THERMAL POWER PLANT WITH HEAT RECOVERY

Abstract

In an energy conversion method and a thermal power plant for converting heat into mechanical or electric energy using a working medium, a vapor state in the working medium is generated at a first pressure in a steam generator. The vaporized working medium is expanded to a lower second pressure in a steam expanding device. An energy obtained by the expansion process is discharged. The expansion of the steam state is carried out using a saturation line of the working medium. The working medium is thereby separated into a non-condensed portion and a condensed portion in a separating device. The non-condensed portion is then compressed into a compressed non-condensed portion in a compressor. The compressed non-condensed portion is cooled and condensed into a compressed condensed portion. The compressed condensed portion and the initially condensed portion are then heated, and both portions are returned to the steam generator together.

Claims

1. Thermal power plant for converting energy by means of a working medium, which has: a steam generator (25) for vaporizing the working medium at a first pressure, a steam expanding device for expanding the working medium present in the vapor state to a lower, second pressure, a condenser (36), which cools and liquefies the working medium let out of the steam expanding device, and a condensate pump (37), characterized in that the steam expanding device is designed in such a way that a working medium expanded by the steam expanding device has a condensed portion and a non-condensed portion, a separation device for separation of the condensed portion and the non-condensed portion and a compressor (51) for compression (5) of the non-condensed portion of the working medium are provided, whereby the non-condensed portion of the expanded working medium condenses at least partially through the condensed portion in the condenser (36).

2. Thermal power plant according to claim 1, characterized in that the separation device comprises a housing (44), whereby provided in an upper region of the housing (44) is the compressor (51), in a lower region of the housing (44) is the steam expanding device and in a bottom region under the lower region is a pump (54) for pumping out the one condensed portion.

3. Thermal power plant according to claim 1, characterized in that the steam expanding device comprises working cylinders (43) with inlet valves (57) for admitting the vaporized working medium and pistons (45), whereby two working cylinders (43) each are disposed opposite on the separation device.

4. Thermal power plant according to claim 1, characterized in that a swinging arm mechanism with at least one swinging arm (48) is provided, which mechanism is coupled to the compressor (51) for compression (5) of the non-condensed portion of the working medium and to a pump (54) for discharging the condensed portion (4) out of the separation device.

5. Thermal power plant according to claim 1, characterized in that the working cylinders (43) and pistons (45) are driven by the swinging arm mechanism.

6. Thermal power plant according to claim 1, characterized in that a swinging arm (48) of the swinging arm mechanism transmits expansion work of the working medium from the working cylinders to a crank mechanism (50).

7. Thermal power plant according to claim 1, characterized in that used as heat source (27) is heat from combustion, geothermal energy, solar systems, waste heat from cooling systems and/or from heat recovery.

8. Thermal power plant according to claim 1, characterized in that the pistons (45) have outlet valves (70), which are built into the piston (45) and are controllable by a switchover pin (69).

9. Thermal power plant according to claim 1, characterized in that the compressor (51) comprises compressor inlet valves (73) and compressor pistons (52), whereby a compressor inlet valve (73) is disposed in the compressor piston (52) and is controllable by means of a piston rod (79).

10. Energy conversion method for converting heat into mechanical or electrical energy by means of a working medium, which has the following steps: a) Generating a steam state in the working medium at a first pressure in a steam generator, b) Expanding (1) the steam state in a steam expanding device at a lower, second pressure, c) Discharging an energy obtained by the expansion, characterized in that d) the expansion (1) of the steam state proceeds through a polytrope of the working medium, the working medium being separated in a separation device (44) into a non-condensed portion (3) and a condensed portion (4), e) compression (5) of the non-condensed portion (3) in a compressor (51) into a compressed, non-condensed portion (3), f) cooling (6) and condensing (7) of the compressed, non-condensed portion (3) into a compressed condensed portion (3), g) heating (8; 9) of the compressed condensed portion (3) and of the initially condensed portion (4) and return of the portions (3, 4) to the steam generator.

11. Method according to claim 10, characterized in that the expansion (1) of the steam state proceeds through a saturation line of the working medium, preferably through the critical point (2) of the working medium.

12. Method according to claim 10 or 11, characterized in that the expansion (1) takes place through a wet steam expansion.

13. Method according to claim 10, characterized in that the cooling (6) and condensing (7) of the compressed, non-condensed portion (3) is realized by means of the condensed portion (4).

14. Method according to claim 1, characterized in that the second pressure is determined by a compressibility factor Z for the working medium at the critical point.

15. Method according to claim 1, characterized in that the non-condensed portion (3) amounts to 50% to 60% of the vaporized working medium.

16. Method according to claim 1, characterized in that a first part of the work performed in the steam expanding device by the working medium is discharged to a generator and a second part of the work performed in the steam expanding device by the working medium is discharged to the compressor, in order to compress and heat the non-condensed portion.

Description

BRIEF DESCRIPTION OF THE DRAWINGS

[0030] The way the method works and one embodiment according to the invention are presented in the following with reference to the drawings, which serve merely explanatory purposes and are not to be interpreted in a limiting way. Features of the invention disclosed from the drawings should be viewed as belonging to the disclosure of the invention individually and in any combination. Shown in the drawings are:

[0031] FIG. 1: A cycle process for a thermal power plant with heat recovery according to the invention;

[0032] FIG. 2: The Maxwell distribution of the cycle process according to FIG. 1 at the critical point;

[0033] FIG. 3: The Maxwell distribution of the cycle process according to FIG. 1 in the final state;

[0034] FIG. 4: The compressibility factor Z for air in the saturation state as a function of the specific volume of the cycle process according to FIG. 1;

[0035] FIG. 5: Comparison of the adiabatic change of state with respect to wet steam expansion of the cycle process according to FIG. 1;

[0036] FIG. 6: A cycle process with wet steam expansion according to the invention;

[0037] FIG. 7: Momentum vectors for the cycle process according to FIG. 6 on a moving wall;

[0038] FIG. 8: Caloric design of a condenser according to the invention;

[0039] FIG. 9: A thermal power plant according to the invention with a condensation motor;

[0040] FIG. 10: A section through the condensation motor according to FIG. 9;

[0041] FIG. 11: A section through the working cylinder of the condensation motor according to FIG. 9;

[0042] FIG. 12: A piston with outlet valve of the condensation motor according to FIG. 9:

[0043] FIG. 13: An outlet valve according to FIG. 12;

[0044] FIG. 14: A valve control of the thermal power plant according to FIG. 9;

[0045] FIG. 15: A residual steam compressor of the thermal power plant according to FIG. 9;

[0046] FIG. 16: A piston of a residual steam compressor of the thermal power plant according to FIG. 9;

[0047] FIG. 17: A steam turbine for phase separation according to the centrifuge principle.

DETAILED DESCRIPTION

[0048] Described in FIGS. 1 to 8 is the cycle process on which the method is based according to the invention for conversion of energy by means of a working medium in a thermal power plant. Presented in FIGS. 9 to 16 is a thermal power plant according to the invention which works according to the energy conversion method according to the invention.

[0049] With the supposition that thermal engines can be equipped with heat recovery, a new method is presented as shown in FIG. 1. This method is characterized primarily in that steam is expanded through the polytrope, preferably through the saturation line and especially preferably through the critical point 2. With this expansion 1 there results a mixed phase, consisting of a non-condensed portion, the steam 3, and a condensed portion, the condensate 4. Seen isentropically, there arises with the expansion 1 through the critical point, for example with air, about 48% steam phase and 52% condensate.

[0050] Made use of for the method according to the invention is that, with expansion in the steam phase, the working medium can condense. This is caused by a condensation owing to the dipolarity of the steam molecules, which is the basis for a loose bridge bonding, on which the liquid phase of the working medium is based. The bridge bonding occurs when the inner energy of two steam molecules, which collide, is less than a bonding energy of the dipole. At the critical point, steam phase and liquid phase exist in thermal equilibrium. Thus at the critical point the sum of the inner energy of the molecules, whose inner energy is higher than the bonding energy of the dipole, is in phase equilibrium with the steam molecules whose inner energy is lesser than that of the dipole.

[0051] Shown in FIG. 2 is the Maxwell distribution 11 of the molecules for the critical point. Since the inner energy is a quadratic function of the molecular velocity, the bonding energy is indicated at the quadratic mean 12. The area under the curve corresponds to the portion of the molecules at the respective molecular velocity. The area 13 on one side of the quadratic mean 12 corresponds approximately to the area 14 on the other side of the quadratic mean 12. In this state no lasting bridge bonding can arise because this bridge bonding is destroyed again and again by the faster molecules.

[0052] As a comparison, the Maxwell distribution for an end state of the working medium is shown in FIG. 3. The temperature after expansion is lower than at the beginning, whereby the distribution function according to Maxwell 15 shifts, while the binding energy 12 is assumed as constant. The number of molecules whose inner energy is lesser than that of the bridge bonding, is significantly greater. The number of molecules whose inner energy is greater than that of the bonding energy is significantly smaller. They can no longer destroy all the bridge bonds, so that condensation occurs. The number of condensed molecules results from the difference between the areas 16 and 17. The above hypothesis that with the isentropic expansion through the critical point condensation occurs is thereby confirmed. The thermal power plant according to the invention thus represents a kind of condensation motor.

[0053] However the losses must also be taken into account, such as frictional, leakage and insulation losses. The friction is transformed into heat, and this will cause a vaporization of condensate. The leakage losses will increase the suction volume of the residual gas compression. An increasing entropy thereby results. With losses of 20%, a phase mixture of about 40% condensate and 60% steam will be achieved.

[0054] The heat of condensation has its maximal value at the triple point T of the working medium. The value of the condensation heat then decreases with increasing temperature, and reaches the value zero at the critical point. Hence the principle of heat recovery by means of internal condensation according to the present invention consists in that the steam portion is heated by means of compression in such a way that it can be liquefied by means of the cold condensate portion.

[0055] Used according to the invention is a cycle process with a working medium, which consists of the following steps, as shown in FIG. 1: [0056] Expansion 1 of the steam through the critical point 2, [0057] Separation of the non-condensed portion, i.e. of the steam portion, 3 and of the condensed portion, i.e. of the condensate portion, 4 in a separation device, [0058] Compression 5 of the non-condensed steam portion 3 in a condenser, [0059] Re-cooling 6 of the compressed, non-condensed steam portion 3, [0060] Condensing 7 of the until now non-condensed steam portion by means of the cold condensate in a condenser into a compressed portion 3, [0061] Heating 8 of the compressed, condensed portion 3, [0062] Heating 9 and if necessary pumping of the already initially condensed portion, and [0063] Vaporization 10 of the entire condensate consisting of compressed, condensed steam portion 3 and initially condensed condensate portion 4.

[0064] The invention makes use of the effect of wet steam expansion. If the pressure at the critical point is determined from the critical density and the critical temperature of the working medium used according to the gas law, a pressure is obtained for air of 131 bar. Now the critical pressure with air is effectively 37.2 bar. This reduced pressure is explained by the effect of the intermolecular attractive forces, and this is determined with the compressibility factor Z, as it is defined, for example, in the VDI Heat Atlas (1984 edition, sheet Da 13).

[0065] Shown in FIG. 4 is the compressibility factor Z as a function of the specific volume v for air in the saturation state 18, on the basis of table 17; Material Values of Air in the Saturation State, VDI Heat Atlas, sheet DB 11. The intermolecular attraction has a very strong effect when the density is high and the intermolecular spacing is small. Immediately after the critical point the intermolecular attraction decreases greatly. That can lead to the decrease in the intermolecular attraction being greater than the volume increase with the expansion. In this range the pressure can remain constant or can even increase with the expansion, which is to be taken into consideration with the construction of the thermal power plant. With increasing volume the steam passes into the gas phase.

[0066] FIG. 5 shows this relationship in a pressure-volume diagram. The expansion 1, taking into account the compressibility factor Z, climbs immediately after the critical point 2, or respectively the pressure increases, but then approaches the adiabatic curve 19, which assumes a pressure of 131 bar. The pressure of 131 bar results, with the general gas law, from the critical temperature and the critical density of the working medium. This means that the greater the specific volume is, the greater the intermolecular spacing will be and the steam passes into the gas state. The adiabatic curve for pure gas expansion, determined according to the general gas law starting with the critical point, would run according to line 20. The area under the state function corresponds to the work performed. Therefore it can be seen from FIG. 5 that with the wet steam expansion with the adiabatic curve 19 more work is performed than with the pure gas expansion according to line 20, starting from the critical point.

[0067] Shown in FIG. 6 as pressure-volume diagram is the cycle process for the thermal power plant according to the invention, or respectively the condensation motor. The course of the wet steam expansion is again indicated by the reference numeral 1. With the compression of the residual steam, the volume is less than 60% and the state change, due to the intermolecular attraction, is flatter. This means that, due to the intermolecular attraction, the compression work is less than according to the general gas theory. Thus the work with the wet steam expansion 1 cannot be determined with the adiabatic function according to the general gas law. Since no explicit function is available for the compressibility factor Z, the stroke is calculated section-wise.

[0068] A calculation of the stroke is all the more exact, the more exactly the processes connected therewith are determined. With the method according to the invention it is assumed, for the conversion of heat into work, that this process is better explained and more precisely determined with the kinetic theory of heat than is possible with the caloric theory.

[0069] In the kinetic theory of gas, the action of force which can be generated with steam pressure is attributed to molecular collision. The mass of the atoms is thereby located for the most part in the atomic nucleus, which is very small. The atomic nucleus corresponds approximately to one hundred thousandth of the atom diameter. Around this atomic nucleus there exists a predominantly positive force field, which is generated by the positrons. Upon collision of two atoms two homopolar force fields clash. The same applies for molecules since these are composed of atoms. Molecular collisions are therefore viewed as elastic. It is assumed here that the collision of a molecule on the moving piston wall of the thermal power plant corresponds to a special case of elastic collision, namely the collision on the moving wall. The velocity of the colliding molecule accordingly changes by twice the wall velocity, respectively the piston velocity.

[0070] Explained in FIG. 7 is the process of collision between the molecules. The collision process consists of two phases, the compression phase and the expansion phase. The compression phase is the phase in which the force fields hit each other. Kinetic energy is thereby converted into potential energy. The expansion phase is the phase in which the molecules repel again; the potential energy is converted back again into kinetic energy. Between the compression phase and the expansion phase lies the turning point of the collision process. It thus changes the direction and absolute value of the velocity vector, as shown in FIG. 7. Velocity and momentum are vectors; accordingly the energy balance per collision must be handled vectorially. Before the collision, a molecule hits the moving piston wall 21 with a median molecular velocity 22. After the collision, the molecule has a median velocity 23. The velocity of the molecule, respectively of its normal components, changes by twice the piston velocity (2 vK), from which a change in the inner energy and a decrease in the temperature results since the temperature is a function of the inner energy.

[0071] With the molecule collision on the wall, the molecule is slowed down from its speed, for example the median molecular velocity, to the wall speed. Through this deceleration it acts upon the wall with a mass force. With the impact on the moving wall, this mass force produces work with the shift of the wall. In the expansion phase the molecule is pushed off again, i.e. accelerated. Here too a mass force arises through the acceleration, with which mass force the molecule acts upon the wall, and here too work is produced with the shift of the wall. According to the principle of the conservation of energy, the work performed by the molecule corresponds to the change in its kinetic energy. The work transmitted to the wall per stroke is the sum of the work performed per molecular impact over the number of all molecular hits. The number of molecular hits on the wall can be calculated from the pressure by means of the second Newtonian principle. This method of calculation was checked in that the power output of the gas compressors was thereby determined. A good agreement resulted.

[0072] According to the invention, the condensation of the working medium through expansion is made use of in a thermal power plant. Condensation is the transition from the gas phase into the liquid phase. In the gas phase the molecules can move freely; they have kinetic, oscillation and rotational energy. The molecules continuously collide with each other and exchange their pulse, according to Brownian molecular motion. The portions of kinetic, oscillation and rotational energy results from the degree of freedom of movement.

[0073] The liquid phase is based on a loose dipole bond among the molecules. In this loose bridge bond the molecules can still swing and rotate; they have no kinetic energy anymore. The bridge bond can arise when the inner energy of the colliding molecules is less than the binding energy of the bridge. Molecules thus condense upon impact when their inner energy is less than the binding energy of the bridge. In order for steam to condense, inner energy must be extracted from the molecules. When hitting the moving wall, the molecules are decelerated by twice the wall velocity. This means that with this impact kinetic energy, respectively inner energy, is transferred to the pistons or, in other words, inner energy is taken away from the molecules during the expansion, so that the steam can condense.

[0074] According to the method of the present invention, a separation of the phase mixture takes place into a condensed portion and a non-condensed portion. This separation can take place by means of the principle of gravity or centrifugal force. In the case of the principle of gravity, the condensate collects as condensed portion at the bottom and can be pumped from there. The non-condensed portion in the form of residual steam can be suctioned out at the top of the separation device, such as e.g. a phase separator.

[0075] Shown in FIG. 8 is the calorific layout of the condenser: re-cooling 6 of the steam portion, condensing 7 of the steam portion on the primary side and heating 9 of the cold condensate portion in counter flow on the secondary side in the condenser. The re-cooling of 60% steam portion with 40% condensate portion is possible because the specific heat of the condensate is about twice as high as that of the steam.

[0076] The degree of efficiency of the thermal power plant can be explained as follows. The final output delivered by the plant corresponds to the difference between the work obtained with the expansion and the energy required for the compression of the residual steam portion and heating and pumping of the condensate portion. The expansion can take place, for example, from 100 to 0.1 bar, the compression of the residual steam portion from about 1 to 30 bar; the mass of the residual steam portion lies between 50-60% of the expanded steam. Thus about 30% of the work generated with the expansion passes over into the residual steam compression. The power output necessary for the pumping and heating of the condensate portion corresponds to about 2% of the work obtained with the expansion.

[0077] Air is preferably used as the working medium with the method according to the invention, on the one hand because it is environmentally safe, but also because it is a well-documented medium. In principle however other working media, such as e.g. ammonia, carbon dioxide or halogenated hydrogens can also be used. The critical point of air lies at 141 C., i.e. in the low temperature range, in which air also appears as steam and liquid.

[0078] FIG. 9 shows diagrammatically a thermal power plant according to the invention with a condensation motor with heat recovery. The thermal power plant has a steam generator 25 with built-in heat input device 26. The steam generator 25 is supplied by a heat source 27. The heat source 27 can be: heat from combustion, geothermal energy, solar systems, cooling systems, heat recovery from the plant, etc. With the heat a high-pressure steam is generated in the plant and is supplied to a working cylinder 43 of the condensation motor. The machine housing 44 operates as separation device for a condensed and a non-condensed portion of the steam according to the invention, whereby the machine housing 44 represents a phase separator. Through a line 29 the high-pressure steam is led into the pressure chambers of the working cylinder 43 with cylinder heads 41 and pistons 45. The construction of the condensation motor corresponds to the so-called boxer principle, in which two cylinders 43 each are disposed in an opposed way in a machine housing 44. Built into the cylinder head 41 are also inlet valves 57 for admission of the steam.

[0079] With a piston rod e.g. via a crosshead 46, which is guided in guiding pieces 47, the pistons 45 are connected to a mechanism with swinging arm 48, to which the stroke of the piston 45 is transmitted. The swinging arm 48 sits on a swinging arm shaft 49 with which the swinging movement is transmitted outwardly to a crank mechanism 50. Driven with the crank mechanism 50 is a transmission, preferably an infinitely variable hydraulic transmission, with which a generator can then be driven. The swinging arm mechanism is coupled to a residual steam compressor 51. With the swinging arm 48, via the crosshead 46, a piston 52 is driven in cylinders of the residual steam compressor 51. The residual steam compressor 51 is connected to a pre-cooler 35 and a condenser 36. A pressure line 53 leads from the cylinders of the residual steam compressor 51 to a pre-cooler and further to the condenser 36. The pressure line 53 is connected on the primary side. A line leads from the condenser 36 to a condensate pump and from there back into the steam generator 25.

[0080] Located at the bottom of the machine housing 44 of the swinging arm mechanism is a piston pump 54 with which the cold condensate is conducted with a line 37 to the secondary side of the condenser 36. The line leads from the condenser 36 back to the steam generator 25. The piston pump 54 is driven by the swinging arm mechanism via a pump lever 55, which swings in a bearing 56.

[0081] With start-up, an electric machine operates as motor, which drives the compressor 51, pressurizes the plant, expands the steam in the working cylinders 42 and thereby cools down the plant and thus brings it to operating temperature.

[0082] FIG. 10 shows a cross section through the swinging arm mechanism of the condensation motor, consisting of the machine housing 44, the working cylinders 43 and the pistons 45 of the expansion part of the condensation motor. With the swinging arm 48, which is coupled to the swinging arm shaft 49, the expansion work of the working medium is transmitted to the crank mechanism 50. Located at the top of the phase separator in the form of the machine housing 44 is the residual steam compressor 51. Located at the bottom of the phase separator is the piston pump 54, which is driven with the pump lever 55, which swings about the bearing 56 and transmits the necessary power output from the swinging arm 48 to the pistons 52 of the piston pump 54.

[0083] FIG. 11 shows a cross section through the working cylinder 43 with the cylinder head 41, the cylinder head gasket 42, the high pressure chamber, in which the high-pressure steam is stored, the inlet valve 57, a valve bridge 58, in which the inlet valve 57 is screwed, a valve rod 60, damper disc 61 with an annular groove 62, a discharge bore 63 and a switching spring 64.

[0084] FIG. 12 shows a cross section through the expansion piston 45 with a built-in outlet valve 70 with a valve cone and a centering ring 65, with a piston tube 66, exhaust port 67, an annular piston 68, the crosshead 46 and a switchover pin 69. The crosshead 46 is provided laterally with rollers, with which it is guided in the guiding piece 47. The centering ring 65 is of a material with good dry-running properties, such as, for example, PCTFE, so that frictional losses can be kept minimal. With the switchover pin 69 the outlet valve 70 can be switched in such a way that it is closed on the one side during expansion of the working medium, while it is open on the other side and the expanded steam can be expelled.

[0085] FIG. 13 shows the outlet valve 70, built into the expansion piston 45, the valve consisting of the valve cone, the valve rod 71, a slider 72 and the switchover pin 69.

[0086] FIG. 14 shows diagrammatically a control of inlet valve 57 and outlet valve 70. Toward the end of the outlet stroke, the switchover pin 69 of the piston 45 travels on the switching spring 64 and thereby closes the outlet valve 70. At the same time the annular piston 68 moves into the annular groove 63<sic. 62> of the damper disc 61 and compresses the enclosed steam. After the necessary pressure has been reached, the damper disc 61 is pushed against the cylinder flange and the inlet valve 57 is thereby opened. The discharge bore 62<sic. 63> is dimensioned in such a way that the enclosed steam flows away at the end of the filling process and the annular piston 68 rests in a close-fitting way on the bottom of the annular groove 63<sic. 62>. A defined spacing thereby results between inlet valve 57 and pistons 45 and thereby a defined filling volume.

[0087] FIG. 15 shows a cross section through the residual steam compressor 51 with pistons 52. Built into pistons 52 is an inlet valve 73 and opposite, built into the cylinder head, an outlet valve 74. Provided in the flange of the cylinder head is also a steam outlet 75. The inlet valve 73 is guided in a guide, such as e.g. a piston star 76, which is provided with a bevel shoulder 77 on both sides. The bevel shoulder 77 is adapted on the one hand to a shoulder of a cone of the inlet valve 73 and on the other hand to a damping sleeve 78.

[0088] FIG. 16 shows the piston 52 of the residual steam compressor 51 with opened inlet valve 73. Built into the piston 52 is the cone of the inlet valve 73, which is attached at the end of the piston rod 79. The piston rod 79 is guided with the piston star 76, and has on both sides one bevel shoulder 77 each. Installed on the piston rod 79 is the damping sleeve 78, which damps the impact during closing of the valve 73. The shoulder of the valve cone likewise moves into the opposite bevel shoulder and thereby damps the impact during opening of the inlet valve 73.

[0089] The operation of the thermal power plant according to the invention runs in the low temperature range. Therefore, with the selection of material for the components, special attention should be paid to the sliding problem in the case of the mechanical parts. Furthermore good heat insulation is helpful.

[0090] In the following the operating mode of the thermal power plant and of the energy conversion method according to the invention will be considered.

[0091] In a thermal power plant with condensation motor according to the invention, as shown in FIG. 9, a high-pressure steam is generated in the steam generator 25. For the working medium air, that is at a temperature between 132-160K and a pressure of 37-100 bar. With the heat input device 26 of the steam generator 25, the necessary heat energy is supplied from the heat source 27 with a suitable heat carrier. The generated high-pressure steam is led via the line 29 into the high pressure chambers of the cylinder heads 41, in which the high-pressure steam is fed into the stroke chambers by means of the inlet valve 57. The stroke is transmitted from the piston 45 through the piston rod to the crosshead 46, which transfers the force to the swinging arm 48 of the swinging arm mechanism. The crossheads 46 are guided in guiding pieces 47, so that no radial forces act on the piston. The crossheads 46 are guided on rollers so that the friction can be kept small. The swinging arm mechanism, which swings on the swinging arm shaft 49, transmits the work to the crank mechanism 50, with which, via a further mechanism, a generator is driven. Suitable as transmission is preferably an infinitely variable hydraulic transmission. A residual steam compressor 51 is also driven with the swinging arm 48. Likewise driven with the swinging arm 48 is the piston pump 54 via the pump lever 55, which swings about the bearing 56.

[0092] Through the expansion of the working medium there results a phase mixture of condensed portion, i.e. a condensate, and non-condensed portion, i.e. a steam portion. The machine housing 44 serves as phase separator, in that, e.g. by means of the principle of gravity, the condensed portion and the non-condensed portion are separated. The steam portion is sucked up and compressed above at the top of the machine housing 44 by the residual steam compressor 51. It is thereby to be observed that only 60% of the expanded steam has to be compressed again and that the intermolecular attraction facilitates the compression, as explained previously. This means that this influence is to be determined with the compressibility factor Z. The superheat and thus the energy balance of the process depend thereon.

[0093] The inlet valve 57 is controlled via the damper disc 61 of the valve rod 60, as shown in FIG. 11. When the damper disc 61 is pushed against the cylinder flange, this movement is transmitted via the valve rods 60 to the valve bridge 58, and the inlet valve 57, which is screwed to the valve bridge 58, is thereby opened. The inlet valve 57 is of cylindrical design, and moves like a piston some millimeters into the cylinder bore. The pressure is thereby limited by the closing spring 59, and pressure peaks, which can arise at the beginning of the stroke, can thereby be absorbed. The inlet valve 57 is closed again by means of the closing spring 59.

[0094] FIG. 12 shows the piston 45 with built-in outlet valve 70. Owing to the operation in low temperature range, lubrication is difficult. Thus contactless pistons 45 are provided for the condensation motor. This requires that the pistons 45 be fitted relatively precisely in the cylinder bore. With a gap width between cylinder bore and piston of 10 m, a leak rate of max. 1%, with 20 m, 6%, must be anticipated. Therefore supporting the crossheads 46 on rollers is foreseen, so that no radial forces act on the pistons 45. So that the pistons 45 really move in a contactless way, a centering ring 65 is provided that is made of a material having good dry-running properties. The front face of the piston 45 is designed as valve seat, on which the valve cone of the outlet valve 70 is installed. The valve cone is connected via the piston rod 71 to the slider 72, into which the switchover pin is built. With the switchover pin 69 the outlet valve 70 can be moved back and forth. The slider 72 has moreover the function of damping the impact of the outlet valve 70. The outlet valve 70 is engineered in such a way that it is closed with expansion stroke of the one piston and at the same time is open for the discharge at the opposite piston. The steam can flow away through the piston tube 66 and then through the exhaust port 67 into the machine housing 44, respectively the phase separator. Toward the end of the expansion stroke the switchover pin 69 moves against the switching spring 64, whereby the outlet valve 70 is switched.

[0095] FIG. 14 shows the control of inlet valve 57 and outlet valve 70 with opened inlet valve 57. Toward the end of the discharge stroke, the switchover pin 69 hits the switching spring 64 and thereby closes the outlet valve 70. Then the annular piston 68 drives into the annular groove 63<sic. 62> of the damper disc 61 and compresses the enclosed steam, whereby the impact is damped. At a pressure of 20-30 bar, the closing force at the inlet valve 57 is overcome and the valve is thereby opened. When the annular gap between the annular piston and the channel of the damper disc is very small, the outflow resistance becomes very great and thus a high pressure can be generated for a short time. During the filling process the air enclosed in the annular groove 63<sic. 62> flows away via the discharge bore 62<sic. 63>, so that the annular piston 68 rests in a close-fitting way on the bottom of the annular groove 63<sic. 62>, and a defined spacing and thus a defined fill quantity results between the inlet valve 57 and the piston 52.

[0096] FIG. 17 shows a simplified schematic representation of a steam turbine, as can be used, for example, for the phase separation of the condensed portion and of the non-condensed portion. FIG. 17a shows a top view of four steam nozzles 38, through which the vaporized working medium can be introduced. Through the centrifugal force in the turbine the two portions are separated. The condensed portion exits at the condensate outlet 39. FIG. 17b shows a longitudinal section through the steam turbine and a steam nozzle 38. In the turbine the working medium is diverted around a plane 40. Residual steam is discharged via a residual steam suction line 33.

[0097] For the design of the thermal power plant with the working fluid air, the following data result: The compressor capacity is regulated in such a way that the pressure in the machine housing 44, i.e. the phase separator, amounts to approximately 1 bar, which corresponds to a temperature of 70 K. In the residual steam compressor 51 the residual steam is compressed to 33 bar, which results in a condensation temperature of 130 K. This heated residual steam is led into the primary side of the condenser 36, in which it is liquefied with cold condensate, which is delivered through the secondary side of the condenser 36. At 130 K there results for 0.62 kg steam a heat of condensation of 40.56 kJ. If 0.38 kg of condensate is heated from 70K to 129 K, 44.84 kJ heat can be discharged. The re-cooling of 60% steam with 40% condensate is possible because the specific heat of the condensate is about twice as high as that of the superheated steam. Thus the steam portion can be condensed internally.

[0098] The resulting condensate is then led back into the steam generator 25 by means of the piston pump 54, so that there is heat recovery.

[0099] An electric machine can serve as motor for the start-up. The residual steam compressor thereby acts as gas compressor and puts the working fluid under pressure. The plant is thereby controlled in such a way that in the machine housing 44, i.e. the phase separator, there is a pressure of about 1 bar and on the overpressure side at least 40 bar. That results in a pressure drop of 1:40 and, seen adiabatically, a cooling from 293 K to 73 K. The condensation motor can thereby be cooled down and brought to operating temperature. When the operating temperature is reached, condensation operation begins and the electric machine is changed to generator operation. At the start the compressed gas can be pre-cooled to 293 K with the pre-cooler.

LIST OF REFERENCE SYMBOLS

[0100] 1 wet steam expansion [0101] 2 critical point [0102] 3 non-condensed portion [0103] 4 condensed portion [0104] 5 residual steam compression [0105] 6 re-cooling [0106] 7 residual steam condensation [0107] 8 pumping and heating of the condensed residual steam [0108] 9 pumping and heating of the cold condensate portion [0109] 10 vaporization [0110] 11 Maxwell distribution at the critical point [0111] 12 binding energy [0112] 13 quasi condensed molecules [0113] 14 non-condensable molecules [0114] 15 distribution curve according to Maxwell in the final state [0115] 16 condensable molecules in the final state [0116] 17 non-condensable molecules in the final state [0117] 18 compressibility factor Z [0118] 19 adiabatic curve for p.sub.A=131 bar [0119] 20 adiabatic curve for p.sub.A=37.2 bar [0120] 21 moving wall [0121] 22 median molecular velocity before impact [0122] 23 median molecular velocity after impact [0123] 24 doubled piston velocity [0124] 25 steam generator [0125] 26 heat input device [0126] 27 heat source [0127] 28 pump [0128] 29 high-pressure line [0129] 30 [0130] 31 [0131] 32 condensate connection [0132] 33 residual steam suction line [0133] 34 compressor [0134] 35 pre-cooler [0135] 36 condenser [0136] 37 condensate pump [0137] 38 steam nozzle [0138] 39 condensate outlet [0139] 40 plane [0140] 41 cylinder head [0141] 42 cylinder head gasket [0142] 43 working cylinder [0143] 44 machine housing/phase separator [0144] 45 piston [0145] 46 crosshead [0146] 47 guiding piece [0147] 48 swinging arm [0148] 49 swinging arm shaft [0149] 50 crank mechanism [0150] 51 residual steam compressor [0151] 52 piston [0152] 53 residual steam pressure line [0153] 54 piston pump [0154] 55 pump lever [0155] 56 pump lever bearing [0156] 57 inlet valve [0157] 58 valve bridge [0158] 59 closing spring [0159] 60 valve rod [0160] 61 damper disc [0161] 62 annular groove [0162] 64 switching spring [0163] 65 centering ring [0164] 66 piston tube [0165] 67 exhaust port [0166] 68 annular piston [0167] 69 switchover pin [0168] 70 outlet valve [0169] 71 valve rod [0170] 72 slider [0171] 73 inlet valve [0172] 74 outlet valve [0173] 75 residual steam outlet [0174] 76 piston star [0175] 77 bevel shoulder [0176] 78 damping sleeve [0177] 79 piston rod