The invention is described in more detail on the basis of the accompanying figure.
According to
Via an absorption medium line 9 and a throttle valve 11, the carbon-dioxide-loaded absorption medium is passed through a desorption column 13. In the lower part of the desorption column 13 the loaded absorption medium is heated and regenerated by means of a heater (which is not shown). The resultant carbon dioxide which is released leaves the desorption column 13 via the off-gas line 15. The desorption column 13 can have (which is not shown), above the absorption medium inlet, backwash trays or backwash sections which are preferably equipped with packings, where entrained absorption medium is separated off from the released CO2 using water or condensate. In line 15, a heat exchanger having a top distributor or condenser can be provided. The regenerated absorption medium is then fed back to the absorption column 3 by means of a pump 17 via a heat exchanger 19. To prevent the accumulation of absorbed substances which are not expelled, or are expelled only incompletely in the regeneration, or of decomposition products in the absorption medium, a substream of the absorption medium taken off from the desorption column 13 can be fed to an evaporator in which low-volatile byproducts and decomposition products arise as residue and the pure absorption medium is taken off as vapors. The condensed vapors are recirculated to the absorption medium circuit. Expediently, a base, such as potassium hydroxide, can be added to the substream, which base forms, for example together with sulfate or chloride ions, low-volatile salts, which are taken off from the system together with the evaporator residue.
All percentages are percentages by weight.
The mass transfer rate was determined in a laminar jet chamber using water vapor-saturated CO2 at 1 bar and 50° C. and 70° C., jet chamber diameter 0.94 mm, jet length 1 to 8 cm, volumetric flow rate of the absorption medium 1.8 mils and is reported as gas volume in cubic meters under standard conditions per unit surface area of the absorption medium, pressure and time (Nm3/m2/bar/h). p The results are summarized in the following table 1. The CO2 mass transfer rate reported in the table is related to the CO2 mass transfer rate of a comparison absorption medium, which comprises 35% by weight MDEA and 5% by weight piperazine.
To determine the capacity of various absorption media for the uptake of CO2 and to estimate the energy consumption in the regeneration of the absorption media, firstly measured values were determined for the CO2 loading at 40 and 120° C. under equilibrium conditions. These measurements were carried out for the systems CO2/Niax/MAPA/water; CO2/TMPDA/MAPA/water; CO2/DEEA/MAPA/water; CO2/DMEA/MAPA/water; CO2/Niax/piperazine/water; CO2/TMPDA/piperazine/water in a glass pressure vessel (volume=110 cm3 or 230 cm3), in which a defined amount of the absorption medium had been charged, evacuated and, at constant temperature, carbon dioxide was added stepwise via a defined gas volume. The amount of carbon dioxide dissolved in the liquid phase was calculated after gas space correction of the gas phase. The equilibrium measurements for the system CO2/MDEA/MAPA/water were performed in the pressure range>1 bar using a high pressure equilibrium cell; in the pressure range<1 bar, the measurements were carried out using headspace chromatography. The equilibrium data for the system CO2/MDEA/piperazine/water were calculated according to the electrolyte approach of Pitzer (Kenneth S. Pitzer, Activity Coefficients in Electrolyte Solutions 2nd ed., CRC-Press, 1991, Chapt. 3, Ion Interaction Approach: Theory and Data Correlation; the parameters were matched to measured data).
To estimate the absorption medium capacity, the following assumptions were made:
1. The absorber is exposed at a total pressure of one bar to a CO2-comprising flue gas of 0.13 bar CO2 partial pressure (=13% CO2 content).
2, In the absorber bottom, a temperature of 40° C. prevails.
3. During the regeneration, a temperature of 120° C. prevails in the desorber bottom.
4. In the absorber bottom, an equilibrium state is achieved, that is the equilibrium partial pressure is equal to the feed gas partial pressure of 13 kPa.
5. During the desorption, a CO2 partial pressure of 5 kPa prevails in the desorber bottom (the desorption is typically operated at 200 kPa. At 120° C. pure water has a partial pressure of about 198 kPa. In an amine solution the partial pressure of water is somewhat lower, therefore a CO2 partial pressure of 5 kPa is assumed).
6. During the desorption, an equilibrium state is achieved.
The capacity of the absorption medium was determined from (i) the loading (mole of CO2 per kg of solution) at the intersection of the 40° C. equilibrium curve with the line of constant feed gas CO2 partial pressure of 13 kPa (loaded solution at the absorber bottom in equilibrium); and (ii) from the intersection of the 120° C. equilibrium curve with the line of constant CO2 partial pressure of 5 kPa (regenerated solution at the desorber bottom in equilibrium). The difference between the two loadings is the circulation capacity of the respective solvent. A high capacity means that less solvent need be circulated and thus the apparatuses such as, for example, pumps, heat exchangers, but also the piping, can be dimensioned so as to be smaller. In addition, the circulation rate also influences the energy required for regeneration.
A further measure of the service properties of an absorption medium is the gradient of the working lines in the McCabe-Thiele diagram (or p-X diagram) of the desorber. For the conditions in the bottom of the desorber, the working line is generally very close to the equilibrium line, so that the gradient of the equilibrium curve to an approximation can be equated to the gradient of the working line. At a constant liquid loading, for the regeneration of an absorption medium having a high gradient of equilibrium curve, a smaller amount of stripping steam is required. The energy requirement to generate the stripping steam makes an important contribution to the total energy requirement of the CO2 absorption process.
Expediently, the reciprocal of the gradient is reported, since this is directly proportional to the amount of steam required per kilogram of absorption medium. If the reciprocal is divided by the capacity of the absorption medium, this gives a comparative value which directly enables a relative statement on the amount of steam required per absorbed amount of CO2.
In table 2, the values of the absorption medium capacity and the steam requirement are standardized to the mixture of MDEA/piperazine. In table 3, the values of the absorption medium capacity and the steam requirement are standardized to the mixture of MDEA/MAPA.
It can be seen that absorption media having a tertiary amine whose reaction enthalpy ΔRH of the protonation reaction is greater than that of methyidiethanolamine have a higher capacity and require a lower amount of steam for regeneration.
Number | Date | Country | Kind |
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10 2004 011 429.3 | Mar 2004 | DE | national |
Filing Document | Filing Date | Country | Kind | 371c Date |
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PCT/EP05/02498 | 3/9/2005 | WO | 00 | 7/13/2007 |