System for determining the content of at least one impurity in a cryogenic liquid

Abstract

System for determining the content of at least one impurity in a cryogenic liquid The present invention relates to a system (2) for determining the content of at least one impurity in a cryogenic liquid, comprising: a capacity (3) capable of receiving an initial volume of the cryogenic liquid, means (84) for vaporizing the initial volume of cryogenic liquid until a volume of residual cryogenic liquid is obtained in which the impurity is concentrated, the vaporization means being arranged in the lower part of the capacity (3), and means for determining the content of the impurity in the residual cryogenic liquid, the determination system (2) being characterized in that the vaporization means (84) comprise a heating surface capable of vaporizing the cryogenic liquid, the vaporization means being configured to keep said heating surface wet with the volume of residual cryogenic liquid (84). Abstract figure: Figure 2

Description

Title of the invention: System for determining the content of at least one impurity in a cryogenic liquid

[0001] The present invention relates to the chemical industry and concerns a system for determining the content of at least one dissolved impurity in a cryogenic liquid, for example taken from an air gas separation system, as well as a corresponding determination method.

[0002] An air gas separation system comprises low and medium pressure distillation columns for separating the various constituents of the air. Although the air is purified before being admitted to the columns, impurities remain in the air fed to the columns and are concentrated in particular in an oxygen vaporizer in one of the columns. Indeed, most of these impurities have a liquid / vapor equilibrium coefficient such that almost all of these impurities remain present in the liquid phase of the vaporizer, with an infinitesimal portion of the impurities leaving the vaporizer in the gas phase. The impurity content in the liquid phase therefore increases as the vaporizations progress and ends up accumulating in the form of a liquid or solid deposit in the aluminum matrix of the vaporizer.

[0003] Adsorption processes, implemented before distillation, make it possible to remove heavy hydrocarbons, i.e. those with more than four carbon atoms, as well as hydrocarbons containing unsaturated bonds, from the air fed to the columns. The impurities which are not or only slightly stopped by these adsorption processes are in particular light hydrocarbons and propane. Light hydrocarbons with one or two carbon atoms are highly soluble in oxygen, and therefore do not create a pure phase which can react with oxygen in the vaporizer. However, propane is relatively poorly soluble in oxygen and can therefore create a pure phase whose contact with liquid oxygen in the vaporizer can generate an explosive situation, in particular when the energy released by this impurity is sufficient to start the combustion of the aluminum vaporizer matrix.

[0004] Furthermore, even when the impurity present in the vaporizer is not reactive with oxygen, it accelerates the accumulation phenomenon of all other impurities, therefore also impurities reactive with oxygen. This is particularly the case for carbon dioxide and nitrous oxide, whose solidification temperature is higher than the operating temperature of liquid oxygen. These impurities may not be stopped by the adsorption processes and create a solid phase in liquid oxygen from the vaporizer, which can clog the vaporization channels of the vaporizer. This mechanism, called "dead end boiling" or "dead-end boiling", accelerates the concentration of all the impurities contained in the vaporizing liquid, particularly hydrocarbons, and therefore increases the risk of combustion of the vaporization matrix.

[0005] It is therefore necessary to monitor the content of impurities entering the distillation columns and / or the oxygen bath of the vaporizer in order to maintain acceptable limit quantities of impurities and to ensure the operational safety of the air gas separation system.

[0006] One difficulty to overcome is that the levels of impurities to be measured are extremely low, given the very low solubilities and liquid / vapor equilibrium coefficients of these impurities, in particular for carbon dioxide and nitrous oxide. In order to be able to control acceptable limit quantities of impurities, it is necessary to measure levels of less than 100 ppb (parts per billion), and preferably between 10 and 50 ppb. These measurements can be continuous or carried out at a frequency allowing intervention well before reaching a critical level of impurities.

[0007] Currently, the techniques for determining the impurity content in the air to be distilled or in the oxygen in the vaporizer use complex devices and require significant operational skill. These techniques use gas analyzers only, which requires sampling the cryogenic liquid entering the distillation columns or the vaporizer, and vaporizing it in specific equipment so that it can then be analyzed. Preferably, the sampling is carried out at the inlet of the vaporizer, or at the outlet of the vaporizer, or even between different vaporization stages if necessary, given that the vaporizer is a critical point in the air gas separation system.

[0008] These prior art techniques include a complete vaporization of the sample with its impurities to obtain a gas to be analyzed, in which the impurity content is identical to the impurity content in the cryogenic liquid sample, the vaporization being carried out under conditions preventing an accumulation of impurities in the sampling device or vaporization of the sample, so as not to distort the measurements of the gas analyzer.

[0009] In order to facilitate the measurement of the impurity content in the cryogenic liquid, the inventors have designed an apparatus and a method for analyzing this content, described in documents FR3066596 and FR3066597. The apparatus allows the vaporization of a large quantity of a sample of cryogenic liquid to be analyzed in a capacity, the gas thus vaporized being evacuated in an open circuit, a residual quantity of cryogenic liquid in which the impurities of the sample have concentrated, being retained at the end of this vaporization. Then the capacity is kept closed and the residual quantity of cryogenic liquid is completely vaporized in the capacity, so as to obtain a gas with a much higher impurity content than that of the initial sample, therefore easier to measure by a gas analyzer.

[0010] This innovative approach requires that the impurities whose concentration is to be measured are less volatile than the cryogenic liquid in which they are present, but also that the quantity of impurities evaporating during open circuit vaporization is negligible compared to the quantity of impurities remaining in the residual cryogenic liquid. These conditions depend on the thermodynamic equilibrium values ​​between the impurities and their solvent, which themselves depend on the vaporization temperature and pressure. The lower the vaporization pressure, the more favorable the vaporization is for the concentration of impurities in the residual cryogenic liquid.

[0011] Based on these thermodynamic equilibrium values, the concentration of impurities in the residual cryogenic liquid should not pose a problem. Indeed, according to these values, when the residual cryogenic liquid is oxygen maintained at 15 bars, the quantity of nitrous oxide, or carbon dioxide, or propane, escaping as vapor during vaporization in an open circuit, remains less than 2% of the quantity of impurities remaining in the cryogenic liquid.

[0012] However, the inventors have found that the quantity of impurities escaping into the gas phase during open circuit vaporization can in reality be much greater when the vaporized cryogenic liquid has areas over-concentrated in impurities, or when dry vaporization of the cryogenic liquid takes place on the wall of the apparatus which transmits the heat of vaporization. In particular, if this wall is overheated, the thermodynamic equilibrium is shifted and the quantity of impurities escaping into the gas phase is greater. To avoid such overheating, the concentration of impurities can be done at a pressure higher than atmospheric pressure, but this does not prevent the formation of areas over-concentrated in impurities in the liquid.

[0013] It should be noted that the techniques of the prior art proposing total vaporization of a sample of cryogenic liquid do not allow the cryogenic liquid to be vaporized at bubble temperature without it vaporizing locally dry on a part of the heating wall of the vaporization device, and causing a deposit of impurities on this heating wall, which charges the gas formed by vaporization with impurities.

[0014] Finally, another difficulty with the approach proposed by the inventors is that to significantly concentrate the impurities in the residual cryogenic liquid, with a concentration factor greater than or equal to 100, it is necessary to vaporize in the circuit open 99% of the cryogenic liquid sample, which makes it difficult not to have a heating wall dry vaporizing the cryogenic liquid during this open circuit vaporization step. This is all the more difficult since to ensure the safety of the air gas separation system, the duration of an analysis cycle is limited to less than one hour. Indeed, the analysis device proposed by the inventors operates in cycles during which the capacity in which the sample is to be vaporized, must, after vaporization of all the residual cryogenic liquid and its sending to a gas analyzer, be cooled to accommodate another sample.

[0015] The present invention aims to remedy at least in part the aforementioned drawbacks by providing a system and a method for determining the content of at least one impurity in a cryogenic liquid, as well as a system for separating gases from air, which make it possible to concentrate the impurity in a portion of the liquid before vaporizing this portion of liquid and sending the vapor thus produced into a gas analyzer, with a concentration factor which is not distorted by excessive vaporization of the impurities during the concentration of the impurity in the portion of the cryogenic liquid.

[0016] To this end, the invention proposes a system for determining the content of at least one impurity dissolved in a cryogenic liquid, the at least one impurity being less volatile than the cryogenic liquid, comprising: • a capacity capable of receiving an initial volume of cryogenic liquid, • means of vaporizing the initial volume of cryogenic liquid up to obtaining a volume of residual cryogenic liquid in which the impurity is concentrated, the vaporization means being arranged in the lower part of the capacity and comprising a heating surface capable of vaporizing the cryogenic liquid, and • means of determining the impurity content of the residual cryogenic liquid,

[0017] the determination system being characterized in that the vaporization means comprise at least one cryogenic liquid inlet duct and a plurality of cryogenic liquid outlet ducts, the vaporization means being capable of producing a thermosiphon effect between the inlet duct and the plurality of outlet ducts, the heating surface comprising the internal surfaces of the outlet ducts.

[0018] In other words, the vaporization means are configured to keep said heating surface wetted by the volume of residual cryogenic liquid.

[0019] Thanks to the invention, the vaporization of the initial volume of cryogenic liquid making it possible to concentrate the impurity in the volume of residual cryogenic liquid, done without the impurity escaping significantly into the gas phase during this vaporization. Indeed, the heating surface of the vaporization means which allows this vaporization is entirely submerged or entirely wetted by the volume of residual cryogenic liquid. There is therefore no dry vaporization of the cryogenic liquid which could create deposits on this heating surface. This is defined as allowing the vaporization of the cryogenic liquid, therefore releasing heat allowing this vaporization. Other surfaces of the vaporization means can be relatively hot compared to the cryogenic liquid without allowing vaporization thereof. The heating surface is for example arranged in the lower part of the capacity.

[0020] The thermosiphon effect, produced by the vaporization means, makes it possible to agitate the cryogenic liquid and therefore to avoid the formation of zones over-concentrated in impurities in the cryogenic liquid, which also avoids excessive vaporization of these impurities.

[0021] In the invention, the discharge conduits are those which allow the vaporization of the cryogenic liquid, their internal surface heating the cryogenic liquid to a temperature allowing this vaporization. The vaporization means are for example arranged in a lower part of the capacity so as to at least partially submerge the discharge conduits in the volume of residual cryogenic liquid by the effect of gravity, the internal surface of the discharge conduits even not submerged by the residual cryogenic liquid, remaining wet by the circulation of residual cryogenic liquid in the discharge conduits due to the thermosiphon effect.

[0022] In one embodiment, the discharge conduits surround, for example, the inlet conduit. In addition, the discharge conduits are preferably smaller in diameter than the inlet conduit. By thus distributing the cryogenic liquid in small-diameter discharge conduits, its evaporation is facilitated and their heating surface is kept wet. The inlet and discharge conduits preferably have a circular section and the inlet conduits are preferably angularly uniformly distributed around the inlet conduit.

[0023] The vaporization means comprise, for example, a thermally conductive body in the overall shape of a cylinder hollowed out in its height by the inlet and outlet conduits, which open onto a face of the body delimiting a lower part of the capacity.

[0024] The lower part of the capacity forms for example a portion of the lower part of the capacity, of the same surface as the face of the body, corresponding to a base of its cylindrical shape. This face is therefore flat if we disregard the orifices of the conduits opening onto this face. This is flush for example with the lower part of the capacity, in order to allow the evaporation means to collect by gravity the entire volume of residual cryogenic liquid, forming for example one percent or less than one percent of the initial volume of cryogenic liquid. The conduits are therefore arranged vertically relative to the ground, the face delimiting the lower part of the capacity being arranged horizontally.

[0025] The thermally conductive body is a good thermal conductor, for example made of copper or aluminum and preferably forming a single piece. The surface of this body is for example smooth or textured, in particular the internal surfaces of the exhaust ducts have for example a surface which improves the vaporization exchange coefficient and / or the wetting of the wall by its roughness, its texturing geometry, the presence of micro-fins or other means.

[0026] Preferably, the body comprises a thermally insulating jacket arranged between the intake duct and the exhaust ducts. Thus the cryogenic liquid in the intake duct remains cold enough not to vaporize there and form deposits on the internal surface of the intake duct. This insulating jacket is for example made of polytetrafluoroethylene (also called “Teflon®”).

[0027] The vaporization means comprise in particular at least one electric heating member arranged in a recess of the body proximal to the discharge ducts. This heating member is for example a heating resistor or a heating cartridge, arranged between the intake duct and the discharge ducts, or around the discharge ducts.

[0028] Preferably, the vaporization means comprise several electric heating members in the form of heating cartridges, the body comprising spaces arranged around the discharge conduits and housing the heating cartridges, the spaces not opening onto the face of the body delimiting the lower part of the capacity. These spaces extend parallel to the discharge conduits, at a distance from them in the thermally conductive body, but close enough to maintain the internal surfaces of the discharge conduits at a temperature allowing the vaporization of the cryogenic liquid. They are preferably arranged uniformly angularly around the discharge conduits.

[0029] The spaces are for example separated by recesses on the circumference of the body, over at least part of the height of the body. These recesses limit the mass of the body to be heated by the heating cartridges during the vaporization of the cryogenic liquid, but also the mass of the body to be cooled during a subsequent step aimed at bringing the walls of the capacity to a filling temperature. This subsequent step is necessary to carry out a new determination of the impurity content in a new initial volume of cryogenic liquid, which must be able to be evaluated accurately when it fills the capacity.

[0030] The recesses between the spaces housing the heating cartridges give by example a barrel shape with a body in the overall shape of a cylinder, opening onto the external cylindrical wall of the body. They allow a reduction in the cost of the determination system according to the invention.

[0031] The body comprises a face opposite the face delimiting the lower part of the capacity and the vaporization means comprise in particular a collector arranged on the opposite face, the collector fluidly connecting the intake duct with the discharge ducts. This collector is for example a copper part attached to the opposite face of the body, comprising a fluid circulation chamber. The collector being arranged vertically under the body, it is always filled with residual cryogenic liquid and therefore does not allow the formation of deposits of impurities.

[0032] In order to cool the capacity between two vaporization steps of two separate determinations according to the invention, a casing surrounds the vaporization means, the casing being configured to contain a cooling liquid coming into contact with the vaporization means. Of course, other cooling means are conceivable.

[0033] The envelope is for example an annular envelope surrounding at least the lower part of the capacity, the latter being for example a cylindrical tank.

[0034] Preferably, the opposite face opens out of the casing, the intake and exhaust ducts extending from the face delimiting the lower part of the capacity, through the casing. Thus, the supply of the heating member(s) is facilitated. The opposite face comprises, for example, orifices for inserting the heating cartridges into the spaces. The installation and replacement of these cartridges are thus also facilitated.

[0035] The invention also relates to a system for separating air gases by cryogenic distillation comprising a system for determining the content of at least one impurity dissolved in a cryogenic liquid according to the invention, means for sampling fluid circulating in the separation system, means for liquefying the sampled fluid if it is gaseous, and means for sending the sampled fluid, possibly liquefied, into the capacity to determine its content of the impurity.

[0036] Of course, the system and the method for determining the content of at least one dissolved impurity in a cryogenic liquid of the invention are applicable to other systems, for example to a system for separating another type of gas, from which one would like to separate, for example, carbon dioxide.

[0037] The invention also relates to a method for determining the content of at least one impurity dissolved in a cryogenic liquid, the at least one impurity being less volatile than the cryogenic liquid, using the system for determining the content of at least one impurity according to the invention and comprising steps of: • filling the capacity with the initial volume of cryogenic liquid, maintained at a filling pressure and temperature preventing vaporization of the cryogenic liquid during this filling step, • vaporization of the cryogenic liquid until the volume of residual cryogenic liquid is obtained by the vaporization means bringing the cryogenic liquid to its vaporization temperature at the pressure of the cryogenic liquid during this vaporization step, this pressure being less than or equal to the filling pressure, the gas resulting from the vaporization being evacuated from the capacity, and • determination of the impurity content in the residual cryogenic liquid.

[0038] The filling temperature and the filling pressure are included in temperature and pressure intervals respectively corresponding to a liquid state of the element or compound forming the cryogenic liquid. This is air in the liquid state or oxygen in the liquid state, depending on where the cryogenic liquid was taken from in the air gas separation system according to the invention. This sampling is in fact carried out for example at the inlet of the distillation columns of the air gas separation system, or at the inlet of an oxygen vaporizer in one of these columns, or at the outlet of the oxygen vaporizer, or even between different vaporization stages if necessary.

[0039] The vaporization step is carried out at atmospheric pressure or under controlled vacuum through a vacuum production system such as a vacuum pump or an ejector. For example, the pressure within the capacity during the vaporization step is brought to a value between 0.2 bars and 0.3 bars and preferably equal to 0.2 bars. This makes it possible to lower the vaporization temperature and consequently to further reduce the liquid / vapor equilibrium coefficients. In addition, this increases the temperature difference between the heating surface and the cryogenic liquid, which makes it possible to reduce the duration of the vaporization step.

[0040] The quantity of cryogenic liquid vaporized during the vaporization step is controlled so as to know precisely the concentration factor corresponding to the ratio between the initial volume of cryogenic liquid and the volume of residual cryogenic liquid. This can be done by monitoring the duration of the vaporization step as well as the temperature and pressure parameters during this vaporization step.

[0041] Then, the determination step involves sampling the residual cryogenic liquid and then vaporizing the sampled liquid into a gas, or else vaporizing all the residual cryogenic liquid into a gas, and then sending the gas obtained by vaporizing the sampled liquid or all the residual cryogenic liquid into a gas analyzer. Thus, the gas analyzer must detect a concentrated impurity content and has so no need to be very precise and very expensive.

[0042] In order to closely monitor the impurity content of the cryogenic liquid in the gas separation system according to the invention, the determination method according to the invention comprises a step of emptying the capacity, followed by a step of cooling the capacity by introducing into the casing of the determination system, a liquid at a temperature lower than or equal to the filling temperature of the cryogenic liquid. The emptying step follows the removal of the residual cryogenic liquid, or the sending of the gas obtained by vaporization of all the residual cryogenic liquid, so as not to disturb the determination of the impurity content carried out by the gas analyzer. Once cooled, the capacity can accommodate a new initial volume of cryogenic liquid taken from the air gas separation system, to carry out a new determination of the impurity content.

[0043] Other characteristics and advantages of the invention will become apparent from the following description on the one hand, and from several exemplary embodiments given for informational and non-limiting purposes with reference to the attached schematic drawings on the other hand, in which:

[0044] [Fig. 1] represents steps of a method for determining the content of at least an impurity dissolved in a cryogenic liquid according to the invention, in one embodiment of the invention,

[0045] [Fig.2] represents a system for determining the content of at least one impurity dissolved in a cryogenic liquid according to the invention, in one embodiment of the invention, the system comprising in particular a capacity and vaporization means shown in section in the lower part of the capacity,

[0046] [Fig.3] represents in perspective an element of the vaporization means represented on [Fig.2],

[0047] [Fig.4] is a perspective view of a section of the element of [Fig.3], and

[0048] [Fig.5] represents steps of a method for determining the content of at least an impurity dissolved in a cryogenic liquid according to the invention, in a variant of the embodiment of the invention shown [Fig.l].

[0049] According to an embodiment of the invention shown [Fig.l], a method 100 for determining the content of at least one dissolved impurity in a cryogenic liquid according to the invention is implemented by a system 2 for determining the content of at least one dissolved impurity in a cryogenic liquid shown [Fig.2], this system 2 being part of a system for separating air gases by cryogenic distillation according to the invention.

[0050] The at least one impurity whose content is determined is, for example, propane. The contents of impurities other than propane in the cryogenic liquid are well also preferably determined by the determination method 100, the determination system 2 allowing these multiple determinations. The impurities determined in this embodiment of the invention are less volatile than the cryogenic liquid.

[0051] This air gas separation system comprises means for sampling fluid circulating in the separation system. In this embodiment of the invention, it is assumed that these sampling means sample liquid oxygen at the inlet of an oxygen vaporizer of the gas separation system, this oxygen vaporizer being arranged in a distillation column of the gas separation system. The liquid oxygen thus sampled is sent to the determination system 2.

[0052] This comprises a capacity 3 in the form of a cylindrical tank, capable of containing liquid oxygen, and arranged vertically on feet not shown. The capacity 3 comprises a liquid inlet 32, a liquid outlet 34 and a gas outlet 36.

[0053] The liquid oxygen taken from the separation system is sent into the capacity 3, via the liquid inlet 32 ​​on the capacity 3, during a first step 110 of the determination method 100, which is a step of filling the capacity 3 with an initial volume of cryogenic liquid, i.e. here liquid oxygen.

[0054] This initial volume of cryogenic liquid is predetermined. In order to obtain it precisely, the capacity 3 is filled until the cryogenic liquid overflows from the capacity 3 through the liquid outlet 34, the position of which on the capacity 3 is determined so that the capacity 3 is filled with the predetermined initial volume of cryogenic liquid when it reaches the liquid outlet 34.

[0055] The height of the cryogenic liquid in capacity 3 is then hl. This height is measured vertically relative to the ground along a vertical axis Z.

[0056] During the filling step 110, the pressure and temperature of the cryogenic liquid prevent it from vaporizing. The temperature of the cryogenic liquid is notably lower than its vaporization temperature at the pressure to which it is subjected during this step.

[0057] The next step of the determination method 100 is a step 120 of vaporizing the cryogenic liquid until a volume of residual cryogenic liquid is obtained. In this step, the liquid inlet 32 ​​and outlet 34 on the capacity 3 are closed, while a gas outlet 36, arranged at the top of the capacity 3, is open. In fact, the cryogenic liquid transformed into vapor is evacuated during this vaporization step 120, through the gas outlet 36.

[0058] This vaporization is carried out by vaporization means 84 arranged in the lower part of the capacity 3, which bring the cryogenic liquid to its vaporization temperature, the vaporization pressure in the capacity 3 being drawn under vacuum until a pressure of approximately 0.2 bar absolute. Thanks to this low pressure, the vaporization temperature (or bubble temperature) is lower than at atmospheric pressure, which reduces the duration of the vaporization step 120. In addition, this low pressure reduces the liquid / vapor equilibrium coefficients, preventing a significant quantity of impurities from escaping into the gas phase.

[0059] The vaporization step 120 makes it possible to concentrate the impurities present in the initial volume of cryogenic liquid, in a volume of residual cryogenic liquid preserved at the end of the vaporization step 120. This volume of residual cryogenic liquid is predetermined by controlling the quantity of gas vaporized during this vaporization step 120, or by controlling the duration of this step and the temperature and pressure parameters in the capacity 3 during this vaporization step 120, or by measuring a variation in the level of liquid and / or mass in the capacity 3. In this way the concentration factor of the impurities in the volume of residual cryogenic liquid is determined precisely as the ratio between the initial volume of cryogenic liquid and the volume of residual cryogenic liquid.For information purposes, in this embodiment of the invention, the capacity 3 has a capacity of 1.3 liters and the initial volume of cryogenic liquid is 0.8 liters.

[0060] The vaporization means 84 are more particularly visible in [Fig. 3]. They comprise a copper body 4, generally in the form of a cylinder of height H. The body 4 is arranged along this height H vertically in the lower part of the capacity 3, so that a face 46 of the body corresponding to a base of the cylinder, is arranged horizontally and forms a lower part of the capacity 3. In other words, the bottom of the cylindrical tank forming the capacity 3 is constituted in part by the face 46 of the body 4, which is flush with the aluminum walls of the cylindrical tank.

[0061] An opposite face 48 of the body 4 corresponding to the other base of the cylinder, is therefore arranged horizontally proximal to the ground relative to the face 46 forming the lower part of the capacity 3.

[0062] The body 4 is traversed along its height by conduits 43 arranged vertically, namely an intake conduit 42, in the center of the body 4, and discharge conduits 44 surrounding the intake conduit 42. The discharge conduits 44 are of smaller diameter than the intake conduit 42. A copper collector 8 is attached to the opposite face 48 so as to provide fluid communication between the intake conduit 42 and the discharge conduits 44. The collector 8 is part of the vaporization means 84.

[0063] Of course, the lower part of the capacity 3 and the vaporization means 84 form sealed means for retaining the cryogenic liquid.

[0064] The vaporization means 84 also comprise heating cartridges housed in spaces 41 (visible [Fig.4]) arranged in the body 4 around the evacuation conduits 44. These spaces 41 extend parallel to the evacuation conduits 44 in the body 4, without opening onto the face 46 forming the lower part of the capacity 3. They however open onto the opposite face 48 in order to allow the insertion of the heating cartridges into these cavities 41 as well as the electrical supply of these heating cartridges.

[0065] Recesses 45 in the form of grooves, hollow out the cylindrical surface of the body 4 between the spaces 41, in particular in order to increase the heat exchange surface between the body 4 and a cooling liquid intended to circulate in a casing 5, surrounding the lower half of the capacity 3 and in particular a part of the vaporization means 84. More precisely, the casing 5 takes the form of an annular casing of which a first circular edge surrounds the body 4 by bordering the opposite face 48 and of which a second circular edge surrounds the capacity 3 slightly below the liquid outlet 34 on the capacity 3. The utility of this casing 5 will be described later.

[0066] The vaporization means 84 operate like a bath vaporizer with a thermosiphon effect in the discharge conduits 44. Indeed, during the vaporization step 120, the heating cartridges are powered, and bring the temperature of the cryogenic liquid present in the discharge conduits 44 to its vaporization temperature, allowing the vaporized oxygen to escape with very few impurities towards the gas outlet 36. A circulation is created due to the thermal flows, the cryogenic liquid circulating in the intake conduit 42 from the face 46 to the opposite face 48 of the body 4, then passing through the collector 8 to supply the discharge conduits 44 with cryogenic liquid.

[0067] This circulation allows good agitation and good homogeneity of the cryogenic liquid in the vaporization means 84 and in particular at the level of its heating surface formed by the internal surfaces of the evacuation conduits 44.

[0068] The vaporization means 84 are configured so that this heating surface is still submerged in the cryogenic liquid or wetted by it at the end of the evaporation step 120, when the volume of non-vaporized cryogenic liquid reaches the predetermined volume of residual cryogenic liquid. For information purposes, in this embodiment of the invention, the body 4 has a height H of 7 mm (millimeters), and the height h reached by the volume of residual cryogenic liquid in the capacity is not less than 50% of the height H of the body 4. The circulation operated by thermosiphon effect in the evacuation conduits 44 thus makes it possible to keep their internal surfaces wet.

[0069] In this way, the heating surface, which is a vaporization surface, transmits the vaporization heat without vaporizing dry even locally. There is no liquid / vapor interface on the heating surface since it is entirely wetted by the cryogenic liquid. No deposits of impurities can form there and the vapor escapes at thermodynamic equilibrium with a negligible amount of impurities compared to the amount of impurities remaining in the liquid phase.

[0070] In order not to transmit heat of vaporization to the cryogenic liquid in the intake duct 42, the internal surface of the latter is covered with a thermally insulating jacket 47, for example made of Teflon®.

[0071] Thanks to the heating cartridges and the good conductivity of the body 4, the heat flow in the vaporization means is controlled, which makes it possible to control the temperature of the heating surface. In particular, the body 4 makes it possible, through its material, to homogenize the temperature of the internal surfaces of the evacuation conduits 44.

[0072] These have a circular section in order to promote good wetting of their internal surfaces, which are smooth or textured, for example porous or having fins in order to improve the exchange coefficient, increase the heat flow and reduce the duration of this vaporization step 120. The low pressure applied in the capacity 3 makes it possible in particular to increase the temperature difference between the temperature of the heating surface and the vaporization temperature of the liquid without risking letting too large a quantity of impurities escape into the gas phase.

[0073] The configuration of the body 4 and in particular the arrangement of its conduits 43, makes it possible to have a heating surface that is always wetted and of large size although the volume of residual cryogenic liquid is very small.

[0074] As an indication, the thermal power of these vaporization means 84 makes it possible to vaporize 99% of the initial volume of cryogenic liquid, in less than 15 minutes.

[0075] At the end of the vaporization step 120, the gas outlet 36 is closed, the capacity being isolated and containing the predetermined volume of residual cryogenic liquid.

[0076] The next step is then a step 130 of determining the impurity content of the residual cryogenic liquid.

[0077] This determination step 130 comprises the vaporization 132 of the entire volume of residual cryogenic liquid, in the capacity 3 kept closed, then the sending 134 of the gas thus vaporized and concentrated in impurities, into a gas analyzer 6 (represented [Fig.2]). This determines the propane content of the gas, then this content is divided by the concentration factor to determine the propane content in the liquid oxygen taken from the air gas separation system. Of course the contents of other types of impurities can also be determined in this determination step 130, in the same way, in particular the nitrous oxide content and the carbon dioxide content in the liquid oxygen taken from the air gas separation system.

[0078] The next step is a step 140 of emptying the capacity 3, for example by sending a neutral gas free of impurities into the capacity 3. Alternatively, the gas remaining in the capacity is drawn under vacuum by an ejector or a vacuum pump.

[0079] Then the capacity 3 is cooled during a cooling step 150, during which a liquid at a temperature lower than or equal to the filling temperature of the cryogenic liquid is sent into the casing 5 via a liquid inlet 52 with which the casing 5 is provided in its lower part. This liquid is for example liquid oxygen. A gas outlet 56 in an upper part of the casing makes it possible to release a gaseous phase produced by evaporation of the liquid in the casing 5 in contact with the hot wall of the capacity 3.

[0080] Then the cooling liquid is evacuated from the casing 5 through an outlet 54 located in the lower part of the casing 5, and the determination system 2 is ready for a new implementation of the determination method 100.

[0081] A variant of the determination method 100 according to the invention is now presented in relation to [Fig.5], showing the steps of a determination method 200 according to the invention.

[0082] The determination method 200 according to the invention comprises steps 210 of filling the capacity 3 and 220 of vaporization of the cryogenic liquid, which are identical to the steps 110 of filling and respectively 120 of vaporization described previously.

[0083] In this variant, during a following step 230 of determining the impurity content of the residual cryogenic liquid, the entire volume of residual cryogenic liquid is not vaporized, but a predetermined volume of this volume of residual cryogenic liquid is taken 232, it is vaporized 234 entirely and it is sent 236 to the gas analyzer 6. The latter determines the impurity content in the same way as in the determination step 130.

[0084] This variant makes it possible to carry out a step 240 of emptying the capacity 3, in parallel with the vaporization of the cryogenic liquid sample in the separate capacity. During this emptying step 240, the cryogenic liquid remaining in the capacity 3 is for example vaporized and evacuated via the gas outlet 36 on the capacity 3.

[0085] Then the capacity 3 is cooled during a cooling step 250, identical to the cooling step 150 of the determination method 100. Once the cooling liquid has been evacuated from the casing 5, the determination system 2 is then ready for a new implementation of the determination method 200.

[0086] The invention is described in the context of a cryogenic liquid originating from air separation, such as oxygen, nitrogen or argon. It goes without saying that the invention applies to any cryogenic liquid, for example carbon dioxide, carbon monoxide, hydrogen, helium, methane, krypton, xenon, neon.

[0087] Of course, the invention is not limited to the examples which have just been described and Many adjustments can be made to these examples without departing from the scope of the invention. In particular, the characteristics of the different variant embodiments of the invention envisaged in this application can be combined to achieve the invention, to the extent that these variants are not incompatible with each other.

Claims

Claims

1. System for determining (2) the content of at least one dissolved impurity in a cryogenic liquid, the at least one impurity being less volatile than the cryogenic liquid, comprising: • a capacity (3) capable of receiving an initial volume of the cryogenic liquid, • means for vaporizing (84) the initial volume of cryogenic liquid until a volume of residual cryogenic liquid is obtained in which the impurity is concentrated, the vaporizing means being arranged in the lower part of the capacity (3) and comprising a heating surface capable of vaporizing the cryogenic liquid, and • means for determining the content of the impurity in the residual cryogenic liquid, the determination system (2) being characterized in that the vaporizing means (84) comprise at least one intake duct (42) for the cryogenic liquid and a plurality of discharge ducts (44) for the cryogenic liquid,the vaporization means (84) being capable of producing a thermosiphon effect between the inlet duct (42) and the plurality of discharge ducts (44), the heating surface comprising the internal surfaces of the discharge ducts (44).,

2. System for determining (2) the content of at least one dissolved impurity in a cryogenic liquid according to claim 1, in which the discharge conduits (44) surround the inlet conduit (42).

3. System for determining (2) the content of at least one dissolved impurity in a cryogenic liquid according to claim 1 or 2, in which the discharge conduits (44) are of smaller diameter than the inlet conduit (42).

4. System for determining (2) the content of at least one dissolved impurity in a cryogenic liquid according to any one of claims 1 to 3, in which the vaporization means (84) comprise a thermally conductive body (4) in the overall shape of a cylinder hollowed out in its height (H) by the inlet (42) and outlet (44) conduits, which open onto a face (46) of the body (4) de- limiting a lower part of the capacity (3).

5. System (2) for determining the content of at least one dissolved impurity in a cryogenic liquid according to claim 4, in which the body (4) comprises a thermally insulating jacket (47) arranged between the inlet duct (42) and the outlet ducts (44).

6. System for determining (2) the content of at least one dissolved impurity in a cryogenic liquid according to claim 4 or 5, in which the vaporization means comprise at least one electric heating member arranged in a recess of the body (4) proximal to the evacuation conduits (44).

7. System for determining (2) the content of at least one dissolved impurity in a cryogenic liquid according to claim 6, in which the vaporization means (84) comprise several electric heating members in the form of heating cartridges, the body (4) comprising spaces (41) arranged around the evacuation conduits (44) and housing the heating cartridges, the spaces (41) not opening onto the face (46) of the body (4) delimiting the lower part of the capacity (3).

8. System for determining (2) the content of at least one dissolved impurity in a cryogenic liquid according to claim 7, in which the spaces (41) are separated by recesses (45) on the circumference of the body (4), over at least part of the height (H) of the body (4).

9. System for determining (2) the content of at least one dissolved impurity in a cryogenic liquid according to any one of claims 4 to 8, in which the body (4) comprises a face (48) opposite the face (46) delimiting the lower part of the capacity (3) and the vaporization means (84) comprise a collector (8) arranged on the opposite face (48), the collector (8) fluidically connecting the intake duct (42) with the discharge ducts (44).

10. System for determining (2) the content of at least one dissolved impurity in a cryogenic liquid according to any one of claims 1 to 9, in which a casing (5) surrounds the vaporization means (84), the casing (5) being configured to contain a cooling liquid coming into contact with the vaporization means (84).

11. System for determining (2) the content of at least one dissolved impurity in a cryogenic liquid according to claims 9 and 10, in which the opposite face (48) opens out of the casing (5), the intake (42) and exhaust (44) conduits extending from the face (46) delimiting the lower part of the capacity (3), through the casing (5).

12. System for determining (2) the content of at least one dissolved impurity in a cryogenic liquid according to claim 11 taken in dependence on claim 7 or 8, in which the opposite face (48) comprises orifices for inserting the heating cartridges into the spaces (41).

13. System for separating air gases by cryogenic distillation comprising a system (2) for determining the content of at least one impurity dissolved in a cryogenic liquid according to any one of claims 1 to 12, means for sampling fluid circulating in the separation system, means for liquefying the sampled fluid if it is gaseous, and means for sending the sampled fluid, possibly liquefied, into the capacity (3) to determine its content of the impurity.

14. Method for determining (100, 200) the content of at least one dissolved impurity in a cryogenic liquid, the at least one impurity being less volatile than the cryogenic liquid, using the system for determining (2) the content of at least one impurity according to any one of claims 1 to 12 and comprising steps of: • filling (110, 210) the capacity (3) with the initial volume of cryogenic liquid, maintained at a filling pressure and temperature preventing vaporization of the cryogenic liquid during this filling step (110, 210), • vaporizing (120, 220) the cryogenic liquid until the volume of residual cryogenic liquid is obtained by the vaporizing means bringing the cryogenic liquid to its vaporization temperature at the pressure of the cryogenic liquid during this vaporization step (120, 220), this pressure being less than or equal to at the filling pressure,the gas resulting from the vaporization being evacuated from the capacity (3), and • determination of the content of the impurity (130, 230) in the residual cryogenic liquid.,

15. Method for determining (100, 200) the content of at least one dissolved impurity in a cryogenic liquid according to the preceding claim, in which the pressure within the capacity (3) during the vaporization step (120, 220) is brought to a value between 0.2 bars and 0.3 bars and preferably equal to 0.2 bars.

16. A method for determining (100, 200) the content of at least one dissolved impurity in a cryogenic liquid according to claim 14 or 15, wherein the determining step (230, 130) comprises sampling (232) the residual cryogenic liquid and then vaporizing (234) the sampled liquid into a gas, or else vaporizing (132) all the residual cryogenic liquid into a gas, and then sending (236, 134) the gas obtained by vaporizing the sampled liquid or all the residual cryogenic liquid, into a gas analyzer.

17. Method for determining (100, 200) the content of at least one dissolved impurity in a cryogenic liquid according to claim 16, using a determination system (2) according to any one of claims 10 to 12, comprising a step of emptying (240, 140) the capacity (3), followed by a step of cooling (250, 150) the capacity (3) by introducing into the casing (5) of the determination system (2), a liquid at a temperature lower than or equal to the filling temperature of the cryogenic liquid.

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