US3535915A - Method of analyzing binary fluid mixtures and device therefor - Google Patents

Method of analyzing binary fluid mixtures and device therefor Download PDF

Info

Publication number
US3535915A
US3535915A US670054A US3535915DA US3535915A US 3535915 A US3535915 A US 3535915A US 670054 A US670054 A US 670054A US 3535915D A US3535915D A US 3535915DA US 3535915 A US3535915 A US 3535915A
Authority
US
United States
Prior art keywords
mixture
pressure
temperature
orifice
binary
Prior art date
Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
Expired - Lifetime
Application number
US670054A
Inventor
Herman R Felton
Adolph Andrew Buehler
Current Assignee (The listed assignees may be inaccurate. Google has not performed a legal analysis and makes no representation or warranty as to the accuracy of the list.)
EIDP Inc
Original Assignee
EI Du Pont de Nemours and Co
Priority date (The priority date is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the date listed.)
Filing date
Publication date
Application filed by EI Du Pont de Nemours and Co filed Critical EI Du Pont de Nemours and Co
Application granted granted Critical
Publication of US3535915A publication Critical patent/US3535915A/en
Anticipated expiration legal-status Critical
Expired - Lifetime legal-status Critical Current

Links

Images

Classifications

    • GPHYSICS
    • G01MEASURING; TESTING
    • G01NINVESTIGATING OR ANALYSING MATERIALS BY DETERMINING THEIR CHEMICAL OR PHYSICAL PROPERTIES
    • G01N25/00Investigating or analyzing materials by the use of thermal means

Definitions

  • binary fluid mixture refers to a mixture which, except for trace amounts of impurities, consists of only two components, either or both of which is a gas, vapor or liquid at about 25 C. and atmospheric pressure.
  • vaporizable means that the binary fluid mixture, and each component thereof, has a boiling point below about 250 C. at atmospheric pressure. Such fluid mixtures will at least partially evaporate upon passing through an orifice into an expansion chamber maintained at a pressure below the pressure before the orifice.
  • Binary vaporizable fluid mixtures are well known and are widely used as propellents for expelling other materials such as insecticides, fungicides, deodorants, hairtreating compositions, foodstuffs, paints, and the like from pressurized containers in the form of aerosols, sprays and foams. These mixtures are also used as refrigerants, dielectrics, reactants in chemical processes and for other purposes.
  • such binary fluid mixtures are produced by one of two methods.
  • the most common method is by mixing the two components in the desired proportions, preferably in a continuous manner.
  • the other is by producing the binary fluid mixture in a chemical process in which the proportions of the components of the mixture can be varied by changing the process conditions. In this manner, it is possible to produce mixtures containing components in the desired proportions.
  • a number of devices which can be used to determine the composition of such mixtures. These devices include mass spectrometers, vapor phase chromatographic units, infrared spectrometers, and the like. However, each of these devices has a characteristic which renders it undesirable for many applications, such as be ing expensive, nontransportable, batchwise in operation which requires that samples of the binary fluid mixture be withdrawn periodically and placed in the device for analysis, or slow in operation which results in a time lapse from sample withdrawal to final analysis of from several minutes to an hour or more.
  • a device and method for continuously determining the components has been described by Felton and Williams in US. Pat. 3,264,862. Their process involves flowing the mixture from a supply chamber at a predetermined temperature and pressure through an orifice, expanding the mixture adiabatically in an expansion chamber maintained at a predetermined pressure, and measuring the temperature of the expanded mixture. This temperature is characteristic of the composition of the mixture and varies regularly with variation in its composition. Thus, the composition of the mixture is determined by measuring the temperature of the expanded mixture under predetermined conditions, and comparing this temperature with the temperatures produced by a series of similarly expanded binary mixtures of the same components of known varying composition.
  • the improved analyzing device of this invention comprises:
  • a pressure reducing means connected to the outlet; from said first side of the heat exchanger, said pressure. reducing means causing a rapid pressure reduction as the binary fluid mixture passes therethrough,
  • Temperature sensing means positioned just after the pressure reducing means so as to measure the temperature of the mixture just after it passes through the pressure reducing means
  • Feed pressure variations are overcome by first passing the sample through a pressure regulator which adjusts the pressure to a predetermined level. Then, by heat exchanging the incoming and outgoing mixtures, an equilibrium or self-cooling temperature after expansion is established for the incoming sample which is substantially independent of the initial temperature of the sample. Accordingly, a greatly reduced sensitivity to initial sample temperature and pressure is accomplished in accordance with this invention.
  • the method and analyzing device of this invention is suitable for use with any binary fluid mixture of known components having a normal boiling point up to about 250 'C.
  • binary fluid mixtures which are gases or liquids having normal boiling points below about 50 C.
  • Binary gas mixtures in which the components have normal boiling points of about -40 to 24 C. are readily liquefied at about room temperature by subjecting them to pressures equal to or above their vapor pressures, and frequently are maintained and handled as liquids under these conditions.
  • This invention is particularly useful for the analysis of such binary liquid mixtures.
  • Suitable binary fluid mixtures include mixtures containing about 40 to 70% by weight monofiuorotrichloromethane (B.P. 23.8 C.) and about 60 to 30% by weight dichlorodifiuoromethane (B.P. --29.8 C.), azeotropic mixtures containing dichlorodifluoromethane and dichlorotetrafluoroethane (B.P. 3.6 C.), mixtures containing monochlorodifiuoromethane (B.P. -40.8 C.) and monochloropentafluoroethane (B.P. -38.7 C.), mixtures containing about to 26% by weight isobutane (B.P.
  • the initial temperature and the initial pressure of the binary fluid mixture will be that of the source of the mixture, such as that of the process stream, blending equipment or storage vessel.
  • the source of the binary fluid mixture will be a storage vessel or blending equipment, in which case the binary fluid mixture will be at about 25 C.
  • the binary fluid mixture When the binary fluid mixture is gaseous, it will usually be at a superatmospheric pressure of about 15 to p.s.i.g.
  • the initial pressure will generally be the vapor pressure of the mixture which may be as high as about 2,000 p.s.i.g.
  • the initial pressure of the binary fluid mixture is at least about 8 p.s.i.g. since this allows the expansion chamber to be operated at substantially atmospheric pressure.
  • the binary fluid mixture undergoes a pressure reduction during determination of its composition.
  • This pressure reduction need only be suflicient to cause the binary fluid mixture to flow through the pressure reducing means.
  • the minimum pressure reduction necessary to accomplish this end will vary depending upon the particular binary fluid mixture being analyzed. Minimum pressure reductions of about 1 to 5 p.s.i. are typical.
  • the pressure after the pressure reducing means is substantially atmospheric, and the pressure before the pressure reducing means is regulated slightly above atmospheric, thereby providing the necessary pressure reduction. Since it is difficult to accurately regulate superatmospheric pressures of less than about 8 p.s.i.g., the pressure before the pressure reducing means is preferably regulated to a constant pressure of about 8 to 12 p.s.i.g.
  • the analyzer When using the analzing device of this invention to determine the composition of a binary fluid mixture of known components in unknown proportions, the analyzer is first calibrated with a series of known binary fluid mixtures of these components. More specifically, a series of mixtures of the two components in varying known proportions is passed through the analyzer and a constant equilibrium temperature is established for each in the expansion chamber. A calibration curve is prepared by plotting the recorded temperature or equivalent measurements, such as thermistor bridge inbalances, against the composition of the known mixtures. The binary fluid mixture to be analyzed is then passed through the analyzer and its composition is determined by comparing its equilibrium temperature or equivalent measurement with those recorded for the known mixtures, that is, the observed measurement is used to read the composition of the analyzed binary fluid mixture from the calibration curve.
  • a binary vaporizable fluid mixture can be analyzed to determine its composition quickly, simply and inexpensively.
  • the analyzing device of this invention may be operated batchwise, intermittently, periodically or continuously as desired. It is portable and easily assembled and calibrated. The accuracy of the analysis will depend primarily upon the sensitivity and accuracy of the temperature sensing means. By the use of a temperature sensing means which is accurate to within 0.01 C., it is usually possible to obtain analyses which are accurate to within 1%, which is suflicient for most purposes in commercial operations.
  • a preferred embodiment of the improved analyzing device of this invention comprises: v
  • Temperature sensing means positioned in said expansion chamber below the level of the overflow outlet, including means extending outside the expansion chamber for indicating the temperature
  • FIG. 1 is a vertical cross-sectional view of one embodiment of the analyzing device of this invention.
  • FIG. 2 is a vertical cross-sectional view of a preferred embodiment of a portion of the analyzing device of FIG. 1.
  • a stream of the binary fluid mixture to be analyzed is introduced at sample inlet 1, at the temperature and pressure of the source of the mixture.
  • the sample proceeds continuously through pressure regulator 2 which is set to pass the sample at a predetermined constant pressure.
  • the pressure regulator passes the incoming sample at a constant pressure of about 8 to 12 p.s.i.g. which allows substantially atmospheric pressure to be used in the expansion chamber.
  • the initial pressure is generally greater than necessary, in which case pressure regulator 2 reduces the pressure to the preferred range of about 8 to 12 p.s.i.g.
  • the binary fluid mixture to be analyzed is a liquid having a normal boiling point of about 25 to 50 C.
  • the mixture is generally passed through pressure regulator 2 at atmospheric pressure and the expansion chamber is maintained at reduced (subatmospheric) pressure by the application of a vacuum at the exit end of the analyzing device.
  • the amount of vacuum necessary will depend upon the volatility and boiling point of the binary liquid mixture, and the amount of pressure drop through the orifice.
  • the sample from pressure regulator 2 passes through the first side of heat exchanger 3.
  • a screen or other filtering means 4 positioned before the pressure reducing orifice, is optional and is provided when necessary to remove solid particles entrained in the binary fluid mixture thereby preventing such particles from clogging the pressure reducing orifice.
  • the mixture is expanded through pressure reducing orifice 5 into a suitable expansion chamber which is maintained at a pressure of at least about 8 p.s.i. below the pressure before the orifice.
  • the expansion chamber may be a separate chamber or it may be the chamber side of heat exchanger 3 as illustrated in FIG. 1.
  • Orifice 5 On passing through orifice 5 the binary fluid mixture expands, resulting in partial evaporation if either of the components of the mixture approaches the orifice as a liquid, whereby the temperature of the mixture is lowered.
  • Orifice 5 may be a constricting orifice, thereby providing the necessary pressure reduction, or it may be of the nonconstricting type as illustrated in FIG. 1. In the latter case, the required pressure reduction results from the difference in size between orifice 5 and exit tube 10.
  • Temperature sensing means 7 is positioned just after orifice 5 so that it measures the temperature of the gaseous mixture just after it passes through the orifice.
  • the temperature sensing means must be spaced sufiiciently distant from the orifice that it does not obstruct the orifice or prevent the binary fluid mixture from expanding on passing through the orifice, but sufliciently close to the orifice that the expanded mixture immediately impinges on the temperature sensing means so that it can measure the reduced temperature caused by the expansion. Since expansion of the binary fluid mixture as it passes through the orifice is substantially instantaneous, the temperature sensing means is usually spaced about ,4, to about inch from the orifice, and preferably about inch.
  • Temperature sensing means 7 is connected to a means 8 extending outside of the expansion chamber for indicating the temperature of the expanded mixture.
  • the embodiment illustrated in FIG. 1 is preferably used when the expanded fluid mixture is a gas. When the expanded mixture is partially liquid, measurement of the temperature of the expanded mixture will be more accurate if the modification illustrated in FIG. 2 is used.
  • the fluid mixture after expansion, passes into the second side of heat exchanger 3 thereby cooling the incoming mixture on the first side, and thereafter out of the analyzer via exit 10.
  • the whole apparatus is enclosed in casing 11 which optionally and preferably is filled with an insulating means such as insulating foam so that the system functions under substantially adiabatic conditions.
  • Bypass valve 12 is optionally provided to temporarily remove pressure regulator 2 from the system during start-up, thereby bringing the system to operating temperature more rapidly.
  • flowing of the binary fluid mixture through orifice 5 is continued until an equilibrium temperature is reached as indicated by a constant temperature reading by temperature sensing means 7.
  • FIG. 2 a preferred variation of the device of FIG. 1 is shown.
  • This embodiment is particularly suitable for analyzing fluid mixtures which are present at least partially in liquid form during operation of the device.
  • This device is the same as the device of FIG. 1 until pressure reducing means is reached.
  • pressure reducing means 5 is illustrated as a constricting orifice in which case the tubing before and after the orifice can be the same size.
  • a separate expansion chamber 6 is provided into which the mixture is expanded through orifice 5.
  • the pressure in expansion chamber 6 is preferably not greater than the vapor pressure of the binary fluid mixture at the operating temperature of the expansion chamber.
  • the fluid mixture has a boiling point in the range of about to C. and the expansion chamber is at substantially atmospheric pressure, the mixture will pass from heat exchanger 3 as a liquid and will only partially vaporize when expanded through orifice 5 into expansion chamber 6. Accordingly, a body of liquid is maintained in expansion chamber 6 by the height of an overflow outlet 9.
  • the fluid mixture boils in the range of about to +250 C.
  • the body of liquid can be maintained in the expansion chamber by maintaining the necessary pressure above or below atmospheric, as the case may be.
  • the suitable pressure range for maintaining a body of liquid in the expansion chamber is quite broad since pressure variations merely lead to variations in the ratio of liquid to gas leaving the expansion chamber via outlet 9.
  • Heat sensing means 7 is positioned in the expansion chamber below the liquid level which provides a very accurate method of measuring the temperature of the expanded mixture.
  • the expanded mixture leaves the expansion chamber through overflow outlet 9 and passes into the second side of heat exchanger 3 as in FIG. 1.
  • heat exchanger 3 may be of any conventional design.
  • the incoming sample passes through the coil side of the heat exchanger while the expanded mixture passes through the chamber side.
  • orifice 5 The actual size of orifice 5 is not important except to the extent of its relationship to the pressure being maintained in pressure regulator 2 and the size of any constrictions beyond the expansion chamber such as outlet 9 and exit 10. In other words, the orifice must be of such size as to provide a pressure drop which causes the binary fluid mixture to pass through it.
  • the orifice provides a pressure drop of at least 8 p.s.i. and has a diameter of about 0.001 to 0.05 inch, and more preferably about 0.002 to 0.025 inch, and most preferably about 0.004 to 0.02 inch, thereby causing a significant cooling of fluids expanded therethrough. It may be of any available shape, but usually a circular orifice is most convenient.
  • the size of the tubing used in the analyzing device is not critical so long as it is not smaller than the size of orifice 5.
  • the tubing has an internal diameter of about 0.001 to 0.125 inch.
  • Expansion chamber 6 and subsequent compartments should be sutficiently large to receive the expanding binary fluid mixture passing from orifice 5 without causing back pressure.
  • the expansion chamber preferably should have a volume of at least about 1.5 ml. and most preferably at least about 2 ml., and a diameter at least twice the diameter of exit 9.
  • the expansion chamber may be as large as desired, the maximum size being dictated only by economic considerations and the like.
  • Temperature sensing means 7 may be a commercial thermistor and may be connected to a Wheatstone bridge circuit as is commonly employed for thermistor type temperature measurements.
  • the circuit contains an ammeter 8 which shows the inbalance of the Wheatstone bridge due to changes in the temperature of the thermistor.
  • the current readings can be converted to temperature readings in degrees, if desired, but this usually is unnecessary as the current readings are equally useful as a measure of the change in the temperature of the thermistor, and it is more convenient to use the current reading for this purpose.
  • Temperature indicating means 8 may also be a potentiometer-recorder used to indicate the bridge output and thereby give a permanent recording of the thermistor temperature.
  • the temperature sensing means is a 3000-0hm Precision Thermistor.
  • Temperature indicating means 8 will be of any conventional form and type that is adapted to indicate and/or record the temperature of the temperature sensing means. In the case of thermometers, means 8 will be the upper portion of the thermometer containing the required temperature markings While temperature sensing means 7 will be the bulb of the thermometer.
  • the various parts of the analyzer may be constructed of any material which will withstand the temperatures and pressures under which it is to be used and which is substantially inert to the binary fluid mixture to be analyzed under those conditions. Suitable materials include brass, copper, steel, stainless steel, nickel, Monel, Inconel, aluminum, polytetrafluoroethylene, polyethylene and the like.
  • EXAMPLE 1 Various samples of mixtures containing trichlorofluoromethane and dichlorodifluoromethane (DCDFM) were analyzed on four separate but identical analyzing devices similar to the device illustrated in FIG. 2 with the pressure regulator maintaining a pressure of 8 p.s.i.g. and the expansion chamber at atmospheric pressure. Samples were charged to the analyzers continuously at their own vapor pressure at 25 C. until equilibrium was established as indicated by a constant temperature reading. The following recorder readings were obtained and the corresponding DCDFM contents were determined from a calibration curve based on a series of samples.
  • DCDFM dichlorodifluoromethane
  • EXAMPLE 4 Five 145-lb. cylinders were filled with mixtures of dichlorodiflu'oromethane and 1,2-dichloro 1,1,2,2 tetrafluoroethane (DCTFE) in 10:90, 25:75, 50:50, 75:25 and 90: 10% ratios. These mixtures were run through the analyzing device illustrated in FIG. 2 until the recorded voltage output on the Wheatstone bridge became constant.
  • the pressure regulator was set to maintain a pressure of 8 p.s.i.g. and the pressure in the expansion chamber was essentially atmospheric.
  • the temperatures in the cylinders ranged from to 30 C. and the initital pressures ranged from 10 to 100 p.s.i.g. The following data were obtained:
  • EXAMPLE 5 Three 145-lb. cylinders were filled with mixtures of dichlorodifluoromethane (DCDFM) and isobutane in 25:75, :70 and :65% ratios. These mixtures were run through the analyzing device illustrated in FIG. 2 until the recorded voltage output on the Wheatstone bridge became constant.
  • the pressure regulator was set to maintain a pressure of 8 p.s.i.g.
  • the temperatures in the cylinders ranged from 20 to 30 C. and the initial pressures ranged from 70 to 150 p.s.i.g. The following data were obtained.
  • a method for determining the composition of a binary vaporizable fluid mixture of known components which comprises:
  • An analyzing device for determining the composition of binary vaporizable fluid mixtures of known components which comprises:
  • the pressure reducing means is a constricting orifice which causes a rapid pressure reduction of at least 8 p.s.i., said orifice being connected to an expansion chamber having an overflo-w outlet for retaining a body of liquid mixture, said orifice discharging binary fluid mixture in the expansion chamber below the level of the overflow outlet, and the temperature sensing means is positioned in the expansion chamber below the level of the overflow outlet and includes means extending outside the extension chamber for indicating the temperature.
  • the analyzing device of claim 5 in which the pressure regulator maintains a constant pressure of 8 to 12 p.s.i.g., and the constricting orifice has a diameter of 0.001 to 0.05 inch.

Landscapes

  • Physics & Mathematics (AREA)
  • Health & Medical Sciences (AREA)
  • Life Sciences & Earth Sciences (AREA)
  • Chemical & Material Sciences (AREA)
  • Analytical Chemistry (AREA)
  • Biochemistry (AREA)
  • General Health & Medical Sciences (AREA)
  • General Physics & Mathematics (AREA)
  • Immunology (AREA)
  • Pathology (AREA)
  • Investigating Or Analyzing Materials Using Thermal Means (AREA)

Description

Oct. 27, 1970 H. R. FELTON ETAL 3,535,915
METHOD OF ANALYZING BINARY FLUID MIXTURES AND DEVICE THEREFOR Filed Sept. 25, 19s?- INVENTORS HERMAN R. FELTON ADOLPH A. BUEHLER BY WE.
ATTORNEY United States Patent ABSTRACT OF THE DISCLOSURE Method of analyzing binary vaporizable fluid mixtures of known components to determine their percent composition by measuring the temperature of the mixture after a controlled expansion, and analyzing device containing a heat exchanger for carrying out such method.
BACKGROUND OF THE INVENTION Field of the invention This invention relates to an improved method of analyzing vaporizable binary fluid mixtures of known components to determine their percent composition and to an improved analyzing device for use in such method. Throughout the specification and claims the term binary fluid mixture refers to a mixture which, except for trace amounts of impurities, consists of only two components, either or both of which is a gas, vapor or liquid at about 25 C. and atmospheric pressure. The term vaporizable means that the binary fluid mixture, and each component thereof, has a boiling point below about 250 C. at atmospheric pressure. Such fluid mixtures will at least partially evaporate upon passing through an orifice into an expansion chamber maintained at a pressure below the pressure before the orifice.
DESCRIPTION OF THE PRIOR ART Binary vaporizable fluid mixtures are well known and are widely used as propellents for expelling other materials such as insecticides, fungicides, deodorants, hairtreating compositions, foodstuffs, paints, and the like from pressurized containers in the form of aerosols, sprays and foams. These mixtures are also used as refrigerants, dielectrics, reactants in chemical processes and for other purposes.
In general, such binary fluid mixtures are produced by one of two methods. The most common method is by mixing the two components in the desired proportions, preferably in a continuous manner. The other is by producing the binary fluid mixture in a chemical process in which the proportions of the components of the mixture can be varied by changing the process conditions. In this manner, it is possible to produce mixtures containing components in the desired proportions. During either method of preparation, it is desirable to frequently analyze such binary fluid mixtures to determine the proportions of the components therein.
A number of devices are known which can be used to determine the composition of such mixtures. These devices include mass spectrometers, vapor phase chromatographic units, infrared spectrometers, and the like. However, each of these devices has a characteristic which renders it undesirable for many applications, such as be ing expensive, nontransportable, batchwise in operation which requires that samples of the binary fluid mixture be withdrawn periodically and placed in the device for analysis, or slow in operation which results in a time lapse from sample withdrawal to final analysis of from several minutes to an hour or more.
A device and method for continuously determining the components has been described by Felton and Williams in US. Pat. 3,264,862. Their process involves flowing the mixture from a supply chamber at a predetermined temperature and pressure through an orifice, expanding the mixture adiabatically in an expansion chamber maintained at a predetermined pressure, and measuring the temperature of the expanded mixture. This temperature is characteristic of the composition of the mixture and varies regularly with variation in its composition. Thus, the composition of the mixture is determined by measuring the temperature of the expanded mixture under predetermined conditions, and comparing this temperature with the temperatures produced by a series of similarly expanded binary mixtures of the same components of known varying composition.
The process of the Felton and Williams patent requires that the binary mixture be available at the predetermined temperature and pressure for accurate analysis. Varia tions in temperature or pressure of the mixture entering the device cause errors in the determination of the composition of the mixture. Accordingly, it would be desirable to provide a method and device for analyzing binary vaporizable fluid mixtures which is not sensitive to the temperature and pressure of the mixture entering the device.
SUMMARY OF THE INVENTION (0) Rapidly reducing the pressure of the mixture thereby expanding and cooling the mixture,
(d) Measuring the temperature of the mixture just after expansion,
(e) Passing the expanded mixture through the second side of the heat exchanger,
Said steps being carried out continuously until the temperature just after expansion remains substantially constant, and
(f) Comparing this temperature with the temperatures recorded for a series of similarly expanded binary fluid mixtures of the same components of known varying composition.
The improved analyzing device of this invention comprises:
(a) An inlet for passing the binary vaporizablefluid mixture into the device, I
(b) A pressure regulator connected to said inlet which passes the mixture at a constant pressure,
(c) A heat exchanger having the inlet to the connected to the pressure regulator,
first side (d) A pressure reducing means connected to the outlet; from said first side of the heat exchanger, said pressure. reducing means causing a rapid pressure reduction as the binary fluid mixture passes therethrough,
(e) Temperature sensing means positioned just after the pressure reducing means so as to measure the temperature of the mixture just after it passes through the pressure reducing means,
(f) Means for connecting the pressure reducing means to the second side of the heat exchanger, and
(g) An outlet connected to said second side of the heat exchanger for removing the mixture from the device.
It is well known that most real gases, as contrasted with an ideal gas, cool when expanded rapidly, and that liquids also cool when expanded by a rapid reduction in pressure which causes partial vaporization. When starting up the device of this invention, a binary fluid mixture is passed through the first side of a heat exchanger and is rapidly expanded through a pressure reducing means thereby causing a reduction in the temperature of the mixture. The expanded fluid of reduced temperature is then heat exchanged with incoming mixture which has not passed through the pressure reducing means. This incoming mixture therefore enters the pressure reducing means at a temperature lower than the original mixture did and cools during expansion to a temperature lower than the original mixture. Accordingly, the temperatures before and after expansion get progressively lower until the equilibrium temperatures of the system are reached. These equilibrium temperatures will depend primarily upon the physical characteristics of the mixture, the magnitude of the pressure reduction experienced as the fluid passes through the pressure reducing means, and the heat exchange efliciency of the device.
When operating in accordance with this invention, it has been found that the temperature at which the sample enters the device has very little effect upon the temperature of the fluid after expansion. This process does not require that the initial temperature and pressure of the sample be predetermined or that they be the same as those of the series of similarly expanded binary fluid mixtures of the same components of known varying composition with which the sample is compared.
In accordance with this invention, the difficulties introduced by variations in the temperature and pressure of the sample when using the Felton and Williams device are overcome. Feed pressure variations are overcome by first passing the sample through a pressure regulator which adjusts the pressure to a predetermined level. Then, by heat exchanging the incoming and outgoing mixtures, an equilibrium or self-cooling temperature after expansion is established for the incoming sample which is substantially independent of the initial temperature of the sample. Accordingly, a greatly reduced sensitivity to initial sample temperature and pressure is accomplished in accordance with this invention.
DETAILED DESCRIPTION OF THE INVENTION General description Although the method and analyzing device of this invention is suitable for use with any binary fluid mixture of known components having a normal boiling point up to about 250 'C., it is particularly useful with binary fluid mixtures which are gases or liquids having normal boiling points below about 50 C. Binary gas mixtures in which the components have normal boiling points of about -40 to 24 C. are readily liquefied at about room temperature by subjecting them to pressures equal to or above their vapor pressures, and frequently are maintained and handled as liquids under these conditions. This invention is particularly useful for the analysis of such binary liquid mixtures.
Typical examples of suitable binary fluid mixtures include mixtures containing about 40 to 70% by weight monofiuorotrichloromethane (B.P. 23.8 C.) and about 60 to 30% by weight dichlorodifiuoromethane (B.P. --29.8 C.), azeotropic mixtures containing dichlorodifluoromethane and dichlorotetrafluoroethane (B.P. 3.6 C.), mixtures containing monochlorodifiuoromethane (B.P. -40.8 C.) and monochloropentafluoroethane (B.P. -38.7 C.), mixtures containing about to 26% by weight isobutane (B.P. '10.2 C.) and about 85 to 74% by weight dichlorodifluoromethane, and mixtures containing octafluorocyclobutane (B.P. -6.1 C.) with nitrous oxide (B.P. 89.5 C.), propane (B.P. -42.5
C.), cyclopropane (B.P. 34.4 C.), hexafluoroethane (B.P. -78.1 C.) or monochloropentafluoroethane. Other binary fluid mixtures which can be analyzed in accordance with the method of the present invention will be apparent to those skilled in the art.
In most cases, the initial temperature and the initial pressure of the binary fluid mixture will be that of the source of the mixture, such as that of the process stream, blending equipment or storage vessel. Usually the source of the binary fluid mixture will be a storage vessel or blending equipment, in which case the binary fluid mixture will be at about 25 C. When the binary fluid mixture is gaseous, it will usually be at a superatmospheric pressure of about 15 to p.s.i.g. When the binary fluid mixture is a liquefied gas, the initial pressure will generally be the vapor pressure of the mixture which may be as high as about 2,000 p.s.i.g. Preferably, the initial pressure of the binary fluid mixture is at least about 8 p.s.i.g. since this allows the expansion chamber to be operated at substantially atmospheric pressure.
In accordance with this invention, the binary fluid mixture undergoes a pressure reduction during determination of its composition. This pressure reduction need only be suflicient to cause the binary fluid mixture to flow through the pressure reducing means. The minimum pressure reduction necessary to accomplish this end will vary depending upon the particular binary fluid mixture being analyzed. Minimum pressure reductions of about 1 to 5 p.s.i. are typical. Preferably the pressure after the pressure reducing means is substantially atmospheric, and the pressure before the pressure reducing means is regulated slightly above atmospheric, thereby providing the necessary pressure reduction. Since it is difficult to accurately regulate superatmospheric pressures of less than about 8 p.s.i.g., the pressure before the pressure reducing means is preferably regulated to a constant pressure of about 8 to 12 p.s.i.g.
When using the analzing device of this invention to determine the composition of a binary fluid mixture of known components in unknown proportions, the analyzer is first calibrated with a series of known binary fluid mixtures of these components. More specifically, a series of mixtures of the two components in varying known proportions is passed through the analyzer and a constant equilibrium temperature is established for each in the expansion chamber. A calibration curve is prepared by plotting the recorded temperature or equivalent measurements, such as thermistor bridge inbalances, against the composition of the known mixtures. The binary fluid mixture to be analyzed is then passed through the analyzer and its composition is determined by comparing its equilibrium temperature or equivalent measurement with those recorded for the known mixtures, that is, the observed measurement is used to read the composition of the analyzed binary fluid mixture from the calibration curve.
Since the equilibrium temperatures of expanded binary fluid mixtures vary regularly with variations in the proportions of the components, it is not necessary to employ a large number of known mixtures with small variations in proportions in preparing the calibration curve. Differences in concentration of about 4 to 6% between adjacent members of the series of known mixtures are usually sufficient. The analyzer is most commonly used in controlling a process for blending the two component of the binary fluid mixture, in which case variations in the composition of the mixture are within a narrow range. Accordingly, it is suflicient if the series employed in the calibration contains only a few mixtures of known composition in which the proportions are varied over a range which approximates the range of expected variations in the mixtures to be analyzed.
By the use of the process and the analyzer of this invention, a binary vaporizable fluid mixture can be analyzed to determine its composition quickly, simply and inexpensively. The analyzing device of this invention may be operated batchwise, intermittently, periodically or continuously as desired. It is portable and easily assembled and calibrated. The accuracy of the analysis will depend primarily upon the sensitivity and accuracy of the temperature sensing means. By the use of a temperature sensing means which is accurate to within 0.01 C., it is usually possible to obtain analyses which are accurate to within 1%, which is suflicient for most purposes in commercial operations.
A preferred embodiment of the improved method of this invention comprises:
(a) Passing a stream of the binary fluid mixture through a pressure regulator which passes the mixture at a constant pressure of at least about 8 p.s.i.g.,
(b) Passing the mixture from the pressure regulator through the first side of a heat exchanger wherein the temperature of the fluid is reduced, Y
(c)) Passing the mixture from the heat exchanger through a constricting orifice into an expansion chamber containing a body of liquid binary fluid mixture, thereby rapidly reducing the pressure of the mixture at least about 8 p.s.i. under substantially adiabatic conditions with a resulting expansion and cooling of the mixture, said expanding mixture discharging from the orifice below the surface of the body of liquid,
(d) Measuring the temperature of the body of liquid,
(e) Passing the expanded mixture through the second side of said heat exchanger, whereby the incoming mixture is cooled to approximately its boiling point at the pressure after the orifice, and
(f) Comparing the measured temperature of the body of liquid with the temperature recorded for a series of similarly expanded binary fluid mixtures of the same components of known varying composition.
, A preferred embodiment of the improved analyzing device of this invention comprises: v
(a) An inlet for passing the binary vaporizable fluid mixture into the device,
(b) A pressure regulator connected to said inlet which passes the mixture at a constant pressure,
(c) A heat exchanger having the inlet to the first side connected to the pressure regulator,
(d) A constricting orifice connected to the outlet from said first side of the heat exchanger, said orifice causing a rapid pressure reduction of at least about 8 p.s.i.,
(e) An expansion chamber connected to said orifice having an overflow outlet for retaining a body of liquid mixture, said orifice discharging binary fluid mixture in the expansion chamber below the level of the overflow outlet,
(13) Temperature sensing means positioned in said expansion chamber below the level of the overflow outlet, including means extending outside the expansion chamber for indicating the temperature,
(g) Means for passing the mixture from the overflow outlet through the second side of the heat exchanger and removing the mixture from the device.
Description of the drawing I In order that the invention may be more readily understood, it will be further described in connection with the accompanying drawing. FIG. 1 is a vertical cross-sectional view of one embodiment of the analyzing device of this invention. FIG. 2 is a vertical cross-sectional view of a preferred embodiment of a portion of the analyzing device of FIG. 1.
Referring now to FIG. 1, a stream of the binary fluid mixture to be analyzed is introduced at sample inlet 1, at the temperature and pressure of the source of the mixture. The sample proceeds continuously through pressure regulator 2 which is set to pass the sample at a predetermined constant pressure. Preferably, the pressure regulator passes the incoming sample at a constant pressure of about 8 to 12 p.s.i.g. which allows substantially atmospheric pressure to be used in the expansion chamber.
When the binary fluid mixture to be analyzed is gaseous or a liquefied gas, the initial pressure is generally greater than necessary, in which case pressure regulator 2 reduces the pressure to the preferred range of about 8 to 12 p.s.i.g. When the binary fluid mixture to be analyzed is a liquid having a normal boiling point of about 25 to 50 C., the mixture is generally passed through pressure regulator 2 at atmospheric pressure and the expansion chamber is maintained at reduced (subatmospheric) pressure by the application of a vacuum at the exit end of the analyzing device. The amount of vacuum necessary will depend upon the volatility and boiling point of the binary liquid mixture, and the amount of pressure drop through the orifice.
The sample from pressure regulator 2 passes through the first side of heat exchanger 3. A screen or other filtering means 4, positioned before the pressure reducing orifice, is optional and is provided when necessary to remove solid particles entrained in the binary fluid mixture thereby preventing such particles from clogging the pressure reducing orifice. The mixture is expanded through pressure reducing orifice 5 into a suitable expansion chamber which is maintained at a pressure of at least about 8 p.s.i. below the pressure before the orifice. The expansion chamber may be a separate chamber or it may be the chamber side of heat exchanger 3 as illustrated in FIG. 1. On passing through orifice 5 the binary fluid mixture expands, resulting in partial evaporation if either of the components of the mixture approaches the orifice as a liquid, whereby the temperature of the mixture is lowered. Orifice 5 may be a constricting orifice, thereby providing the necessary pressure reduction, or it may be of the nonconstricting type as illustrated in FIG. 1. In the latter case, the required pressure reduction results from the difference in size between orifice 5 and exit tube 10.
Temperature sensing means 7 is positioned just after orifice 5 so that it measures the temperature of the gaseous mixture just after it passes through the orifice. The temperature sensing means must be spaced sufiiciently distant from the orifice that it does not obstruct the orifice or prevent the binary fluid mixture from expanding on passing through the orifice, but sufliciently close to the orifice that the expanded mixture immediately impinges on the temperature sensing means so that it can measure the reduced temperature caused by the expansion. Since expansion of the binary fluid mixture as it passes through the orifice is substantially instantaneous, the temperature sensing means is usually spaced about ,4, to about inch from the orifice, and preferably about inch.
Temperature sensing means 7 is connected to a means 8 extending outside of the expansion chamber for indicating the temperature of the expanded mixture. The embodiment illustrated in FIG. 1 is preferably used when the expanded fluid mixture is a gas. When the expanded mixture is partially liquid, measurement of the temperature of the expanded mixture will be more accurate if the modification illustrated in FIG. 2 is used.
The fluid mixture, after expansion, passes into the second side of heat exchanger 3 thereby cooling the incoming mixture on the first side, and thereafter out of the analyzer via exit 10. The whole apparatus is enclosed in casing 11 which optionally and preferably is filled with an insulating means such as insulating foam so that the system functions under substantially adiabatic conditions. Bypass valve 12 is optionally provided to temporarily remove pressure regulator 2 from the system during start-up, thereby bringing the system to operating temperature more rapidly. During start-up, flowing of the binary fluid mixture through orifice 5 is continued until an equilibrium temperature is reached as indicated by a constant temperature reading by temperature sensing means 7.
In FIG. 2 a preferred variation of the device of FIG. 1 is shown. This embodiment is particularly suitable for analyzing fluid mixtures which are present at least partially in liquid form during operation of the device. This device is the same as the device of FIG. 1 until pressure reducing means is reached. In this modification, pressure reducing means 5 is illustrated as a constricting orifice in which case the tubing before and after the orifice can be the same size. A separate expansion chamber 6 is provided into which the mixture is expanded through orifice 5.
When using the embodiment of FIG. 2, the pressure in expansion chamber 6 is preferably not greater than the vapor pressure of the binary fluid mixture at the operating temperature of the expansion chamber. When the fluid mixture has a boiling point in the range of about to C. and the expansion chamber is at substantially atmospheric pressure, the mixture will pass from heat exchanger 3 as a liquid and will only partially vaporize when expanded through orifice 5 into expansion chamber 6. Accordingly, a body of liquid is maintained in expansion chamber 6 by the height of an overflow outlet 9. When the fluid mixture boils in the range of about to +250 C., the body of liquid can be maintained in the expansion chamber by maintaining the necessary pressure above or below atmospheric, as the case may be. For any given sample, the suitable pressure range for maintaining a body of liquid in the expansion chamber is quite broad since pressure variations merely lead to variations in the ratio of liquid to gas leaving the expansion chamber via outlet 9.
Heat sensing means 7 is positioned in the expansion chamber below the liquid level which provides a very accurate method of measuring the temperature of the expanded mixture. The expanded mixture leaves the expansion chamber through overflow outlet 9 and passes into the second side of heat exchanger 3 as in FIG. 1.
In the analyzing device of this invention, heat exchanger 3 may be of any conventional design. The more efficient the heat exchanger is, the more quickly equilibrium is established and the more accurate the analysis will be. Preferably, the incoming sample passes through the coil side of the heat exchanger while the expanded mixture passes through the chamber side.
The actual size of orifice 5 is not important except to the extent of its relationship to the pressure being maintained in pressure regulator 2 and the size of any constrictions beyond the expansion chamber such as outlet 9 and exit 10. In other words, the orifice must be of such size as to provide a pressure drop which causes the binary fluid mixture to pass through it. Preferably the orifice provides a pressure drop of at least 8 p.s.i. and has a diameter of about 0.001 to 0.05 inch, and more preferably about 0.002 to 0.025 inch, and most preferably about 0.004 to 0.02 inch, thereby causing a significant cooling of fluids expanded therethrough. It may be of any available shape, but usually a circular orifice is most convenient.
The size of the tubing used in the analyzing device is not critical so long as it is not smaller than the size of orifice 5. Preferably, the tubing has an internal diameter of about 0.001 to 0.125 inch.
Expansion chamber 6 and subsequent compartments should be sutficiently large to receive the expanding binary fluid mixture passing from orifice 5 without causing back pressure. For such purpose, the expansion chamber preferably should have a volume of at least about 1.5 ml. and most preferably at least about 2 ml., and a diameter at least twice the diameter of exit 9. The expansion chamber may be as large as desired, the maximum size being dictated only by economic considerations and the like.
Temperature sensing means 7 may be a commercial thermistor and may be connected to a Wheatstone bridge circuit as is commonly employed for thermistor type temperature measurements. The circuit contains an ammeter 8 which shows the inbalance of the Wheatstone bridge due to changes in the temperature of the thermistor. The current readings can be converted to temperature readings in degrees, if desired, but this usually is unnecessary as the current readings are equally useful as a measure of the change in the temperature of the thermistor, and it is more convenient to use the current reading for this purpose. Temperature indicating means 8 may also be a potentiometer-recorder used to indicate the bridge output and thereby give a permanent recording of the thermistor temperature. Preferably, the temperature sensing means is a 3000-0hm Precision Thermistor.
While a thermistor is the preferred form of temperature sensing means 7, other forms may also be used, particularly thermocouples and other like electronic temperature sensing devices which rapidly detect and measure rather small changes in temperature, particularly those which are accurate to 11 C. Thermometers, such as mercury and toluene filled types, can be used but usually are less desirable because they are slow acting and are not sufficiently sensitive for most applications. Temperature indicating means 8 will be of any conventional form and type that is adapted to indicate and/or record the temperature of the temperature sensing means. In the case of thermometers, means 8 will be the upper portion of the thermometer containing the required temperature markings While temperature sensing means 7 will be the bulb of the thermometer.
The various parts of the analyzer may be constructed of any material which will withstand the temperatures and pressures under which it is to be used and which is substantially inert to the binary fluid mixture to be analyzed under those conditions. Suitable materials include brass, copper, steel, stainless steel, nickel, Monel, Inconel, aluminum, polytetrafluoroethylene, polyethylene and the like.
Examples The following examples, illustrating the novel method and analyzing device disclosed herein for determining the composition of binary vaporizable fluid mixtures of known components, are given without any intention that the invention be limited thereto. All percentages are by weight.
EXAMPLE 1 Various samples of mixtures containing trichlorofluoromethane and dichlorodifluoromethane (DCDFM) were analyzed on four separate but identical analyzing devices similar to the device illustrated in FIG. 2 with the pressure regulator maintaining a pressure of 8 p.s.i.g. and the expansion chamber at atmospheric pressure. Samples were charged to the analyzers continuously at their own vapor pressure at 25 C. until equilibrium was established as indicated by a constant temperature reading. The following recorder readings were obtained and the corresponding DCDFM contents were determined from a calibration curve based on a series of samples.
TABLE I Percent Recorder Deviation from DCDFM Analyzer reading, actual percent in sample used mieroamperes 87. 0 +0. 25 85. 8 0. 35 86. 8 +0. 15 86. 2 0. 15 48. 7 +0. 06 47. 4 0. 49. 0 +0. 30 49. 5 +0. 14. 0 O. 47 15. 5 +0. 53 13. 7 0. 70 13. 8 -0. 1 92. 0 0. 30 1 94. 0 +0. 1 91. 8 0. 40 1 91. 0 O. 1 56. 5 +1. 40 1 53. 0 0. 35 l 51. 8 0.
1 A high range measuring Wheatstone bridge was used.
9 EXAMPLE 2 TABLE II Recorder Apparent Initial sample reading, percent; pressure, p.s.i. g. microemperes D C DFM EXAMPLE 3 TABLE III I: Recorder Apparen Initial sample reading, percen temp., O. microamperes DCDFM The average deviation of apparent dichlorodifluoromethane analysis was only 510.3%. This is to be compared with a 6% error observed for a 10 C. change in the anlayzer device illustrated in FIG. 1 of the Felton and Williams patent.
EXAMPLE 4 Five 145-lb. cylinders were filled with mixtures of dichlorodiflu'oromethane and 1,2-dichloro 1,1,2,2 tetrafluoroethane (DCTFE) in 10:90, 25:75, 50:50, 75:25 and 90: 10% ratios. These mixtures were run through the analyzing device illustrated in FIG. 2 until the recorded voltage output on the Wheatstone bridge became constant. The pressure regulator was set to maintain a pressure of 8 p.s.i.g. and the pressure in the expansion chamber was essentially atmospheric. The temperatures in the cylinders ranged from to 30 C. and the initital pressures ranged from 10 to 100 p.s.i.g. The following data were obtained:
TABLE IV Percent DCTFE Recorder reading,
in sample: volts DC.
1 A high range Wheatstone bridge was used.
When the percent 1,2-dichloro-1,1,2,2-tetrafluoroethane is graphically plotted against the recorder reading in volts, a straight line curve is obtained in spite of the variations in temperature and pressure.
EXAMPLE 5 Three 145-lb. cylinders were filled with mixtures of dichlorodifluoromethane (DCDFM) and isobutane in 25:75, :70 and :65% ratios. These mixtures were run through the analyzing device illustrated in FIG. 2 until the recorded voltage output on the Wheatstone bridge became constant. The pressure regulator was set to maintain a pressure of 8 p.s.i.g. The temperatures in the cylinders ranged from 20 to 30 C. and the initial pressures ranged from 70 to 150 p.s.i.g. The following data were obtained.
TABLE V Percent DCDFM in sample:
Recorder reading,
volts,D.C.
When the percent dichlorodifluoromethane is graphically plotted against the recorder reading in volts, a straight line curve is obtained in spite of the variations in temperature and pressure.
Although the invention has been described and exemplified by way of specific embodiments, it is to be understood that it is not limited thereto. As will be apparent to those skilled in the art, numerous modifications and variations in the composition of the samples, the condi tions of the analysis and the details of the analyzing devices illustrated above may be made without departing from the spirit of the invention or the scope of the fol- 35 lowing claims.
The embodiments of the invention in which an exclusive property or privilege is claimed are defined as follows:
1. A method for determining the composition of a binary vaporizable fluid mixture of known components which comprises:
(a) regulating the pressure of a stream of the binary vaporizable fluid mixture so that it flows at a constant pressure,
(b) passing the mixture at a constant pressure through the first side of a heat exchanger,
(0) rapidly reducing the pressure of the mixture thereby expanding and cooling the mixture,
(d) measuring the temperature of the mixture just after expansion,
(e) passing the expanded mixture through the second side of the heat exchanger,
said steps being carried out continuously until the temperature just after expansion remains substantially constant, and
(f) comparing this temperature with the temperatures recorded for a series of similarly expanded binary fluid mixtures of the same components of known varying composition.
2. The method of claim 1 which comprises:
(a) passing the mixture through a pressure regulator which passes the mixture at a constant pressure of at least 8 p.s.i.g.,
(b) passing the mixture from the pressure regulator through the first side of the heat exchanger wherein the temperature of the fluid is reduced,
(c) passing the mixture from the first side of the heat exchanger through a constricted orifice into an expansion chamber containing a body of liquid binary fluid mixture, thereby rapidly reducing the pressure of the mixture at least 8 p.s.i. under substantially adiabatic conditions with a resulting expansion and cooling of the mixture, said expanded mixture discharging from the orifice below the surface of the body of liquid,
(d) measuring the temperature of the body of liquid,
(e) passing the expanded mixture through the other side of the heat exchanger whereby the incoming mixture is cooled to approximately its boiling point at the pressure after the orifice, and
(f) comparing the measured temperature of the body of liquid within the temperatures recorded for a series of similarly expanded binary fluid mixtures of the same components of known varying composition.
3. The method of claim 2, in which the incoming binary fluid mixture is initially at a pressure of 8 to 2,000 p.s.i.g., and is regulated to a constant pressure of 8 to 12 p.s.i.g., the constricted orifice has a diameter of 0.001 to 0.05 inch, and the pressure after the constricted orifice is substantially atmospheric.
4. An analyzing device for determining the composition of binary vaporizable fluid mixtures of known components which comprises:
(a) an inlet for passing the binary vaporizable fluid mixture into the device,
(b) a pressure regulator connected to said inlet which passes the mixture at a constant pressure,
(c) a heat exchanger having the inlet to the first side connected to the pressure regulator,
(d) a pressure reducing means connected to the outlet from said first side of the heat exchanger, said pressure reducing means causing a rapid pressure reduction as the binary fluid mixture passes therethrough,
(e) temperature sensing means positioned just after the pressure reducing means so as to measure the temperature of the mixture just after it passes through the pressure reducing means,
(f) means for connecting the pressure reducing means to the second side of the heat exchanger, and
(g) an outlet connected to said second side of the heat exchanger for removing the mixture from the device.
5. The analyzing device of claim 4 in which the pressure reducing means is a constricting orifice which causes a rapid pressure reduction of at least 8 p.s.i., said orifice being connected to an expansion chamber having an overflo-w outlet for retaining a body of liquid mixture, said orifice discharging binary fluid mixture in the expansion chamber below the level of the overflow outlet, and the temperature sensing means is positioned in the expansion chamber below the level of the overflow outlet and includes means extending outside the extension chamber for indicating the temperature.
6. The analyzing device of claim 5 in which the pressure regulator maintains a constant pressure of 8 to 12 p.s.i.g., and the constricting orifice has a diameter of 0.001 to 0.05 inch.
References Cited UNITED STATES PATENTS 2,429,474 10/1947 McMahon 73-29 3,221,541 12/1965 Osborne 7361.1 3,264,862 8/1966 Felton 73-25 3,273,356 10/1966 Hoffman -66 X 3,048,021 8/1962 Coles .Q 62-514 X 3,354,052 11/1967 Williams 73-25 X FOREIGN PATENTS 1,064,210 4/1967 Great Britain.
RICHARD C. QUEISSER, Primary Examiner C. E. SNEE III, Assistant Examiner
US670054A 1967-09-25 1967-09-25 Method of analyzing binary fluid mixtures and device therefor Expired - Lifetime US3535915A (en)

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
US67005467A 1967-09-25 1967-09-25

Publications (1)

Publication Number Publication Date
US3535915A true US3535915A (en) 1970-10-27

Family

ID=24688791

Family Applications (1)

Application Number Title Priority Date Filing Date
US670054A Expired - Lifetime US3535915A (en) 1967-09-25 1967-09-25 Method of analyzing binary fluid mixtures and device therefor

Country Status (1)

Country Link
US (1) US3535915A (en)

Cited By (6)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
EP0070188A2 (en) * 1981-07-13 1983-01-19 Atlantic Richfield Company An analyzer for distillable materials
US5158747A (en) * 1991-04-26 1992-10-27 Spx Corporation Apparatus for identifying and distinguishing different refrigerants
US5392639A (en) * 1993-06-17 1995-02-28 Spx Corporation Apparatus and method for identifying and distinguishing different refrigerants
US5580793A (en) * 1994-02-03 1996-12-03 Linde Aktiengesellschaft Process and device for determining the para content of a hydrogen gas stream
WO2012123641A1 (en) * 2011-03-17 2012-09-20 Rami Hakala Method and apparatus for gas analysis
US20150293002A1 (en) * 2012-10-25 2015-10-15 Carrier Corporation Method of measuring concentrations of gas mixtures

Citations (7)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US2429474A (en) * 1945-04-25 1947-10-21 Little Inc A Apparatus for determining the vapor content of a gas
US3048021A (en) * 1959-02-17 1962-08-07 Itt Joule-thomson effect gas liquefier
US3221541A (en) * 1961-12-20 1965-12-07 Entroputers Inc Method of and apparatus for accurately and instantaneously determining the ratio of the constituents of a vapor-liquid-solid mixture or a mixture of any two of the components thereof
US3264862A (en) * 1963-09-25 1966-08-09 Du Pont Process and device for analyzing binary fluid mixtures
US3273356A (en) * 1964-09-28 1966-09-20 Little Inc A Heat exchanger-expander adapted to deliver refrigeration
GB1064210A (en) * 1964-10-22 1967-04-05 British Petroleum Co Detector adapted to respond to changes in the composition of a gas stream
US3354052A (en) * 1964-05-18 1967-11-21 Texaco Inc Apparatus for distilling and controlling proportion of components of a mixture

Patent Citations (7)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US2429474A (en) * 1945-04-25 1947-10-21 Little Inc A Apparatus for determining the vapor content of a gas
US3048021A (en) * 1959-02-17 1962-08-07 Itt Joule-thomson effect gas liquefier
US3221541A (en) * 1961-12-20 1965-12-07 Entroputers Inc Method of and apparatus for accurately and instantaneously determining the ratio of the constituents of a vapor-liquid-solid mixture or a mixture of any two of the components thereof
US3264862A (en) * 1963-09-25 1966-08-09 Du Pont Process and device for analyzing binary fluid mixtures
US3354052A (en) * 1964-05-18 1967-11-21 Texaco Inc Apparatus for distilling and controlling proportion of components of a mixture
US3273356A (en) * 1964-09-28 1966-09-20 Little Inc A Heat exchanger-expander adapted to deliver refrigeration
GB1064210A (en) * 1964-10-22 1967-04-05 British Petroleum Co Detector adapted to respond to changes in the composition of a gas stream

Cited By (10)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
EP0070188A2 (en) * 1981-07-13 1983-01-19 Atlantic Richfield Company An analyzer for distillable materials
US4427305A (en) 1981-07-13 1984-01-24 Atlantic Richfield Company Analyzer for distillable materials
EP0070188A3 (en) * 1981-07-13 1984-08-01 Atlantic Richfield Company An analyzer for distillable materials
US5158747A (en) * 1991-04-26 1992-10-27 Spx Corporation Apparatus for identifying and distinguishing different refrigerants
DE4213270A1 (en) * 1991-04-26 1992-10-29 Spx Corp DEVICE FOR IDENTIFYING AND DISTINATING DIFFERENT REFRIGERANTS
US5392639A (en) * 1993-06-17 1995-02-28 Spx Corporation Apparatus and method for identifying and distinguishing different refrigerants
US5580793A (en) * 1994-02-03 1996-12-03 Linde Aktiengesellschaft Process and device for determining the para content of a hydrogen gas stream
WO2012123641A1 (en) * 2011-03-17 2012-09-20 Rami Hakala Method and apparatus for gas analysis
US20150293002A1 (en) * 2012-10-25 2015-10-15 Carrier Corporation Method of measuring concentrations of gas mixtures
US9574982B2 (en) * 2012-10-25 2017-02-21 Carrier Corporation Method of measuring concentrations of gas mixtures

Similar Documents

Publication Publication Date Title
Kay Vapor-liquid equilibrium relations of binary systems. Propane-n-alkane systems. n-Butane and n-pentane
Rogalski et al. Ebulliometers modified for the accurate determination of vapour—liquid equilibrium
Lerol et al. Accurate measurement of activity coefficient at infinite dilution by inert gas stripping and gas chromatography
Price et al. Low Temperature Vapor-Liquid Equilibrium in Light Hydrocarbon Mixtures: Methane-Ethane-Propane System.
Rizvi et al. Vapor-Liquid equilibria in the ammonia-water system
Goellner et al. Thermodynamic properties of liquid 3 He-4 He mixtures near the tricritical point. I. Vapor pressure measurements and their thermodynamic analysis
US3264862A (en) Process and device for analyzing binary fluid mixtures
US3535915A (en) Method of analyzing binary fluid mixtures and device therefor
Srivastava et al. Mutual diffusion of pairs of rare gases at different temperatures
Douslin et al. The Pressure-Volume-Temperature Properties of Fluorobenzene1
Hämeri et al. Homogeneous nucleation in a laminar flow diffusion chamber: The operation principles and possibilities for quantitative rate measurements
Burfield et al. Vapor‐liquid equilibria and dielectric constants for the helium‐carbon dioxide system
Guillevic et al. Vapor-liquid equilibrium measurements up to 558 K and 7 MPa: a new apparatus
Fredenslund et al. An apparatus for accurate determinations of vapour-liquid equilibrium properties and gas PVT properties
Walker et al. Precision Thermal‐Conductivity Gas Analyzer Using Thermistors
Butcher et al. An apparatus for determining high‐pressure liquid‐vapour equilibrium data. I. The methanol—ethanol system
Rouquerol et al. Suggested practice for classification of calorimeters
Price et al. The determination of thermodynamic properties of polymer solutions by finite-concentration gas chromatography
Warowny Volumetric and Phase Behavior of Acetonitrile at Temperatures from 363 to 463 K
Masi Survey of Experimental Determinations of Heat Capacity of Ten Technically Important Gases
US3515001A (en) Instrument for measuring the adiabatic saturation temperature (thermodynamic wet-bulb temperature) of a vapor-gas mixture
Yamamoto et al. Method for calibration of nuclear magnetic resonance standard samples for measuring temperature
US3229502A (en) Gas condensation pressure analyzer
US5097698A (en) Detection method for determining phase boundaries
Prydz et al. Properties of Fluorine along the Vapor–Liquid Coexistence Boundary