The present invention relates to a process and to a plant for producing pressurized air gases by cryogenic air distillation.
Certain (type 1) processes, such as those described in EP-A-0 504 029, produce oxygen at high pressure (>15 bar) using a single compressor to compress the air to a pressure well above the pressure of the medium-pressure column.
These processes are suitable for a context in which investment costs are of prime importance, as they have the drawback of consuming a very large amount of energy when no liquid production is required.
Other (type 2) processes, using a high air pressure only for producing pressurized gaseous oxygen, are disclosed in U.S. Pat. No. 5,475,980 and have a better specific energy for producing gaseous oxygen at high pressure, without producing liquid (or with a low production of liquid). They use cryogenic compression of air pressurized by means of a blower mechanically linked to an expansion turbine.
However, this energy advantage is counterbalanced by an investment substantially greater than that of type 1, as this is an expensive process in terms of exchanger volume. This is because in general a large fraction (60% to 80%) of the main air stream undergoes adiabatic cryogenic compression before being reintroduced into the main exchange line.
Finally, these types of process seem to be economically advantageous, and the choice will depend on the intended utilization of the energy, available at low or high cost.
In this document, the term “condensation” includes pseudo-condensation and the term “vaporization” includes pseudo-vaporization.
Temperatures are considered as being similar if they differ by at most 10° C., preferably at most 5° C.
The exchange line is the main exchanger where the gases produced by the column system are warmed and/or where the air intended for distillation is cooled.
It is an object of the invention to propose an alternative for producing process schemes allowing the energy performance to be improved over type-1 processes, while retaining an exchange volume requirement of less than that of cold-compression, type-2 schemes, as described above.
According to the invention, only a fraction of the air (the fraction that liquefies at the cold end) undergoes cryogenic compression, which minimizes the increase in volume of the exchanger. However, this allows the main air pressure to be very substantially reduced, since the air output by the cryogenic booster remains at a pressure sufficient to vaporize oxygen.
One of the objects of the invention is to provide a process for separating air by cryogenic distillation in a system of columns, comprising a double column or a triple column, the column operating at the highest pressure operating at a pressure called medium pressure, in which:
a) all the air is raised to a high pressure at least 5 to 10 bar above the medium pressure;
b) a portion of the air, comprising between 10% and 50% of the flow of air at high pressure, is withdrawn from an exchange line at a temperature close to the (pseudo) vaporization temperature of the liquid, boosted to above at least the high pressure by means of a cold booster and then sent back into the exchange line, and at least one portion liquefies at the cold end and is then sent, after expansion, into at least one column of the column system;
c) another fraction of the air at at least the high pressure, possibly constituting the remainder of the high-pressure air, is expanded in a Claude turbine and then sent into the medium-pressure column;
d) at least one liquid stream is withdrawn from one of the columns of the column system, pressurized, and vaporized in the exchange line; and
e) the cold booster is coupled to one of the following drive devices:
According to other, optional aspects:
at least one portion of the high-pressure air is boosted, before entering the main exchange line, in a hot booster and then cooled in the exchange line;
all the air to be distilled is boosted to a pressure above the high pressure in the hot booster;
a portion of the air coming from the hot booster is sent to the Claude turbine at the outlet pressure of the hot booster;
a portion of the air coming from the hot booster is cooled in the exchange line, is expanded and liquefied, and sent to at least one column of the column system;
all the air coming from the hot booster is sent only to the Claude turbine or to the Claude turbine and to the cold booster;
the hot booster is coupled to the Claude turbine;
all the gaseous air intended for distillation comes from the turbine and optionally from another air expansion turbine;
all the air boosted in the cold booster is cooled in the exchange line, expanded and liquefied, and sent to at least one column of the column system;
a nitrogen-enriched gas stream coming from a column of the column system is slightly warmed in the exchange line, expanded in the expansion turbine constituting (or forming part of) the drive device and warmed in the exchange line;
a stream of air is expanded in the expansion turbine constituting (or forming part of) the drive device and the expanded air is sent to a column of the column system, in particular to the low-pressure column;
the liquid coming from the column, which vaporizes, is oxygen-enriched compared with air;
the intake temperature of the cold booster is close and preferably substantially equal to the vaporization temperature of the liquid withdrawn from the columns and is introduced, pressurized, into the exchange line;
the intake temperature of the Claude turbine is below the intake temperature of the cold booster;
the intake temperature of the turbine constituting, or forming part of, the drive device is above the intake temperature of the cold booster; and
all the air raised to a high pressure at least 5 to 10 bar above the medium pressure is purified at this high pressure.
Another object of the invention is to provide a cryogenic-distillation air-separation plant comprising:
a) a heat exchange line;
b) a double or triple air-separation column, of which the column operating at the highest pressure operates at a medium pressure;
c) a Claude turbine;
d) a hot booster coupled to the Claude turbine;
e) a cold booster;
f) a device for driving the cold booster, consisting of a turbine, an electric motor or a combination of the two;
g) means for sending all the compressed air intended for distillation to the hot booster and means for sending the boosted air to the heat exchange line;
h) means for withdrawing a first portion of the boosted air to an intermediate level of the exchange line, preferably constituting between 10 and 50% of the compressed air, and for sending it to the cold booster, means for sending the air coming from the cold booster back to the exchange line, and means for outputting the air coming from the cold booster from the cold end of the exchange line, in order to expand it and to send it on;
i) means for withdrawing a second portion of the boosted air to an intermediate level of the exchange line and for sending it to the Claude turbine; and
j) means for sending a liquid to be vaporized from the double or triple column into the exchange line.
The turbine turbine constituting the drive device or forming part of the latter may be an air expansion turbine, in particular a blowing turbine or a nitrogen expansion turbine.
The invention will be described in greater detail with respect to the drawings, FIGS. 1 to 4 of which each show an air-separation unit according to the invention. In
A nitrogen-enriched gas stream 31, coming from the medium-pressure column 100, is warmed in the exchange line, exits therefrom at a temperature higher than the inlet temperature of the Claude turbine 17, and is sent to an expansion turbine 119. The nitrogen expanded substantially at the low pressure and substantially at the temperature of the cold end of the exchange line is reintroduced into the exchange line, where it warms up or joins a nitrogen-enriched gas 33 withdrawn from the low-pressure column, and the nitrogen stream 29 formed is warmed while passing through the entire exchange line.
The nitrogen turbine 119 is coupled to the cold booster 23, while the Claude turbine 17 is coupled to the hot booster 5.
The expansion turbine 119 is not an essential element of the invention and the drive for the cold booster 23 may be replaced by an electric motor. Likewise, the expansion turbine 119 may be replaced with an air-expansion turbine.
The column system of
The medium-pressure column 100 operates at a pressure of 5.5 bar, but it may operate at higher pressure.
The gaseous air 35 coming from the turbine 17 is sent into the bottom of the medium-pressure column 100.
The liquefied air 37 is expanded in the valve 39 and divided into two, one portion being sent to the medium-pressure column 100 and the remainder to the low-pressure column 200.
Rich liquid 51, lower lean liquid 53 and upper lean liquid 55 are sent from the medium-pressure column 100 into the low-pressure column 200 after in-valve expansion and subcooling steps.
Oxygen-enriched liquid 57 and nitrogen-enriched liquid 59 are possibly withdrawn from the double column as final products.
Oxygen-enriched liquid is pressurized by the pump 500 and sent, as pressurized liquid 25, towards the exchange line 9. Alternatively or additionally, other, pressurized or non-pressurized, liquids, such as other liquid oxygen streams at a different pressure, liquid nitrogen and liquid argon, may be vaporized in the exchange line 9.
Waste nitrogen 27 is withdrawn from the top of the low-pressure column and is warmed in the exchange line 9, after having been used to subcool the reflux liquids 51, 53, 55.
The column may optionally produce argon by treating a stream withdrawn from the low-pressure column 200.
As a variant, as shown in dotted lines, a portion 41 of the high-pressure air, not boosted in the booster 23, may liquefy in the exchange line by heat exchange with the oxygen, which vaporizes, is expanded in a valve 43 down to the medium pressure, and is mixed with the liquefied air 37. It will be understood that if the air is at a supercritical pressure on leaving the booster 5 liquefaction will take place only after expansion in the valves 39, 43.
The hot booster 5 is again coupled to the Claude turbine, but the cold booster 23 is coupled to the blowing turbine.
The liquid-air expansion valves are also different in
As in
This kind of process is more suitable for the production of low-purity oxygen.
In
The remaining portion 2 of the air at about 15 bar (and therefore between 10 and 50% of the total high-pressure flow) is cooled in the exchange line 9 down to an intermediate temperature above the intake temperature of the Claude turbine 17 and is then boosted in the cold booster 23. This air then liquefies in the exchange line 9. As in
Number | Date | Country | Kind |
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0350142 | May 2003 | FR | national |
Filing Document | Filing Date | Country | Kind | 371c Date |
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PCT/FR04/50146 | 4/6/2004 | WO | 11/4/2005 |