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CA1066968A - Exhaust steam reheater - Google Patents

Exhaust steam reheater

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Publication number
CA1066968A
CA1066968A CA274,790A CA274790A CA1066968A CA 1066968 A CA1066968 A CA 1066968A CA 274790 A CA274790 A CA 274790A CA 1066968 A CA1066968 A CA 1066968A
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CA
Canada
Prior art keywords
steam
drums
drum
turbine
pressure
Prior art date
Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
Expired
Application number
CA274,790A
Other languages
French (fr)
Inventor
Paul Morcov
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Individual
Original Assignee
Individual
Priority date (The priority date is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the date listed.)
Filing date
Publication date
Application filed by Individual filed Critical Individual
Priority to CA274,790A priority Critical patent/CA1066968A/en
Application granted granted Critical
Publication of CA1066968A publication Critical patent/CA1066968A/en
Expired legal-status Critical Current

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Abstract

ABSTRACT OF THE DISCLOSURE

Apparatus for reheating the exhaust steam or other working fluid from an external combustion engine e.g. a turbine, comprises two contra-rotating drums, each containing conduit means arranged in a spiral through which the exhaust fluid flows in succession, the drums being located in a cylindrical housing which is divided into four quadrants through which the drums rotate, two of the quadrants being supplied with heat from an external source, one quadrant being neutral and one quadrant being cooled.

Description

~66968 BACKGROUND OF THE IN~IENTION
This invention relates to apparatus for reheating the exhaust steam or other working fluid from an external combustion engine, e.g. a turbine.
One of the most important uses of the apparatus is that of a steam regenerator in power stations where it receives exhaust steam from the turbine and takes over some or all of the functions of the stationary boiler.
In a nuclear power station the apparatus may be used as a steam superheater thus increasing the thermal efficiency.
The conventional condensers are eliminated by the present invention.
A vacuum (0.04 atm.) in the condenser of a conventional steam plant allows a further expansion in the exhaust stage of the turbine which contributes to increasing the latter's efficiency. Since the condenser~ however, requires a lot of water (60 - l00 times as much as steam) the construction of a power station mainly depends on the water supply.
The solution of this problem has become more and more difficult especially with respect to nuclear power stations as the events of recent days : have taught us.
The condensing-turbine works nowadays with a degree of efficiency of its own of 70-72%, whereas its total degree of efficiency, however, may decrease to 35-40% according to the technological design governing the utility of heat. In other words, the total efficiency oE a powcr statioll operating with steam turbilles depends on the thermal Eall or, in our case, of the steam enthalpy being 400-500 Kcal/Kg for condensing-turbines with great efficiency and 150-250 Kcal/Kg for counter-pressure turbines, whereas the total enthalpy of fresh steam amounts to 700-860 Kcal/Kg (for 600C and 200 atm.). So we can observe an enormous loss of heat in such stations and as a consequence, only 30% of the fuel energy which is supplied is transformed into mechanical work.

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- For years the phenomenon of condensation has supported the con-viction that heat from steam evaporation can be obtained by means of the con-denser. Nevertheless, it is a well known fact that 60% of the total steam heat is taken away by the cooling medium, plus 5% other heat losses.
A temperature fall takes place in the condenser, but the vacuum is the only effect of condensation and it is paralleled by the decrease in enthalpy and is advantageous. Some authors give the following results: 1%
vacuum (more than 90%) corresponds to 1% of fresh steam. But they all agree : upon the statement that for thermodynamic reasons the condenser requires an enormous supply of energy. According to the Mollier h-s diagram the decrease in enthalpy can maximally amount to 210 Kcal/~g for steam under a pressure of 1 atm. (97% vacuum). Consequently 329.4 Kcal/Kg are lost. The same applies to the counter-pressure turbine in which after having passed the turbine the - steam is reutilized and transformed into water by condensation -- a natural phenomenon -- but this transformation results in the evaporation heat being lost (at a minimum 539.4 Kcal/Kg with 1 atm. and 100C). In order to avoid such an important loss of heat, the enthalpy of the steam must be increased again after having passed the last stage of the turbine to avoid being a quan-tity of steam transformed into water. Consequently, the condenser must be substituted by a new device.
The apparatus of the present invention can be used as a steam sup-ply for an energy producing plant irrespectivo of whether it is stationary or mobile (locomotives, vessels or other vehicles). In chemical plants there are processes which require very high pressures and temperatures, and in this field of application the compressors and fans presently used can be success-fully replaced by a regenerator in accordance with the present invention. In metallurgy the present invention can be used as a hot-air compressor, as for example, for a blast furnace; or it can replace axial compressors in power stations operating with gas turbines.

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1066~6~3 SUMMARY OF THE INVENTION
The pressure regenerator of the present invention comprises two contra-rotating drums each containing conduit means arranged in a spiral through which the exhaust fluid flows in succession. The drums are located in a cylindrical housing which is divided into four quadrants through which the drums rotate in opposite directionsO Two of the quadrants are supplied with heat (180), one quadrant (135) is neutral, and the last quadrant (45) is cooledO During rotation of the drums the exhaust steam is heated (150C
to 520C), and consequently the pressure increases from 5 atm. to 36.5 atm.
At a discharge point (after 180), a predetermined quantity of steam is . delivered as fresh steam back to the turbine. In the third quadrant the "rest-pressure" (5 atm.) will be uniformly delivered to the sections in the first and second quadrants~ Thus, the pressure increases due to the temperature rise and the admission of steamO In the fourth quadrant (45-cooled) the steam pressure is reduced to a minimum value (1-3 atmO) thus allowing the sections to be recharged in the first quadrantO
The part, improvement or combination which is claimed as the i.nvention herein is an apparatus for increasing the pressure and temperature of exhaust working fluid from a heat engine, comprising a casing defining two heating zones, a neutral zone and a cooled zone, at ].cast one pair of contra-rotating drums in thc casing arranged such that successive sections of each drum pass in sequence through such zones, and a spiral].y-coiled pipe in each drum, the pipes being connected such that fluid fed to one drum passes in succession through the pipes of both drums to an outlet from the other drumD The invention may include a fuel burner to supply heat to the heated zones, stationary steam raising pipes within the heated zones to feed steam to the first drum and/or means for directing a flow of fresh air to cool the cooled zone~ The drums may be arranged to rotate about a common . ~ -3-..

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1C~669~8 ' vertical axisO Other constructional variations of the basic invention are also claimed in the claims herein.
~- The apparatus of the present invention may be used as a pressure regenerator, heated with combustion gases or with an appropriate burning unit or as a rotating steam boiler as a substitute for a stationary boiler.
BRIEF DESCRIPTION OF THE DR~WINGS
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The pressure regenerator will now bP described in detail with reference to the accompanying drawings wherein:
Figure 1 is a vertical sectional view of the apparatus according to ~he invention;
" Figure 2 is a partial plan view of the apparatus of Figure l;
Figure 3 diagrammatically shows the flow of steam between two rotating drums;
Figure 4 is a plan view of a plant incorporating the pressure :, :
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~066968 . regenerator heated with combustion gases;
Figure 5 is a partial sectional elevation of the rotating steam boiler with four drums;
Figure 6 is an enlarged view of detail "X" in Figure 5;
Figure 7 is a plan view of the apparatus shown in Figure 5;
Figure 8 is a cross-sectional view showing the flow of lubricant . and coolant to the apparatus particularly in the principal axis;
Figure 9 is a partial plan view of the arrangement shown in Figure - 8;
Figure 10 is an enlarged view of detail "X" in Figure 9;
Figure 11 is a sectional view taken along the line A-A in Figure 10; and .. Figure 12 is a diagrammati.c illustration of Table No. 1 showing the increase and decrease of pressures for both drums (above the line), the increase and decrease of the weight (below the line), and the temperature variation (below the line) Eor each section of the drum.
:. DESCRIPTION OF THE PREFERRED EMBODIMENT
As shown in Figures 1 - 3 a pressure regenerator comprises two drums l, 2, one of which is situated below the other, revolving in opposite directions and subdivided into sixteen sections. These sections consist o:~
"spiral pipes" which are mounted on an inner ring G. 'I'he :intcrior o:E the casing 18 enclosing the drums is subdivided into four quadrants. As the drums rotate, each section passes through two quadrants (180) of hot space whereas . the third quadrant is neutral space (135) and the last, the fourth quadrant (45), is cooled by fresh air. The inner ring also is subdivided into sixteen cells and surrounds an inner pipe 7 enclosing a water cooling jacket. The water flows upwardly to where the inner pipe 7 is connected wi.th the spiral pipe 5. In this spiral pipe is the steam produced (about 10%) in order to ;: .
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compensate the loss of steam in a turbine connected to the regenerator. After a section has been filled with exhaust steam through a supply pipe the steam pressure is raised in the first and second quadrants during the rotation of the drum.
At a discharging point ~after 180) a certain quantity of steam (here: G=0.24 Kg) is discharging from the section. The charging and discharg-- ing points are indicated in Figure 2. The sections are discharged in the third quadrant and the steam passes from the first drum 2 to the second drum through channels between pipe 7 and pipe 8. This process which causes raising and reducing the steam pressure is illustrated in Figures 3 and 12 which dia-grammatically illustrate Table No. 1 hereinafter. Whereas in the first and second quadrants the sections are charged with steam, the opposite process takes place in the third quadrant where the cells are partially discharged.
Since the heat only "walks" from one drum to the other, this "ballast" cannot be considered as a thermal disadvantage. It is obvious that as a result of this the dimension of the drum must increase, since this is the only feasible way to raise the steam pressure.
In the fourth quadrant the pressure decreases as a result of the - cooling (in our example to 3 atm.) thus allowing the sections to be recharged in the first quadrant.
According to the increase of steam speed in the cells thc heat transition coefficient is increasing too. Therefore in certain cases (extreme-ly loaded units) it is advisable to provide the different parts of the sections with a "bypass" 34 (Figure 3). The inner pipe 8 is attached to a base plate 16 and serves as a steam supply line and a support for the two drums. A ball bearing 15 and condensation water pipes are situated at the lower end.
The two drums are driven by an electric motor 27 (Figure 7) through pairs of gear rings 14 (Figures 5 and 6). A packing placed between the ring . -.. .

and the pipe consists of a pair of plates lO (Figures 9 - 11), which are pressed against the pipe by oil pressure fed by a pump 11 and through a cooler 12.
The drums form a "battery" with one common function of raising the steam pressure. Two batteries may be coupled in series as shown in Figure 5 thus avoiding an increase in the drum diameter. By using the pressure regenerator in place of the condenser, the importance of the stationary boiler can be very much reduced, since only the latter is responsible for the steam losses (10 - 15%).
If a power station is profiled for the production of electric cur-rent, it is more advantageous to replace the stationary boiler by a device according to the invention so all additional equipment, e.g. water supply, burning unit, can be reduced.
Figure 5 shows a very simple compact plant including the following units:
- four drums (1-4) operating as a rotating steam boiler, - a fresh-air fan with air-preheater 21, - a burner unit 22, - a water supply (from a pump 23 water enters the water cooling jacket of the inner pipe 7, subsequently the preheater 24), - an evaporation pipc 25, - a superheater 26, - an electric geared drive motor 27, - an exhaust stack 28, - lagged casing 29, - seals 30.
From the low-pressure superheater 26 the steam passes to an accumulator 31 which is connected with a line 32. When the steam enters the line a great ,.

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part of it passes to the turbine through a valve 33. When the turbine is working the steam escapes directly into the line 32 and the valve 33 remains partly closed. The cool air which is required to cool the drum is taken in at the fourth quadrant and pumped ~o the burner, so an air-preheater is replaced - by the rotating boiler itself. The drums are driven by a single gear 27, a few satellites 14 and small conical gearwheels 13 are situated between the gearwheels 13 of the drums.
The rotating boiler has the following advantages:
- a greater thermal efficiency, - a simple and more flexible way of operating, - a cooling water supply for a condenser becomes superfluous, and for the boiler it can be reduced by 90%, - it requires little capital and short erection time, - safety, since a breakdown can only concern 1/32 of the rotating boiler, - power station, nuclear power station included, can be built any-where because they become independent of river water.
One example of the invention is based on the following presuppos-tions:
A pressure regenerator for a counter-pressure turbine of 4,400 IIP
has the following characteristics:
- steam consumption = 8.63 Kg/seg - steam pressure = 33 atm. spec. vol. = 0.09 mc/Kg super spec. wt. = 11 Kg/mc heated - steam temperature = 400C steam - enthalpy = 770 Kcal/Kg - steam quantity/sec. = 7.77 Kg :;.

' 106~968 - steam pressure = 5 atm. spec. vol. = 0.38 mc/Kg spec. wt. = 0.262 Kg/mc~ exhaust - steam temperature = 170C I steam - enthalpy = 673 Kcal/Kg The section of the pressure regenerator is supplied with exhaust steam, and after half a turn of the drums the pressure increase from 5 atm. to 36.5 atm., since there is a counter-pressure of 33 atm. at the discharging point.
- Increase of enthalpy = 770-673 = 97 Kcal/Kg - The steam loss in the turbine is estimated at 10%, - This example is based on two drums, each of which is provided with sixteen sections and which rotate at 60 revs./min.
The volume of the sections is chosen so that a steam remains in the section at the discharging point after 0.24 Kg of steam have passed to the turbine. According to the diagram (Figure 12) this remainder = 2.190 Kg.
In the fourth quadrant the steam pressure temperature decreases to 3 atm. and 135C. According to Table 1, the weight per section in this state is G = 0.390 Kg of steam. The results of this process are:
- 0.390 Kg steam = remainder in the section - 0.240 Kg exhaust steam = from the turbine ' - 1.800 Kg transfer steam = pass:ing b~tween th~ two drums Total = 2.430 Kg steam/section at the discharging point.
The section volume is calculated in the following way:

V = ~ = i43 = 0.24 mc According to the state equation the result at the discharging point is:

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~(~6696~

PV = GRT PV = 10,33Q x 36.5 x 0.24 = 90,500 kgmgrd ; GRT = 2.43 x 47 x 793 = 90,500 kgmgrd Steam consumption/sec. = 0.240 Kg - heated exhaust steam 0.030 Kg - fresh steam Total = 0.270 Kg x 32 sections = 8.64 Kg/sec;
The drum volume (sixteen sections) is : 0.24 x 16 = 3.84 mc.
A diameter of 50 x 4.5 mm is selected for the spiral-pipes which are made of austenitic steel, net profile F = 1320 mm2.
The total length of a section is:

L = F = o l32 = 180 m for the whole drum: L = 180 x 16 = 2900 m. The outer surface of a section is: 180 x D x 3.14 = 28.3 m2. The spiral pipe is curved with a radius of R = 2D = 2 x 50 = 100 mm. Each section consists of three spirals at 60 m.
The diameter for a drum per 1 m height of the spiral pipe is:
F = H = = gross volume and is F x H 2 Gross profile/pi~e = 50 x 50 = 2,500 mm Against 1,320 mm~ (net profile) = an increase of 88%.
Also gross volume V = 3.84 x 88% = 7.25 mc and F = i25 = 7.25 m and Drum Diameter D = 4 x 37 124 = 3 m For rigid construction the spiral pipe is attached to the ring 6 by means of creep resistant steel. All other constructional details are carried out in accordance with DIN (The German Industrial Standard).
By means of flowing exhaust gas with the temperature tl the heat is imparted by convection to the surface of the spiral pipe with the temperature tWl conducted through the wall with the thermal conductivity ~ and the thick-_ g _ , ...- ' :.

669~;~
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nessV~ and finally -- by convection of the opposite wall surface, the tempera-ture of which is tW2 -- into the exhaust steam which originally had a temperature of 170C.
q/section = ~lF. (tl-tW~ .F.(twl tw2) 2 w2 2 or q = k.F.(tl-t2) where k = thermal conduction coef.
It is obvious that k is the most important factor. It depends on material, temperature, steam speed, etc.
The heat consumption is calculated as follows:
- 0.39 Kg steam (135 and 3 atm.) = 770-660 Kcal =
110 x 0.39 = 43 Kcal - 0.24 Kg exhaust steam ~170 and 5 atm.) =
770 = 673 Kcal = 97 x 0.24 = 23 Kcal Total = 66 Kcal It is to be noted that the 0.030 Kg fresh steam, which is produced by the pipe 3, does not arise from the regenerator pressure.
: In the present case, calculations are based on the following values:
k = 60 Kcal/mhgrd F = 28.3 m /section tl = 560C temperature of the combustion gas t2 = 280C average temperature of the exhaust steam Also q = 60 x 28.3 x (560 - 280) = 475,4~0 Kcal/h per sec. = 473'4640 = 132 Kcal and for 1/2 sec. = 122 = 66 Kcal as already indicated above.
It can be seen in the scheme shown in Figure 4 how the rotating boiler operates in an existing power station. If "radiating bodies" (gas-supplied infrared radiators) are required these bodies can be mounted directly on the casing 18. This device, however, is only used with extremely loaded ~t~
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~L066968 ` units. For new plants it is adYisable to utilize the rotating steam boiler as a substitute for a conventional boiler.
In the fourth quadrant the drums are cooled by means of fresh air thus reducing the pressure from 5 to 3 atm. and temperature from 400 C to 135C.
The necessary heat transport is calculated as follows:
q = G.cv ~t2-tl) Kcal = 0.39 x 0.28 x ~400 - 135) Kcal.
q = 0.109 x 265 = 29 Kcal/section ===============
The carrying of heat results:

a.F. ~tl-t2) a = 40 Kcal/mhgrd q=
F = 28.3 m2 ~r = 0.0045 m tl = 400C t2 = 20 + 135 = 77 5C

Consequently:
q = 40 x 28 3bX ~400-77-5? = 81,000,000 Kcal/mhgrd-` per one sec. q = ~l'3'6-00- = 22,500 Kcallsec.

or per lt8 sec. q = '8 = 2,810 Kcal/section > 29 Kcal.

In order to guarantee a perfect functioning of the apparatus, it is provided with measuring and regulating instruments. Especially the tempera-'~ ture in the quadrants and the steam pressure ln the sections IllUst be strict]y observed.

The heat balance sheet of the apparatus shows:

- supplied heat (after the turbine)/sec. = 8.63 x 770 = 6,645 - losses (caused by cooling - decrease in enthalpy) =

29 x 32 = 930 Kcal loss = 6 945 = 14 % (without quota for actuation = 1%) A condenser heat balance sheet shows:

~' .
'~' ~066968 - supplied heat (after the turbine)/sec. = 8.63 x 770 = 6,645 - loss (caused by cool water in the condenser):
539.4 - 110 = 329 Kcal/Kg and 8.63 x 429 = 3,700.
- quota for actuation = 5% (self consumption) = 5% x 6,645 = 332 Kcal Total = 4,032 Kcal Loss = 6'645 = 60.7%
The results show that the heat loss in a condenser can be four times as important as in a pressure regenerator according to the invention.
The loss is reduced still further when the regenerator is utilized as a boiler substitute. Generally in a conventional plant (with boiler and condenser) the energy supplied by fuel ~00%) is distributed in:
- 15% losses in the boiler ~exhaust gas, lines, convection) - 30% mechanical work ' - 7% loss of steam in the turbine ' - 42% carried away by cooling water in the condenser ~, - 5% for actuation (self consumption) - 1% other losses By utilizing the present invention, the energy supplied by the fuel is distributed in:
- 8% boiler losses - 68% mechanical work - 7% steam loss~s in the turbine
- 2~ for actuation - 14% losses caused by cooling the drums - 1% other losses So twice as much mechanical work can be produced Wit}l the present invention than with a condenser.

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Claims (12)

THE EMBODIMENTS OF THE INVENTION IN WHICH AN EXCLUSIVE
PROPERTY OR PRIVILEGE IS CLAIMED ARE DEFINED AS FOLLOWS:
1. Apparatus for increasing the pressure and temperature of exhaust working fluid from a heat engine, comprising a casing defining two heated zones, a neutral zone and a cooled zone; at least one pair of contra-rotating drums in said casing arranged such that successive sections of each drum pass in sequence through said zones; and a spirally-coiled pipe in each drum, said pipes being connected such that fluid fed to one drum passes in succes-sion through the pipes of both drums to an outlet from the other drum.
2. Apparatus according to claim 1 including a fuel burner to supply heat to said heated zones.
3. Apparatus according to claim 2 including stationary steam raising pipes within said heated zones to feed steam to said one drum.
4. Apparatus according to claim 1, 2 or 3 further comprising means for directing a flow of fresh air to cool said cooled zone.
5. Apparatus according to claim 1 wherein said drums are arranged to rotate about a common vertical axis, said apparatus further comprising an electric motor and gearing to drive said drums.
6. Apparatus according to claim 5 further comprising a hollow support for mounting said drums, inlet and outlet pipes within said hollow support for said drums and a cooling water jacket surrounding said hollow support.
7. Apparatus according to claim 6 wherein said drum sections are sealed and wherein they engage the hollow support by sealing laminae disposed on the wall of said support and by hydraulic pressure of lubricating fluid applied to the surface of said support.
8. Apparatus according to claim 7 further comprising an oil pump and a radiator for supplying said lubricating fluid.
9. Apparatus according to claim 1 further comprising peripheral ring gears meshing in pairs with bevel drive gears for rotatably driving said drums.
10. Apparatus according to claim 1 further comprising a pipe spiral provided above said drums for receiving cooling water from said drums to com-pensate for vapor losses.
11. Apparatus according to claim 1 wherein said cooling zone serves as a preheater for air supplied to said heated zone.
12. A steam-driven power plant including a turbine and apparatus accor-ding to claim 1 connected to said turbine such that the exhaust steam from said turbine is fed into and through said apparatus and returned to the steam inlet of said turbine in a closed cycle.
CA274,790A 1977-03-25 1977-03-25 Exhaust steam reheater Expired CA1066968A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
CA274,790A CA1066968A (en) 1977-03-25 1977-03-25 Exhaust steam reheater

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
CA274,790A CA1066968A (en) 1977-03-25 1977-03-25 Exhaust steam reheater

Publications (1)

Publication Number Publication Date
CA1066968A true CA1066968A (en) 1979-11-27

Family

ID=4108245

Family Applications (1)

Application Number Title Priority Date Filing Date
CA274,790A Expired CA1066968A (en) 1977-03-25 1977-03-25 Exhaust steam reheater

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