EP0358714A1

EP0358714A1 - Process for helium enrichment

Info

Publication number: EP0358714A1
Application number: EP88904951A
Authority: EP
Inventors: Karl Knoblauch; Erwin Pilarczyk; Klaus Giessler; Hans Bukowski; Joseph S. D'amico; Herbert Reinhold
Original assignee: Bergwerksverband GmbH
Current assignee: Bergwerksverband GmbH
Priority date: 1987-05-20
Filing date: 1988-05-19
Publication date: 1990-03-21
Also published as: PL272594A1; EP0291975A1; RU1816229C; JPH02503553A; DE3716898C2; US5089048A; EP0291975B1; JPH0832549B2; AU1930788A; DE3716898A1; AU604140B2; PL160299B1; WO1988009306A1; DE3863391D1; ES2023976B3; DD270125A5

Abstract

Le procédé concerne l'enrichissement d'hélium à faible teneur en hélium pour obtenir de l'hélium brut présentant une teneur en hélium supérieure à 50%, par adsorption en pression alternée, avec un rendement en hélium supérieur. Le mélange gazeux contenant par exemple de l'oxygène et/ou du méthane en plus de l'hélium passe à travers des adsorbeurs remplis de tamis moléculaires au carbone qui adsorbent l'azote et/ou le méthane. Quatre adsorbeurs (A, B, C, D) reliés en parallèle sont chargés cycliquement, la phase de montée en pression se déroulant en trois étapes et la phase de détente en pression en quatre étapes. La montée et la détente en pression dans chaque adsorbeur s'effectuent en alternance par égalisation de la pression, partiellement à contre-courant. La phase finale de montée en pression s'effectue avec du gaz reconstitué. Des hydrocarbures supérieurs et d'autres impuretés peuvent être séparés dans des filtres préliminaires (F1, F2, F3, F4) remplis de charbon actif. Le procédé s'utilise de préférence pour enrichir de l'hélium à partir de gaz naturels contenant de 2 à 10% d'hélium et exige moins d'énergie que l'enrichissement par décomposition à basse température dans des installations frigorifiques.The method relates to the enrichment of helium with a low helium content to obtain crude helium having a helium content greater than 50%, by adsorption at alternating pressure, with a higher helium yield. The gaseous mixture containing for example oxygen and / or methane in addition to helium passes through adsorbers filled with carbon molecular sieves which adsorb nitrogen and / or methane. Four adsorbers (A, B, C, D) connected in parallel are cyclically charged, the pressure build-up phase taking place in three stages and the pressure relief phase in four stages. The pressure rise and expansion in each adsorber is carried out alternately by equalization of the pressure, partially against the current. The final pressure build-up phase is carried out with reconstituted gas. Higher hydrocarbons and other impurities can be separated in preliminary filters (F1, F2, F3, F4) filled with activated carbon. The process is preferably used to enrich helium from natural gases containing 2 to 10% helium and requires less energy than enrichment by low temperature decomposition in refrigeration plants.

Description

Helium enrichment process

The invention relates to a process for helium enrichment after a pressure-swing adsorption process from gas mixtures which contain helium, nitrogen and methane and optionally further gases and are passed through carbon molecular sieves which adsorb nitrogen and methane and optionally the further gases, the gas mixture cyclically four adsorbers connected in parallel are given, each of which successively goes through a pressure build-up phase, an adsorption phase and a pressure relief phase, and pressure build-up and pressure relief take place partly by pressure equalization with another adsorber.

Such a pressure swing adsorption process is known from EP 00 02 695, which is used for the purification of helium from a starting gas mixture with helium and essentially nitrogen, argon and oxygen and smaller proportions of carbon dioxide and methane, and in which using carbon molecular sieves helium with a purity of over 99.9 vol .-. ό is obtained. However, the starting gas mixture already contains 50-95 vol .-% helium. With this method, helium cannot be enriched from gas mixtures with up to 10% helium because the procedure and the combination of the process steps are not suitable for this. Helium is increasingly required for various applications, e.g. B. in refrigeration systems for refrigeration, as a protective gas in welding and in the chemical industry, in airspace technology as an inert gas, in diving work in the form of breathing gas, in chromatography as a carrier gas, in leak detection, as a balloon gas and for other purposes. For these applications, helium is required which has a high purity. In order to obtain these high purities, several process stages are required for gas mixtures which have only low helium contents, in order first to enrich the gas mixture with helium and then finally to obtain helium with high purity from the gas mixture enriched with helium.

Helium is mainly enriched and extracted from helium-containing natural gases. The main constituents of helium-containing natural gases include methane and nitrogen and up to 10% by volume of helium in addition to smaller amounts of various higher hydrocarbons and carbon dioxide.

According to the prior art, the following method for helium enrichment is used, which is known from "Bureau of Mines, Pre = print from Bulletin 675 - Helium - 1985 Edition, United States of Interior", pp. 3 and 4 is.

The helium-containing natural gas is cooled in a refrigeration system to approx. -150 ° C, whereby mainly the hydrocarbons are condensed out. The gas mixture produced in this way contains, apart from small amounts of other gases, more than 50 vol. Helium and nitrogen. »In some cases, this crude helium is further processed on-site to high-purity helium, namely by a process combination in which a pressure ¬ interchangeable adsorption system interacts with a second refrigeration system. The crude helium is also commercially available as an intermediate product and in these cases is further processed to pure helium elsewhere.

The invention has for its object to achieve the enrichment of helium from natural gases with low helium contents to crude helium with a higher helium content than 50 .. solely by pressure swing adsorption and without intermediate enrichment in refrigeration systems with a high yield.

Starting from a method of the type mentioned at the outset, this object is achieved in that

a) the pressure build-up phase comprises three steps:

1. pressure build-up step from a final vacuum pressure (P.) to a medium pressure level (P,);

2. pressure build-up step from the medium pressure level (P- _$ ) to a higher pressure level (P.);

3rd pressure build-up step from the higher pressure level (P,) to the highest pressure level (P.) - adsorption pressure;

b) the pressure-relief phase comprises four steps:

1. pressure relief step from the highest pressure level (P-) to the higher pressure level (P,);

2nd pressure relief step from the higher pressure stage (P,) to the middle pressure stage (P-,);

3rd pressure relief step from the middle pressure stage (P,) to the atmospheric pressure (P-);

4. Pressure relief step from atmospheric pressure (P ") to the final vacuum pressure (P,);

c) the pressure equalization takes place in two stages and the first stage from the outlet of a first adsorber, which load step (from P _. to P.) to the output of a second adsorber, which carries out the second pressure build-up step (from P, to P.) and the second step from the output of the first adsorber, which carries out the second relief step (from P. on P,), to the input of a third adsorber, which carries out the first pressure build-up step (from P to P,), and

the 3rd relief step and the 4th relief step take place in countercurrent, a low-helium exhaust gas being produced, and the 3rd pressure build-up step is carried out with product gas.

Carbon molecular sieves with an average adsorption pore diameter between 0.1 and 0.4 nm, preferably 0.3 and 0.4 nm, are used as adsorbents for the process according to the invention, because they can separate nitrogen and methane from helium extremely effectively , so that, surprisingly, crude helium with a comparatively high helium content of over 50% can already be produced in a single stage, an unexpectedly high helium yield of over 90% being achieved when the proposed teaching is used. According to the proposed enrichment process, this can be achieved by using the pressure swing technique alone from starting gas mixtures with a comparatively low helium content of about 2 to 8% without the need for a refrigeration system. h_, with very low energy consumption.

It is recommended that the adsorbers are preceded by prefilters which are filled with activated carbon in order to avoid higher hydrocarbons and possibly further impurities. separate from the natural gas beforehand. In this way it is avoided that these impurities get into the carbon molecular sieves and impair their ability to adsorb and regenerate.

Tests have shown that the highest pressure level (P _< -) - adsorption pressure - should be above 1 bar, preferably 10-30 bar, and the final vacuum pressure should be below 500 mbar, preferably 50 mbar.

According to a preferred embodiment, the following pressure values are assigned to the individual pressure stages:

P. = 50 mbar P- = 1 bar P-. = 4 bar P ₄ = 11.7 bar P. = 20 bar

As tests have shown, the total cycle time can be between 450 and 3600 s, preferably 720 s.

According to a preferred embodiment, the pressure relief phase comprises the following time intervals with a total cycle time of 720 s:

1. Relief step from P_ to P. 55 s rest position 115 s

2. Relief step from P. to P-. 10 s

3. Relief step from P to P „55 s

4. Relief step from P_ to P. 115 s Also in accordance with a preferred embodiment, the pressure build-up phase comprises the following time intervals with a total cycle time of 720 s.

1-. Pressure build-up step from P to P, 10 s

2nd pressure build-up step from P, to P. 55 s-

3. Pressure build-up step from P. to P. 125 s

The time interval for product gas extraction is expediently 180 s with a total cycle time of 720 s.

The method according to the invention ^"is particularly suitable for An¬ enrichment of helium from feed gases, the helium content 10 vol .- ό. Or less, preferably 2 to 8 vol ?. is, the helium content in the recovered crude helium up to 95 V0I.- .0 can be.

The method according to the invention is preferably used in the helium enrichment from natural gases which, after a prior separation of higher hydrocarbons and trace impurities, eg. B. in known adsorption prefilters, the following composition (data in Vol .-. Ό) _

He 2-10

CH, 10-40

C0, <0.1-10

Further advantages and configurations result from the following description of exemplary embodiments with reference to the accompanying drawings. The drawings show: 1 shows a single-stage system with four parallel adsorbers for the enrichment of helium up to 95 vol.

FIG. 2 shows a pressure-time diagram of an adsorber of the system according to FIG. 1;

FIG. 3 shows a pressure-time diagram with an assigned partial step sequence table for the four adsorbers of the plant according to FIG. 1;

FIG. 4 shows a valve circuit diagram for the four adsorbers of the system according to FIG. 1;

5 shows a diagram of the dependence of the helium yield on the helium purity in a system according to FIG. 1;

The system according to FIG. 1 consists of four adsorbers A to D filled with a carbon molecular sieve in a parallel circuit and optionally of four prefilters F1 to F4 filled with activated carbon, in which, if necessary, higher hydrocarbons and trace impurities present in the feed gas mixture can be removed before entering adsorbers A to D. Each adsorber cycles through the following eight sub-steps cyclically, with a time lag to the other three adsorbers:

Tl adsorption

T2 pressure relief through pressure equalization (Da 1)

T3 pressure relief through pressure equalization (Da 2)

T4 countercurrent relaxation (GEE)

T5 evacuation (Ev)

T6 pressure build-up through pressure equalization (DA 1)

T7 pressure build-up through pressure equalization (DA 2)

T8 pressure build-up with product gas (DA 3) Before FIG. 1 is explained in detail, the sequence of the eight sub-steps T1 to T8 is first clarified using the pressure-time profiles shown in FIGS. 2 and 3.

Fig. 2 shows an example of. an adsorption pressure of 20 bar and a total cycle time of 720 s the pressure-time profile that occurs in each of the four adsorbers, staggered from the other adsorbers. Five pressure values Pl to P5 are marked on the pressure axis, between which the pressure build-up and pressure relief steps take place in the present example.

3 shows the time-shifted pressure-time profiles in the four adsorbers A to D. The procedure for adsorber A is described below by way of example. Corresponding procedures apply to the other three adsorbers B, C and D.

The adsorption (sub-step T1) takes place at a constant increased pressure, for example at 20 bar. The adsorber A is flowed through at this pressure with the feed gas mixture, nitrogen, methane and other gas components being adsorbed by the carbon molecular sieve, so that helium which is not adsorbed flows out at the adsorber outlet in a highly enriched manner.

After adsorption, the loaded adsorber A is regenerated by several pressure relief steps (sub-steps T2 to T5).

First, there is a first pressure equalization Da 1 (sub-step T2), the gas under adsorption pressure from adsorber A being in cocurrent from the adsorption pressure P _. is relaxed in the adsorber C, which is at a lower pressure P. The gas release from adsorber A (T2) to adsorber C (T7) is in the Partial sequence table of FIG. 3 illustrated by an arrow.

During the first pressure equalization (Da 1), the pressure in the adsorber A is released to a pressure P, for example to 11.7 bar, while at the same time the pressure in the adsorber C increases from the pressure P to the pressure P. (pressure build-up DA 2) .

After a short standstill (stand by), a second pressure compensation takes place in adsorber A (Da 2, substep T3), the gas under pressure P from adsorber A again

4 in direct current - in the adsorber D standing on the vacuum final pressure P. is relaxed. The pressure in the adsorber A drops from the pressure P. to a pressure P.sub.1, which is, for example, 4 bar. During both pressure equalization steps, a helium-enriched gas mixture flows from adsorber A into adsorber C or into adsorber D.

After the two pressure equalization steps (Da 1 and Da 2), adsorber A is further expanded in countercurrent from the pressure P to atmospheric pressure P (GEE, substep T4). This results in a low helium gas mixture in which the components desorbing during countercurrent expansion (GEE) such as nitrogen and methane are enriched and which is discarded as waste gas.

Adsorber A is then evacuated to the final vacuum pressure P, for example 50 mbar, using a vacuum pump 80 (Ev, substep T5). Here, there is an increased desorption of nitrogen and methane and of the other gas components π adsorbed in the partial step T1. The extracted gas is extremely low in helium and is also discarded as waste gas.

After the evacuation, the regeneration of the adsorber A has ended. In the adsorber A, the pressure in the sub-steps T6 to T8 is then increased successively to the adsorption pressure P_. First, there is pressure equalization (sub-step T6) between adsorber A and adsorber B, which has previously gone through sub-step T2 and is at a higher intermediate pressure P. at the end of the evacuation of adsorber A. During the pressure equalization, a helium-enriched gas mixture flows from adsorber B into adsorber A, the gas mixture preferably being drawn off from adsorber B in cocurrent and introduced into adsorber A in cocurrent (head-to-bottom pressure equalization). The pressure in the adsorber A (pressure build-up DA 1) increases from the final vacuum pressure P to an intermediate pressure P, for example 4 bar, while at the same time the pressure in the adsorber B drops from the intermediate pressure P to the intermediate pressure P ₃ .

The pressure in adsorber A (pressure build-up DA 2) is increased further by a further pressure equalization (sub-step T7) with adsorber C. Adsorber C has previously passed through the sub-step T1, adsorption, and is at adsorption pressure P_ before the pressure equalization with adsorber A. In the example, the pressure equalization is carried out in such a way that the helium-enriched gas mixture is drawn off from adsorber C in cocurrent and expanded in countercurrent into adsorber A (head-to-head pressure equalization). The pressure in the adsorber A rises from the intermediate pressure P to the intermediate pressure P., for example 11.7 bar, while at the same time the pressure in the adsorber C drops from the adsorption pressure P 1 to the intermediate pressure P.

5 4

After the pressure has been equalized twice, the pressure in adsorber A is finally reduced by the higher intermediate pressure using product gas. P. on the adsorption pressure P _. , for example 20 bar, increased (pressure build-up DA 3, substep T8). A new adsorption step then begins in adsorber A (sub-step T1). The four adsorbers A to D are, as shown in FIG. 1, connected via a series of valves in such a way that one of the four adsorbers is constantly on adsorption and produces high purity helium as product gas. The circuit of the valves is shown in Fig. 4. The gas supply and discharge in the pressure change system shown in FIG. 1 is explained below with reference to FIGS. 4 and 1, by way of example for adsorber A. Before the adsorbers A to D, prefilters F1 to F4 can be provided, which are state of the art and in which strongly adsorbing gas components, such as, for. B. higher hydrocarbons from borehole gases can be pre-separated. Its operation is as shown in the ^'rule in the example, the same as that of the downstream in the series circuit main adsorbers A to D takes, so to be not addressed thereto einge¬ in detail below.

After the pressure build-up with product gas (DA 3, substep T8), adsorber A is at the adsorption pressure P_. During the subsequent adsorption (sub-step T1), the feed gas mixture flows through a line 1 at a pressure which is slightly above the adsorption pressure to overcome the pressure loss in the system, with valves 10 and 13 open, which are upstream and downstream in the direction of flow the adsorber A are arranged through the adsorber A. Apart from helium, all other components of the feed gas mixture, such as nitrogen and methane, are adsorbed on the carbon molecular sieve, so that at the head of the adsorber A a helium rich gas flows out via a line 4 into a product gas line 91, in which a needle valve 71 (control valve) is arranged. According to the valve circuit diagram in FIG. 4, the adsorption is divided into three time steps ZI, Z2 and Z3. In time step ZI, a valve 50 contained in a line 5 is closed, so that the entire product gas flows via line 4 into the product gas line 91. In the time steps Z2 and Z3, valve 50 is opened, so that part of the product gas flows through a downstream throttle valve 72 and via line 5 and an open valve 25, which is connected upstream of adsorber B, into adsorber B, which flows with the Product gas in substep T8 from the intermediate pressure P. to the adsorption pressure P ,. is pressed. For a total cycle time of 720 s, the duration of the three time steps ZI, Z2 and Z3 can be 55 s for time step ZI, 115 s for time step Z2 and 10 s for time step Z3.

After the adsorption, adsorber A is expanded to a higher intermediate pressure P 1 in sub-step T2 (Da 1), the gas flowing out of the adsorber A when the valve 15 is open (valve 50 is closed) in a head-to-head pressure compensation a throttle valve 73 in line 5 flows into the adsorber C when the valve 35 is open, which is pressed in step T7 from an intermediate pressure P to an intermediate pressure P. According to the valve circuit diagram in FIG. 4, a time step ZI is required for this pressure compensation (Da 1), which in the example has a duration of 55 s with a total cycle time of 720 s.

After this first pressure equalization and a standstill (stand by), which has a duration of 115 s, for example with a total cycle time of 720 s, adsorber A is increased in sub-step T3 (Da 2) via a further pressure equalization with adsorber D from the higher intermediate pressure P. a lower intermediate pressure P, further relaxed. For this purpose, gas is released from the adsorber A via a ring line 3 (valve 60 in line 92 is closed) and a throttle valve 74 in the adsorber D, which is released in the partial step T6 of the final vacuum pressure P to the intermediate pressure P-. is pushed open. The pressure equalization takes place in the example, as described, as head-to-floor pressure equalization. According to the valve circuit diagram in FIG. 4, a time step Z3 is required for pressure equalization Da 2, which in the example has a duration of 10 s with a total cycle time of 720 s.

Adsorber A is then further relaxed in partial step T4 (GEE) with opened valves 12 and 60 via throttle valve 75 in counterflow from the intermediate pressure P to the atmospheric pressure P. The gas flowing out is fed into an exhaust pipe 92. With a total cycle time of 720 s, the countercurrent relaxation in the example has a duration of 55 s.

After the countercurrent relaxation, adsorber A is evacuated in sub-step T5 (Ev) with the valve 11 open using the vacuum pump 80 from the atmospheric pressure P "to the final vacuum pressure P-, for example to 50 mbar. The low-helium gas mixture extracted in the process is fed into an exhaust line 93. With a total cycle time of 720 s, the evacuation in the example has a duration of 115 s.

The evacuated adsorber A is then pressed in partial step T6 (DA 1) in a pressure equalization with adsorber B, which is preferably carried out as head-to-bottom pressure equalization, from the initial vacuum pressure P to the intermediate pressure P. A helium-enriched gas mixture is expanded from the outlet end of adsorber B with valves 24 and 12 open (valve 60 is closed) via ring line 3 and throttle valve 74 into the inlet end of adsorber A. Adsorber B passes through sub-step T3. When the pressure is equalized, the pressure in the adsorber B falls from the intermediate pressure P 1 the intermediate pressure P ,. With a total cycle time of 720 s, the pressure compensation DA 1 in the example takes 10 s.

Adsorber A, which is partially pressed onto intermediate pressure P, is then further pressed onto intermediate pressure P. in partial step T7 (DA 2) by a further pressure equalization with adsorber C. This pressure equalization is preferably carried out as head-to-head pressure equalization in such a way that a gas mixture enriched with hydrogen is expanded from the outlet end of the adsorber C when the valves 35 and 15 are open via throttle valve 73 in line 5 into the outlet end of the adsorber A. Adsorber C passes through sub-step T2, the pressure in adsorber C dropping from adsorption pressure P, _ to intermediate pressure P. The time for pressure equalization DA 2 is 55 s in the example with a total cycle time of 720 s.

Finally, in partial step T8 (DA 3), adsorber A is pressed with product gas from the intermediate pressure P. to the adsorption pressure P_. For this purpose, part of the product gas is passed into the adsorber A via the throttle valve 72 when the valves 50 and 15 are open. According to the valve circuit diagram in FIG. 4, the pressure build-up DA 3 is composed of the two time steps Z2 and Z3, which in the example have a duration of 115 or 10 s with a total cycle time of 720 s.

After the pressure build-up DA 3 with product gas, a new pressure change cycle begins in adsorber A, which begins again with the adsorption step. The pressure change cycle in adsorbers B, C and D takes place accordingly, but with a time shift, as can be seen from FIG. 3.

As described, regeneration of the adsorbent is achieved by an evacuation step. Admittedly the gas components to be removed here from the helium-containing feed gas, such as nitrogen and methane, are also desorbed according to the prior art by flushing with product gas. Such a rinsing desorption would, however, occur in helium enrichment from natural gases with a helium content of ax. 10 vol.-._ lead to extremely high yield losses for helium, since due to the low helium content in the feed gas mixture, only a small amount of helium raw gas is obtained as product gas and large amounts of gas must be desorbed at the same time, because the gas to be removed and desorbed by adsorption Components in the feed gas mixture have a share of at least 90% by volume.

B E I S P I E L E

In a laboratory pressure change system according to FIG. 1 (but without a prefilter F1 to F4), separation tests were carried out with a gas mixture at an adsorption pressure of 20 bar, a vacuum end pressure of 50 mbar and a total cycle time of 720 s, corresponding to 5 cycles / h Helium (approx. 5 vol .-. Ό), methane (approx. 29 vol .-. Ά) and nitrogen (approx. 66 vol .-. Ό) contained. The four adsorbers A to D were filled with a carbon molecular sieve with an average adsorption pore diameter of 0.35 nm and had a filling volume of 2 l / adsorber. In the tests, the amount of product gas generated was changed by adjusting the needle valve 71 and the helium purity in the product gas was varied thereby. The test results listed in Tables 1 to 4 below demonstrate that with the method according to the invention helium from a feed gas with a helium content of <10% by volume to a helium content of 75-95% by volume. can be accumulated in the crude helium (product gas) obtained, depending on the helium content in the crude helium (product gas) a helium yield of 90 - 99.9 .ό is achieved. The test results are shown in the form of a complete mass balance.

Table 1

Concentration amount (Vol .-.,.) (Nl / h)

Hey CH _A

Gas mixture 5.1 28.9 66.0 602.2

Exhaust gas off

Evacuation 0.7 23.1 76.2 191.3

Exhaust gas from countercurrent relaxation 0.5 34.0 65.5 381.7

Product gas (crude helium) 95.0 - 5.0 29.2

From this a He yield of 90.3 ._ is calculated.

Table 2

Concentration quantity (Vol.-._) (Nl / h)

He CH ₄ N ₂

Feed gas mixture 5.3 28.9 65.8 593.6

Exhaust gas off

Evacuation 0.2 23.8 76.0 188.5

Exhaust gas from countercurrent relaxation 0.2 34.1 65.7 371.5

Product gas (crude helium) 90.0 - 10.0 33.6 From this, a He yield of 96.1 is calculated

Table 3

Concentration quantity (Vol.-._) (Nl / h)

Hey CH.

Feed gas mixture 5.1 28.6 66.3 604.1

Exhaust gas from evacuation - 24.5 75.5 190.4

Exhaust gas from countercurrent relaxation <0.1 33.7 66.2 375.2

Product gas (crude helium) 80.0 __ 20.0 38.5

From this, a He yield of 99.9 is calculated

Table 4

Concentration amount

(Vol .-? _) (Nl / h)

He CH ₄ N ₂

Feed gas mixture 5.4 28.5 66.1 609.4

Exhaust gas from evacuation - 26.0 74.0 194.1

Exhaust gas from countercurrent relaxation <0.1 33.1 66.8 372.4

Product gas (crude helium) 76.4 - 23.6 42.9

From this a He yield of 99.6? Ό is calculated. With increasing helium purity (helium content of the raw helium obtained), the helium yield decreases and vice versa. The relationship between helium purity (helium content of the crude helium obtained and helium yield is shown in FIG. 5.

Claims

Process for helium enrichment Claims: Process for helium enrichment according to a pressure-swing adsorption process from gas mixtures which contain helium, nitrogen and methane and possibly other gases and are passed through carbon molecular sieves which adsorb nitrogen and methane and possibly the other gases, wherein the gas mixture is cyclically fed into four adsorbers connected in parallel, each of which successively goes through a pressure build-up phase, an adsorption phase and a pressure relief phase, and pressure build-up and pressure relief are partially achieved by pressure equalization with another adsorber, characterized in that a) the pressure build-up phase comprises three steps :

1. Pressure build-up step from a final vacuum pressure (P-i ) to a medium pressure level (P-,);

2. Pressure build-up step from the medium pressure stage (P- ) to a higher pressure stage (P _Δ );

3. Pressure build-up step from the higher pressure level (P _Δ ) to the highest pressure level (P-) - adsorption pressure; b) the pressure relief phase includes four steps:

1. Pressure relief step from the highest pressure level (P_) to the higher pressure level (P .) ;

2. Pressure relief step from the higher pressure stage (P.) to the medium pressure stage (P-,);

3. Pressure relief step from the medium pressure stage (P,) to atmospheric pressure (P _? );

4o Pressure relief step from atmospheric pressure (P-,)- to final vacuum pressure (P,);

c) the pressure equalization takes place in two stages and the first stage from the output of a first adsorber, which carries out the 1st relief step (from P,. to P,), to the output of a second adsorber, which carries out the 2nd pressure build-up step (from P -. on P.) and the second step from the exit of the first adsorber, which carries out the 2nd relief step (from P. to P,), to the entrance of a third adsorber, which carries out the 1st pressure build-up step (from P, to P. ,) carries out, is carried out, and

d) the 3rd relief step and the 4th relief step take place in countercurrent, resulting in a low-helium exhaust gas, and the 3rd pressure build-up step is carried out with product gas.

2. The method according to claim 1, characterized in that the adsorbers are preceded by pre-filters which are filled with activated carbon and separate higher hydrocarbons and, if necessary, further impurities from the gas mixture. 3. The method according to claim 1 or 2, characterized in that the highest pressure level (P,. ) - adsorption pressure - is above 1 bar, preferably 10 - 30 bar, and the final vacuum pressure is below 500 mbar, preferably 50 mbar.

4. The method according to claim 3, characterized in that the following pressure values are preferably assigned to the individual pressure stages:

50 mbar

1 bar

4 bar

11.7 bar

20 bar

5. Method according to one of the preceding claims, characterized in that the total cycle time can be between 450 and 3600 s, preferably 720 s.

6. The method according to any one of the preceding claims, characterized in that the pressure relief phase preferably comprises the following time intervals with a total cycle time of 720 s;

1st unloading step from P_ to P. 55 s rest position 115 s

2nd unloading step from P, to P-, 10 s

³ 4 3

3. Relief step from P, to P„ 55 s

4. Relieving step of P _? on P, 115 s

7. Method according to one of the preceding claims, characterized in that the pressure build-up phase preferably comprises the following time intervals with a total cycle time of 720 s: 1. Pressure build-up step from P. to P, 10 s

2. Pressure build-up step from P_ to P. 55 s

3. Pressure build-up step from P. to P,. 125s

8. The method according to any one of the preceding claims, characterized in that the product gas extraction comprises a time interval of 180 s with a total cycle time of 720 s.

9. The method according to any one of the preceding claims, characterized in that the helium content in the feed gas is 10 vol.-?_ or less, preferably 2 - 8 vol.-?., and the helium proportion in the product gas is up to 95 vol.-?ά .

10. The method according to any one of the preceding claims, characterized in that helium-containing natural gases serve as gas mixtures.