METHOD FOR ANALYZING TRACES OF CONTAMINANTS OF A CRYOGENIC LIQUID

Abstract

The invention relates to a method for analyzing the content of at least one contaminant in a cryogenic liquid, wherein a known amount of liquid L constituting the initial liquid is injected at the pressure P into an enclosure; a predetermined fraction of the liquid present in the enclosure is vaporized by heating same; the vapor thus generated is discharged from the vaporizing enclosure to maintain a pressure no higher than the pressure P during the vaporization phase; the amount of liquid thus vaporized, less than L, is precisely controlled so that the amount of contaminant in the residual liquid present in the enclosure is substantially equal to that of the initial liquid, which implies that the concentration thereof is multiplied by a previously determined factor; a sample of residual liquid is collected; the contaminant content is measured after total vaporization of the residual liquid sample; and the contaminant content in the initial liquid is deduced from the measurement of contaminant in the residual liquid.

Description

TECHNICAL FIELD OF THE INVENTION

The present invention relates to a method for analyzing traces of contaminants of a cryogenic liquid, i.e. a liquid that liquefies at a cryogenic temperature. The oxygen vaporizer of a unit for separating air by cryogenic distillation is the location where many impurities, contained in the feed air of the distillation columns, and that have not been able to be eliminated upstream, concentrate.

BACKGROUND OF THE INVENTION

Most impurities have a liquid/vapor equilibrium coefficient such that almost all of the impurity is present in the liquid phase, and an infinitesimal part is distributed in the gas phase. The content in the liquid phase therefore increases during the vaporization phases.

Furthermore, numerous studies have shown that the higher the content of an impurity in the liquid phase, the more this impurity accumulates in the form of a solid or liquid deposit in the aluminum vaporization matrix. Too high a concentration of impurities is therefore not acceptable because:

• • Either the impurity reacts directly with oxygen, and can give rise to situations with a high risk of explosion, in particular when the energy released by this reactive impurity is sufficient to start the combustion of the aluminum matrix. This is the case for hydrocarbons. Heavy hydrocarbons (C4+) or hydrocarbons having unsaturated bonds are well known to be stopped upstream of the distillation system by an adsorption process. Light saturated hydrocarbons (C1, C2) are stopped very little or not at all, but have a high solubility in liquid oxygen, which makes the presence of a virtually pure phase of hydrocarbons of this type very unlikely. The hydrocarbon that is well known to be the most critical is propane, taking into account an only partial stoppage in the adsorption systems, and its relatively low solubility in liquid oxygen. Thus, propane entering via the air can accumulate in the liquid oxygen bath until a content greater than its solubility limit is reached and can therefore generate a pure phase in contact with oxygen.
  • Or the impurity is not reactive, but accelerates the phenomenon of accumulation of all the other impurities, including those which are reactive. This is the case with compounds having a solidification point that is above the operating temperature of liquid oxygen. CO₂ and N₂O are the most critical compounds from this point of view because they can, unintentionally or intentionally, not be completely stopped by the adsorption system. Since they are then found in the oxygen, a solid phase is created and may plug the vaporization channels of the exchanger vaporizing the liquid oxygen. It is known that this mechanism, referred to as “dead end boiling” accelerates the concentration of all the impurities contained in the liquid being vaporized, and therefore the risk related to the hydrocarbons and to the combustion of the aluminum matrix is increased.

It is therefore necessary and critical to monitor the content of impurities in the air entering the distillation system and/or the oxygen bath in order to control the acceptable maximum amounts of impurities and to ensure the operating safety of the unit.

However, the degrees of purities to be analyzed are extremely low, given the very low liquid/vapor equilibrium coefficients of the constituents in the oxygen, in particular for N₂O and CO₂. In order to be able to evaluate and control the acceptable maximum amounts of impurities, it is necessary to measure contents of less than 100 ppb, preferentially of from 10 to 50 ppb. However, the measurement frequency may be low.

Current industrial analysis techniques for achieving these detection levels use complex devices and require significant operational expertise.

FR2797325 discloses a method for analyzing a liquid according to the prior art. According to this method, during a main step, a small flow of liquid (oxygen possibly loaded with impurities) continuously enters a chamber and is completely vaporized under a small difference in temperature.

At the same time, the vaporized oxygen is discharged continuously out of the chamber and the impurities are retained in the form of crystals or liquid inside the chamber. It is therefore a complete vaporization of the liquid oxygen in an open circuit.

This step must be long enough (several days continuously) so as to be able to deposit a significant amount of impurities that is sufficient to be able to be detected during the following step (increase to a higher temperature).

The amount of moles of impurities accumulated is determined in a next step by the pressure measurement of the chamber (during the increase in temperature in a closed circuit) and by the calculation of the number of moles in the chamber. The change in the pressure measured in the closed chamber gives the amount of material initially present in the liquid or solid phase. As a function of the temperatures at which the pressure changes take place, the nature of the body which vaporizes is known. In this step, the flow ofliquid was previously stopped and the impurities are previously concentrated in a gaseous oxygen atmosphere.

The determination of the nature of the impurities is spurious via this principle, in particular when there are several types of impurities.

Another way that is proposed is to wash the impurities with a solvent in order to perform an analysis. The drawback is the fact of diluting the impurities.

The determination of the nature of the impurities and the quantitative analysis of each impurity deposited is not possible:

• • without complete interruption of the various phases,
  • without a means of at least partial sampling of these impurities,
  • and without a means of analysis outside the proposed system.

SUMMARY OF THE INVENTION

One object of the invention is to provide an alternative for measuring contents of impurities in a cryogenic liquid, while using known analyzers that are simple to operate, the detection limit of which remains of the order of 1 ppm.

According to one subject of the invention, a method is provided for analyzing the content of at least one contaminant in a cryogenic liquid wherein:

a) a known amount of liquid L constituting the initial liquid is introduced at the pressure P into a chamber, previously brought to a temperature identical to or below the vaporization temperature at the pressure P of the liquid to be analyzed, so that no vaporization of the liquid occurs in this step a), characterized in that:

b) a given fraction of the liquid present in the chamber is vaporized by heating it, the vapor thus generated is discharged from the vaporization chamber to maintain a pressure equal to the pressure P, or preferably below the pressure P during the vaporization phase,

c) the amount of liquid thus vaporized, less than L, is precisely controlled, so that the amount of contaminant in the residual liquid present in the chamber is substantially equal to that in the initial liquid, which implies that its concentration is multiplied by a predetermined factor and

either

i. a sample of residual liquid is drawn off, and the content of contaminant is measured after complete vaporization of the sample of residual liquid

or

ii. the contaminant content of the residual liquid is measured by completely vaporizing the residual liquid with at least one contaminant contained therein, the vaporization chamber then being insulated from any inlet or outlet of material and then the content of contaminant in the vaporized residual liquid is analyzed

and

d) the content of contaminant in the initial liquid is deduced from the measurement of contaminant in the residual liquid.

According to other optional aspects that can be combined with one another in any logically consistent manner:

• • during step ii) the liquid is completely vaporized, thus increasing the pressure in the insulated and closed chamber and then the vapor generated is sent to an analyzer.
  • the vapor generated is heated to a temperature higher than the vaporization temperature of the contaminant at the pressure of the chamber before sending it to the analyzer.
  • the analyzer is capable of measuring a concentration of a contaminant of less than 10 ppm, or even 1 ppm, or even 0.1 ppm.
  • no liquid is introduced into the chamber during steps b), c) and i) or ii).
  • the pressure under which the partial vaporization of the liquid of step b) is carried out is at least 1 bar lower than the filling pressure P of the chamber.
  • the factor of step c) is at least essentially equal to the ratio of the initial and final material amounts, in terms of volume or mass, of the liquid, before and after the partial vaporization of step b).
  • the factor of step c) is calculated as a function of the ratio between the amount of vaporized liquid of step b) and L.
  • the factor of step c) is known by material balance between the initial amount of liquid introduced L and the sum of the amounts vaporized and amounts of residual liquid.
  • the chamber is insulated after step b).
  • the ratio between the volume (respectively mass) of liquid initially introduced L and the volume (respectively mass) of liquid present in the vaporization chamber at the time of the insulation is determined by counting the amount of material vaporized, or by counting the energy introduced into the vaporization exchanger by the heat source or else by measuring the variation of the liquid level and/or mass level in the chamber.
  • the fraction of step b) is greater than 10%, preferentially greater than 30%, or even greater than 90%.
  • the fraction of step b) is less than 100%.
  • the vaporization pressure of step b) and/or c) is less than 0.8 bar absolute.
  • the liquid originates from a unit for separating air by cryogenic distillation, being drawn off from the unit either in a liquid state or in a gaseous state, being in this case liquefied before being sent to the chamber.
  • the air separation unit comprises an adsorption purification unit and a system of columns for distilling a gas purified in the purification unit, the liquid being gas drawn off downstream of the purification unit and then liquefied.
  • the air separation unit comprises an adsorption purification unit and a system of columns for distilling a gas purified in the purification unit, the liquid being a bottom liquid from a column of the system or an intermediate liquid from a column of the system.
  • according to a step e) the chamber is cooled between step i) or ii) and step a) to bring the chamber to a temperature below the boiling point of the cryogenic liquid sent into the chamber.
  • the chamber is cooled by sending a portion of the cryogenic liquid into a space surrounding the chamber.
  • the cryogenic liquid of the space is not present during steps b) and/or c).
  • the process does not comprise a step of solidifying the cryogenic liquid.
  • the vaporization of step b) is carried out at atmospheric pressure or under vacuum.

The cryogenic liquid may be liquefied air, liquid oxygen, liquid nitrogen, liquid methane, liquid carbon monoxide, liquid helium, etc.

According to optional aspects of the present invention:

• • the entire known amount of liquid L constituting the initial liquid is introduced at the pressure P into a chamber, previously brought to a temperature identical to or below the vaporization temperature at the pressure P of the liquid to be analyzed, without being vaporized.
  • once the amount L of liquid has been sent to the chamber, the sending of liquid to the chamber stops.
  • the chamber is filled with cryogenic liquid, for example liquid oxygen, discontinuously.
  • this cryogenic liquid is liquid oxygen which is partially vaporized. The ratio between the initial amount of liquid. I, and the amount of liquid remaining defines a concentration factor of the liquid phase, if the equilibrium coefficients are very low (for example less than 100). At the same time, the vaporized (gaseous) oxygen is discharged out of the chamber and the impurities are kept inside the chamber.
  • the contaminants are previously and predominantly concentrated by a known factor in a volume of liquid oxygen.
  • in the next step, the remainder of concentrated liquid oxygen and the contaminants are vaporized in closed volume in order to be able to carry out the analysis of the impurities.
  • the volume of liquid available in the chamber and the contents of the vaporized contaminants are sufficient to be directly analyzed via the devices available on the production unit (ASU).
  • the total duration of a complete cycle is between 15 min and 40 min.
  • between each cycle, the impurities are discharged from the chamber and therefore are not kept.

For this, a known amount of liquid is partially vaporized, and it is the very low equilibrium coefficients of the contaminants in the liquid that will allow this concentration. The contaminant remains in the liquid phase as it is evaporated. Therefore, what could not be measured by a known analyzer because of very (excessively) low contents, will become measurable. The measurement of the content is therefore known not by the pressure variation during an iso-volume reheating, but by a direct analysis of a liquid concentrated by a controlled factor.

According to one variant the content of at least one contaminant in the concentrated liquid is measured by completely vaporizing the liquid and by significantly superheating the vapor thus formed beyond the vaporization temperature of the impurity to be analyzed, for example to at least 10° C. above the vaporization temperature, to be certain not to have residual traces of liquid that is highly concentrated in contaminants, and by analyzing the content of at least one contaminant in the vaporized phase.

However it is possible to want to measure the content of this concentrated liquid phase by a known sampling technique (for example one of those described in FR2858416 or FR2839153).

The main thing is therefore to have concentrated a known amount of liquid by controlled partial vaporization in order to be able to analyze what could not be analyzed, rather than to deduce the content by monitoring the change in pressure in a closed chamber as described in the prior art.

BRIEF DESCRIPTION OF THE DRAWINGS

The present invention will be clearly understood and its advantages will arise from the description which follows, given merely as a non-limitative example, and with reference to the attached drawings in which:

The FIGURE provides an embodiment of the present invention.

DETAILED DESCRIPTION

The method will be described in more detail with reference to the FIGURE, which illustrates a method and a unit according to the invention.

A sample to be analyzed is preferentially drawn off from the liquid oxygen bath from the bottom of the low-pressure column of a double column for separating air by cryogenic distillation. It can be drawn off upstream of the latter, between the various stages of vaporizers of the low-pressure column if this is the case or at the inlet of the vaporizer located at the bottom of the low-pressure column. The sample may also be drawn off at any stage of the unit for producing air gases. It can therefore be drawn off at the outlet of the front end purification (FEP), which serves to strip the air to be distilled of water and of carbon dioxide, to be pre-liquefied before being concentrated.

During step a), a given volume (respectively mass) L of this sample is sent to a vaporization chamber through the lines 1 and 3 and the open valve V1. The volume L is in the chamber E. The line 9 and the valve 4 are used to discharge the excess liquid during the filling of the chamber E. There is a calibrated orifice at the outlet of the chamber E (toward the line 9 and the valve 4). The flow rate of liquid that can escape therefrom is smaller than the feed flow rate through V1. Therefore, during filling, the chamber is deliberately filled with liquid to a level located above the orifice (and line 9 and valve 4).

Then the feed valve is closed and the excess liquid located above the orifice is discharged by gravity until a liquid level corresponding to the bottom point of the calibrated orifice is obtained.

The advantage of this procedure and of this calibrated orifice is to monitor the amount of liquid introduced into the chamber E and to ensure that this amount of liquid introduced is identical and reproducible at each cycle. This makes it possible to subsequently control (and by also controlling the amount remaining or vaporized) the concentration factor.

Then according to step b) liquid is no longer sent into the chamber, the valve V1 being closed. During step b) the valve V6 of the line 19 is open and the valves V7 and V5 of the lines 17 and 15 respectively are closed as well as valve V3. The liquid L is heated by a heat source H and partially vaporizes, leaving an amount of residual liquid R. A heat exchanger supplied by an external heat source (heat exchange with a heat-generating fluid, electricity, waves, etc.) partially vaporizes the liquid. The vapor generated is discharged from the vaporization chamber through the valve V6 and the lines 13, 19. The vaporization takes place at atmospheric pressure or under vacuum controlled by way of a vacuum-producing system such as a vacuum pump or an ejector. There are two advantages of a vaporization under vacuum. The first is to lower the vaporization temperature and therefore to further reduce the liquid/vapor equilibrium coefficients. The second is to be able to increase the temperature difference (ΔT) between the heating system and the liquid to be vaporized in order to reduce the vaporization cycle time. The vaporization may also be carried out without the use of a vacuum pump.

In this case, the pressure of the chamber is considered to be equal to the atmospheric pressure, even though it should be slightly higher than this because of the pressure drops. After a given time, the vaporization chamber is insulated in such a way that the ratio between the volume (respectively mass) of liquid initially introduced and the volume (respectively mass) of liquid present in the vaporization chamber at the time of the insulation is perfectly determined.

This determination can be made by counting the amount of material vaporized, or by counting the energy introduced into the vaporization exchanger by the heat source or else by measuring the variation of the liquid level and/or mass level in the chamber E.

Taking into account the equilibrium coefficient, the impurities will remain at least essentially contained in the liquid phase, and the concentration will have varied by a factor at least essentially equal to the ratio of the initial and final material amounts, in terms of volume or mass. For a more precise evaluation, the amount of impurities discharged into the gas phase can be taken into account in the calculation of the concentration factor and/or in the calculation of the initial concentration. The concentration factor is known by material balance between the initial amount of liquid introduced, and the sum of the amounts vaporized and amounts of residual liquid. The amount of liquid thus vaporized, less than L, is therefore precisely controlled, according to step c), so that the content of contaminant in the residual liquid present in the chamber is substantially equal to that in the initial liquid, multiplied by a predetermined factor.

Then, according to a variant of step i), the contaminant content of the residual liquid is measured directly. A sample of residual liquid is drawn off, and the contaminant content is measured after complete vaporization of the sample of residual liquid; the content of contaminant in the initial liquid is deduced from the measurement of contaminant in the residual liquid.

Or else step ii) makes provision for deducing the contaminant content of the residual liquid by completely vaporizing the residual liquid with the at least one contaminant contained therein, the vaporization chamber E then being insulated from any inlet or outlet of material and then the content of contaminant in the vaporized residual liquid is analyzed. The contaminant content of the residual liquid is measured by completely vaporizing the residual liquid with at least one contaminant contained therein, the vaporization chamber then being insulated from any inlet or outlet of material, then the content of contaminant in the vaporized residual liquid is analyzed and the content of contaminant in the initial liquid is deduced from the measurement of contaminant in the residual liquid.

The vaporization is therefore continued, according to step ii), until complete vaporization of the residual liquid, the vaporization chamber being thermally insulated in order to have no further exchange of material with the outside of the chamber, then the phase vaporized inside the chamber is superheated until complete vaporization of the deposits of impurities (up to a temperature of −70° C. for example), thus creating a rise in pressure in the vaporization chamber. It is certain that all the impurities are vaporized if the chamber is brought to a high enough temperature, significantly higher than the vaporization temperature of the impurities at the pressure of the chamber.

During this step ii), all the valves allowing an inlet of fluid into the chamber or an outlet of fluid originating from the chamber are closed.

At the end of this complete vaporization, according to step ii), the gas phase is sent in the analysis line 15 of the chamber E to the analyzer through the open valve V5. Since the content of the liquid initially drawn off has been multiplied by the predefined concentration factor during the partial vaporization phase (step b)), the content of impurity contained in the vapor at the end of the sequence is therefore high enough to be measured by a conventional analyzer (of NDIR type for example).

After step i) or ii), the chamber will then be cooled back down. This step may be carried out by internal or preferably external circulation of a cryogenic liquid, for example the cryogenic liquid to be analyzed, in order to restart a concentration cycle as defined previously.

The total time of steps a) and b) and c) and d) including one of steps i) or ii) is bet wen 15 min and 40 min, preferably less than 20 minutes.

The unit comprises a jacket V placed around the chamber E forming a cylindrical space for regulating the temperature of the chamber.

At the end of step i) or ii), it is necessary to cool the chamber via a step e). If the cooling down is carried out simply by sending the liquid to be analyzed into the chamber, the liquid is partially vaporized during this phase and thus the analysis of impurities is distorted. It is therefore necessary to carry out the cooling down by another means. This step will be within the time of between 15 and 40 min.

During step d) of cooling the chamber E, the space V is filled with a liquid at a temperature below the equilibrium temperature of the liquid to be analyzed. In this way, the liquid to be analyzed is sent into the chamber during step a), and the latter remains completely liquid.

In the example of the FIGURE, a portion of the liquid to be analyzed is sent via the line 5 and the valve V2 to the space V to cool the chamber E.

As the space V is brought into communication at atmospheric pressure, the filled space is colder than the liquid oxygen originating from the column. Alternatively, the liquid used to cool down the chamber E could be liquid nitrogen, but the system would be more complicated.

Preferably, the liquid contained in the space V is removed during steps b) and c) so that the heat source H only heats the liquid present in the chamber E. The liquid exits via the line 7 through the valve V3. The line 6 makes it possible for vapor to exit the space V.

Compared to the system described in the prior art FR2797325, this double jacket E, V is rendered necessary by the different operating mode of the units.

• • The unit according to the invention operates by concentration, in the liquid phase, of the impurities. The cycle time is therefore short and it is important to be accurate regarding the amount of impurities deposited. Thus, it is desired to avoid “concentrating” by deposition of impurities that would occur by the “internal” cooling down as described above.
  • The unit of FR2797325 works by cryotrap and accumulation of impurity over a long period. As a result, the amount deposited during the cooling down of the system after heating becomes negligible compared to the amount trapped over the entire accumulation period.

On reading this description, those skilled in the art will understand that the amount of liquid product remaining at the end of the partial vaporization phase will be necessary and sufficient to ensure, during the analysis phase, an amount of material necessary for the purging flow of the analysis line and for a sufficient analysis time to allow an accurate determination of the measurement.

While the invention has been described in conjunction with specific embodiments thereof, it is evident that many alternatives, modifications, and variations will be apparent to those skilled in the art in light of the foregoing description. Accordingly, it is intended to embrace all such alternatives, modifications, and variations as fall within the spirit and broad scope of the appended claims. The present invention may suitably comprise, consist or consist essentially of the elements disclosed and may be practiced in the absence of an element not disclosed. Furthermore, if there is language referring to order, such as first and second, it should be understood in an exemplary sense and not in a limiting sense. For example, it can be recognized by those skilled in the art that certain steps can be combined into a single step.

The singular forms “a”, “an” and “the” include plural referents, unless the context clearly dictates otherwise.

“Comprising” in a claim is an open transitional term which means the subsequently identified claim elements are a nonexclusive listing (i.e., anything else may be additionally included and remain within the scope of “comprising”). “Comprising” as used herein may be replaced by the more limited transitional terms “consisting essentially of” and “consisting of” unless otherwise indicated herein.

“Providing” in a claim is defined to mean furnishing, supplying, making available, or preparing something. The step may be performed by any actor in the absence of express language in the claim to the contrary.

Optional or optionally means that the subsequently described event or circumstances may or may not occur. The description includes instances where the event or circumstance occurs and instances where it does not occur.

Ranges may be expressed herein as from about one particular value, and/or to about another particular value. When such a range is expressed, it is to be understood that another embodiment is from the one particular value and/or to the other particular value, along with all combinations within said range.

All references identified herein are each hereby incorporated by reference into this application in their entireties, as well as for the specific information for which each is cited.

Claims

1-15. (canceled)

16. A method for analyzing the content of at least one contaminant in a cryogenic liquid wherein: a) introducing a known amount of liquid L constituting the initial liquid at a pressure P into a chamber, the chamber being previously brought to a temperature identical to or below the vaporization temperature at the pressure P of the liquid to be analyzed, so that no vaporization of the liquid occurs in this step a);b) vaporizing a given fraction of the liquid present in the chamber by heating the liquid, the vapor thus generated is discharged from the chamber to maintain a pressure equal to the pressure P;c) controlling the amount of liquid thus vaporized, less than L, so that the amount of contaminant in residual liquid present in the chamber is substantially equal to that in the initial liquid, such that the residual liquid has a higher concentration of contaminant as compared to the initial liquid;d) measuring the contaminant within the residual liquid by either i. drawing off a sample of residual liquid, and the content of contaminant is measured after complete vaporization of the sample of residual liquid, orii. completely vaporizing the residual liquid with at least one contaminant contained therein, the vaporization chamber then being insulated from any inlet or outlet of material and then the content of contaminant in the vaporized residual liquid is analyzed; ande) deducing the content of contaminant in the initial liquid from the measurement of contaminant in the residual liquid.

17. The method as claimed in claim 16, wherein during step ii) the liquid is completely vaporized, thus increasing the pressure in the insulated and closed chamber and then the vapor generated is sent to an analyzer.

18. The method as claimed in claim 17, wherein the vapor generated is heated to a temperature higher than the vaporization temperature of the contaminant at the pressure of the chamber before sending it to the analyzer.

19. The method as claimed in claim 16, wherein no liquid is introduced into the chamber during steps b), c) and i) or ii).

20. The method as claimed in claim 16, wherein the pressure under which the partial vaporization of the liquid of step b) is carried out is at least 1 bar lower than the filling pressure P of the chamber.

21. The method as claimed in claim 16, wherein the increase in concentration of contaminant in step c) is at least essentially equal to the ratio of the initial and final material amounts, in terms of volume or mass, of the liquid, before and after the partial vaporization of step b).

22. The method as claimed in claim 16, wherein the increase in concentration of contaminant in step c) is known by material balance between the initial amount of liquid introduced L, and the sum of the amounts vaporized and amounts of residual liquid.

23. The method as claimed in claim 16, wherein the fraction of step b) is greater than 10%.

24. The method as claimed in claim 16, wherein the fraction of step b) is greater than 30%.

25. The method as claimed in claim 16, wherein the fraction of step b) is greater than 90%.

26. The method as claimed in claim 16, wherein the vaporization pressure of step b) and/or c) is less than 0.8 bar absolute.

27. The method as claimed in claim 16, wherein the liquid originates from a unit for separating air by cryogenic distillation, being drawn off from the unit either in a liquid state or in a gaseous state, being in this case liquefied before being sent to the chamber.

28. The method as claimed in claim 27, wherein the air separation unit comprises an adsorption purification unit and a system of columns for distilling a gas purified in the purification unit, the liquid being gas drawn off downstream of the purification unit and then liquefied.

29. The method as claimed in claim 27, wherein the air separation unit comprises an adsorption purification unit and a system of columns for distilling a gas purified in the purification unit, the liquid being a bottom liquid from a column of the system or an intermediate liquid from a column of the system.

30. The method as claimed in claim 16, wherein the vaporization of step b) is carried out at atmospheric pressure or under vacuum.

31. The method as claimed in claim 16, wherein the chamber is insulated after step b).

32. The method as claimed in claim 31, wherein the ratio between the volume (respectively mass) of liquid initially introduced L and the volume (respectively mass) of liquid present in the vaporization chamber at the time of the insulation is determined by counting the amount of material vaporized, or by counting the energy introduced into the vaporization exchanger by the heat source or else by measuring the variation of the liquid level and/or mass level in the chamber.