ
スに対する上記分析計の出力電圧が変化しても、新らた
に求めた基準特性曲線の直線性等は、当初に求めた基準
特性曲線のものと殆んど変化しないことを見い出した。
本発明は上記の事実に基づいて、従来の内燃機関の排ガ
ス測定方法に卦ける上記問題を解消すべくなされたもの
であつて、当初求めた基準特性曲線に卦けるゼロガス相
当の発生電圧とゼロガスを分析計に流して得た第1発生
電圧との差(ΔVO)と、上記基準特性曲線に}けるス
パンガス相当の発生電圧とスパンガスを分析計に流して
得た第2発生電圧との差(ΔVs)との電圧差変化量(
ΔVsΔo)を上記基準特剛曲線に対して比例配分して
仮特性曲線を求め、該仮特性曲線を新らたな基準特性曲
線とすることにより1測定のたびに新たな基準特性曲線
を求め直す必要をなくし、高価な基準ガスの使用量を少
くするとともに測定の過程を簡略化するようにした、測
定コストの低い内燃機関の排ガス沖淀方法を提供するこ
とを目的としている。On the other hand, in the process of analyzing a large amount of measured data, the inventor of the present application discovered that even if the output voltage of the above-mentioned analyzer for zero gas or the output voltage of the above-mentioned analyzer for span gas changes, the newly obtained standard characteristic curve It has been found that the linearity etc. are almost unchanged from those of the standard characteristic curve originally determined.
The present invention has been made based on the above-mentioned facts to solve the above-mentioned problems in the conventional exhaust gas measurement method for internal combustion engines. The difference (ΔVO) between the first generated voltage obtained by flowing the gas through the analyzer and the difference (ΔVO) between the generated voltage corresponding to the span gas in the above reference characteristic curve and the second generated voltage obtained by flowing the span gas through the analyzer. ΔVs) and the voltage difference change amount (
A temporary characteristic curve is obtained by proportionally distributing ΔVsΔo) to the above standard characteristic curve, and by using this temporary characteristic curve as a new standard characteristic curve, a new standard characteristic curve is recalculated for each measurement. It is an object of the present invention to provide a method for measuring exhaust gas from an internal combustion engine at a low measurement cost, which eliminates the need for an expensive reference gas, reduces the amount of expensive reference gas used, and simplifies the measurement process.
以下、本発明の実施例を示す図面を参照して詳細に説明
する。Hereinafter, embodiments of the present invention will be described in detail with reference to the drawings.
先ず、本願発明の方法を実施する場合、例えば、第2図
に示すような基本構成を有する分析装置を使用すること
ができる。First, when implementing the method of the present invention, for example, an analyzer having a basic configuration as shown in FIG. 2 can be used.
第2図に卦いて、1は(非分散形赤外)分析計、2は増
巾器、3はA/Dコンバータ、4はコンピユータであつ
て、上記分析計1は、パイプ5aから導入された排ガス
をパイプ5bから排出するようにした試料セル5、予め
定められた濃度のCO(COを検出する場合)を含有す
る気体を封入した対照セル6、これら試料セル5および
対照セル6の上部に夫々取り付けられて赤外線を下方に
放射する光源7訃よび8、測定成分と同じCOガスが封
入されるとともにその圧力を電気に変換する検出セル9
卦よび10、検出セル9の出力電圧と検出セル10の出
力電圧との差を出力する差動増巾器11等からなつてい
る。In FIG. 2, 1 is a (non-dispersive infrared) analyzer, 2 is an amplifier, 3 is an A/D converter, and 4 is a computer, and the analyzer 1 is introduced from the pipe 5a. A sample cell 5 in which exhaust gas is discharged from a pipe 5b, a control cell 6 filled with a gas containing CO at a predetermined concentration (in the case of detecting CO), and the upper parts of these sample cells 5 and control cells 6. light sources 7 and 8 that are respectively attached to and emit infrared rays downward, and a detection cell 9 that is filled with CO gas, which is the same as the component to be measured, and that converts the pressure into electricity.
It consists of a differential amplifier 11 that outputs the difference between the output voltage of the detection cell 9 and the output voltage of the detection cell 10.
上記分析計1は、光源7から赤外線を放射して試料セル
5内でCO成分の濃度に応じた吸収を行わせた後に上記
赤外線を検出セル9に入射し、該検出セル9内でCOの
吸収波長のものだけを選択的に吸収させ、封入されてい
るCOガスの温度を上昇させてその圧力を増加させる一
方、光源8から赤外線を放射して対照セル6内で丁定の
吸収を行わせた後に検出セル10に入力し、上記と同様
にして、該検出セル10に封入されているCOガスの圧
力を上記参照セル6内のCO濃度によつて決まる一定値
だけ増加させるようにし、差動増巾11によつて、上記
検出セル9の出力電圧と検出セル10の出力電圧の差か
ら試料セル5内のガスのCO濃度を検出するようにした
ものであつて、上記差動増巾器11の出力を増巾器2を
介してA/Dコンバータ3に入力してデイジタル信号に
変換した後、コンピユータ4に入力して以下に述べるよ
うなデータ処理を行うようにしている。The analyzer 1 emits infrared rays from a light source 7, causes absorption in a sample cell 5 according to the concentration of CO components, and then enters the infrared rays into a detection cell 9. Only the absorption wavelength is selectively absorbed, and the temperature of the enclosed CO gas is raised to increase its pressure, while infrared rays are emitted from the light source 8 and a certain amount of absorption is carried out in the control cell 6. and then input it into the detection cell 10 in the same way as above, increasing the pressure of the CO gas sealed in the detection cell 10 by a constant value determined by the CO concentration in the reference cell 6, The differential amplifier 11 detects the CO concentration of the gas in the sample cell 5 from the difference between the output voltage of the detection cell 9 and the output voltage of the detection cell 10. The output of the amplifier 11 is input to the A/D converter 3 via the amplifier 2 and converted into a digital signal, and then input to the computer 4 for data processing as described below.
本願発明者は、上記分析装置を使用して、従来と同様に
、先ず、1ゼロガスを上記分析計1に流し、差動増巾器
11の調節器(図示せず。)によつてその出力電圧を(
0±0.3)MVに調節した後、2C0濃度が100p
pmのスパンガスを分析計1に流し、上記出力電圧を(
100±0.3)MVに調節し、3次いで、CO濃度が
夫々、6.4,14.0,22.0,31.0,40,
0,49.0,60.0,72.0卦よび85.0pp
mの資料ガスを分析計1に流し、これら資料ガスに対す
る差動増巾器11の出力電圧10.0,30.0,40
.0,50.0,60.0,70.0,80.0卦よび
90.0mVをデイジタル信号に変換してコンピユータ
4に入力し、第3図に示すような基準特性曲線B−B7
を上記コンピユータに記憶させた。しかる後、ゼロガス
相当のときの差動増巾器11の出力電圧(以下、ゼロ点
と記す。The inventor of the present application used the above analyzer to first flow 1 zero gas to the above analyzer 1, as in the conventional case, and controlled the output of the differential amplifier 11 by adjusting the regulator (not shown). Voltage (
0±0.3) After adjusting to MV, the 2C0 concentration is 100p
pm span gas is passed through analyzer 1, and the above output voltage is (
100±0.3) MV, and then the CO concentration was adjusted to 6.4, 14.0, 22.0, 31.0, 40, respectively.
0,49.0,60.0,72.0 trigrams and 85.0pp
m sample gases are passed through the analyzer 1, and the output voltages of the differential amplifier 11 for these sample gases are 10.0, 30.0, 40.
.. 0, 50.0, 60.0, 70.0, 80.0 hexagrams and 90.0 mV are converted into digital signals and input into the computer 4, and a reference characteristic curve B-B7 as shown in FIG.
was stored in the computer. Thereafter, the output voltage of the differential amplifier 11 when equivalent to zero gas (hereinafter referred to as zero point).
)が零MVもしくは(±5)MV変化し、また、スパン
ガス相当のときの差動増巾器11の出力電圧(以下、ス
パン点と記す。)が零Mvもしくは(±5)MV変化し
たとき、上記基準特性曲線B−B7は、その直線性を保
存しながら、次の第1表に対応して第3図に細線で示す
ような仮特性曲線A−A″,C−σ,A−B′,B−C
1卦よびA−C7のように変化することを想定した。上
記のように想定した、例えば仮特性曲線A一Ck基づく
CO濃度の予想値と、ゼロ点卦よびスパン点が夫々(+
5)MVl(−5)MVだけ変化した場合のCO濃度の
実測値との誤差を求めると、ゼロガスからスパンガスに
わたるCO濃度の全濃度で0.13%を越えないことが
判明した(他の仮特性曲線A−N,C−σ,A−B′,
B−C′VCついても同様)。) changes by 0 MV or (±5) MV, and the output voltage of the differential amplifier 11 when equivalent to span gas (hereinafter referred to as the span point) changes by 0 MV or (±5) MV. , the above reference characteristic curve B-B7 is converted into provisional characteristic curves A-A'', C-σ, A- as shown by thin lines in FIG. 3 corresponding to the following Table 1 while preserving its linearity. B', B-C
I assumed that it would change like 1 trigram and A-C7. Assumed above, for example, the predicted value of CO concentration based on the temporary characteristic curve A-Ck, the zero point and the span point are respectively (+
5) When calculating the error from the actual measured value of CO concentration when MVl (-5) MV changes, it was found that the total CO concentration from zero gas to span gas does not exceed 0.13% (other hypothetical Characteristic curves AN, C-σ, AB',
The same applies to B-C'VC).
従つて、上記1から3によつて当初に求めた基準特性曲
線B−B脅、例えば、そのゼロ点が(+5)MVlスパ
ン点が(−5)m変化しても、上記基準特性曲線B−B
′(7)直線性は保存したま\で、仮特性曲線A−C″
に変化する(仮特性曲線A−N,c−σ,A−B′,B
−σについても同様)ものとみなすことができ、このた
め、上記仮特性曲線A−C社、スパン点の変動量(−5
)MVとゼロ点(+5)MVとの差(−10)MVをC
O濃度によつて、上記基準特性曲線B−Bk比例配分す
ることによつて求めることができる。Therefore, even if the zero point of the standard characteristic curve B-B originally obtained from 1 to 3 above changes by (+5) m and the MV1 span point changes by (-5) m, the standard characteristic curve B -B
′(7) While preserving the linearity, create a temporary characteristic curve A-C″
(temporary characteristic curves AN, c-σ, A-B', B
-σ can also be considered as
) MV and the difference (-10) MV from the zero point (+5) MV is C
It can be determined by proportionally distributing the reference characteristic curve B-Bk according to the O concentration.
本発明に卦いては、上記事実に基づいて、一般に第4図
に示すように、基準特性曲線B−B″のゼロ点がVOか
らv′oに、また、スパン点がVsからv″sに夫々変
化した場合に訃いて、任意のCO濃度Cxに対する差動
増巾器11の出力電圧の修正量Δx=v′x−xは、次
のようにして求めるようにしている。In the present invention, based on the above facts, the zero point of the reference characteristic curve B-B'' is generally set from VO to v'o, and the span point is from Vs to v's The correction amount Δx=v'x-x of the output voltage of the differential amplifier 11 for any given CO concentration Cx is determined as follows.
であつて、これら(1)、(2)式から、となる(但し
、CsはスパンガスのCO濃度、COはゼロガスのCO
濃度)。From equations (1) and (2), it becomes (where, Cs is the CO concentration of the span gas, and CO is the CO concentration of the zero gas.
concentration).
従つて、既に説明した従来の1から3の操作によつて基
準特性曲線B−B″を求め、該基準特性曲線B−B7を
コンピユータ4に記憶させて卦けば、以後、次のように
して、再度上記1から3の操作を行うことなく、CO濃
度を検出することができる。Therefore, by calculating the standard characteristic curve B-B'' by the conventional operations 1 to 3 already explained, and storing the standard characteristic curve B-B7 in the computer 4, from now on, proceed as follows. Thus, the CO concentration can be detected without performing the operations 1 to 3 above again.
15先ず、ゼロガスおよびスパンガスを分析計1に流し
て、ゼロ点の変動量ΔVO−Vら−VOとスパン点の変
動量ΔVs=Vく一sとを検出し、25次いで、コンピ
ユータ4によつて、これら変動量ΔVOおよびΔsに基
づいて上記(3)式の演算を行い、修正量ΔX−(−X
を求め、35該修正量ΔX=V′x−Vxによつて基準
特性曲線B−B′を修正し、仮特性曲線を求めて、コン
ピユータ4に記憶する、45被測定排ガスを分析計に流
し、そのときの差動増巾器11の出力電圧に対応するC
O濃度を、コンピユータ4により、上記仮特性曲線から
検出して上記コンピユーヨ4に記憶する。15 First, zero gas and span gas are passed through the analyzer 1 to detect the zero point fluctuation amount ΔVO−V−VO and the span point fluctuation amount ΔVs=V×s. , based on these fluctuation amounts ΔVO and Δs, calculate the above equation (3) to obtain the correction amount ΔX−(−X
35 Correct the reference characteristic curve B-B' by the correction amount ΔX=V'x-Vx, obtain a temporary characteristic curve, and store it in the computer 4. 45 Flow the exhaust gas to be measured into the analyzer. , C corresponding to the output voltage of the differential amplifier 11 at that time
The O concentration is detected from the temporary characteristic curve by the computer 4 and stored in the computer 4.
以上のようにすれば、排ガス中のCO濃度を測定するた
びに、厳密に検定された種々の濃度を有する高価な基準
ガスを使用して、新たな基準特性曲線を求め直す必要は
なく、従つて、基準ガスの使用量が少くなる一方、基準
特性曲線を求め直す必要がないため、測定工数も簡略化
され、本発明の実施により1基準ガス購入費用を大巾に
低減を図ることができ、また、測定工数は約1/3に低
減させることができた。By doing the above, there is no need to re-determine a new reference characteristic curve using expensive reference gases with various concentrations that have been rigorously verified each time the CO concentration in exhaust gas is measured. As a result, the amount of reference gas used is reduced, and there is no need to recalculate the reference characteristic curve, which simplifies the measurement process. By implementing the present invention, it is possible to significantly reduce the cost of purchasing one reference gas. Moreover, the number of measurement steps could be reduced to about 1/3.
な訃、以上の説明に卦いては排ガス中のCO濃度を測定
する場合について説明したが、CO2、HC訃よびNO
x等の濃度の測定についても、上記と全く同様に行うこ
とができる。In the above explanation, we have explained the case of measuring CO concentration in exhaust gas, but CO2, HC and NO
Measurement of the concentration of x, etc. can also be carried out in exactly the same manner as described above.
以上、説細に説明したことからも明らかなように、本発
明は、ゼロ点とスパン点の変動から求めた電圧差変化量
(ΔVs−ΔVO)を当初に求めた基準特性曲線に対し
て比例配分して仮特性曲線を求め、該仮特性曲線を新た
な基準特性曲線として排ガスを測定するようにしたから
、従来のように、排ガスの測定のたびに新たな基準特性
曲線を求め直す必要はなく、従つて、上記基準特性曲線
を求める過程で必要とする高価な基準ガスの使用量や測
定工数を従来に比べて、大巾に削減することができる。As is clear from the above detailed explanation, the present invention is capable of proportionally changing the amount of voltage difference change (ΔVs - ΔVO) obtained from the fluctuation of the zero point and the span point with respect to the initially obtained reference characteristic curve. Since we have determined the provisional characteristic curve by allocating the data and used the provisional characteristic curve as a new standard characteristic curve to measure exhaust gas, there is no need to re-determine a new standard characteristic curve every time we measure exhaust gas, as was the case in the past. Therefore, the amount of expensive reference gas used and the number of measurement steps required in the process of determining the reference characteristic curve can be significantly reduced compared to the conventional method.
第1図は基準特性曲線を求める場合の説明図、第2図は
分析装置のプロツク図、第3図は予め想定した基準特性
曲線の変化を示す説明図、第4図は仮特性曲線の検出方
法を示す説明図である。
1・・・・・・分析計、2・・・・・増巾器、3・・・
・・・A/Dコンバータ、4・・・・・・コンピユータ
、5・・・・・・試料セル、6・・・・・・対照セル、
7,8・・・・・光源、9,10・・・・・・検出セル
、11・・・・・・差動増巾器。Fig. 1 is an explanatory diagram for determining the standard characteristic curve, Fig. 2 is a diagram of the analytical device, Fig. 3 is an explanatory diagram showing changes in the standard characteristic curve assumed in advance, and Fig. 4 is the detection of a temporary characteristic curve. It is an explanatory diagram showing a method. 1...Analyzer, 2...Amplifier, 3...
... A/D converter, 4 ... Computer, 5 ... Sample cell, 6 ... Control cell,
7, 8... Light source, 9, 10... Detection cell, 11... Differential amplifier.
Claims (1)
ガス成分の含有量を測定する内燃機関の非ガス測定方法
において、予め定められた各種濃度のガスを分析計に流
して発生電圧を順次測定し、ガス濃度と電圧値との基準
特性曲線を求めた後、被測定ガスの測定に際し、先ずゼ
ロガスを上記分析計に流して、その時の発生電圧値を第
1発生電圧値として読み取り、次いでスパンガスを上記
分析計に流して、その時の発生電圧値を第2発生電圧値
として読み取つた後、上記基準特性曲線における上記ゼ
ロガス相当の発生電圧値と上記第1発生電圧値との差(
ΔV_0)と、上記基準特性曲線における上記スパンガ
ス相当の発生電圧値と上記第2発生電圧値との差(ΔV
_s)との電圧差変化量(ΔV_s−ΔV_0)を上記
基準特性曲線に対し比例配分して仮特性曲線を求め、次
に上記被測定ガスを分析計に流してこの時発生する電圧
値から上記仮特性曲線によつて濃度値を求め、該濃度値
を被測定ガスの濃度値とする、ことを特徴とする内燃機
関の排ガス測定方法。1 In a non-gas measurement method for internal combustion engines that measures the content of a specified gas component based on the detected voltage value of a non-dispersive infrared analyzer, etc., the generated voltage is measured by flowing gases of various predetermined concentrations through the analyzer. After sequentially measuring the gas concentration and determining the reference characteristic curve of the voltage value, when measuring the gas to be measured, first flow the zero gas through the analyzer and read the generated voltage value at that time as the first generated voltage value. Then, after flowing span gas through the analyzer and reading the generated voltage value at that time as the second generated voltage value, the difference between the generated voltage value corresponding to the zero gas and the first generated voltage value in the reference characteristic curve (
ΔV_0) and the difference (ΔV
A temporary characteristic curve is obtained by proportionally distributing the voltage difference variation (ΔV_s - ΔV_0) between A method for measuring exhaust gas from an internal combustion engine, characterized in that a concentration value is determined based on a temporary characteristic curve, and the concentration value is used as a concentration value of a gas to be measured.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP1683579A JPS5928855B2 (en) | 1979-02-15 | 1979-02-15 | How to measure exhaust gas from internal combustion engines |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP1683579A JPS5928855B2 (en) | 1979-02-15 | 1979-02-15 | How to measure exhaust gas from internal combustion engines |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPS55109948A JPS55109948A (en) | 1980-08-23 |
| JPS5928855B2 true JPS5928855B2 (en) | 1984-07-16 |
Family
ID=11927247
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP1683579A Expired JPS5928855B2 (en) | 1979-02-15 | 1979-02-15 | How to measure exhaust gas from internal combustion engines |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPS5928855B2 (en) |
Families Citing this family (7)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPS58109837A (en) * | 1981-12-24 | 1983-06-30 | Olympus Optical Co Ltd | Compensating method of calibration curve |
| JPS61243343A (en) * | 1985-04-20 | 1986-10-29 | Koyo Kensetsu Kogyo Kk | Ultraviolet ray absorption gas analyzer |
| JPS6378053A (en) * | 1986-09-20 | 1988-04-08 | Horiba Ltd | Gas analyzer |
| US5340987A (en) * | 1991-03-15 | 1994-08-23 | Li-Cor, Inc. | Apparatus and method for analyzing gas |
| US6369387B1 (en) | 1999-10-15 | 2002-04-09 | Li-Cor, Inc. | Gas analyzer |
| JP6571476B2 (en) * | 2015-06-29 | 2019-09-04 | 旭化成エレクトロニクス株式会社 | Gas concentration measuring device |
| JP6530669B2 (en) * | 2015-07-29 | 2019-06-12 | 旭化成エレクトロニクス株式会社 | Gas concentration measuring device |
-
1979
- 1979-02-15 JP JP1683579A patent/JPS5928855B2/en not_active Expired
Also Published As
| Publication number | Publication date |
|---|---|
| JPS55109948A (en) | 1980-08-23 |
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