WO2019186794A1 - Gas detecting method and gas detecting device - Google Patents
Gas detecting method and gas detecting device Download PDFInfo
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- WO2019186794A1 WO2019186794A1 PCT/JP2018/012862 JP2018012862W WO2019186794A1 WO 2019186794 A1 WO2019186794 A1 WO 2019186794A1 JP 2018012862 W JP2018012862 W JP 2018012862W WO 2019186794 A1 WO2019186794 A1 WO 2019186794A1
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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
- G01N21/41—Refractivity; Phase-affecting properties, e.g. optical path length
- G01N21/45—Refractivity; Phase-affecting properties, e.g. optical path length using interferometric methods; using Schlieren methods
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- G—PHYSICS
- G01—MEASURING; TESTING
- G01N—INVESTIGATING OR ANALYSING MATERIALS BY DETERMINING THEIR CHEMICAL OR PHYSICAL PROPERTIES
- G01N29/00—Investigating or analysing materials by the use of ultrasonic, sonic or infrasonic waves; Visualisation of the interior of objects by transmitting ultrasonic or sonic waves through the object
- G01N29/02—Analysing fluids
- G01N29/024—Analysing fluids by measuring propagation velocity or propagation time of acoustic waves
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- G—PHYSICS
- G01—MEASURING; TESTING
- G01N—INVESTIGATING OR ANALYSING MATERIALS BY DETERMINING THEIR CHEMICAL OR PHYSICAL PROPERTIES
- G01N33/00—Investigating or analysing materials by specific methods not covered by groups G01N1/00 - G01N31/00
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- G—PHYSICS
- G01—MEASURING; TESTING
- G01N—INVESTIGATING OR ANALYSING MATERIALS BY DETERMINING THEIR CHEMICAL OR PHYSICAL PROPERTIES
- G01N33/00—Investigating or analysing materials by specific methods not covered by groups G01N1/00 - G01N31/00
- G01N33/22—Fuels; Explosives
Definitions
- the present invention relates to a gas detection method and a gas detection device.
- a loading arm is usually used. After unloading, LNG vaporized gas remains in the loading arm. Therefore, when disconnecting the loading arm, it is required to purge the LNG vaporized gas in the loading arm with an inert gas and confirm that the concentration of the LNG vaporized gas discharged from the loading arm is below the lower explosion limit concentration. It has been.
- nitrogen is used as an inert gas when purging for the purpose of discharging LNG vaporized gas.
- nitrogen is used as the inert gas is that if moisture or carbon dioxide is contained, the moisture or carbon dioxide is solidified at the temperature of LNG, which may damage the inside of the pipe or equipment.
- Patent Document 1 describes that an LNG vaporized gas or an LPG vaporized gas is detected by a catalytic combustion gas detector.
- the main component of LNG is methane
- paraffinic hydrocarbon components such as ethane, propane, and butane are also included
- the composition of LNG varies depending on the place of production.
- the gas discharged by purging the LNG vaporized gas in the loading arm with an inert gas contains a large amount of methane that is easily vaporized at the initial stage.
- the boiling point of ethane, propane, butane, etc. is high.
- the ratio of paraffinic hydrocarbon components is high.
- the tendency of the composition of the LNG vaporized gas to change with time varies depending on the place where the LNG is produced, and it is difficult to predict the tendency of the composition to change with time.
- the catalytic combustion type sensor and the semiconductor type sensor cannot detect the concentration of the paraffinic hydrocarbon component in the inert gas such as nitrogen gas because oxygen is indispensable from the detection principle.
- a non-dispersive infrared sensor cannot detect a plurality of types of paraffinic hydrocarbon components contained in LNG at the same sensitivity level. As described above, for example, there is no gas sensor having an equivalent sensitivity level with respect to all paraffinic hydrocarbon components contained in the LNG vaporized gas having an inert gas as a base gas.
- the present invention has been made based on the above circumstances, and even for a test gas containing an inert gas as a base gas, the total concentration of paraffinic hydrocarbon components in the test gas and the test It is an object of the present invention to provide a gas detection method and a gas detection device that can obtain the lower explosion limit concentration of gas with a certain accuracy.
- the gas detection method of the present invention uses a mixed gas containing two or more paraffinic hydrocarbon components as a test gas, Measure the refractive index and specific gravity of the test gas, Based on the ratio ( ⁇ s / ⁇ n) of the specific gravity difference ( ⁇ s) between the test gas and the base gas in the test gas to the refractive index difference ( ⁇ n) between the test gas and the base gas.
- ⁇ s / ⁇ n the specific gravity difference
- ⁇ n refractive index difference
- the total concentration of paraffinic hydrocarbon components in the test gas and the lower explosive limit concentration of the test gas are calculated, It is preferable to calculate a lower explosion limit percentage concentration indicating a percentage of the total concentration of paraffinic hydrocarbon components of the test gas with respect to the lower explosion limit concentration of the test gas.
- the test gas is preferably an LNG vaporized gas or an LPG vaporized gas containing an inert gas as a base gas, and the inert gas is preferably a nitrogen gas.
- the specific gravity difference ( ⁇ s) between the test gas and the nitrogen gas that is the base gas of the test gas is determined by the specific gravity difference between the specific hydrocarbon component and the nitrogen gas (specific gravity difference normalized value normalized by Delta] s H) calculates a ( ⁇ s / ⁇ s H), the refractive index difference between the test gas and nitrogen gas ([Delta] n), and nitrogen gas that particular hydrocarbon component refractive index difference refractive index difference normalized value normalized by ( ⁇ n H) ( ⁇ n / ⁇ n H) calculated for, It is preferable to calculate a ratio of the specific gravity difference normalized value ( ⁇ s / ⁇ s H ) to the refractive index difference normalized value ( ⁇ n / ⁇ n H ).
- the specific hydrocarbon component is methane gas
- the ratio of the specific gravity difference normalized value normalized based on methane gas to the refractive index difference normalized value is taken as the X axis
- y is the lower explosion limit concentration [vol%]
- x is the ratio of the specific gravity difference normalized value based on methane gas to the refractive index difference normalized value. It is.
- the ratio of the specific gravity difference normalized value normalized with respect to methane gas to the refractive index difference normalized value is x
- the refractive index difference between the test gas and nitrogen gas is ⁇ n
- the gas detection apparatus of the present invention uses a mixed gas containing two or more paraffinic hydrocarbon components as a test gas, A refractive index measuring means for measuring the refractive index of the test gas; Specific gravity measuring means for measuring the specific gravity of the test gas; The ratio ( ⁇ s / ⁇ n) of the specific gravity difference ( ⁇ s) between the test gas and the base gas in the test gas to the refractive index difference ( ⁇ n) between the test gas and the base gas in the test gas is calculated.
- a ratio calculating means for One or both of HC component concentration calculating means for calculating the total concentration of paraffinic hydrocarbon components in the test gas based on the ratio and LEL calculating means for calculating the lower explosion limit concentration of the test gas are provided. It is characterized by.
- the gas detection device of the present invention comprises both the HC component concentration calculating means and the LEL calculating means,
- the lower explosive limit percentage concentration calculating means for calculating the lower explosive limit percentage concentration indicating the percentage of the total concentration of the paraffinic hydrocarbon components of the detected gas with respect to the explosive lower limit concentration of the detected gas is provided. It is preferable.
- the test gas is preferably an LNG vaporized gas or an LPG vaporized gas containing an inert gas as a base gas, and the inert gas is preferably a nitrogen gas.
- the gas detection method and the gas detection apparatus of the present invention regardless of the composition ratio of the paraffinic hydrocarbon component, the total concentration of the paraffinic hydrocarbon component contained in the test gas, the lower explosive limit concentration of the test gas , And the lower explosion limit percentage concentration can be obtained with a certain accuracy.
- a mixed gas containing two or more paraffinic hydrocarbon components is used as a test gas.
- the test gas include LNG vaporized gas and LPG vaporized gas mainly containing paraffinic hydrocarbons containing inert gas such as nitrogen gas or air as a base gas.
- inert gas such as nitrogen gas or air
- FIG. 1 is a block diagram schematically showing the configuration of an example of the gas detection apparatus of the present invention.
- the gas detection apparatus includes a gas detection unit 10 that measures a physical property value of a test gas, and an arithmetic processing unit 20 that processes data output from the gas detection unit 10.
- the gas detection unit 10 includes a sound speed measuring unit 11 that measures the sound speed V d of the test gas, and a refractive index measurement unit 15 that measures the refractive index n d of the test gas.
- the test gas is sequentially supplied to the sound velocity measuring means 11 and the refractive index measuring means 15 as indicated by white arrows in FIG.
- an ultrasonic sensor can be used as the sound speed measuring means 11.
- the ultrasonic sensor has a measurement tube in which a sound wave transmission source is provided at one end and a sound wave reception source is provided at the other end.
- the time (propagation time) required for the sound wave from the sound wave source to propagate through the test gas and reach the sound wave receiving source is measured in the state where the test gas is circulated in the measuring tube.
- the sound velocity V d of the test gas is obtained from the value of the propagation time.
- the refractive index measuring means 15 for example, a difference in refractive index of light between a test gas and a reference gas such as air is detected as a displacement of interference fringes, and the refraction of the test gas is based on the amount of displacement.
- a light wave interferometer that measures the rate n d can be used.
- the arithmetic processing unit 20 includes a specific gravity measuring mechanism 25 that obtains the specific gravity S d of the test gas based on the value of the sound velocity V d of the test gas and the refractive index n d of the test gas.
- the specific gravity measuring mechanism 25 is measured by a sound speed-specific gravity conversion processing means 26 for obtaining a sound speed converted specific gravity S a based on the value of the sound speed V d of the test gas measured by the sound speed measuring means 11 and the refractive index measuring means 15.
- refractive index determine the refractive index in terms of the specific gravity S b based on the value of the refractive index n d of the test gas - relative density conversion processing means 27, the gas to be detected on the basis of the sound speed in terms of the specific gravity S a and refractive index in terms of the specific gravity S b
- Specific gravity calculating means 28 for obtaining the specific gravity S d of
- the sound velocity-specific gravity conversion processing means 26 uses, for example, the correlation between the sound speed and specific gravity of the specific gas that has been acquired in advance for the specific gas consisting only of the paraffinic hydrocarbon component, and the sound velocity conversion specific gravity of the test gas. Sa is calculated. Specifically, assuming that the test gas is a specific gas, the sound speed conversion specific gravity Sa is calculated by comparing the value of the sound speed V d acquired for the test gas with the correlation.
- the refractive index-specific gravity conversion processing means 27 uses, for example, the correlation between the refractive index and specific gravity of the specific gas acquired in advance for the specific gas consisting only of the paraffinic hydrocarbon component, to refract the test gas.
- the rate conversion specific gravity Sb is calculated. Specifically, assuming that the test gas is a specific gas, the refractive index conversion specific gravity S b is calculated by comparing the value of the refractive index n d acquired for the test gas with the correlation.
- the specific gravity calculating means 28 is based on the sound speed converted specific gravity S a obtained by the sound speed-specific gravity conversion processing means 26 and the refractive index converted specific gravity S b obtained by the refractive index-specific gravity conversion processing means 27, as shown in the following formula (3).
- the specific gravity S d of the test gas is calculated.
- the specific gravity S d , the sound velocity converted specific gravity S a , and the refractive index converted specific gravity S b of the test gas are all values when the specific gravity of air is 1.
- ⁇ is a correction factor.
- the correction factor ⁇ is preferably a value within a numerical range of, for example, 2.4 or more and 9.3 or less, and more preferably a value within a numerical range of 3.0 or more and 6.2 or less. Since the correction factor ⁇ is a value within the above numerical range, even if the sample gas contains a mixed gas, the correction factor ⁇ is obtained regardless of the composition of the mixed gas and the sample gas. The difference between the specific gravity S d of the test gas and the true value of the specific gravity of the test gas is small.
- the arithmetic processing unit 20 in the gas detection device includes a ratio calculation unit 30 that calculates a ratio between data related to the specific gravity S d of the test gas and data related to the refractive index n d of the test gas.
- the LEL calculating means 35 for calculating the lower explosion limit concentration y of the test gas based on the ratio, and the HC component for calculating the total concentration y ′ of paraffinic hydrocarbon components in the test gas based on the ratio
- the concentration calculation means 40 and the lower explosion limit percentage concentration y L of the test gas are calculated based on the lower explosion limit concentration y of the test gas and the total concentration y ′ of paraffinic hydrocarbon components in the test gas. Explosive lower limit percentage concentration calculation means 45 is provided.
- the ratio calculating means 30 is configured to calculate a ratio ( ⁇ s) of a specific gravity difference ( ⁇ s) between the test gas and the base gas in the test gas to a refractive index difference ( ⁇ n) between the test gas and the base gas in the test gas. / ⁇ n).
- the ratio calculation means 30 normalizes the specific gravity difference ( ⁇ s) between the test gas and the base gas and the refractive index difference ( ⁇ n) between the test gas and the base gas, and the respective normalized values obtained thereby are normalized. It is preferable to have a function of calculating the ratio using the data relating to the specific gravity S d of the test gas and the data relating to the refractive index n d of the test gas. Specifically, the specific gravity difference ( ⁇ s) between the test gas and the base gas is normalized by the specific gravity difference ( ⁇ s H ) between the specific hydrocarbon component and the base gas, and the specific gravity difference normalized value ( ⁇ s / ⁇ s) H ) is calculated.
- the refractive index difference ( ⁇ n) between the test gas and the base gas is normalized based on the refractive index difference ( ⁇ n H ) between the specific hydrocarbon component and the base gas, and the refractive index difference normalized value ( ⁇ n) / ⁇ n H ) is calculated.
- the normalized value to calculate the ratio of the data related to the specific gravity of the test gas to the data related to the refractive index of the test gas, the evaluation can be performed on a constant basis regardless of the composition of the test gas.
- the specific hydrocarbon component is preferably methane gas. This is because the ratio x obtained by the ratio calculation means 30 can be normalized (normalized) so that the maximum value is 1.
- the ratio x of the specific gravity difference normalized value normalized with respect to methane gas to the refractive index difference normalized value is calculated by, for example, the following formula (4).
- ⁇ n is the difference in refractive index between the test gas and nitrogen gas (n ⁇ n N2 )
- ⁇ n CH4 is the difference in refractive index between methane gas and nitrogen gas (n CH4 ⁇ n N2 )
- ⁇ s CH4 is the specific gravity difference between the methane gas and nitrogen gas (s CH4 ⁇ s N2 ).
- the refractive index and specific gravity of air may be used instead of the refractive index n N2 and specific gravity s N2 of nitrogen gas.
- the refractive index and specific gravity of the specific hydrocarbon component used as a reference instead of the refractive index n CH4 and specific gravity s CH4 of methane gas are used. Use it.
- the LEL calculation means 35 calculates the lower explosion limit concentration y [vol%] of the test gas based on the calibration curve indicating the correlation between the ratio x obtained by the ratio calculation means 30 and the lower explosion limit concentration y.
- the calibration curve is, for example, the ratio x of the specific gravity difference normalized value ( ⁇ s / ⁇ s CH4 ) normalized with respect to methane gas to the refractive index difference normalized value ( ⁇ n / ⁇ n CH4 ) as the X axis, and the lower explosion limit concentration
- the curve is approximated by a curve or a broken line included in a region between the curve represented by the equation (1-a) and the curve represented by the equation (1-b). Is.
- the reason why the calibration curve is set in this way is as follows.
- the specific gravity and refractive index of each of a plurality of kinds of test gases having a paraffinic hydrocarbon component as the main component and different compositions are actually measured, and the refractive index difference of the specific gravity difference normalized value based on methane gas.
- a ratio x to the normalized value is calculated.
- the lower explosion limit concentration is calculated based on the composition of each test gas, and the actually measured values thus obtained are represented by the ratio x as the X axis and the lower explosion limit concentration as the Y axis. And plotted in an XY coordinate system. As a result, as indicated by a solid line in FIG.
- the relationship between the ratio x and the lower explosion limit concentration y is drawn by a single curve (hereinafter referred to as “reference calibration curve”) Cs, regardless of the composition of the test gas. It was confirmed that it was possible.
- the reference calibration curve Cs is a curve represented by the following mathematical formula (5).
- the value of the lower explosive limit concentration of various paraffinic hydrocarbon components is shown in, for example, IEC standard, ISO standard, or ICSC (International Chemical Safety Card, International Chemical Safety Card).
- IEC standard International Chemical Safety Card
- ISO standard International Chemical Safety Card
- ICSC International Chemical Safety Card
- y the value of the lower explosion limit concentration y.
- the allowable range ⁇ for the value of the lower explosion limit concentration y obtained from the reference calibration curve Cs is set based on the lower explosion limit concentration values of various hydrocarbon components according to the respective standards.
- the allowable range ⁇ is preferably in the range of ⁇ 0.2 vol% or more and 0.7 vol% or less with respect to the value of the lower explosion limit concentration y obtained from the reference calibration curve Cs.
- the curve (a) indicated by a broken line in FIG. 2 is a curve indicating the upper limit of the allowable range
- the curve (b) is a curve indicating the lower limit of the allowable range. Therefore, if a curve or a broken line set in the region between the curves (a) and (b) is set as a calibration curve, the lower explosion limit concentration y can be obtained with a certain accuracy.
- the HC component concentration calculation means 40 calculates the total concentration y ′ [vol%] of the paraffinic hydrocarbon component contained in the test gas based on the value of the ratio x obtained by the ratio calculation means 30. Calculated by In addition, when the base gas is air, or when a specific hydrocarbon component that is used as a standard when standardizing data on the refractive index and specific gravity of the test gas is set to a hydrocarbon component other than methane gas For this purpose, the values of the coefficients in the equations (1-a) and (1-b) and the equation (2) may be appropriately changed.
- the lower explosion limit percentage calculating means 45 converts the value of the lower explosion limit concentration y obtained by the LEL calculating means 35 and the value of the total concentration y ′ of the paraffinic hydrocarbon components obtained by the HC component concentration calculating means 40. Based on this, the lower explosion limit percentage concentration y L [% LEL] is calculated.
- test gas contains nitrogen gas as the base gas.
- a test gas is supplied to each of the sound velocity measuring means 11 and the refractive index measuring means 15, and a reference gas such as air is supplied to the refractive index measuring means 15.
- a reference gas such as air is supplied to the refractive index measuring means 15.
- the sound velocity V d of the test gas is measured by the sound velocity measuring means 11 and the refractive index n d of the test gas is measured by the refractive index measuring means 15.
- the specific gravity measuring mechanism 25 based on the value of the acoustic velocity V d of the measured test gas, the acoustic velocity in terms of the specific gravity S a of the test gas to sonic velocity - is determined by the specific gravity conversion processing unit 26.
- the refractive index conversion specific gravity S b of the test gas is obtained by the refractive index-specific gravity conversion processing means 27.
- the specific gravity S d of the test gas is calculated by the specific gravity calculating means 28.
- the specific gravity difference ⁇ s between the test gas and nitrogen gas is normalized by, for example, the specific gravity difference ⁇ s CH4 between methane gas and nitrogen gas, so that the specific gravity difference normalized value ( ⁇ s / ⁇ s) is obtained.
- CH4 is calculated.
- the refractive index difference normalized value ( ⁇ n / ⁇ n CH4 ) is calculated by normalizing the refractive index difference ⁇ n between the test gas and nitrogen gas, for example, with the refractive index difference ⁇ n CH4 between methane gas and nitrogen gas. Is done.
- the specific gravity difference normalized value ( ⁇ s / ⁇ s CH4 ) is A ratio x to the refractive index difference normalized value ( ⁇ n / ⁇ n CH4 ) is calculated.
- the lower explosion limit concentration y of the test gas is calculated by, for example, the reference calibration curve Cs represented by the above formula (5). Further, based on the ratio x, the total concentration y ′ of the paraffinic hydrocarbon components contained in the test gas is calculated by the HC component concentration calculating means 40 by the above formula (2). Further, based on the value of the lower explosion limit concentration y of the test gas and the total concentration y ′ of the paraffinic hydrocarbon component, the lower explosion limit percentage concentration y L of the test gas is calculated as the lower explosion limit percentage concentration calculation means. 45.
- the lower explosion limit of the test gas regardless of the composition ratio of the paraffinic hydrocarbon component
- concentration y, the total concentration y ′ of the paraffinic hydrocarbon components contained in the test gas, and the lower explosion limit percentage concentration y L can be obtained with a certain degree of accuracy.
- the refractive index value and the sound velocity value obtained by the sound velocity measuring means 11 and the refractive index measuring means 15 each made of a physical sensor are used, so that a high response speed is obtained. Continuous measurement can be performed.
- the physical sensor is less susceptible to sensitivity deterioration, highly reliable gas detection can be performed.
- the above gas detection apparatus in which such a gas detection method is executed includes, for example, the loading arm by purging the gas in which the fuel gas remaining in the loading arm after the landing operation of the fuel gas is vaporized with nitrogen gas
- the gas discharged from the loading arm used in the LNG ship is a gas containing a large amount of methane, which is a hydrocarbon component that easily vaporizes, at the initial stage when the purge of nitrogen gas is started.
- Propane, butane and other high boiling hydrocarbon components are discharged.
- the degree of composition change with the passage of time of the gas discharged from the loading arm varies depending on the production area of the LNG and is difficult to predict.
- the gas remaining in the loading arm is below the lower explosion limit concentration regardless of the composition ratio of the paraffinic hydrocarbon component contained in the test gas. Can be detected by sex. Moreover, the purge work by nitrogen gas can be performed efficiently.
- the total concentration of paraffinic hydrocarbon components contained in the test gas was calculated by the above formula (2).
- the lower explosion limit percentage concentration [% LEL] (hereinafter referred to as “theoretical value”) of each test gas was calculated by a method based on the IEC standard. The data obtained as described above was plotted on a graph with the horizontal axis representing the theoretical value and the vertical axis representing the measured value. The results are shown by the diamond-shaped plots in FIG. A straight line indicated by a broken line in FIG. 3 is an ideal straight line in which a theoretical value and a measured value coincide with each other.
- the lower explosion limit percentage concentration can be obtained within a certain error range even for theoretical values based on ISO standards and ICSC. Furthermore, for a single gas mainly composed of one hydrocarbon component, such as methane, ethane, butane or isobutane, the lower explosion limit unit concentration was determined in the same manner as in Experimental Example 1, and the theoretical value according to any standard. However, it was confirmed that the lower explosion limit unit concentration can be obtained within a certain error range.
- the present invention can specify the concentration of the paraffinic hydrocarbon component of the mixed gas in terms of the lower explosion limit percentage concentration for the mixed gas containing a plurality of types of paraffinic hydrocarbon components using the inert gas as a base gas. It is expected to be extremely useful when detecting the gas remaining in the loading arm after the completion of the landing operation of the fuel gas.
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Abstract
Description
本発明は、ガス検出方法およびガス検出装置に関する。 The present invention relates to a gas detection method and a gas detection device.
例えば、液化天然ガス(LNG)を輸送する運搬船から陸上設備へLNGを荷揚げする場合には、通常、ローディングアームが用いられている。荷揚げ後においては、LNG気化ガスがローディングアーム内に残留している。このため、ローディングアームを切り離すに際しては、ローディングアーム内のLNG気化ガスをイナートガスでパージし、ローディングアームから排出されるLNG気化ガスの濃度が爆発下限界濃度以下になったことを確認することが求められている。特にLNG気化ガスの排出を目的としたパージの際には、イナートガスとして窒素が使用される。ここに、イナートガスとして窒素が用いられる理由は、水分や二酸化炭素などが含まれていると、水分や二酸化炭素がLNGの温度で凝固し、配管内部や機器を損傷させるおそれがあるためである。 For example, when unloading LNG from a carrier ship that transports liquefied natural gas (LNG) to land facilities, a loading arm is usually used. After unloading, LNG vaporized gas remains in the loading arm. Therefore, when disconnecting the loading arm, it is required to purge the LNG vaporized gas in the loading arm with an inert gas and confirm that the concentration of the LNG vaporized gas discharged from the loading arm is below the lower explosion limit concentration. It has been. In particular, nitrogen is used as an inert gas when purging for the purpose of discharging LNG vaporized gas. Here, the reason why nitrogen is used as the inert gas is that if moisture or carbon dioxide is contained, the moisture or carbon dioxide is solidified at the temperature of LNG, which may damage the inside of the pipe or equipment.
一般に、可燃性ガスの検出にあっては、例えば接触燃焼式ガスセンサ、半導体式ガスセンサもしくは非分散型赤外線式センサなどが用いられている。例えば特許文献1には、LNG気化ガスやLPG気化ガスを接触燃焼式ガス検知器により検出することが記載されている。
Generally, for detecting a combustible gas, for example, a contact combustion type gas sensor, a semiconductor type gas sensor, a non-dispersion type infrared sensor or the like is used. For example,
而して、LNGの主成分はメタンであるが、エタン、プロパン、ブタンなどのパラフィン系炭化水素成分も含まれており、LNGの組成は産出地によって異なる。
ローディングアーム内のLNG気化ガスをイナートガスでパージすることにより排出されるガスは、初期時には気化しやすいメタンが多く含まれたものであるが、時間経過と共に、エタン、プロパン、ブタンなどの沸点の高いパラフィン系炭化水素成分の割合が高いものとなる。このようなLNG気化ガスの組成の経時的変化の傾向は、LNGの産出地によって異なり、また、組成の経時的変化の傾向を予想することが困難である。このため、イナートガスをベースガスとするLNG気化ガスについて、パラフィン系炭化水素成分の総濃度の、爆発下限界濃度に対する百分率を示す爆発下限界百分率濃度を測定する場合には、LNG気化ガスに含まれるいずれのパラフィン系炭化水素成分に対しても、同等の感度レベルを有するガスセンサが必要となる。
Thus, although the main component of LNG is methane, paraffinic hydrocarbon components such as ethane, propane, and butane are also included, and the composition of LNG varies depending on the place of production.
The gas discharged by purging the LNG vaporized gas in the loading arm with an inert gas contains a large amount of methane that is easily vaporized at the initial stage. However, with the passage of time, the boiling point of ethane, propane, butane, etc. is high. The ratio of paraffinic hydrocarbon components is high. The tendency of the composition of the LNG vaporized gas to change with time varies depending on the place where the LNG is produced, and it is difficult to predict the tendency of the composition to change with time. For this reason, in the case of measuring the lower explosion limit percentage concentration indicating the percentage of the total concentration of paraffinic hydrocarbon components with respect to the lower explosion limit concentration of the LNG vaporized gas using the inert gas as a base gas, it is included in the LNG vaporized gas. A gas sensor having an equivalent sensitivity level is required for any paraffinic hydrocarbon component.
しかしながら、接触燃焼式センサや半導体式センサは、検知原理上、酸素が不可欠であるため、窒素ガスのようなイナートガス中のパラフィン系炭化水素成分の濃度を検出することはできない。一方、非分散型赤外線式センサでは、LNGに含まれる複数種のパラフィン系炭化水素成分を同一の感度レベルで検出することができない。
このように、例えばイナートガスをベースガスとするLNG気化ガスに含まれるすべてのパラフィン系炭化水素成分に対して、同等の感度レベルを有するガスセンサは存在しないのが実情であった。
However, the catalytic combustion type sensor and the semiconductor type sensor cannot detect the concentration of the paraffinic hydrocarbon component in the inert gas such as nitrogen gas because oxygen is indispensable from the detection principle. On the other hand, a non-dispersive infrared sensor cannot detect a plurality of types of paraffinic hydrocarbon components contained in LNG at the same sensitivity level.
As described above, for example, there is no gas sensor having an equivalent sensitivity level with respect to all paraffinic hydrocarbon components contained in the LNG vaporized gas having an inert gas as a base gas.
本発明は、以上のような事情に基づいてなされたものであって、イナートガスをベースガスとして含む被検ガスであっても、当該被検ガスにおけるパラフィン系炭化水素成分の総濃度および当該被検ガスの爆発下限界濃度を一定の確度で得ることのできるガス検出方法およびガス検出装置を提供することを目的とする。 The present invention has been made based on the above circumstances, and even for a test gas containing an inert gas as a base gas, the total concentration of paraffinic hydrocarbon components in the test gas and the test It is an object of the present invention to provide a gas detection method and a gas detection device that can obtain the lower explosion limit concentration of gas with a certain accuracy.
本発明のガス検出方法は、二種以上のパラフィン系炭化水素成分を含む混合ガスを被検ガスとし、
当該被検ガスの屈折率および比重を測定し、
当該被検ガスと当該被検ガスにおけるベースガスとの比重差(Δs)の、当該被検ガスと当該ベースガスとの屈折率差(Δn)に対する比率(Δs/Δn)に基づいて、当該被検ガスにおけるパラフィン系炭化水素成分の総濃度および当該被検ガスの爆発下限界濃度のいずれか一方または両方を算出することを特徴とする。
The gas detection method of the present invention uses a mixed gas containing two or more paraffinic hydrocarbon components as a test gas,
Measure the refractive index and specific gravity of the test gas,
Based on the ratio (Δs / Δn) of the specific gravity difference (Δs) between the test gas and the base gas in the test gas to the refractive index difference (Δn) between the test gas and the base gas. One or both of the total concentration of the paraffinic hydrocarbon components in the detected gas and the lower explosion limit concentration of the detected gas are calculated.
本発明のガス検出方法においては、被検ガスにおけるパラフィン系炭化水素成分の総濃度および当該被検ガスの爆発下限界濃度を算出し、
被検ガスのパラフィン系炭化水素成分の総濃度の、当該被検ガスの爆発下限界濃度に対する百分率を示す爆発下限界百分率濃度を算出することが好ましい。
In the gas detection method of the present invention, the total concentration of paraffinic hydrocarbon components in the test gas and the lower explosive limit concentration of the test gas are calculated,
It is preferable to calculate a lower explosion limit percentage concentration indicating a percentage of the total concentration of paraffinic hydrocarbon components of the test gas with respect to the lower explosion limit concentration of the test gas.
さらにまた、本発明のガス検出方法においては、被検ガスが、イナートガスをベースガスとして含む、LNG気化ガスまたはLPG気化ガスであることが好ましく、イナートガスが窒素ガスであることが好ましい。 Furthermore, in the gas detection method of the present invention, the test gas is preferably an LNG vaporized gas or an LPG vaporized gas containing an inert gas as a base gas, and the inert gas is preferably a nitrogen gas.
さらにまた、本発明のガス検出方法においては、前記被検ガスと当該被検ガスのベースガスである窒素ガスとの比重差(Δs)を、特定の炭化水素成分と窒素ガスとの比重差(ΔsH )により規格化して比重差規格化値(Δs/ΔsH )を算出すると共に、前記被検ガスと窒素ガスとの屈折率差(Δn)を、当該特定の炭化水素成分と窒素ガスとの屈折率差(ΔnH )により規格化して屈折率差規格化値(Δn/ΔnH )を算出し、
当該比重差規格化値(Δs/ΔsH )の、当該屈折率差規格化値(Δn/ΔnH )に対する比率を算出することが好ましい。
Furthermore, in the gas detection method of the present invention, the specific gravity difference (Δs) between the test gas and the nitrogen gas that is the base gas of the test gas is determined by the specific gravity difference between the specific hydrocarbon component and the nitrogen gas ( specific gravity difference normalized value normalized by Delta] s H) calculates a (Δs / Δs H), the refractive index difference between the test gas and nitrogen gas ([Delta] n), and nitrogen gas that particular hydrocarbon component refractive index difference refractive index difference normalized value normalized by (Δn H) (Δn / Δn H) calculated for,
It is preferable to calculate a ratio of the specific gravity difference normalized value (Δs / Δs H ) to the refractive index difference normalized value (Δn / Δn H ).
さらにまた、本発明のガス検出方法においては、前記特定の炭化水素成分がメタンガスであって、メタンガスを基準に規格化した比重差規格化値の屈折率差規格化値に対する比率をX軸とし、爆発下限界濃度をY軸とするX-Y座標系において、下記数式(1-a)で示される曲線と下記数式(1-b)で示される曲線との間の領域内に含まれる曲線または折れ線で示される検量線に基づいて、被検ガスの爆発下限界濃度を算出することが好ましい。 Furthermore, in the gas detection method of the present invention, the specific hydrocarbon component is methane gas, and the ratio of the specific gravity difference normalized value normalized based on methane gas to the refractive index difference normalized value is taken as the X axis, In an XY coordinate system with the explosion lower limit concentration as the Y axis, a curve included in a region between a curve represented by the following formula (1-a) and a curve represented by the following formula (1-b) or It is preferable to calculate the lower explosion limit concentration of the test gas based on a calibration curve indicated by a broken line.
上記数式(1-a)および数式(1-b)において、yは爆発下限界濃度〔vol%〕、xはメタンガスを基準に規格化した比重差規格化値の屈折率差規格化値に対する比率である。 In the above formulas (1-a) and (1-b), y is the lower explosion limit concentration [vol%], and x is the ratio of the specific gravity difference normalized value based on methane gas to the refractive index difference normalized value. It is.
さらにまた、本発明のガス検出方法においては、メタンガスを基準に規格化した比重差規格化値の屈折率差規格化値に対する比率をx、被検ガスと窒素ガスとの屈折率差をΔn、メタンガスと窒素ガスとの屈折率差をΔnCH4 としたとき、被検ガスにおける炭化水素成分の総濃度y´を下記数式(2)に基づいて算出することが好ましい。 Furthermore, in the gas detection method of the present invention, the ratio of the specific gravity difference normalized value normalized with respect to methane gas to the refractive index difference normalized value is x, the refractive index difference between the test gas and nitrogen gas is Δn, When the refractive index difference between methane gas and nitrogen gas is Δn CH4 , it is preferable to calculate the total concentration y ′ of hydrocarbon components in the test gas based on the following mathematical formula (2).
本発明のガス検出装置は、二種以上のパラフィン系炭化水素成分を含む混合ガスを被検ガスとし、
当該被検ガスの屈折率を測定する屈折率測定手段と、
当該被検ガスの比重を測定する比重測定手段と、
当該被検ガスと当該被検ガスにおけるベースガスとの比重差(Δs)の、当該被検ガスと当該被検ガスにおけるベースガスとの屈折率差(Δn)に対する比率(Δs/Δn)を出する比率算出手段と、
当該被検ガスにおけるパラフィン系炭化水素成分の総濃度を当該比率に基づいて算出するHC成分濃度算出手段および当該被検ガスの爆発下限界濃度を算出するLEL算出手段のいずれか一方または両方
を備えていることを特徴とする。
The gas detection apparatus of the present invention uses a mixed gas containing two or more paraffinic hydrocarbon components as a test gas,
A refractive index measuring means for measuring the refractive index of the test gas;
Specific gravity measuring means for measuring the specific gravity of the test gas;
The ratio (Δs / Δn) of the specific gravity difference (Δs) between the test gas and the base gas in the test gas to the refractive index difference (Δn) between the test gas and the base gas in the test gas is calculated. A ratio calculating means for
One or both of HC component concentration calculating means for calculating the total concentration of paraffinic hydrocarbon components in the test gas based on the ratio and LEL calculating means for calculating the lower explosion limit concentration of the test gas are provided. It is characterized by.
本発明のガス検出装置においては、前記HC成分濃度算出手段および前記LEL算出手段の両方を備えており、
被検ガスのパラフィン系炭化水素成分の総濃度の、当該被検ガスの爆発下限界濃度に対する百分率を示す爆発下限界百分率濃度を算出する爆発下限界百分率濃度算出手段をさらに備えた構成とされることが好ましい。
The gas detection device of the present invention comprises both the HC component concentration calculating means and the LEL calculating means,
The lower explosive limit percentage concentration calculating means for calculating the lower explosive limit percentage concentration indicating the percentage of the total concentration of the paraffinic hydrocarbon components of the detected gas with respect to the explosive lower limit concentration of the detected gas is provided. It is preferable.
また、本発明のガス検出装置においては、被検ガスが、イナートガスをベースガスとして含む、LNG気化ガスまたはLPG気化ガスであることが好ましく、イナートガスが窒素ガスであることが好ましい。 In the gas detection apparatus of the present invention, the test gas is preferably an LNG vaporized gas or an LPG vaporized gas containing an inert gas as a base gas, and the inert gas is preferably a nitrogen gas.
本発明のガス検出方法およびガス検出装置によれば、パラフィン系炭化水素成分の組成比に拘わらず、被検ガスに含まれるパラフィン系炭化水素成分の総濃度、当該被検ガスの爆発下限界濃度、および爆発下限界百分率濃度を一定の確度で得ることができる。 According to the gas detection method and the gas detection apparatus of the present invention, regardless of the composition ratio of the paraffinic hydrocarbon component, the total concentration of the paraffinic hydrocarbon component contained in the test gas, the lower explosive limit concentration of the test gas , And the lower explosion limit percentage concentration can be obtained with a certain accuracy.
以下、本発明の実施の形態について詳細に説明する。 Hereinafter, embodiments of the present invention will be described in detail.
本発明のガス検出方法および当該ガス検出方法が実行される本発明のガス検出装置においては、二種以上のパラフィン系炭化水素成分を含む混合ガスが被検ガスとされる。
被検ガスとしては、例えば、窒素ガスなどのイナートガスまたは空気をベースガスとして含む、パラフィン系炭化水素を主成分とするLNG気化ガスやLPG気化ガスなどを例示することができる。具体的には例えば、LNGまたはLPGの陸揚げ作業終了後のローディングアーム内に残留するLNG気化ガスまたはLPG気化ガスをイナートガスでパージすることにより当該ローディングアーム内から排出されるガスなどを例示することができる。
In the gas detection method of the present invention and the gas detection device of the present invention in which the gas detection method is executed, a mixed gas containing two or more paraffinic hydrocarbon components is used as a test gas.
Examples of the test gas include LNG vaporized gas and LPG vaporized gas mainly containing paraffinic hydrocarbons containing inert gas such as nitrogen gas or air as a base gas. Specifically, for example, gas discharged from the loading arm by purging the LNG vaporized gas or LPG vaporized gas remaining in the loading arm after completion of the LNG or LPG landing work with an inert gas, etc. it can.
図1は、本発明のガス検出装置の一例における構成を概略的に示すブロック図である。
このガス検出装置は、被検ガスの物性値を測定するガス検出部10と、ガス検出部10から出力されるデータを処理する演算処理部20とを有する。
FIG. 1 is a block diagram schematically showing the configuration of an example of the gas detection apparatus of the present invention.
The gas detection apparatus includes a
ガス検出部10は、被検ガスの音速Vd を測定する音速測定手段11と、当該被検ガスの屈折率nd を測定する屈折率測定手段15とを備えている。このガス検出装置においては、図1において白抜きの矢印で示されるように、被検ガスは、音速測定手段11および屈折率測定手段15に順次に供給される。
The
音速測定手段11としては、例えば超音波式センサを用いることができる。超音波式センサは、一端に音波発信源が設けられると共に他端に音波受信源が設けられた測定管を備えた構成とされる。超音波式センサにおいては、測定管内に被検ガスを流通させた状態において、音波発信源からの音波が被検ガス中を伝播して音波受信源に至るまでに要する時間(伝播時間)が測定され、その伝播時間の値から被検ガスの音速Vd が求められる。 As the sound speed measuring means 11, for example, an ultrasonic sensor can be used. The ultrasonic sensor has a measurement tube in which a sound wave transmission source is provided at one end and a sound wave reception source is provided at the other end. In the ultrasonic sensor, the time (propagation time) required for the sound wave from the sound wave source to propagate through the test gas and reach the sound wave receiving source is measured in the state where the test gas is circulated in the measuring tube. The sound velocity V d of the test gas is obtained from the value of the propagation time.
屈折率測定手段15としては、例えば、被検ガスと例えば空気などの参照ガスとの光の屈折率の相異を干渉縞の変位として検出し、この変位量に基づいて、被検ガスの屈折率nd を測定する光波干渉計を用いることができる。 As the refractive index measuring means 15, for example, a difference in refractive index of light between a test gas and a reference gas such as air is detected as a displacement of interference fringes, and the refraction of the test gas is based on the amount of displacement. A light wave interferometer that measures the rate n d can be used.
演算処理部20は、被検ガスの比重Sd を被検ガスの音速Vd の値および被検ガスの屈折率nd の値に基づいて求める比重測定機構25を備えている。
The
比重測定機構25は、音速測定手段11によって測定された被検ガスの音速Vd の値に基づいて音速換算比重Sa を求める音速-比重換算処理手段26と、屈折率測定手段15によって測定された被検ガスの屈折率nd の値に基づいて屈折率換算比重Sb を求める屈折率-比重換算処理手段27と、音速換算比重Sa および屈折率換算比重Sb に基づいて被検ガスの比重Sd を求める比重算出手段28とを備えている。
The specific
音速-比重換算処理手段26は、例えばパラフィン系炭化水素成分のみからなる特定ガスについて予め取得しておいた当該特定ガスの音速と比重との相関関係を利用して、被検ガスの音速換算比重Sa を算出する。具体的には、被検ガスが特定ガスであると仮定して、被検ガスについて取得された音速Vd の値を相関関係に対照することにより音速換算比重Sa を算出する。 The sound velocity-specific gravity conversion processing means 26 uses, for example, the correlation between the sound speed and specific gravity of the specific gas that has been acquired in advance for the specific gas consisting only of the paraffinic hydrocarbon component, and the sound velocity conversion specific gravity of the test gas. Sa is calculated. Specifically, assuming that the test gas is a specific gas, the sound speed conversion specific gravity Sa is calculated by comparing the value of the sound speed V d acquired for the test gas with the correlation.
屈折率-比重換算処理手段27は、例えばパラフィン系炭化水素成分のみからなる特定ガスについて予め取得しておいた当該特定ガスの屈折率と比重との相関関係を利用して、被検ガスの屈折率換算比重Sb を算出する。具体的には、被検ガスが特定ガスであると仮定して、被検ガスについて取得された屈折率nd の値を相関関係に対照することにより屈折率換算比重Sb を算出する。 The refractive index-specific gravity conversion processing means 27 uses, for example, the correlation between the refractive index and specific gravity of the specific gas acquired in advance for the specific gas consisting only of the paraffinic hydrocarbon component, to refract the test gas. The rate conversion specific gravity Sb is calculated. Specifically, assuming that the test gas is a specific gas, the refractive index conversion specific gravity S b is calculated by comparing the value of the refractive index n d acquired for the test gas with the correlation.
比重算出手段28は、音速-比重換算処理手段26によって得られる音速換算比重Sa と、屈折率-比重換算処理手段27によって得られる屈折率換算比重Sb とに基づいて、下記数式(3)により、被検ガスの比重Sd を算出する。ここに、被検ガスの比重Sd の値、音速換算比重Sa の値および屈折率換算比重Sb の値は、いずれも、空気の比重を1としたときの値である。 The specific gravity calculating means 28 is based on the sound speed converted specific gravity S a obtained by the sound speed-specific gravity conversion processing means 26 and the refractive index converted specific gravity S b obtained by the refractive index-specific gravity conversion processing means 27, as shown in the following formula (3). Thus, the specific gravity S d of the test gas is calculated. Here, the specific gravity S d , the sound velocity converted specific gravity S a , and the refractive index converted specific gravity S b of the test gas are all values when the specific gravity of air is 1.
上記数式(3)におけるαは補正因子である。補正因子αは、例えば2.4以上9.3以下の数値範囲内の値とされることが好ましく、より好ましくは、3.0以上6.2以下の数値範囲内の値とされる。
補正因子αが上記の数値範囲内の値であることにより、被検ガスに混入ガスが含有されている場合であっても、その混入ガスの組成および被検ガスの組成にかかわらず、得られる被検ガスの比重Sd の値が、当該被検ガスの比重の真値との差が小さいものとなる。
In the above formula (3), α is a correction factor. The correction factor α is preferably a value within a numerical range of, for example, 2.4 or more and 9.3 or less, and more preferably a value within a numerical range of 3.0 or more and 6.2 or less.
Since the correction factor α is a value within the above numerical range, even if the sample gas contains a mixed gas, the correction factor α is obtained regardless of the composition of the mixed gas and the sample gas. The difference between the specific gravity S d of the test gas and the true value of the specific gravity of the test gas is small.
而して、このガス検出装置における演算処理部20は、被検ガスの比重Sd に係るデータと、当該被検ガスの屈折率nd に係るデータとの比率を算出する比率算出手段30と、当該被検ガスの爆発下限界濃度yを当該比率に基づいて算出するLEL算出手段35と、当該被検ガスにおけるパラフィン系炭化水素成分の総濃度y´を当該比率に基づいて算出するHC成分濃度算出手段40と、被検ガスの爆発下限界百分率濃度yL を、被検ガスの爆発下限界濃度yと当該被検ガスにおけるパラフィン系炭化水素成分の総濃度y´とに基づいて算出する爆発下限界百分率濃度算出手段45とを備えている。
Thus, the
比率算出手段30は、被検ガスと当該被検ガスにおけるベースガスとの比重差(Δs)の、当該被検ガスと当該被検ガスにおけるベースガスとの屈折率差(Δn)に対する比率(Δs/Δn)を算出する。 The ratio calculating means 30 is configured to calculate a ratio (Δs) of a specific gravity difference (Δs) between the test gas and the base gas in the test gas to a refractive index difference (Δn) between the test gas and the base gas in the test gas. / Δn).
また、比率算出手段30は、被検ガスとベースガスとの比重差(Δs)および被検ガスとベースガスとの屈折率差(Δn)を規格化し、これにより得られる各々の規格化値を被検ガスの比重Sd に係るデータおよび被検ガスの屈折率nd に係るデータとして用いて比率を算出する機能を有することが好ましい。
具体的には、被検ガスとベースガスとの比重差(Δs)を、特定の炭化水素成分と当該ベースガスとの比重差(ΔsH )で規格化して比重差規格化値(Δs/ΔsH )を算出する。また、被検ガスとベースガスとの屈折率差(Δn)を、特定の炭化水素成分と当該ベースガスとの屈折率差(ΔnH )を基準として規格化して屈折率差規格化値(Δn/ΔnH )を算出する。
被検ガスの比重に係るデータの、被検ガスの屈折率に係るデータに対する比率を、規格化値を用いて算出することにより、被検ガスの組成に拘わらず、一定基準で評価を行うことができる。ここに、特定の炭化水素成分は、メタンガスであることが好ましい。この理由は、比率算出手段30によって得られる比率xを最大値が1となるよう規格化(正規化)することができるためである。
Further, the ratio calculation means 30 normalizes the specific gravity difference (Δs) between the test gas and the base gas and the refractive index difference (Δn) between the test gas and the base gas, and the respective normalized values obtained thereby are normalized. It is preferable to have a function of calculating the ratio using the data relating to the specific gravity S d of the test gas and the data relating to the refractive index n d of the test gas.
Specifically, the specific gravity difference (Δs) between the test gas and the base gas is normalized by the specific gravity difference (Δs H ) between the specific hydrocarbon component and the base gas, and the specific gravity difference normalized value (Δs / Δs) H ) is calculated. Further, the refractive index difference (Δn) between the test gas and the base gas is normalized based on the refractive index difference (Δn H ) between the specific hydrocarbon component and the base gas, and the refractive index difference normalized value (Δn) / Δn H ) is calculated.
By using the normalized value to calculate the ratio of the data related to the specific gravity of the test gas to the data related to the refractive index of the test gas, the evaluation can be performed on a constant basis regardless of the composition of the test gas. Can do. Here, the specific hydrocarbon component is preferably methane gas. This is because the ratio x obtained by the ratio calculation means 30 can be normalized (normalized) so that the maximum value is 1.
メタンガスを基準として規格化した比重差規格化値の、屈折率差規格化値に対する比率xは、例えば下記数式(4)によって、算出される。下記数式(4)において、Δnは、被検ガスと窒素ガスとの屈折率差(n-nN2 )、ΔnCH4 は、メタンガスと窒素ガスとの屈折率差(nCH4 -nN2 )、Δsは、被検ガスと窒素ガスとの比重差(s-sN2 )、ΔsCH4 は、メタンガスと窒素ガスとの比重差(sCH4 -sN2 )である。
なお、下記数式(4)において、被検ガスにおけるベースガスが例えば空気である場合には、窒素ガスの屈折率nN2 および比重sN2 に代えて空気の屈折率および比重を用いればよい。また、メタンガス以外の特定の炭化水素成分を基準としてデータを規格化する場合には、メタンガスの屈折率nCH4 および比重sCH4 に代えて基準とされる特定の炭化水素成分の屈折率および比重を用いればよい。
The ratio x of the specific gravity difference normalized value normalized with respect to methane gas to the refractive index difference normalized value is calculated by, for example, the following formula (4). In the following mathematical formula (4), Δn is the difference in refractive index between the test gas and nitrogen gas (n−n N2 ), Δn CH4 is the difference in refractive index between methane gas and nitrogen gas (n CH4 −n N2 ), Δs Is the specific gravity difference (s−s N2 ) between the test gas and nitrogen gas, and Δs CH4 is the specific gravity difference between the methane gas and nitrogen gas (s CH4 −s N2 ).
In the following formula (4), when the base gas in the test gas is, for example, air, the refractive index and specific gravity of air may be used instead of the refractive index n N2 and specific gravity s N2 of nitrogen gas. In addition, when standardizing data based on a specific hydrocarbon component other than methane gas, the refractive index and specific gravity of the specific hydrocarbon component used as a reference instead of the refractive index n CH4 and specific gravity s CH4 of methane gas are used. Use it.
LEL算出手段35は、比率算出手段30によって得られた比率xと、爆発下限界濃度yとの相関関係を示す検量線に基づいて、被検ガスの爆発下限界濃度y〔vol%〕を算出する。
検量線は、例えば、メタンガスを基準に規格化した比重差規格化値(Δs/ΔsCH4 )の、屈折率差規格化値(Δn/ΔnCH4 )に対する比率xをX軸とし、爆発下限界濃度をY軸とするX-Y座標系において、上記数式(1-a)で示される曲線と上記数式(1-b)で示される曲線との間の領域内に含まれる曲線または折れ線で近似されるものである。このようにして検量線が設定される理由は次に示すとおりである。
The LEL calculation means 35 calculates the lower explosion limit concentration y [vol%] of the test gas based on the calibration curve indicating the correlation between the ratio x obtained by the ratio calculation means 30 and the lower explosion limit concentration y. To do.
The calibration curve is, for example, the ratio x of the specific gravity difference normalized value (Δs / Δs CH4 ) normalized with respect to methane gas to the refractive index difference normalized value (Δn / Δn CH4 ) as the X axis, and the lower explosion limit concentration In the XY coordinate system with Y as the Y axis, the curve is approximated by a curve or a broken line included in a region between the curve represented by the equation (1-a) and the curve represented by the equation (1-b). Is. The reason why the calibration curve is set in this way is as follows.
先ず、パラフィン系炭化水素成分を主成分とする互いに組成の異なる複数種の試験用ガス各々の比重および屈折率を実際に測定し、メタンガスを基準に規格化した比重差規格化値の屈折率差規格化値に対する比率xを算出する。また、各々の試験用ガスの組成に基づいて爆発下限界濃度(理論値)を算出し、このようにして得られた各実測値を、比率xをX軸とし、爆発下限界濃度をY軸とするX-Y座標系にプロットした。その結果、図2において実線で示すように、試験用ガスの組成に拘わらず、比率xと爆発下限界濃度yとの関係を一の曲線(以下、「基準検量線」という。)Csで描くことができることが確認された。ここに、基準検量線Csは、下記数式(5)により示される曲線である。 First of all, the specific gravity and refractive index of each of a plurality of kinds of test gases having a paraffinic hydrocarbon component as the main component and different compositions are actually measured, and the refractive index difference of the specific gravity difference normalized value based on methane gas. A ratio x to the normalized value is calculated. Further, the lower explosion limit concentration (theoretical value) is calculated based on the composition of each test gas, and the actually measured values thus obtained are represented by the ratio x as the X axis and the lower explosion limit concentration as the Y axis. And plotted in an XY coordinate system. As a result, as indicated by a solid line in FIG. 2, the relationship between the ratio x and the lower explosion limit concentration y is drawn by a single curve (hereinafter referred to as “reference calibration curve”) Cs, regardless of the composition of the test gas. It was confirmed that it was possible. Here, the reference calibration curve Cs is a curve represented by the following mathematical formula (5).
一方、各種のパラフィン系炭化水素成分の爆発下限界濃度の値が、例えばIEC規格、ISO規格あるいはICSC(International Chemical Safty Card,国際化学物質安全カード)において示されているが、同一の炭化水素成分であっても、爆発下限界濃度yの値として互いに異なる値が示されているものもある。例えば、イソブタンガス(x=-0.35)についての爆発下限界濃度の値は、IEC規格では1.3vol%(図2における丸印のプロット)、ISO規格では1.5vol%(図2における三角印のプロット)、ICSCでは、1.8vol%(図2における四角印のプロット)とされている。なお、図2においては、メタンガス(x=1.00)、エタンガス(x=-0.06)およびプロパンガス(x=-0.26)の値も示されており、丸印のプロットがIEC規格に基づく値、三角印のプロットがISO規格に基づく値、四角印がICSCに基づく値である。
このため、本発明においては、基準検量線Csにより得られる爆発下限界濃度yの値についての許容範囲βが、各々の規格による各種の炭化水素成分の爆発下限界濃度の値に基づいて設定される。許容範囲βは、基準検量線Csにより得られる爆発下限界濃度yの値に対して例えば-0.2vol%以上0.7vol%以下の範囲とされることが好ましい。すなわち、図2において破線で示す曲線(a)が許容範囲の上限を示す曲線となり、曲線(b)が許容範囲の下限を示す曲線となる。従って、曲線(a)と曲線(b)との間の領域内で設定された曲線または折れ線を検量線として設定すれば、爆発下限界濃度yを一定の確度で得ることができる。
On the other hand, the value of the lower explosive limit concentration of various paraffinic hydrocarbon components is shown in, for example, IEC standard, ISO standard, or ICSC (International Chemical Safety Card, International Chemical Safety Card). However, there are some values that are different from each other as the value of the lower explosion limit concentration y. For example, the lower explosion limit value for isobutane gas (x = −0.35) is 1.3 vol% in the IEC standard (circled plot in FIG. 2) and 1.5 vol% in the ISO standard (in FIG. 2). (Triangle mark plot), in ICSC, it is 1.8 vol% (square mark plot in FIG. 2). In FIG. 2, the values of methane gas (x = 1.00), ethane gas (x = −0.06), and propane gas (x = −0.26) are also shown. The values based on the standard, the triangle marks are values based on the ISO standard, and the square marks are values based on the ICSC.
For this reason, in the present invention, the allowable range β for the value of the lower explosion limit concentration y obtained from the reference calibration curve Cs is set based on the lower explosion limit concentration values of various hydrocarbon components according to the respective standards. The The allowable range β is preferably in the range of −0.2 vol% or more and 0.7 vol% or less with respect to the value of the lower explosion limit concentration y obtained from the reference calibration curve Cs. That is, the curve (a) indicated by a broken line in FIG. 2 is a curve indicating the upper limit of the allowable range, and the curve (b) is a curve indicating the lower limit of the allowable range. Therefore, if a curve or a broken line set in the region between the curves (a) and (b) is set as a calibration curve, the lower explosion limit concentration y can be obtained with a certain accuracy.
HC成分濃度算出手段40は、被検ガスに含まれるパラフィン系炭化水素成分の総濃度y´〔vol%〕を比率算出手段30によって得られた比率xの値に基づいて、上記数式(2)により算出する。
なお、ベースガスが空気である場合や、被検ガスの屈折率に係るデータおよび比重に係るデータの規格化に際して基準とされる特定の炭化水素成分がメタンガス以外の炭化水素成分に設定される場合には、上記数式(1-a)、(1-b)および上記数式(2)における係数の値を適宜変更すればよい。
The HC component concentration calculation means 40 calculates the total concentration y ′ [vol%] of the paraffinic hydrocarbon component contained in the test gas based on the value of the ratio x obtained by the ratio calculation means 30. Calculated by
In addition, when the base gas is air, or when a specific hydrocarbon component that is used as a standard when standardizing data on the refractive index and specific gravity of the test gas is set to a hydrocarbon component other than methane gas For this purpose, the values of the coefficients in the equations (1-a) and (1-b) and the equation (2) may be appropriately changed.
爆発下限界百分率算出手段45は、LEL算出手段35によって得られた爆発下限界濃度yの値と、HC成分濃度算出手段40によって得られたパラフィン系炭化水素成分の総濃度y´の値とに基づいて、爆発下限界百分率濃度yL [%LEL]を算出する。爆発下限界百分率濃度yL は、パラフィン系炭化水素成分の総濃度y´の、爆発下限界濃度yに対する百分率を示す値であって、yL =(y´/y)×100により求められる。 The lower explosion limit percentage calculating means 45 converts the value of the lower explosion limit concentration y obtained by the LEL calculating means 35 and the value of the total concentration y ′ of the paraffinic hydrocarbon components obtained by the HC component concentration calculating means 40. Based on this, the lower explosion limit percentage concentration y L [% LEL] is calculated. The lower explosion limit percentage concentration y L is a value indicating the percentage of the total concentration y ′ of paraffinic hydrocarbon components with respect to the lower explosion limit concentration y, and is obtained by y L = (y ′ / y) × 100.
以下、上記のガス検出装置によるガス検出動作について、被検ガスがベースガスとして窒素ガスを含むものである場合を例に挙げて説明する。 Hereinafter, the gas detection operation by the above gas detection device will be described by taking as an example the case where the test gas contains nitrogen gas as the base gas.
上記のガス検出装置においては、被検ガスが音速測定手段11および屈折率測定手段15の各々に供給されると共に、例えば空気などの参照ガスが屈折率測定手段15に供給される。これにより、被検ガスの音速Vd が音速測定手段11によって測定されると共に当該被検ガスの屈折率nd が屈折率測定手段15によって測定される。比重測定機構25においては、測定された被検ガスの音速Vd の値に基づいて、被検ガスの音速換算比重Sa が音速-比重換算処理手段26によって求められる。また、測定された被検ガスの屈折率nd の値に基づいて、被検ガスの屈折率換算比重Sb が屈折率-比重換算処理手段27によって求められる。このようにして得られた音速換算比重Sa の値および屈折率換算比重Sb の値に基づいて、被検ガスの比重Sd が比重算出手段28によって算出される。
In the above gas detection device, a test gas is supplied to each of the sound velocity measuring means 11 and the refractive index measuring means 15, and a reference gas such as air is supplied to the refractive index measuring means 15. Thereby, the sound velocity V d of the test gas is measured by the sound velocity measuring means 11 and the refractive index n d of the test gas is measured by the refractive index measuring means 15. In the specific
比率算出手段30においては、先ず、被検ガスと窒素ガスとの比重差Δsが、例えばメタンガスと窒素ガスとの比重差ΔsCH4 で規格化されることにより、比重差規格化値(Δs/ΔsCH4 )が算出される。また、被検ガスと窒素ガスとの屈折率差Δnが、例えばメタンガスと窒素ガスとの屈折率差ΔnCH4 で規格化されることにより、屈折率差規格化値(Δn/ΔnCH4 )が算出される。次いで、比重差規格化値(Δs/ΔsCH4 )および屈折率差規格化値(Δn/ΔnCH4 )に基づいて、上記数式(4)によって、比重差規格化値(Δs/ΔsCH4 )の、屈折率差規格化値(Δn/ΔnCH4 )に対する比率xが算出される。 In the ratio calculation means 30, first, the specific gravity difference Δs between the test gas and nitrogen gas is normalized by, for example, the specific gravity difference Δs CH4 between methane gas and nitrogen gas, so that the specific gravity difference normalized value (Δs / Δs) is obtained. CH4 ) is calculated. Also, the refractive index difference normalized value (Δn / Δn CH4 ) is calculated by normalizing the refractive index difference Δn between the test gas and nitrogen gas, for example, with the refractive index difference Δn CH4 between methane gas and nitrogen gas. Is done. Next, based on the specific gravity difference normalized value (Δs / Δs CH4 ) and the refractive index difference normalized value (Δn / Δn CH4 ), the specific gravity difference normalized value (Δs / Δs CH4 ) is A ratio x to the refractive index difference normalized value (Δn / Δn CH4 ) is calculated.
以上のようにして得られた比率xに基づいて、LEL算出手段35においては、被検ガスの爆発下限界濃度yが、例えば上記数式(5)で示される基準検量線Csによって算出される。また、当該比率xに基づいて、上記数式(2)によって、被検ガスに含まれるパラフィン系炭化水素成分の総濃度y´がHC成分濃度算出手段40によって算出される。
さらに、被検ガスの爆発下限界濃度yの値とパラフィン系炭化水素成分の総濃度y´の値とに基づいて、被検ガスの爆発下限界百分率濃度yL が爆発下限界百分率濃度算出手段45によって算出される。
Based on the ratio x obtained as described above, in the LEL calculating means 35, the lower explosion limit concentration y of the test gas is calculated by, for example, the reference calibration curve Cs represented by the above formula (5). Further, based on the ratio x, the total concentration y ′ of the paraffinic hydrocarbon components contained in the test gas is calculated by the HC component concentration calculating means 40 by the above formula (2).
Further, based on the value of the lower explosion limit concentration y of the test gas and the total concentration y ′ of the paraffinic hydrocarbon component, the lower explosion limit percentage concentration y L of the test gas is calculated as the lower explosion limit percentage concentration calculation means. 45.
而して、上記のガス検出方法によれば、被検ガスにおけるベースガスが例えば窒素ガスなどのイナートガスであっても、パラフィン系炭化水素成分の組成比に拘わらず、被検ガスの爆発下限界濃度y、被検ガスに含まれるパラフィン系炭化水素成分の総濃度y´および爆発下限界百分率濃度yL を一定の確度で得ることができる。
また、これらの特性値の算出にあっては、各々物理センサよりなる音速測定手段11および屈折率測定手段15により取得された屈折率の値および音速の値が用いられるので、高い応答速度を得ることができて連続測定を行うことができる。しかも、物理センサは、感度の劣化が生じにくいものであるため、信頼性の高いガス検出を行うことができる。
Thus, according to the above gas detection method, even if the base gas in the test gas is an inert gas such as nitrogen gas, the lower explosion limit of the test gas regardless of the composition ratio of the paraffinic hydrocarbon component The concentration y, the total concentration y ′ of the paraffinic hydrocarbon components contained in the test gas, and the lower explosion limit percentage concentration y L can be obtained with a certain degree of accuracy.
In calculating these characteristic values, the refractive index value and the sound velocity value obtained by the sound velocity measuring means 11 and the refractive index measuring means 15 each made of a physical sensor are used, so that a high response speed is obtained. Continuous measurement can be performed. In addition, since the physical sensor is less susceptible to sensitivity deterioration, highly reliable gas detection can be performed.
このようなガス検出方法が実行される上記のガス検出装置は、例えば燃料ガスの陸揚げ作業終了後のローディングアーム内に残留する燃料ガスが気化されたガスを窒素ガスでパージすることにより当該ローディングアーム内から排出されるガスの検出を行う場合に好適なものとなる。
例えばLNG船において用いられるローディングアーム内から排出されるガスは、窒素ガスのパージが開始された初期時においては、気化しやすい炭化水素成分であるメタンを多く含むガスが排出され、時間経過と共にエタン、プロパン、ブタンなどの高沸点の炭化水素成分の割合が多くなったガスが排出される。また、ローディングアーム内から排出されるガスの時間経過に伴う組成の変化の程度は、LNGの産地によって異なるものとなり、予想しにくいものである。然るに、上記のガス検出装置によれば、当該被検ガスに含まれるパラフィン系炭化水素成分の組成比に拘わらず、ローディングアーム内に残留するガスが爆発下限界濃度以下となったことを高い信頼性で検出することができる。また、窒素ガスによるパージ作業を効率的に行うことができる。
The above gas detection apparatus in which such a gas detection method is executed includes, for example, the loading arm by purging the gas in which the fuel gas remaining in the loading arm after the landing operation of the fuel gas is vaporized with nitrogen gas This is suitable for detecting the gas discharged from the inside.
For example, the gas discharged from the loading arm used in the LNG ship is a gas containing a large amount of methane, which is a hydrocarbon component that easily vaporizes, at the initial stage when the purge of nitrogen gas is started. , Propane, butane and other high boiling hydrocarbon components are discharged. In addition, the degree of composition change with the passage of time of the gas discharged from the loading arm varies depending on the production area of the LNG and is difficult to predict. However, according to the above-described gas detection device, it is highly reliable that the gas remaining in the loading arm is below the lower explosion limit concentration regardless of the composition ratio of the paraffinic hydrocarbon component contained in the test gas. Can be detected by sex. Moreover, the purge work by nitrogen gas can be performed efficiently.
以下、本発明の実験例について説明する。 Hereinafter, experimental examples of the present invention will be described.
〔実験例1〕
メタンガス(CH4 )およびエタンガス(C2 H6 )よりなる混合ガス(CH4 :C2 H6 =50:50)を窒素ガスで希釈した、パラフィン系炭化水素成分の総濃度が互いに異なる複数種の試験用ガスを用意した。
図1に示す構成のガス検出装置を用いて、各々の試験用ガスにおける爆発下限界百分率濃度〔%LEL〕(以下、「実測値」という。)を求めた。ここに、試験用ガスの比重は、上記式(3)により、補正因子αの値を3.32とする条件で算出した。また、試験用ガスの爆発下限界濃度は、上記数式(5)により示される基準検量線に基づいて算出した。さらにまた、試験用ガスに含まれるパラフィン系炭化水素成分の総濃度は、上記数式(2)により算出した。
また、IEC規格に準拠した方法により、各々の試験用ガスの爆発下限界百分率濃度〔%LEL〕(以下、「理論値」という。)を算出した。
以上のようにして得られたデータを、横軸を理論値、縦軸を測定値とするグラフ上にプロットした。結果を図3において菱形印のプロットで示す。図3において破線で示す直線は、理論値と測定値とが一致した理想直線である。
[Experimental Example 1]
Plural kinds of paraffinic hydrocarbon components having different total concentrations obtained by diluting a mixed gas (CH 4 : C 2 H 6 = 50: 50) composed of methane gas (CH 4 ) and ethane gas (C 2 H 6 ) with nitrogen gas The test gas was prepared.
Using the gas detection apparatus having the configuration shown in FIG. 1, the lower explosion limit percentage concentration [% LEL] (hereinafter referred to as “actual measurement value”) in each test gas was obtained. Here, the specific gravity of the test gas was calculated by the above equation (3) under the condition that the value of the correction factor α was 3.32. Further, the lower explosion limit concentration of the test gas was calculated based on the reference calibration curve expressed by the above mathematical formula (5). Furthermore, the total concentration of paraffinic hydrocarbon components contained in the test gas was calculated by the above formula (2).
Further, the lower explosion limit percentage concentration [% LEL] (hereinafter referred to as “theoretical value”) of each test gas was calculated by a method based on the IEC standard.
The data obtained as described above was plotted on a graph with the horizontal axis representing the theoretical value and the vertical axis representing the measured value. The results are shown by the diamond-shaped plots in FIG. A straight line indicated by a broken line in FIG. 3 is an ideal straight line in which a theoretical value and a measured value coincide with each other.
〔実験例2〕
メタンガス(CH4 )、エタンガス(C2 H6 )およびプロパンガス(C3 H8 )よりなる混合ガス(CH4 :C2 H6 :C3 H8 =33.3:33.3:33.3)を窒素ガスで希釈した、パラフィン系炭化水素成分の総濃度が互いに異なる複数種の試験用ガスを用意した。
実験例1と同様にして、各々の試験用ガスの爆発下限界百分率濃度の実測値および理論値を求めた。結果を図3において丸印のプロットで示す。
[Experimental example 2]
Mixed gas (CH 4 : C 2 H 6 : C 3 H 8 ) consisting of methane gas (CH 4 ), ethane gas (C 2 H 6 ) and propane gas (C 3 H 8 ) = 33.3: 33.3: 33. A plurality of types of test gases having different total concentrations of paraffinic hydrocarbon components were prepared by diluting 3) with nitrogen gas.
In the same manner as in Experimental Example 1, the actual measurement value and the theoretical value of the lower explosion limit percentage concentration of each test gas were obtained. The results are shown as circled plots in FIG.
〔実験例3〕
エタンガス(C2 H6 )、プロパンガス(C3 H8 )およびイソブタンガス(i-C4 H10 )よりなる混合ガス(C2 H6 :C3 H8 :i-C4 H10 =33.3:33.3:33.3)を窒素ガスで希釈した、パラフィン系炭化水素成分の総濃度が互いに異なる複数種の試験用ガスを用意した。
実験例1と同様にして、各々の試験用ガスの爆発下限界百分率濃度の実測値および理論値を求めた。結果を図3において四角印のプロットで示す。
[Experimental Example 3]
Mixed gas (C 2 H 6 : C 3 H 8 : i-C 4 H 10) = 33 consisting of ethane gas (C 2 H 6 ), propane gas (C 3 H 8 ) and isobutane gas (i-C 4 H 10 ) .3: 33.3: 33.3) diluted with nitrogen gas, a plurality of types of test gases having different total concentrations of paraffinic hydrocarbon components were prepared.
In the same manner as in Experimental Example 1, the actual measurement value and the theoretical value of the lower explosion limit percentage concentration of each test gas were obtained. The results are shown by the square marks in FIG.
以上の結果より明らかなように、本発明によれば、ガスの組成に拘わらず、爆発下限界百分率濃度を理論値に対して一定の誤差範囲内で得ることができることが確認された。 As is clear from the above results, according to the present invention, it was confirmed that the lower explosion limit percentage concentration can be obtained within a certain error range with respect to the theoretical value regardless of the gas composition.
また、ISO規格やICSCに基づく理論値に対しても、爆発下限界百分率濃度を一定の誤差範囲内で得ることができることが確認された。
さらにまた、一つの炭化水素成分、例えばメタン、エタン、ブタンもしくはイソブタンを主成分とする単ガスについても、実験例1と同様にして爆発下限界単位濃度を求めたところ、いずれの規格による理論値に対しても、爆発下限界単位濃度を一定の誤差範囲内で得ることができることが確認された。
It was also confirmed that the lower explosion limit percentage concentration can be obtained within a certain error range even for theoretical values based on ISO standards and ICSC.
Furthermore, for a single gas mainly composed of one hydrocarbon component, such as methane, ethane, butane or isobutane, the lower explosion limit unit concentration was determined in the same manner as in Experimental Example 1, and the theoretical value according to any standard. However, it was confirmed that the lower explosion limit unit concentration can be obtained within a certain error range.
本発明は、イナートガスをベースガスとする複数種のパラフィン系炭化水素成分を含む混合ガスについて、当該混合ガスのパラフィン系炭化水素成分の濃度を爆発下限界百分率濃度で特定することができるので、例えば、燃料ガスの陸揚げ作業終了後のローディングアーム内に残留するガスの検出を行うに際して、極めて有用なものとなることが期待される。 The present invention can specify the concentration of the paraffinic hydrocarbon component of the mixed gas in terms of the lower explosion limit percentage concentration for the mixed gas containing a plurality of types of paraffinic hydrocarbon components using the inert gas as a base gas. It is expected to be extremely useful when detecting the gas remaining in the loading arm after the completion of the landing operation of the fuel gas.
10 ガス検出部
11 音速測定手段
15 屈折率測定手段
20 演算処理部
25 比重測定機構
26 音速-比重換算処理手段
27 屈折率-比重換算処理手段
28 比重算出手段
30 比率算出手段
35 LEL算出手段
40 HC成分濃度算出手段
45 爆発下限界百分率濃度算出手段
DESCRIPTION OF
Claims (11)
当該被検ガスの屈折率および比重を測定し、
当該被検ガスと当該被検ガスにおけるベースガスとの比重差(Δs)の、当該被検ガスと当該ベースガスとの屈折率差(Δn)に対する比率(Δs/Δn)に基づいて、当該被検ガスにおけるパラフィン系炭化水素成分の総濃度および当該被検ガスの爆発下限界濃度のいずれか一方または両方を算出することを特徴とするガス検出方法。 A mixed gas containing two or more paraffinic hydrocarbon components is used as a test gas.
Measure the refractive index and specific gravity of the test gas,
Based on the ratio (Δs / Δn) of the specific gravity difference (Δs) between the test gas and the base gas in the test gas to the refractive index difference (Δn) between the test gas and the base gas. A gas detection method comprising calculating one or both of a total concentration of paraffinic hydrocarbon components in a detected gas and a lower explosion limit concentration of the detected gas.
被検ガスのパラフィン系炭化水素成分の総濃度の、当該被検ガスの爆発下限界濃度に対する百分率を示す爆発下限界百分率濃度を算出することを特徴とする請求項1に記載のガス検出方法。 Calculate the total concentration of paraffinic hydrocarbon components in the test gas and the lower explosive limit concentration of the test gas,
2. The gas detection method according to claim 1, wherein a lower explosion limit percentage concentration indicating a percentage of a total concentration of paraffinic hydrocarbon components of the test gas with respect to a lower explosion limit concentration of the test gas is calculated.
当該比重差規格化値(Δs/ΔsH )の、当該屈折率差規格化値(Δn/ΔnH )に対する比率を算出することを特徴とする請求項4に記載のガス検出方法。 The specific gravity difference (Δs) between the test gas and the nitrogen gas that is the base gas of the test gas is normalized by the specific gravity difference (Δs H ) between the specific hydrocarbon component and the nitrogen gas, and the specific gravity difference normalized value (Δs / Δs H ) is calculated, and the refractive index difference (Δn) between the test gas and nitrogen gas is normalized by the refractive index difference (Δn H ) between the specific hydrocarbon component and nitrogen gas. Calculate the refractive index difference normalized value (Δn / Δn H ),
The gas detection method according to claim 4, wherein a ratio of the specific gravity difference normalized value (Δs / Δs H ) to the refractive index difference normalized value (Δn / Δn H ) is calculated.
メタンガスを基準に規格化した比重差規格化値の屈折率差規格化値に対する比率をX軸とし、爆発下限界濃度をY軸とするX-Y座標系において、下記数式(1-a)で示される曲線と下記数式(1-b)で示される曲線との間の領域内に含まれる曲線または折れ線で示される検量線に基づいて、被検ガスの爆発下限界濃度を算出することを特徴とする請求項5に記載のガス検出方法。
In the XY coordinate system in which the ratio of the specific gravity difference normalized value normalized with respect to methane gas to the refractive index difference normalized value is the X axis and the lower explosion limit concentration is the Y axis, The lower explosive limit concentration of the test gas is calculated based on a calibration curve indicated by a curve or a broken line included in a region between the indicated curve and the curve indicated by the following mathematical formula (1-b) The gas detection method according to claim 5.
当該被検ガスの屈折率を測定する屈折率測定手段と、
当該被検ガスの比重を測定する比重測定手段と、
当該被検ガスと当該被検ガスにおけるベースガスとの比重差(Δs)の、当該被検ガスと当該被検ガスにおけるベースガスとの屈折率差(Δn)に対する比率(Δs/Δn)を出する比率算出手段と、
当該被検ガスにおけるパラフィン系炭化水素成分の総濃度を当該比率に基づいて算出するHC成分濃度算出手段および当該被検ガスの爆発下限界濃度を算出するLEL算出手段のいずれか一方または両方
を備えていることを特徴とするガス検出装置。 A mixed gas containing two or more paraffinic hydrocarbon components is used as a test gas.
A refractive index measuring means for measuring the refractive index of the test gas;
Specific gravity measuring means for measuring the specific gravity of the test gas;
The ratio (Δs / Δn) of the specific gravity difference (Δs) between the test gas and the base gas in the test gas to the refractive index difference (Δn) between the test gas and the base gas in the test gas is calculated. A ratio calculating means for
One or both of HC component concentration calculating means for calculating the total concentration of paraffinic hydrocarbon components in the test gas based on the ratio and LEL calculating means for calculating the lower explosion limit concentration of the test gas are provided. A gas detection device characterized by comprising:
被検ガスのパラフィン系炭化水素成分の総濃度の、当該被検ガスの爆発下限界濃度に対する百分率を示す爆発下限界百分率濃度を算出する爆発下限界百分率濃度算出手段をさらに備えることを特徴とする請求項8に記載のガス検出装置。 Both the HC component concentration calculating means and the LEL calculating means,
It further comprises a lower explosion limit percentage concentration calculating means for calculating a lower explosion limit percentage concentration indicating a percentage of the total concentration of paraffinic hydrocarbon components of the test gas with respect to the lower explosion limit concentration of the test gas. The gas detection device according to claim 8.
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