US20030167769A1 - Mixed working fluid power system with incremental vapor generation - Google Patents
Mixed working fluid power system with incremental vapor generation Download PDFInfo
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- US20030167769A1 US20030167769A1 US10/258,718 US25871803A US2003167769A1 US 20030167769 A1 US20030167769 A1 US 20030167769A1 US 25871803 A US25871803 A US 25871803A US 2003167769 A1 US2003167769 A1 US 2003167769A1
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- 239000012530 fluid Substances 0.000 title claims abstract description 278
- 238000010438 heat treatment Methods 0.000 claims abstract description 215
- 239000007788 liquid Substances 0.000 claims abstract description 92
- 238000006243 chemical reaction Methods 0.000 claims abstract description 37
- 238000000034 method Methods 0.000 claims description 13
- 230000008016 vaporization Effects 0.000 claims description 6
- 230000003134 recirculating effect Effects 0.000 claims 2
- HPALAKNZSZLMCH-UHFFFAOYSA-M sodium;chloride;hydrate Chemical compound O.[Na+].[Cl-] HPALAKNZSZLMCH-UHFFFAOYSA-M 0.000 description 48
- QGZKDVFQNNGYKY-UHFFFAOYSA-N Ammonia Chemical compound N QGZKDVFQNNGYKY-UHFFFAOYSA-N 0.000 description 40
- 239000012267 brine Substances 0.000 description 26
- 229910021529 ammonia Inorganic materials 0.000 description 20
- 238000001816 cooling Methods 0.000 description 16
- 239000000203 mixture Substances 0.000 description 15
- 238000010248 power generation Methods 0.000 description 15
- XLYOFNOQVPJJNP-UHFFFAOYSA-N water Substances O XLYOFNOQVPJJNP-UHFFFAOYSA-N 0.000 description 11
- 239000006200 vaporizer Substances 0.000 description 6
- 230000005611 electricity Effects 0.000 description 5
- 238000010587 phase diagram Methods 0.000 description 4
- 238000012546 transfer Methods 0.000 description 4
- 238000004891 communication Methods 0.000 description 3
- 239000000284 extract Substances 0.000 description 3
- 238000009834 vaporization Methods 0.000 description 3
- 238000009833 condensation Methods 0.000 description 2
- 230000005494 condensation Effects 0.000 description 2
- 238000013461 design Methods 0.000 description 2
- 238000010586 diagram Methods 0.000 description 2
- 239000002803 fossil fuel Substances 0.000 description 2
- 239000000463 material Substances 0.000 description 2
- VNWKTOKETHGBQD-UHFFFAOYSA-N methane Chemical compound C VNWKTOKETHGBQD-UHFFFAOYSA-N 0.000 description 2
- 239000003034 coal gas Substances 0.000 description 1
- 239000000470 constituent Substances 0.000 description 1
- 238000002156 mixing Methods 0.000 description 1
- 239000003345 natural gas Substances 0.000 description 1
- 238000011160 research Methods 0.000 description 1
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- F—MECHANICAL ENGINEERING; LIGHTING; HEATING; WEAPONS; BLASTING
- F01—MACHINES OR ENGINES IN GENERAL; ENGINE PLANTS IN GENERAL; STEAM ENGINES
- F01K—STEAM ENGINE PLANTS; STEAM ACCUMULATORS; ENGINE PLANTS NOT OTHERWISE PROVIDED FOR; ENGINES USING SPECIAL WORKING FLUIDS OR CYCLES
- F01K25/00—Plants or engines characterised by use of special working fluids, not otherwise provided for; Plants operating in closed cycles and not otherwise provided for
- F01K25/06—Plants or engines characterised by use of special working fluids, not otherwise provided for; Plants operating in closed cycles and not otherwise provided for using mixtures of different fluids
- F01K25/065—Plants or engines characterised by use of special working fluids, not otherwise provided for; Plants operating in closed cycles and not otherwise provided for using mixtures of different fluids with an absorption fluid remaining at least partly in the liquid state, e.g. water for ammonia
Definitions
- the ammonia/water mixture that comprises the mixed working fluid 114 vaporizes progressively over an increasing temperature range. That is, the temperature of the vapor and liquid comprising the heated mixed working fluid increases with increasing quality.
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- General Engineering & Computer Science (AREA)
- Engine Equipment That Uses Special Cycles (AREA)
Abstract
Description
- [0001] The United States Government has rights in this invention pursuant to Contract No. DEAC36-99GO10337 between the U.S. Department of Energy, and the National Renewable Energy Laboratory, a division of the Midwest Research Institute.
- This invention relates to power generation systems in general and more specifically to power generation systems utilizing mixed working fluids.
- Power generation systems or power plants are well-known in the art and are widely used to generate electricity. Most such power generation systems generate electricity from heat energy derived from burning fossil fuels (e.g., coal or natural gas) and are referred to herein as thermal power plants. In addition to using heat energy derived from burning fossil fuels, thermal power plants can also be used with a wide variety of other heat sources, such as solar, geothermal, and nuclear sources.
- Traditionally, thermal power plants have operated in accordance with the well-known Rankine thermodynamic cycle. In the Rankine cycle, a so-called “pure” working fluid, such as water, is heated to produce vapor or steam. The steam is then expanded, typically through a turbine, in order to convert heat energy contained therein into mechanical work. In the case of an electric power generation system, the turbine is operatively connected to an electrical generator which produces the electricity. While power plants operating in accordance with the Rankine cycle are well-known and widely used, certain characteristics of the Rankine cycle impose fundamental limitations on the thermodynamic efficiency of the cycle. For example, a Rankine cycle operating with a pure working fluid suffers some thermodynamic irreversibilities due to the fact that the pure working fluid vaporizes at substantially constant temperature. These irreversibilities can be larger or smaller depending on the temperature difference between the heating medium and working fluid.
- Partly in an effort to solve some of the limitations associated with the use of a pure working fluid in the Rankine cycle, other types of thermodynamic cycles (e.g., any of the so-called Kalina cycles) have been developed which utilize mixed working fluids. Briefly, a mixed component working fluid comprises two or more vaporizable components which vaporize and condense progressively over a temperature range rather than at the relatively constant temperature of a so-called “pure” working fluid (e.g., water). Accordingly, thermodynamic cycles utilizing mixed working fluids can, if properly designed, realize increased efficiencies over similar thermodynamic cycles (e.g., the Rankine cycle) that utilize pure working fluids, such as water.
- One design consideration for mixed working fluid systems relates to the boiler or vapor generator that is used to vaporize the mixed working fluid. That is, since the mixed working fluid vaporizes over a temperature range, it is generally preferred to design the vapor generator so that heating function of the mixed working fluid closely follows the cooling function of the heating medium. Closely matching the heating and cooling functions of the working and heating fluids reduces the thermodynamic irreversibilities during the heating cycle, thus increasing the overall thermodynamic efficiency of the system. In accordance with this consideration, thermodynamic cycles utilizing mixed fluids often make use of countercurrent heat exchangers, in which the heating medium and mixed working fluid flow in opposite directions. In this manner, the heating function of the mixed working fluid can be made to more closely follow the cooling function of the heating medium.
- While such countercurrent heat exchangers have been used in mixed working fluid systems to achieve some performance and efficiency gains, there is still room for improvement, particularly in light of other requirements or limitations of the particular type of power generation system in which the heat exchanger is to be used. For example, a primary consideration of geothermal power generation systems relates to the so-called “brine effectiveness,” that is, the amount of useful work that can be extracted or derived from a given brine flow rate. A desirable geothermal power generation system will seek to maximize brine effectiveness.
- A power generating system according to the present invention may comprise a heat source and an incremental vapor generator system operatively associated with the heat source. The incremental vapor generator system includes a first heating section and a second heating section. The first heating section receives a mixed working fluid and generates a first heated working fluid stream comprising a vapor portion and a liquid portion. The second heating section is operatively associated with the first heating section and receives the liquid portion from the first heated working fluid stream. The second heating section generates a second heated working fluid stream comprising a vapor portion. An energy conversion device operatively associated with the incremental vapor generator system converts into useful work heat energy contained in the vapor portions of the first and second heated working fluid streams.
- Also disclosed is a method for generating power from a mixed working fluid that comprises the steps of incrementally heating the mixed working fluid to produce a first vapor stream and a second vapor stream; and converting into useful work heat energy contained in the first and second vapor streams.
- Illustrative and presently preferred embodiments of the invention are shown in the accompanying drawings in which:
- FIG. 1 is a schematic diagram of a power generating system according to the present invention utilizing parallel flow incremental vapor generation;
- FIG. 2 is an equilibrium/phase diagram of the mixed working fluid at the various stations of the power generating system shown in FIG. 1;
- FIG. 3 is a graphical representation of the heating and cooling functions of the mixed working fluid and the heating fluid for the power generating system shown in FIG. 1;
- FIG. 4 is a schematic diagram of a second embodiment of a power generating system according to the present invention utilizing serial flow incremental vapor generation;
- FIG. 5 is an equilibrium/phase diagram of the mixed working fluid at the various stations of the power generating system shown in FIG. 4; and
- FIG. 6 is a graphical representation of the heating and cooling functions of the mixed working fluid and the heating fluid for the power generating system of FIG. 4.
- A
power generating system 110 according to one embodiment of the present invention is shown in FIG. 1 and may comprise an incrementalvapor generator system 112 for vaporizing a mixed working fluid 114. The incrementalvapor generator system 112 incrementally vaporizes the mixed working fluid 114 with heat energy extracted from a heat source, such as, for example,geothermal brine 116. Alternatively, and as will be described in greater detail below, the present invention may be utilized with other types of heat sources and/or other types of heating fluids. - In the embodiment shown in FIG. 1, the incremental
vapor generator system 112 comprises a parallel flow incrementalvapor generation system 118 in which the mixed working fluid 114 is incrementally vaporized to form afirst vapor portion 120 and asecond vapor portion 122. The first andsecond vapor portions vapor mixer 124 before being directed to anenergy conversion system 126, which converts energy contained in the first andsecond vapor portions energy conversion system 126 comprises aturbine 128 and anelectrical generator 130. Accordingly, heat energy contained in the first andsecond vapor portions energy conversion system 126. In an alternate embodiment described below, the incremental vapor generator system may comprise a series flow incremental vapor generation system 218 (FIG. 4) in which the mixed working fluid is incrementally vaporized in a serial manner. - The parallel flow incremental
vapor generating system 118 utilized in thefirst embodiment 110 of the power generating system according to the present invention is shown in FIG. 1 and may comprise a heat exchanger orvaporizer 132 having aprimary loop 134 through which is caused to flow the heating fluid, e.g.,geothermal brine 116. The heat exchanger orvaporizer 132 may also comprise first andsecond heating sections primary loop 134 so that heat energy contained in the heating fluid (e.g., brine 116) is transferred to the mixed working fluid 114 flowing through the first andsecond heating sections heat exchanger 132 may also be provided with athird heating section 140 suitable for additionally heating the first andsecond vapor portions - The first and
second heating sections second separator systems second separator systems second heating sections first inlet 146 of thefirst separator 142 is connected to theoutlet 148 of thefirst heating section 136, whereas aliquid outlet 150 of thefirst separator 142 is connected to theinlet 152 of thesecond heating section 138. Asecond inlet 154 offirst separator 142 is connected to ahigh temperature recuperator 156. Avapor outlet 158 offirst separator 142 is connected to thevapor mixer 124. - The
second separator 144 is provided with aninlet 160 that is connected to theoutlet 162 of thesecond heating section 138. Aliquid outlet 164 ofsecond separator 144 is connected to thehigh temperature recuperator 156, whereas avapor outlet 166 is connected to thevapor mixer 124. - The
vapor mixer 124 is provided with avapor outlet 168 which, in the embodiment shown and described herein, is connected to thethird heating section 140. Thethird heating section 140 is used to further heat (e.g., superheat) the vaporized mixed working fluid 114 exiting themixer 124. Theoutlet 170 of thethird heating section 140 is connected to theenergy conversion system 126. As mentioned above, theenergy conversion system 126 may comprise aturbine 128 andelectrical generator 130. Theexhaust outlet 172 ofturbine 128 is connected to a low temperature recuperator 174. The low temperature recuperator 174 is in turn connected to acondenser 176 via amixer 178. Thecondenser 176 is operatively connected to theheat exchanger 132 via apump 180 and the high andlow temperature recuperators 156 and 174, respectively. - The
power generation system 110 may be operated as follows to convert into useful work heat energy contained in the heating fluid (e.g., geothermal brine 116). As was briefly described above, the mixed working fluid 114 utilized herein vaporizes progressively over an increasing temperature range. That is, the temperature of the vapor and liquid comprising the heated mixed working fluid 114 increases with increasing quality. The point at which vaporization begins (i.e., at 0% quality) is referred to herein as the “bubble point,” whereas the point at which vaporization is complete (i.e., at 100% quality) is referred to herein as the “dew point.” By way of example, the mixed working fluid 114 utilized in the preferred embodiments shown and described herein comprises a mixture of ammonia and water. Alternatively, other mixed working fluids could be used as well. - Referring now to FIGS. 1 and 2 simultaneously, the mixed working fluid feed stream114 exits the
condenser 176 at about the bubble point for the mixture. This corresponds to station L0 in FIG. 1 and the corresponding point L0 in FIG. 2. Before proceeding with the description, it should be noted that various points in thesystem 110 that are of interest thermodynamically are referred to herein as “stations” and are indicated in FIGS. 1 and 4 as encircled numbers or encircled letter-number combinations. Such stations are indicated on the equilibrium/phase diagrams (e.g., FIGS. 2 and 5) as points having corresponding numbers or letter-number combinations. Hence, station L0 is designated in FIG. 1 as encircled legend “L0”. The corresponding point in the equilibrium/phase diagram illustrated in FIG. 2 is also designated “L0”. - Continuing now with the description, the
pump 180 increases the pressure of the mixed working fluid 114 to a point suitable for use in the high pressure side of thepower generation system 110. The flow of the working fluid 114 is then split, with afirst stream 182 being directed through thehigh temperature recuperator 156 and asecond stream 184 being directed to the low temperature recuperator 174. The heating characteristics of thehigh temperature recuperator 156 and the flow rate of thefirst stream 182 are selected so that thefirst stream 182 is heated to a point above its bubble point at the particular pressure involved (e.g., about 425 pounds per square inch absolute (psia)). That is, thefirst stream 182 is heated to a quality greater than zero. By way of example, in one preferred embodiment, thefirst stream 182 is heated to a quality in the range of about 10% to about 40% (30% preferred). This quality corresponds to a vapor portion in the range of about 80% to about 96% (90% preferred) on a volume basis. The heatedfirst stream 182 is then directed to theinlet 154 offirst separator system 142. This is identified asstation 2 1 in FIG. 1 and aspoint 2 1 in FIG. 2. - The
second stream 184 is heated by the low temperature recuperator 174 and thereafter is directed to thefirst heating section 136 ofheat exchanger 132 where it is additionally heated to a temperature that exceeds the bubble point. This corresponds tostation 2 3 in FIG. 1 and to point 2 3 in FIG. 2. It is generally preferred that the heating characteristics of the low temperature recuperator 174 and thefirst heating section 136, as well as the flow rate of thesecond stream 184 be such that the mixed working fluid 114 comprising thesecond stream 184 is heated to about the same quality as thefirst stream 182. That is, it is preferred that thepoints second stream 148 from thefirst heating section 136 is then directed to thefirst inlet 146 of thefirst separator 142. - The
first separator system 142 receives the first and secondheated streams streams liquid outlet 150 of theseparator 142 and is directed to theinlet 152 of thesecond heating section 138. The vapor portion exits thevapor outlet 158 of thefirst separator 142 asfirst vapor stream 120. Thefirst vapor stream 120 is at about the dew point (i.e., 100% quality) for the particular concentration of the mixed working fluid 114 comprising thevapor portion stream 120. This corresponds to station v1 in FIG. 1 and to point v1 in FIG. 2. - Before proceeding with the description it should be noted that the concentrations of the constituents (e.g., ammonia and water) comprising the mixed working fluid114 are different for the liquid and vapor portions. For example, with reference now to FIG. 2, in one preferred embodiment wherein the mixed working fluid 114 comprises a mixture of ammonia and water, the first vapor portion stream 120 (corresponding to point v1 in FIG. 2) of the mixed working fluid 114 comprises a higher concentration of ammonia (e.g., slightly greater than about 0.95 on a mass basis) than does the liquid portion (
point 3 in FIG. 2) of the mixed working fluid 114. The liquid portion of the mixed working fluid 114 atpoint 3 has an ammonia concentration that is slightly less than about 0.55 (on a mass basis). Consequently, any characteristics (e.g., quality) specifically recited herein for the mixed working fluid 114 at a particular station refer to the working fluid 114 in the particular state (e.g., vapor or liquid) and at the corresponding concentration at the referenced station. For example, at station v1, the mixed working fluid 114 comprises a vapor having an ammonia concentration that is slightly greater than about 0.95 and is at about the dew point (i.e., a quality of about 100%) for the mixture at that particular ammonia concentration. Atstation 3, the mixed working fluid 114 comprises a liquid having an ammonia concentration that is slightly less than about 0.55 and is at about the bubble point (i.e., a quality of about 0%) for the mixture at the lower ammonia concentration. The ammonia concentrations (i.e., mass fractions) for the ammonia/water mixed working fluid 114 that may be utilized in the preferred embodiments of the present invention are shown in FIGS. 2 and 4 for the corresponding liquid and vapor portions of the mixed working fluid at the various stations. - With the foregoing points in mind, the liquid portion of the mixed working fluid114 from the
first separator 142 is at about the bubble point of the liquid portion of mixed working fluid 114 at the corresponding ammonia concentration. That is, the liquid portion is at about the bubble point for the lower ammonia concentration of the liquid portion of the mixed working fluid 114. This corresponds tostation 3 in FIG. 1 and to point 3 in FIG. 2. The liquid portion is directed into theinlet 152 of thesecond heating section 138 whereupon it is heated to a temperature in excess of the bubble point. It is generally preferred that the liquid portion be heated in thesecond heating section 138 to about the same quality as the mixed working fluid atstations second heating section 138 should be about the same as the qualities of the working fluid streams exiting thefirst heating section 136 and thehigh temperature recuperator 156. For example, in the embodiment shown and described herein, the mixed working fluid stream exits thesecond heating section 138 at a quality in the range of about 10% to about 40% (30% preferred), which corresponds to a vapor portion in the range of about 80% to about 96% (90% preferred) on a volume basis. This corresponds tostation 4 in FIG. 1 and to point 4 in FIG. 2. - The
second separator system 144 receives the heated mixed fluid from thesecond heating section 138 and separates the heated mixed fluid into a liquid portion and a vapor portion. The liquid portion exits theliquid outlet 164 of theseparator 144 and is directed to thehigh temperature recuperator 156 whereupon it surrenders a portion of its heat to thefirst working stream 182. The vapor portion fromseparator 144 exits thevapor outlet 166 as the secondvapor portion stream 122. The secondvapor portion stream 122 is at about the dew point (i.e., 100% quality) for the higher ammonia concentration of the mixed working fluid 114 that comprises the secondvapor portion stream 122. See station v2 in FIG. 1 and point v2 in FIG. 2. - The
vapor mixer 124 receives the first and second vapor streams 120 and 122 and combines them into a combinedvapor stream 186. The combinedvapor stream 186 corresponds to station v3 in FIG. 1 and to point v3 in FIG. 2. The combinedvapor stream 186 may be additionally heated (e.g., superheated) by thethird heating section 140 to a temperature greater than the dew point temperature for the combinedvapor stream 186. Thesuperheated stream 188 exiting thethird heating section 140 corresponds to station v4 in FIG. 1 and to point v4 in FIG. 2. Thestream 188 is then directed to theenergy conversion system 126. - The
energy conversion system 126 extracts heat energy from thesuperheated stream 188, converting it into useful work. In the embodiment shown and described herein, heat energy contained in the first and second vapor streams 120 and 122 (which comprise combinedstream 186 and superheated stream 188) is converted into electrical work by theturbine 128 and theelectrical generator 130 comprising theenergy conversion system 126. - The
exhaust stream 172 from theturbine 128 corresponds to station v5 in FIG. 1 and to point v5 in FIG. 2 and is at a temperature that is greater than the dew point temperature for the mixed working fluid at the reduced pressure on the low pressure side of thepower generating system 110. By way of example, in the embodiment shown and described herein, the mixed working fluid 114 is at a pressure of about 71 psia on the low pressure side. Alternatively, the exhaust stream could exit theturbine 128 at a temperature below the dew point of the mixed working fluid if the turbine is capable of handling wet mixtures. Theexhaust stream 172 fromturbine 128 is thereafter directed to the low temperature recuperator 174 wherein it surrenders a portion of its heat energy to the second workingfluid stream 184. The cooledexhaust stream 172 exits the low temperature recuperator 174 at station v6 at a temperature between the bubble and dew points for the mixed working fluid. By way of example, in one preferred embodiment, the cooledexhaust stream 172 exits the low temperature recuperator 174 at a quality in the range of about 0% to about 100% (45% preferred). See also point v6 in FIG. 2. - The mixed working fluid exiting the low temperature recuperator174 is then mixed with the liquid portion exiting the
high temperature recuperator 156 in themixer 178. The combined working fluid stream exitsmixer 178 at station v7 which corresponds to point v7 in FIG. 2. The combined working fluid stream is then condensed to the bubble point (station L0 in FIG. 1 and point L0 in FIG. 2) by thecondenser 176. The condensed stream is then returned to the high pressure side of the system bypump 180 and the cycle is repeated. - A significant advantage of the
power generating system 110 according to the present invention is that it results in closely matched heating and cooling curves for the working and heating fluids, respectively. For example, with reference now to FIG. 3 the heating curve or function 190 of the mixed working fluid closely follows the cooling curve or function 192 of the heating fluid (e.g., brine 116). The closely matched heating andcooling functions heat exchanger 132. The closely matched heating and cooling functions also allow thebrine 116 to be cooled to a lower temperature, closer to the bubble point of the working fluid, than is possible with prior systems. Consequently, thepower generating system 110 of the present invention substantially reduces the heating fluid (e.g., brine 116) flow rate required for a given amount of useful work. Accordingly, thepower generating system 110 can be used with considerable advantage in geothermal power generation systems wherein it is desired to minimize the brine flow rate per kilowatt of electricity produced. - Having briefly described one embodiment of the
power generating system 110, as well as some of its more significant features and advantages, the various embodiments of the power generating system according to the present invention will now be described in detail. However, before proceeding with the description, it should be noted that while the various embodiments of the power generating system are shown and described herein as they could be used in a geothermal electrical generating system utilizinghot brine 116 as the heating fluid, the present invention is not limited to use in geothermal electrical generating systems. In fact, power generating systems according to the present invention could be used with any of a wide variety of heating fluids and working fluids that are now known in the art or that may be developed in the future, as would be obvious to persons having ordinary skill in the art after having become familiar with the teachings of the present invention. Consequently, the present invention should not be regarded as limited to the particular applications and/or heating and working fluids shown and described herein. - With the foregoing considerations in mind, one embodiment of a
power generating system 110 according to the present invention comprises an incrementalvapor generator system 112 for vaporizing a mixed working fluid 114 utilizing heat obtained from a suitable heat source. By way of example, in the embodiments shown and described herein, the heat source may comprisegeothermal brine 116. Thegeothermal brine 116 comprises the heat source or heating fluid and is used to vaporize the working fluid 114 in the incrementalvapor generator system 112. - The working fluid114 used in the
power generation system 110 may comprise any of a wide range of mixed, non-azeotropic fluids now known in the art or that may be developed in the future suitable for use in the particular application. As used herein, the term “mixed fluid” refers to any fluid wherein the temperature of the vapor and liquid components increases with increasing quality. By way of example, in the embodiment shown and described herein, the mixed working fluid comprises a mixture of ammonia and water. - As was briefly mentioned above, in one embodiment of the invention the incremental
vapor generator system 112 comprises a parallel flow incrementalvapor generation system 118. In the parallel flow incrementalvapor generation system 118, the mixed working. fluid 114 is incrementally vaporized to form afirst vapor portion 120 and asecond vapor portion 122. The first andsecond vapor portions energy conversion system 126, hence the designation parallel flow incrementalvapor generation system 118. - With reference now primarily to FIG. 1, the parallel flow incremental
vapor generating system 118 utilized in one embodiment of thepower generating system 110 according to the present invention comprises a heat exchanger orvaporizer 132 having aprimary loop 134 through which is caused to flow the heating fluid. As mentioned above, in the embodiment shown and described herein, the heating fluid comprisesgeothermal brine 116. Alternatively, other types of heating fluids may be used, as would be obvious to persons having ordinary skill in the art after having become familiar with the teachings of the present invention. - The heat exchanger or
vaporizer 132 may also comprise first andsecond heating sections primary loop 134. Accordingly, heat energy contained in thebrine 116 is transferred to the mixed working fluid 114 flowing in the first andsecond heating sections heat exchanger 132 may also be provided with athird heating section 140 suitable for additionally heating the first andsecond vapor portions third heating section 140 is used to heat the first andsecond vapor portions - It is generally preferred that the
heat exchanger 132 comprise a counter-current heat exchanger in which the inlet end of theprimary loop 134 is thermally adjacent the “hottest” heating section (e.g., the third heating section 140) and in which the outlet end is thermally adjacent the “coolest” heating section (e.g, the first heating section 136). Such an arrangement makes it easier to more closely match theheating function 190 of the working fluid 114 with thecooling function 192 of the heating fluid (e.g., brine 116). See FIG. 3. - The exact number of heating sections (e.g.,
heating sections heat exchanger 132 may vary depending on the particular application, the particular heating and working fluids used, as well as on the number of stages (e.g., vapor separators) used to achieve the incremental heating of the working fluid in the manner shown and described herein. That is, the number of heating sections comprising the heat exchanger in any given application could be readily determined by persons having ordinary skill in the art after having become familiar with the teachings of the present invention and by applying the teachings to the particular application. Consequently, the present invention should not be regarded as limited to a heat exchanger having any particular number of heating sections. - The
heat exchanger 132 may be constructed from any of a wide range of materials and in accordance with any of a wide range of techniques that are now known in the art or that may be developed in the future that would be suitable for the particular application. However, since heat exchangers of the type described herein could be readily fabricated by persons having ordinary skill in the art after having become familiar with the teachings of the present invention, and since the details of such heat exchangers are not necessary to understand or practice the present invention, the heat exchangers used in the embodiments shown and described herein will not be described in further detail herein. - The first and
second heating sections heat exchanger 132 are operatively associated with first andsecond separator systems second separator systems second heating sections - The
first separator system 142 comprises afirst inlet 146, asecond inlet 154, aliquid outlet 150, and avapor outlet 158. Thefirst inlet 146 is connected to theoutlet 148 of thefirst heating section 136 so that heated mixed working fluid from thefirst heating section 136 enters theseparator system 142. Thesecond inlet 154 of thefirst separator system 142 is connected to thehigh temperature recuperator 156 so that the first mixed workingfluid stream 182 from thehigh temperature recuperator 156 is also directed into theseparator system 142. Theliquid outlet 150 of thefirst separator system 142 is connected to theinlet 152 of thesecond heating section 138 ofheat exchanger 132. Thevapor outlet 158 of thefirst separator system 142 is connected to thevapor mixer 124. - The
first separator system 142 may comprise any of a wide range of separator systems that are well-known in the art that would be suitable for separating vapor and liquid portions from an incoming wet mixture stream (e.g., the heated working fluid 114). Consequently, the present invention should not be regarded as limited to any particular type of separator system. - The
second separator system 144 may be similar to thefirst separator system 142, except that thesecond separator system 144 is provided with but asingle inlet 160 connected to theoutlet 162 of thesecond heating section 138. The arrangement is such that thesecond separator system 144 receives the heated mixed working fluid 114 from thesecond heating section 138 ofheat exchanger 132. Aliquid outlet 164 of thesecond separator 144 is connected to thehigh temperature recuperator 156, whereas avapor outlet 166 is connected to thevapor mixer 124. - The
high temperature recuperator 156 connected to theliquid outlet 164 ofsecond separator system 144 is used to recover heat contained in the liquid portion separated by thesecond separator 144. The recovered heat is used to pre-heat the first mixed workingfluid stream 182. In the embodiment shown and described herein, theliquid outlet 164 of thesecond separator 144 is connected to aheating loop 155 of thehigh temperature recuperator 156, whereas aheated loop 157 ofhigh temperature recuperator 156 is connected between thepump 180 and thesecond inlet 154 offirst separator system 142. The separated liquid portion in the heating loop surrenders heat to the first mixed workingfluid stream 182 in theheated loop 157, thereby pre-heating the first mixed workingfluid stream 182. Thereafter, the separated liquid portion passes through anexpansion valve 194 before entering the low pressure side of thesystem 110. - The
vapor mixer 124 is connected to thevapor outlets second separator systems second vapor portions vapor outlet 168 on themixer 124 is connected to thethird heating section 140. Theoutlet 170 of thethird heating section 140 is connected to theenergy conversion system 126. - The
vapor mixer 124 may comprise any of a wide range of devices known in the art or that may be developed in the future that would be suitable for mixing together the first andsecond vapor portions - The
energy conversion system 126 may comprise any of a wide range of systems and devices suitable for converting into useful work heat energy contained in the heated mixed working fluid 114 exiting the parallel flow vapor generator 118 (orthird heating section 140, if a third heating section is used). By way of example, in the embodiments shown and described herein, theenergy conversion system 126 comprises aturbine 128 and anelectric generator 130 connected thereto. Theturbine 128 andelectric generator 130 may comprise any of a wide range of systems and devices that are well-known in the art and readily commercially available. Consequently, theturbine 128 andelectric generator 130 utilized in one preferred embodiment of the invention will not be described in greater detail herein. - The
exhaust outlet 172 ofturbine 128 is connected to a low temperature recuperator 174. The low temperature recuperator 174 recovers heat contained in the turbine exhaust stream and uses it to pre-heat the second mixed workingfluid stream 184. More specifically, theexhaust outlet 172 ofturbine 128 is connected to aheating loop 173 of the low temperature recuperator 174, whereas aheated loop 175 of the low temperature recuperator 174 is connected between thepump 180 and thefirst heating section 136 of theheat exchanger 132. The turbine exhaust stream in theheating loop 173 surrenders heat to the second mixed workingfluid stream 184 in theheated loop 175, thereby pre-heating the second mixed workingfluid stream 184 before the same enters thefirst heating section 136. Thereafter, the exhaust stream is combined in themixer 178 with the separated liquid portion exiting theexpansion valve 194. Acondenser 176 connected to themixer 178 receives the combined cooled mixed working fluid 114, condenses it, and returns it to pump 180. - The
condenser 176 may comprise any of a wide range of condensers that are well-known in the art or that may be developed in the future that would be suitable for condensing the combined cooled mixed working fluid 114 from themixer 178. By way of example, in the embodiment shown and described herein, thecondenser 176 comprises an air-cooled condenser in whichair 196 is used to condense the mixed working fluid 114 flowing in thecondenser 176. Alternatively, other cooling media besides air may be used to condense the mixed working fluid 114. - The
power generation system 110 may be operated as follows to convert into useful work heat energy derived from the heating fluid. Consider, for example, a geothermal power generation system which generates electricity fromgeothermal brine 116 extracted from the earth. Thegeothermal brine 116 serves as the heating fluid and, in the example described herein, enters theprimary loop 134 of theheat exchanger 132 at a temperature of about 335° F., although other temperatures are possible. The mixed working fluid 114 may comprise a mixture of ammonia and water and is maintained at a pressure of about 425 pounds per square inch absolute (psia) on the high pressure side of thepower generating system 110. The low pressure side of thepower generating system 110 is maintained at a pressure of about 71 psia. Alternatively, other mixed fluids may be used at other pressures, as would be obvious to persons having ordinary skill in the art after having become familiar with the teachings of the present invention. The ammonia/water mixture that comprises the mixed working fluid 114 vaporizes progressively over an increasing temperature range. That is, the temperature of the vapor and liquid comprising the heated mixed working fluid increases with increasing quality. - Referring now to FIGS.1-3, the mixed working fluid feed stream 114 exits the
condenser 176 at station L0 at about the bubble point for the mixture 114. This station corresponds to point L0 in FIG. 2. Thepump 180 increases the pressure of the mixed working fluid 114 to a pressure suitable for use in the high pressure side of thepower generating system 110. In the embodiment shown and described herein, the high pressure side of thesystem 110 is maintained at a pressure of about 425 psia. Therefore, thepump 180 increases the pressure of the mixed working fluid 114 to a pressure of about 425 psia. The mixed working fluid stream 114 exiting thepump 180 is then split into a first workingfluid stream 182 and a second workingfluid stream 184. The first workingfluid stream 182 is directed through theheated loop 157 of thehigh temperature recuperator 156 whereupon it is heated by the liquid portion from thesecond separator 144 passing through theheating loop 155. The heating characteristics of thehigh temperature recuperator 156 and the flow rate of thefirst stream 182 are such that thefirst stream 182 is heated to a temperature in excess of its bubble point. This corresponds tostation 2 1 in FIG. 1 and to point 2 1 in FIG. 2. - By way of example, in the embodiment shown and described herein, the
first stream 182 is heated to a quality in the range of about 10% to about 40% (30% preferred). This quality range corresponds to a vapor portion range of about 80% to about 96% (90% preferred) on a volume basis. So heating the first workingfluid stream 182 to a vapor portion in the range specified herein provides for good heat transfer characteristics in thehigh temperature recuperator 156. That is, some loss of efficiency in thehigh temperature recuperator 156 will occur if the first workingfluid stream 182 is heated to a vapor portion that is substantially greater than the vapor portion range specified herein. After being heated in thehigh temperature recuperator 156, the heated first workingfluid stream 182 is directed to theinlet 154 of thefirst separator system 142. - The second working
fluid stream 184 is directed to theheated loop 175 of the low temperature recuperator 174 whereupon it is pre-heated by theexhaust stream 172 exiting theturbine 128. Thereafter, the pre-heated second workingfluid stream 184 is directed to thefirst heating section 136 ofheat exchanger 132 which heats the second workingfluid stream 184 to a temperature in excess of the bubble point. This corresponds tostation 2 3 in FIG. 1 and to point 2 3 in FIG. 2. It is generally preferred that the flow rate of thesecond stream 184 be matched to the heating characteristics of the low temperature recuperator 174 and thefirst heating section 136 so that the mixed working fluid 114 comprising the second workingfluid stream 184 is heated to about the same quality as thefirst stream 182. That is, it is preferred that thepoints fluid stream 184 is heated to a quality in the range of about 10% to about 40% (30% preferred), which corresponds to a vapor portion in the range of about 80% to about 96% (90% preferred). - In the embodiment shown and described herein, the mass ratio of the first working
fluid stream 182 to the second workingfluid stream 184 is about 1:4. That is, most of the working fluid 114 is directed to thesecond stream 184, with only a small amount (i.e., ¼ on a mass basis) being directed through thehigh temperature recuperator 156 as first workingfluid stream 182. Of course, the mixed working fluid stream 114 may be divided in accordance with other mass ratios depending on the characteristics of the particular system. - Referring back now primarily to FIG. 1, the
first separator system 142 receives the first and secondheated streams streams liquid outlet 150 of thefirst separator 142 and is directed to theinlet 152 of thesecond heating section 138. The vapor portion exits thevapor outlet 158 of thefirst separator 142 as a firstvapor portion stream 120. The first vapor portion stream is at about the dew point (i.e., 100% quality) for the mixed working fluid 114. This corresponds to station v1 in FIG. 1 and to point v1 in FIG. 2. - The liquid portion from the
first separator 142 is at about the bubble point of the mixed working fluid 114. Seestation 3 in FIG. 1 andpoint 3 in FIG. 2. The liquid portion is directed into theinlet 152 of thesecond heating section 138 whereupon it is heated to a temperature in excess of the bubble point. It is generally preferred that the liquid portion be heated to about the same quality as the mixed working fluid atstations second heating section 138 should be about the same as the qualities of the working fluid streams exiting thefirst heating section 136 and thehigh temperature recuperator 156. For example, in the embodiment shown and described herein, the mixed working fluid stream exits thesecond heating section 138 at a quality in the range of about 10% to about 40% (30% preferred). This corresponds to a vapor portion in the range of about 80% to about 96% (90% preferred). Seestation 4 in FIG. 1 andpoint 4 in FIG. 2. As discussed above, heating the mixed working fluid to the quality ranges specified herein provides a good balance between temperature rise and heat transfer efficiency in thesecond heating section 138. - The
second separator system 144 receives the heated mixed fluid from thesecond heating section 138 and separates the heated mixed fluid into a liquid portion and a vapor portion. The liquid portion exits theliquid outlet 164 of theseparator 144 and is directed to thehigh temperature recuperator 156 whereupon it surrenders a portion of its heat to the first workingfluid stream 182. Thereafter, the cooled liquid portion is expanded through theexpansion valve 194 to the low pressure side of thepower generating system 110. Seestation 5 2 in FIG. 1 andpoint 5 2 in FIG. 2. The cooled, expanded liquid portion is then combined with the turbine exhaust stream inmixer 178. - The vapor portion from the
second separator 144 exits thevapor outlet 166 ofseparator 144 as the secondvapor portion stream 122. The secondvapor portion stream 122 is at about the dew point (i.e., 100% quality) and corresponds to station v2 in FIG. 1 and to point v2 in FIG. 2. - The
vapor mixer 124 receives the first and second vapor streams 120 and 122 and combines them into a combinedvapor stream 186. The combinedvapor stream 186 corresponds to station v3 in FIG. 1 and to point v3 in FIG. 2. If desired, the combinedvapor stream 186 may be additionally heated by thethird heating section 140 to a temperature greater than the dew point temperature for the combinedvapor stream 186. That is, the combinedvapor stream 186 may be superheated in thethird heating section 140. Thesuperheated stream 188 exiting thethird heating section 140 is designated as station v4 in FIG. 1 and corresponds to point v4 in FIG. 2. Thestream 188 is then directed to theenergy conversion system 126. - The
energy conversion system 126 extracts heat energy from thesuperheated stream 188, converting it into useful work. In the embodiment shown and described herein, heat energy contained in the first and second vapor streams 120 and 122 (which comprise combinedstream 186 and superheated stream 188) is converted into electrical work by theturbine 128 and theelectrical generator 130 comprising theenergy conversion system 126. - The
superheated stream 188 is expanded in theturbine 128 and exits theturbine 128 asexhaust stream 172. See station v5 in FIG. 1 and point v5 in FIG. 2. It is generally preferred that the expansion process be terminated before the mixed working fluid 114 is cooled below the dew point temperature. By way of example, in the embodiment shown and described herein, the mixed working fluid 114 is expanded to a pressure of about 71 psia and to a temperature of about 150° F., which is below the dew point. That is, the mixed working fluid 114 is cooled to a temperature below the dew point temperature since, in the embodiment shown and described herein, theenergy conversion device 126 functions effectively with wet mixtures. Theexhaust stream 172 is thereafter directed to the low temperature recuperator 174 wherein it surrenders a portion of its heat energy to the second workingfluid stream 184 flowing in theheated loop 175 of low temperature recuperator 174. The cooledexhaust stream 172 exits the low temperature recuperator 174 at station v6 at a temperature between the bubble and dew points for the mixed working fluid. See point v6 in FIG. 2. By way of example, in the embodiment shown and described herein, the cooledexhaust stream 172 exits the low temperature recuperator 174 at a quality in the range of about 0% to about 100% (45% preferred). - The mixed working fluid exiting the low temperature recuperator174 is then mixed in
mixer 178 with the liquid portion flowing through theexpansion valve 194. The combined working fluid stream that exitsmixer 178 is designated as station v7 and corresponds to point v7 in FIG. 2. The combined working fluid stream is then condensed by thecondenser 176 to about the bubble point, (i.e., at station L0 in FIG. 1 and point L0 in FIG. 2). The condensed stream is then returned to the high pressure side of the system bypump 180 and the cycle is repeated. - The
power generating system 110 just described results in the closely matched heating andcooling functions heating curve 190 of the mixed working fluid 114 closely follows thecooling curve 192 of the heating fluid (e.g., geothermal brine 116). - As mentioned above, the
first embodiment 110 of the power generating system according to the present invention utilizes a parallel flowvapor generator system 118 in which the working fluid is incrementally vaporized to produce first and second vapor portion streams 120 and 122 which are then combined in a parallel manner (e.g., by mixer 124) before being superheated (if desired) and directed to theenergy conversion system 126. However, other incremental vaporization arrangements are possible in accordance with the teachings of the present invention. - With reference now to FIGS.4-6, a
second embodiment 210 of a power generating system according to the present invention embodies an incrementalvapor generator system 212 that comprises a series flowvapor generator system 218. Briefly, in the series flowvapor generator system 218, the mixed workingfluid 214 is incrementally vaporized to form afirst vapor portion 220 and asecond vapor portion 222. Thefirst vapor portion 220 is then used to condense or separate a liquid portion from a heated mixed workingfluid stream 221 from which is derived thesecond vapor portion 222. Since, in the case of the mixed workingfluid 214, the liquid is “lean” and thefirst vapor portion 220 is “rich,” thefirst vapor portion 220 condenses on the lean liquid. The heat of condensation causes additional vapor to be produced. Accordingly, the series flowvapor generator system 218 produces the vapor streams 220 and 222 in a serial manner. - With reference now primarily to FIG. 4, the serial flow incremental
vapor generating system 218 utilized in thesecond embodiment 210 of the power generating system according to the present invention comprises a heat exchanger orvaporizer 232 having aprimary loop 234 through which is caused to flow the heating fluid. In the embodiment shown and described herein, the heating fluid comprisesgeothermal brine 216, although other types of heating fluids may be used, as would be obvious to persons having ordinary skill in the art after having become familiar with the teachings of the present invention. The heat exchanger orvaporizer 232 may also comprise first andsecond heating sections primary loop 234 so that heat energy contained in thebrine 216 is transferred to the mixed workingfluid 214 flowing in the first andsecond heating sections heat exchanger 232 may also be provided with athird heating section 240 suitable for additionally heating the combined first andsecond vapor portions first embodiment 110, thethird heating section 240 of thesecond embodiment 210 is used to heat the first andsecond vapor portions - It is generally preferred that the
heat exchanger 232 be of the counter-current type in which the inlet end of theprimary loop 234 is thermally adjacent the “hottest” heating section (e.g., the third heating section 240) and the outlet end is thermally adjacent the “coolest” heating section (e.g, the first heating section 236). Such an arrangement allows thesystem 210 to more closely match theheating function 290 of the workingfluid 214 with thecooling function 292 of the heating fluid (e.g., brine 216). See FIG. 6. - The exact number of heating sections (e.g.,
heating sections heat exchanger 232 may vary depending on the particular application, the particular heating and working fluids used, as well as the number of stages used to achieve the incremental heating of the workingfluid 214 in the serial manner described herein. The number of heating sections comprising the heat exchanger in any given application could be readily determined by persons having ordinary skill in the art after having become familiar with the teachings of the present invention and by applying the teachings to the particular application. Consequently, the present invention should not be regarded as limited to a heat exchanger having any particular number of heating sections. - The
heat exchanger 232 may be constructed from any of a wide range of materials and in accordance with any of a wide range of techniques that are now known in the art or that may be developed in the future that would be suitable for the particular application. However, since heat exchangers of the type described herein could be readily fabricated by persons having ordinary skill in the art after having become familiar with the teachings of the present invention, and since the details of such heat exchangers are not necessary to understand or practice the present invention, the heat exchangers used in the embodiments shown and described herein will not be described in further detail herein. - The first and
second heating sections heat exchanger 232 are operatively associated with anintegral separator system 241 comprising afirst separator section 242 and asecond separator section 244. As will be described in greater detail below, the first andsecond separator sections integral separator system 241 separate liquid and vapor portions (not shown) from respective first and second heated mixed workingfluid streams - The
first separator section 242 ofintegral separator system 241 is provided with aninlet 246 that is connected to thehigh temperature recuperator 256 and thefirst heating section 236 in the manner best seen in FIG. 4. The arrangement is such that thefirst separator section 242 receives the first heated workingfluid stream 219. Theliquid outlet 250 of thefirst separator section 242 is connected to aninlet 252 of thesecond heating section 238. - The
second separator section 244 ofintegral separator system 241 is provided with aninlet 260 connected to theoutlet 262 ofsecond heating section 238 so that thesecond separator section 244 receives the second heated workingfluid stream 221 from thesecond heating section 238. Thesecond separator section 244 is also provided with acollector 264 for collecting additional amounts of separated liquid. Thecollector 264 is connected to aheating loop 255 of thehigh temperature recuperator 256. Avapor outlet 266 provided in thesecond separator section 244 is connected to thethird heating section 240. Theoutlet 270 of thethird heating section 240 is connected to theenergy conversion system 226. - The
high temperature recuperator 256 is connected to thecollector 264 of thesecond separator section 244 ofintegral separator 241. Thehigh temperature recuperator 256 recovers heat contained in the liquid portion separated by thesecond separator section 244 of theintegral separator 241. The recovered heat is used to heat the pre-heated second workingfluid stream 282. In the embodiment shown and described herein, thecollector 264 is connected to theheating loop 255 of thehigh temperature recuperator 256, whereas aheated loop 257 ofhigh temperature recuperator 256 is connected in parallel with thefirst heating section 236 of theheat exchanger 232. Theheating loop 255 is connected to anexpansion valve 294 which returns the cooled liquid portion to the low pressure side of thepower generating system 210. - As was the case for the first embodiment110 (FIG. 1) of the power generating system, the
energy conversion system 226 of thesecond embodiment 210 of the power generating system may comprise any of a wide range of systems and devices suitable for converting into useful work heat energy contained in the heated mixed workingfluid 214 exiting the series flow vapor generator 218 (orthird heating section 240, if a third heating section is used). By way of example, theenergy conversion system 226 comprises aturbine 228 and anelectric generator 230 connected thereto. Theturbine 228 andelectric generator 230 may comprise any of a wide range of systems and devices that are well-known in the art and readily commercially available. Consequently, theturbine 228 andelectric generator 230 utilized in one preferred embodiment of the invention will not be described in greater detail herein. - The
exhaust outlet 272 ofturbine 228 is connected to alow temperature recuperator 274. Thelow temperature recuperator 274 recovers heat contained in the turbine exhaust stream and uses it to pre-heat the mixed workingfluid stream 214. More specifically, theexhaust outlet 272 ofturbine 228 is connected to aheating loop 273 of thelow temperature recuperator 274, whereas aheated loop 275 of thelow temperature recuperator 274 is connected between thepump 280 and the parallel arrangement of theheating loop 257 of thehigh temperature recuperator 256 and thefirst heating section 236 ofheat exchanger 232. The turbine exhaust stream in theheating loop 273 surrenders heat to the mixed workingfluid stream 214 in theheated loop 275, thereby pre-heating the mixed workingfluid stream 214 before the same enters thehigh temperature recuperator 256 and thefirst heating section 236. Thereafter, the exhaust stream is combined with the separated liquid portion exiting theexpansion valve 294. Acondenser 276 connected to thelow temperature recuperator 274 andexpansion valve 294 receives the combined cooled mixed workingfluid 214, condenses it, and returns it to pump 280. - The
condenser 276 may comprise any of a wide range of condensers that are well-known in the art or that may be developed in the future that would be suitable for condensing the combined cooled mixed workingfluid 214. By way of example, in the embodiment shown and described herein, thecondenser 276 comprises an air-cooled condenser in which air 296 is used to condense the mixed workingfluid 214 flowing in thecondenser 276. - The
second embodiment 210 of the power generation system of the present invention may be operated as follows to convert into useful work heat energy derived from the heating fluid, i.e.,geothermal brine 216 extracted from the earth. As was the case for the first embodiment, thegeothermal brine 216 may enter theprimary loop 234 of theheat exchanger 232 at a temperature of about 335° F., although other temperatures are possible. The mixed workingfluid 214 may comprise a mixture of ammonia and water and is maintained at a pressure of about 250 psia on the high pressure side of thepower generating system 210. The low pressure side is maintained at a pressure of about 43 psia. Alternatively, other mixed working fluids may be used at other pressures, as would be obvious to persons having ordinary skill in the art after having become familiar with the teachings of the present invention. - With reference now to FIGS.4-6, the mixed working
fluid stream 214 exits thecondenser 276 at station L0 about the bubble point for themixture 214. This station corresponds to point L0 in FIG. 5. Thepump 280 increases the pressure of the mixed workingfluid 214 to a pressure suitable for use in the high pressure side of thepower generating system 210. In the embodiment shown and described herein, the high pressure side of thesystem 210 is maintained at a pressure of about 250 psia. Therefore, thepump 280 increases the pressure of the mixed workingfluid 214 to a pressure of about 250 psia. The mixed workingfluid stream 214 exiting thepump 280 is then directed to theheated loop 275 of thelow temperature recuperator 274 which pre-heats the mixed workingfluid 214. Seestation 2 of FIG. 4 andcorresponding point 2 in FIG. 5. The pre-heated mixed workingfluid stream 214 is then split or divided into afirst stream 282 and asecond stream 284. Thefirst stream 282 is directed through theheated loop 257 of thehigh temperature recuperator 256 whereupon it is heated by the liquid portion extracted from thesecond separator section 244 by thecollector 264. The heating characteristics of thehigh temperature recuperator 256 and the flow rate of thefirst stream 282 are such that thefirst stream 282 is heated to a temperature in excess of its bubble point. This corresponds tostation 3 2 in FIG. 4 and to point 3 2 in FIG. 5. - In the embodiment shown and described herein, the
first stream 282 is heated to a quality in the range of about 10% to about 40% (30% preferred). This quality range corresponds to a vapor portion range of about 80% to about 96% (90% preferred) on a volume basis. So heating the first workingfluid stream 282 to a vapor portion in the specified range provides for good heat transfer characteristics in thehigh temperature recuperator 256. That is, some loss of efficiency in thehigh temperature recuperator 256 will be experienced if the first workingfluid stream 282 is heated to a vapor portion that is substantially greater than the vapor portion range described herein. After being heated in thehigh temperature recuperator 256, the heated first workingfluid stream 282 mixed with the heated workingfluid stream 284 exiting thefirst heating section 236 and directed into theinlet 246 offirst separator section 242 as first heated workingfluid stream 219. Seestation 3 in FIG. 4 andcorresponding point 3 in FIG. 5. - The
second stream 284 is directed to thefirst heating section 236 of theheat exchanger 232 which heats the second workingfluid stream 284 to a temperature in excess of the bubble point. This corresponds tostation 3 1 in FIG. 4 and to point 3 1 in FIG. 5. It is generally preferred that the flow rate of thesecond stream 284 be matched to the heating characteristics of thefirst heating section 236 so that the mixed workingfluid 214 comprising the second workingfluid stream 284 is heated to about the same quality as thefirst stream 282. That is, it is preferred that thepoints fluid stream 284 is heated to a quality in the range of about 10% to about 40% (30% preferred), which corresponds to a vapor portion in the range of about 80% to about 98% (90% preferred). - In the embodiment shown and described herein, the mass ratio of the first working
fluid stream 282 to the second workingfluid stream 284 is about 1:4. That is, most of the workingfluid 214 is directed to thesecond stream 284, with only a small amount (i.e., ¼ on a mass basis) being directed through thehigh temperature recuperator 256 as first workingfluid stream 282. Of course, the mixed workingfluid 214 may be divided in accordance with other mass ratios depending on the characteristics of the particular system. - Still referring primarily to FIG. 4, the
first separator section 242 inintegral separator system 241 receives the first and secondheated streams fluid stream 219 and separates thestream 219 into a liquid portion and avapor portion 220. The liquid portion exits theliquid outlet 250 of thefirst separator section 242 and is directed to theinlet 252 of thesecond heating section 238. Thevapor portion 220 is at about the dew point (i.e., 100% quality) for the mixed workingfluid 214. This corresponds to station v1 in FIG. 4 and to point v1 in FIG. 5. - The liquid portion from the
first separator 242 is at about the bubble point of the mixed workingfluid 214. Seestation 4 in FIG. 4 andpoint 4 in FIG. 5. The liquid portion is directed into theinlet 252 of thesecond heating section 238 whereupon it is heated to a temperature in excess of the bubble point. This corresponds tostation 5 in FIG. 4 and to point 5 in FIG. 5. It is generally preferred that the liquid portion be heated to about the same quality as the mixed working fluid atstations second heating section 238 should be about the same as the qualities of the working fluid streams exiting thefirst heating section 236 and thehigh temperature recuperator 256. For example, in the embodiment shown and described herein, the mixed working fluid stream exits thesecond heating section 238 at a quality in the range of about 10% to about 40% (30% preferred). This corresponds to a vapor portion in the range of about 80% to about 98% (90% preferred). As discussed above, heating the mixed working fluid to the quality ranges specified herein provides a good balance between temperature rise and heat transfer efficiency in thesecond heating section 238. - The
second separator section 244 ofintegral separator system 241 receives the heated mixed fluid from thesecond heating section 238 as second heated mixed workingfluid stream 221. Thesecond separator section 244 separates the second heated workingfluid stream 221 into a liquid portion (not shown) and avapor portion 222. As mentioned earlier, thefirst vapor portion 220 from thefirst separator section 242 is used to further separate the vapor portion from the heated mixed workingfluid stream 221. Since, the liquid portion to be separated from the second heated mixed working fluid stream is “lean” (e.g., lower ammonia concentration) and since thefirst vapor portion 220 is “rich” (e.g., higher ammonia concentration), portions of thefirst vapor portion 220 will condense on the lean liquid portion in thesecond separator section 244. The heat of condensation causes additional amounts ofvapor portion 222 to be produced. - The liquid portion drained from
separator 244 is collected by thecollector 264 and exits theintegral separator system 241. This corresponds tostation 6 in FIG. 4 and to point 6 in FIG. 5. The collected liquid portion then proceeds to thehigh temperature recuperator 256 whereupon it surrenders a portion of its heat to the first workingfluid stream 282. See station 7 in FIG. 4 and corresponding point 7 in FIG. 5. Thereafter, the cooled liquid portion is expanded through theexpansion valve 294 to the low pressure side of thepower generating system 210. Seestation 8 in FIG. 4 andpoint 8 in FIG. 5. The cooled, expanded liquid portion is then combined with the turbine exhaust stream at station v6 and corresponding point v6 in FIG. 5. - The
vapor portion 222 produced in thesecond separator portion 244 combines with residual amounts of thefirst vapor portion 220 from thefirst separator portion 242 and exits the integralvapor separator system 241 as combinedvapor stream 286. This corresponds to station v2 in FIG. 4 and to point v2 in FIG. 5. The combinedvapor stream 286 may be additionally heated by thethird heating section 240 to a temperature that is greater than the dew point temperature for the combinedvapor stream 286. That is, the combinedvapor stream 286 is superheated in thethird heating section 240. Thesuperheated stream 288 exiting thethird heating section 240 corresponds to station v3 in FIG. 4 and to point v3 in FIG. 5. Thestream 288 is then directed to theenergy conversion system 226. - As was the case for the
first embodiment 110, theenergy conversion system 226 of thesecond embodiment 210 extracts heat energy from thesuperheated stream 288, converting it into useful work. In the embodiment shown and described herein, heat energy contained in the first and second vapor streams 220 and 222 (which comprise combinedstream 286 and superheated stream 288) is converted into electrical work by theturbine 228 and theelectrical generator 230 comprising theenergy conversion system 226. - The
superheated stream 288 is expanded in theturbine 228 and exits theturbine 228 asexhaust stream 272. See station v4 in FIG. 4 and point v4 in FIG. 5. It is generally preferred that the expansion process be terminated before the mixed workingfluid 214 is cooled below the dew point temperature. By way of example, in the embodiment shown and described herein, the mixed workingfluid 214 is expanded to a pressure of about 43 psia and to a temperature of about 160° F., which is below the dew point of the mixed workingfluid 214 at the designated pressure. The mixed workingfluid 214 can be cooled to a temperature below the dew point temperature since theenergy conversion device 226 can function effectively with wet mixtures. Theexhaust stream 272 is thereafter directed to thelow temperature recuperator 274 wherein it surrenders a portion of its heat energy to the workingfluid stream 214 flowing in theheated loop 275 oflow temperature recuperator 274. The cooledexhaust stream 272 exits thelow temperature recuperator 274 at station v5 at a temperature between the bubble and dew points for the mixed working fluid. See point v5 in FIG. 5. By way of example, in this embodiment, the cooledexhaust stream 272 exits thelow temperature recuperator 274 at a quality in the range of about 0% to about 100% (45% preferred). - The mixed working fluid exiting the
low temperature recuperator 274 is then mixed with the liquid portion flowing through theexpansion valve 294. See station v6 in FIG. 4 and point v6 in FIG. 5. The combined working fluid stream is then condensed by thecondenser 276 to about the bubble point (station L0 in FIG. 4 and point L0 in FIG. 5). The condensed stream is then returned to the high pressure side of thesystem 210 bypump 280 and the cycle is repeated. - The
second embodiment 210 of the power generating system just described results in the closely matched heating andcooling functions heating curve 290 of the mixed workingfluid 214 closely follows thecooling curve 292 of the heating fluid (e.g., geothermal brine 216). - It is contemplated that the inventive concepts herein described may be variously otherwise embodied and it is intended that the appended claims be construed to include alternative embodiments of the invention except insofar as limited by the prior art.
Claims (21)
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US10/258,718 US20030167769A1 (en) | 2003-03-31 | 2001-07-19 | Mixed working fluid power system with incremental vapor generation |
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US10/258,718 US20030167769A1 (en) | 2003-03-31 | 2001-07-19 | Mixed working fluid power system with incremental vapor generation |
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