This application is a Continuation of, and claims priority under 35 U.S.C. § 120 to, International application number PCT/EP03/50053, filed 11 Mar. 2003, and claims priority under 35 U.S.C. § 119 to Swiss application number 2002 0443/02, filed 14 Mar. 2002, the entireties of both of which are incorporated by reference herein.
1. Field of the Invention
The present invention concerns a thermal power process. It furthermore concerns a device suitable for carrying out a cyclic process as well as a power generation unit that utilizes the device based on the process of the invention.
2. Brief Description of the Related Art
Power generation units with closed processes are known per se in the state of the art. Examples are the two-phase steam turbine processes. Also known and often technically realized are processes in which a gaseous performance fluid initially is compressed, heated and then expanded in an engine accompanied by thermodynamic performance. Then the fluid is cooled again, compressed and returned to the compression. Examples are the realization of the closed Carnot Process in the Stirling engine. Another example that was very prominent in the past is the closed Ackeret-Keller process in which especially a gasturbo component group is operated in a closed cycle. The advantage of this process is the fact that the line can be controlled through the charging degree of the process, i.e., through the variable admission pressure prior to the compressor and the independent selection of the performance medium. A disadvantage per se is the fact that external heat must be supplied to the cycle process, which means that such a gas turbine with a closed process is limited with regard to the turbine entry temperatures. Consequently only a small pressure ratio in conjunction with lower effectiveness and performance potential can be realized, if a meaningful quantity of heat is to be supplied through the heat exchange. Another option would be to use a large number of costly intermediate cooling stages in the compressor. In any case the compressor temperature must be clearly below the maximum realizable process temperature in order to arrive at a technically meaningful realization. If there is a high pressure ratio, the waste heat utilization based on recuperating the enthalpy streams exiting the turbine are limited because the compressor end temperature quickly exceeds the turbine exit temperature with increasing pressure ratio. Nevertheless gas turbines with closed cycles for low temperature utilization recently have received more attention again. Other closed cycle processes and energy generation units that work in a closed process environment are increasingly interesting from a technical point of view again as well.
DE 36 05 466 describes a closed gas turbine unit in which an amount of steam is generated and introduced into the process fluid. The steam is introduced between two expansion stages. This means that the generated steam only supports a part of the performance generating expansion. DE 36 05 466 does not use the steam generation for utilizing the process waste heat.
Therefore one aspect of the present invention is to provide a thermal power process as described in the introduction that avoids the disadvantages of the state of the art and that especially allows for utilizing the process waste heat even with limited upper process temperatures and high pressure ratios.
Another aspect of the present invention therefore is to at least recuperate part of the heat to be dissipated following the expansion and to return it to the cycle process in a power generation unit that primarily works with a gaseous process fluid that is heated up in the heat exchange prior to the expansion process. This, taking the given limitations of the upper process temperature into account, is not possible by increasing the specific enthalpy of the compressed process gas but rather by adding another enthalpy stream in the form of a medium that is heated by the process waste heat. Important is the fact that the primary process fluid does not undergo any phase alterations during the change in thermodynamic state while the supplementary medium undergoes a two-phase process so that it condenses following the expansion and is separated from the gaseous primary process fluid in this manner. The liquefied supplementary medium is returned to high pressure, is heated using the waste heat to be removed from the process, evaporated and, if necessary, overheated. As a cooling agent it absorbs heat during a heat sink of the process and is added to the compressed primary process fluid prior to the expansion, depending on the present thermodynamic state of the media, either upstream or downstream of the heater for the primary process fluid. Both media are expanded afterwards, optionally while delivering thermodynamic performance. In order to close the cycle process, heat must be removed from the expanded performance medium and a large part of the steam is condensed which results in the closing of the cycle of the supplementary fluid as well. In order to realize the cycle process it furthermore is advantageous to arrange at least a second heat sink upstream from the first compression process in order to define the temperature at the compressor entry as low as possible.
From a global point of view the process that the primary cycle medium undergoes initially is a compression of a first thermodynamic state to a second thermodynamic state, a change in thermodynamic state from the second thermodynamic state to a third thermodynamic state during which the primary process medium is supplied with heat, a change in thermodynamic state from the third thermodynamic state to a fourth thermodynamic state during which the primary process medium is expanded and a change in thermodynamic state in which the process medium is returned to the first thermodynamic state due to heat dissipation. This does not yet provide any information on the course of the changes in thermodynamic state that in fact is not primarily significant for the invention but rather is determined based on how the special process is realized from a technical point of view. This means the compression and expansion, at least that of the theoretical cycle process, can be isothermal or quasi-isothermal or isotropic, for example, or approximately isotropic, and the heat supply and dissipation is isochoric or isobar. In reality the process is determined by what technical means are being used. This does not provide perfect theoretical changes in thermodynamic state as they are described. Ideally the pressure of the process fluid is identical for the first and fourth thermodynamic state and for the second and third thermodynamic state. In reality there are of course streaming pressure losses when streaming through lines and heat transfer devices as well as pressure loss due to adding heat to the streaming fluid. These are not intended total pressure changes as they are due to expansion or compression. Rather, these are inevitable pressure changes and especially total pressure losses. Since total pressure changes that occur in the real process during the change in thermodynamic state from the second thermodynamic state to the third thermodynamic state and from the fourth thermodynamic state to the first thermodynamic state are not desired and are kept as low as possible, these changes in thermodynamic state mainly are considered to be isobar or quasi-isobar in this context.
Depending on the existing temperature conditions the generated steam is added to the primary process fluid either following the heat supply but prior to the expansion or wholly or partially prior to or during the heat supply to the primary process fluid and heat is added to this steam together with the primary process fluid. It also is possible to add a part of the steam to the primary process medium during the expansion from the third to the fourth thermodynamic state.
In one embodiment of the thermal power process embodying principles of the present invention, the process fluid is being cooled during the compression. In another embodiment embodying principles of the present invention, heat is supplied to the process fluid during the expansion. If the design is accordingly, at least approximate isothermal changes in thermodynamic state can be realized.
Another aspect of the present invention can include that the primary process fluid and the steam provide thermodynamic performance during the expansion from the third to the fourth thermodynamic state, especially in a power engine.
The complete, closed process in principle allows the choice of any process fluid. Nonetheless the process is especially easy to handle when non-toxic media are used and in particular when air is used as a primary process fluid and water is used as a supplementary two-phase fluid.
In a device for carrying out the thermal power process according to the principles of the present invention, at least one compression medium is arranged for the primary performance fluid, downstream from it at least one medium is arranged for supplying heat, especially a heat exchanger through which the process fluid streams from the secondary side, downstream from it at least one expansion medium is arranged, furthermore at least one steam generator as a first heat sink is arranged downstream from the expansion medium. Process fluid streams through the steam generator from the primary side with the process fluid cooling off. When the cooling of the process fluid reaches the dew point of the contained steam, the condensation of the steam commences and continues with further cooling. This causes the partial pressure of the steam and thus the dew point to sink with the overall pressure remaining constant. Contrary to the change in thermodynamic state in the Clausis-Rankine cycle process the condensation of the steam is not isobar and isothermal but rather occurs at a temperature that corresponds to the partial pressure of the steam. The advantage is that the condensation heat of the condensate that is separated with a higher partial pressure occurs at a temperature level at which this heat can be used for pre-heating the condensate that is returned to the secondary side of the steam generator. In an exemplary embodiment at least one additional heat sink is arranged downstream from the first heat sink to especially lower the temperature of the first thermodynamic state as low as possible and also to lower the remaining steam content in the primary process fluid as much as possible. Furthermore this is where the second heat sink for defining a process temperature is especially suitably arranged in order to define the lowest process temperature at this point that is determined by the temperature of the cooling agent, such as cooling water. Downstream from the water sink or water sinks or in their flow path for the primary process fluid, devices for separating the resulting condensate are arranged. Furthermore there are means, especially a feed pump, for transporting the condensate to the secondary side of the steam generator as well as means for supplying the generated steam downstream from the compression means and upstream from at least one expansion means. It should be noted that for the purpose of the present invention the side of the heat exchanger from which the heat is transferred is always called the primary side. The side to which the heat is transferred is always called the secondary side. In an embodiment of the device the compression means have at least one intermediate cooler or means for supplying fluid drops into the process fluid that flows through the compression means. These drops evaporate during the compression process and cool the compression means on the inside. Both measures are suitable to realize at least an approximate isothermal or quasi-isothermal compression. In the same manner means for supplying heat to the process fluid can be arranged within the expansion means or between at least two compression means. If the embodiment is suitable, at least one approximate isothermal expansion process can be realized. When arranging an intermediate cooler the possible condensation of residual moisture at the compressor entry in the primary performance medium must be taken into consideration. The described heat supply to the performance fluid can be used to maintain the temperature level available for generating steam at a sufficient level when there is a high pressure ratio of the process and a limited upper process temperature in order to ensure that the available steam is not overheated much. As an alternative the steam is supplied to the primary process fluid at reduced pressure following a partial expansion of the primary process fluid if the available temperature level is insufficient to make an at least somewhat overheated amount of steam on the upper process pressure available.
Especially at least one expansion means is a power engine in which the primary process fluid and at least a part of the steam are expanded using thermodynamic performance. An example is a power engine that acts as an expansion means that has at least one machine that acts as a compression means and/or a sink, all of them arranged on a mutual shaft.
One exemplary means for supplying heat to the process fluid is a heat exchanger that is connected to a heat generator on the primary side or through which the waste gas of a gas turbine flows from the primary side. Possible heat generators are especially charged furnaces that work with overpressure. The charge can result in a decrease of the component size and the heat transmission in the heat exchanger can be intensified on the primary side. In another exemplary embodiment the means for supplying steam are arranged upstream from the first heat supply means, which further intensifies the heat transmission in the heat exchanger on the secondary side as well.
In one exemplary embodiment the device has means that allow the changing of the pressure level of the entire process and consequently the amount of fluid in circulation. This provides an especially practical possibility for varying the performance of machines that function based on the thermal power process according to the invention. In such a machine the pressure ratio of the process remains constant for the most part, for example, which is why all machine components are operated close to the concept point, even with partial loads. In addition, it is possible to adjust the counter-pressure of the expansion means, i.e. the low process pressure, so that the steam does not have any moisture during the expansion process even with a comparatively low upper process temperature.
A shunt line with a blocking and/or throttle device can advantageously be arranged downstream from the compression means through which compressed performance medium can be transported directly to the low-pressure portion of the device in accordance with the invention. This is important when the sink that is coupled to the power engine that acts as an expansion medium, displays quick load reductions, for example the load shedding of a generator. In this case the compressed process fluid is directly moved to the low-pressure portion of the thermal power unit.
Turbo compressors can be used as compression means and turbines can be used as expansion means, especially when high mass flow rates and thus continuously working machines are required for high performance output. However, it also is easily possible to use propeller compressors and —expanders or piston machines and other types that are known to one skilled in the art. Especially in the case of very high-pressure conditions a suitable serial connection of turbo and displacement machines is quite practical.
An exemplary embodiment of a thermal power unit for realizing the process in accordance with principles of the present invention is a gas turbo group with a closed cycle and in which downstream from a last turbine at least one waste heat steam generator is arranged as a first heat sink. Also downstream from it one or several additional heat sinks are arranged in which steam contained in the process fluid is condensed and separated. A boiler feed pump transports the resulting condensate into the waste heat steam generator where an optionally overheated amount of steam or a saturated steam is generated. The generated steam is returned to the performance fluid on the high-pressure side of the closed gas turbine, expanded, cooled and condensed in the turbine. To this extent such a machine is similar to a conventional STIG machine that is known per se. Nonetheless known STIG machines work in an open cycle and have a correspondingly large water consumption rate. The closed gas turbine in accordance with the invention recirculates the water. This can be accomplished easily within the low pressure part of the thermal power unit is operated under hyperbaric pressure. Already above the ambient temperature a main part of the contained steam is separated from the gas cycle. The pressure in the low-pressure part of the thermal power unit, i.e. during the fourth and first thermodynamic state, ranges above 5 bar, for example at 10 bar, in an exemplary embodiment. Low pressure in the range between 5 and 10 bar proves to be especially advantageous with regard to the condensation temperatures, the performance density and the required dimensions of the components. The smaller streaming cross sections on one hand are favorable with regard to stability but on the other hand they require increasing process pressure and thus stronger dimensions in order to provide the necessary stability. The specified pressure range also proves to be a favorable compromise. The higher temperature level of the condensation makes it possible to use the condensation heat in the steam generator. In addition, the largely free setting of the counterpressure of the turbine allows the setting of conditions with which the exergetic potential of the steam can always be utilized optimally without generating any significant moisture in the turbine, even if the pressure ratio is almost constant, the available heat varies strongly and the upper process temperatures vary. In addition, it is possible to freely select the performance media with regard to the performance gas as primary process medium and with regard to the medium used for the steam generation, which does not necessarily have to be water in the closed process. A gas turbine working with the process in accordance with the invention can be optimally adjusted to different conditions and can especially favorably be used for low temperature utilization.
A process in accordance with principles of the present invention allows for an advantageous realization of a power generation unit in which an open cycle gasturbo group is followed by a thermal power unit in accordance with the invention. In general the design of such a unit can be substantially simpler than a conventional water-steam cycle used for wastewater utilization and, as explained above, is especially suitable to handle strongly fluctuating waste heat.
The invention will be explained in more detail based on the exemplary embodiments illustrated in the drawings. In particular,
The exemplary embodiments that are shown only present a small instructive section of the invention described in the claims.
The process in accordance with the invention of course can also be realized with a multi-shaft gasturbo group. Of course it is possible to easily arrange a cooling process during the compression process or heat supply during expansion in a manner that is known per se.
Furthermore, a high-pressure reservoir 45 is arranged in connection with the high-pressure part of the closed gasturbo group. In an operating state it is charged by a compressor 48 via a recooler 47, a condensate separator 50 and a check device 46. This charging process removes process fluid from the cycle which causes the pressure level of the entire process, and thus that of the circulating mass flow, to sink. This means with constant pressure ratio and operation of the gasturbo group in or near the starting point it is possible to lower performance. In another operating state the high pressure fluid stored in the reservoir 45 is returned to the cycle via the blocking and throttle device 49 which increases the density of the circulating medium and thus the mass flow and the performance permanently. The feeding of fluid from the high-pressure reservoir 45 has a direct effect as an increase of the turbine mass flow. The energy that is stored in a gas volume can be quickly made available and therefore is suitable for spontaneous performance increases as it might be necessary for supporting the frequency of a network, for example. This is how the performance potential of the closed gasturbo group can be varied easily. These are the main advantages of the power generation unit shown in
List of Reference Numerals
While the invention has been described in detail with reference to exemplary embodiments thereof, it will be apparent to one skilled in the art that various changes can be made, and equivalents employed, without departing from the scope of the invention. Each of the aforementioned documents is incorporated by reference herein in its entirety.
Number | Date | Country | Kind |
---|---|---|---|
2002 0443/02 | Mar 2002 | CH | national |
Number | Date | Country | |
---|---|---|---|
Parent | PCT/EP03/50053 | Mar 2003 | US |
Child | 10939375 | Sep 2004 | US |