CA1160465A - Multi-stage, wet steam turbine - Google Patents
Multi-stage, wet steam turbineInfo
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- CA1160465A CA1160465A CA000412808A CA412808A CA1160465A CA 1160465 A CA1160465 A CA 1160465A CA 000412808 A CA000412808 A CA 000412808A CA 412808 A CA412808 A CA 412808A CA 1160465 A CA1160465 A CA 1160465A
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Abstract
ABSTRACT OF THE DISCLOSURE
A multi-stage, wet steam turbine employs working fluid, such as steam for example, in its two-phase region with vapor and liquid occurring simultaneously for at least part of the cycle, in particular the nozzle expansion. A smaller number of stages than usual is made possible, and the turbine may handle liquid only.
Simple construction, low fuel consumption and high reliability are achieved.
A multi-stage, wet steam turbine employs working fluid, such as steam for example, in its two-phase region with vapor and liquid occurring simultaneously for at least part of the cycle, in particular the nozzle expansion. A smaller number of stages than usual is made possible, and the turbine may handle liquid only.
Simple construction, low fuel consumption and high reliability are achieved.
Description
1 ~0~
BACKGROI~ND OF THE - INVENTION
This invention is concerned with a new class of heat engines where the working fluid, for example steam, is used in its two-phase region with vapor and liquid occurring simultaneously for at least part of the cycle, in particular the nozzle expansion. The fields of use are primarily those where lower speeds and high torques are required, for example~ as a prime mover driving an electric generator, an engine ~or marine and ~o land propulsion, and generally as units of small power output. No restrictions are imposea on the heat source, which may be utilizing ~ossil fuels burned in air, waste heat, solar heat, or nuclear reaction heat etc.
The proposed engine is related to existing steam tu.rbine engines; however, as a consequence of using large fractions of liquid in the expanding part of the cycle, a much smaller number of stages may usually be required, and the tuxbine ma.y handle liquid only. Also, the thermodyn.amic cycle ~ay be altered considera~ly from the usual Rankine cycle, inasmuch as the expansion is taking place near the liquid line of $he temperature~
entropy diapgram, and essentially parallel to that line, as described below. In contrast to other proposed two-phase engines with two components (a high-~apor pressure component and a low-vapor pressure component, see U.S. Patents Nos.3,879,949 and 3,972,195), the present engine is limited to a single-component fluid, as for example water, the intent being to simplify the working ~ .~
04¢5 fluid storage and handling, and to improve engine reliability by employing well proven working medla of high chemical stability.
SUMMARY OF TE~E INVENTION
It is a major object of the invention to provide an economical engine of low capital cost due to simple construction, low fuel consum~tion, high reliability, and minimum maintenance requirements.
The ob]ective of low fuel consumption is achieved by "Carnotizi~g"the,leat engine cycle in a fashion similar to regenerative feed-water preheating, which consists in extracting ~xpanding steam from the turbine in order to preheat feed-water by condensation of the ext~acted steam. Since the pressure of the heat emitting condensing vapor and the heat absorbing feed-water can be made the same, a direct-contact heat exchanger may he used, which is of high effectiveness and typically of very small size.
Further, and in contrast to the co~ventional regenerative feed-water heating scheme~ the expanding steam is of low quality, typically o~ lO to 20~ mass fraction o vapor in the total wet mixture flow. As a result, the enthalpy change across the nozzle is reduced to such a degree that a two-stage turbine, for example, is able to handle the entire expansion head at moderate stress levels.
By way of contrast, a comparable conventional im~ulse steam turbines would require about ~ifteen stages. The turbine itself may consist of a liquid turbine that may be combined with a rotary separator in the manner to be described.
1 lB0465 These and other objects and advantages oE the inven-tion, as well as the details of an illustrative embodiment, will be more fully understood from the following description and drawings, in which:
i DRAWING DESCRIPTION
Fig. 1 is an axial vertical elevation, in section, schematically showing a two-stage liquid turbine, with recuperator;
Fig. 2 is a vertical section showing details of the Fig. 1 apparatus, and taken along the axis;
Fig. 3 is an axial view of the Fi~. 2 apparatus;
Fig. 4 is a flow diagram;
Fig. 5 is a temperature-entropy diagram; and Fig. 6 is a side elevation of a nozzle, taken in section.
~ETAILED DE5CRIPTION
Referring first to Fig. 1, the ~rime mover apparatus shown includeslfixed, non-rotating structure 19 including a casing 20,1 an output shaft 21 rotatable about axis 22 to drive and do work upon external device 23;
rotary structure 24 with~h the casing and direc~ly connected to shaft 21; and a free w~eeling rotor 25 within the casing.
A bearing 26 mounts the ~otor 25 to a casing flange 20a;
a bearing 27 enters sha~t 21 in the casing bore 20bi ~5 bearings 28 and 29 mount ~-tructure 24 on fixed structure 19; and bearing 30 cente~s rotor 25 relative to structure 24.
In accordance ~ith the invention, firs-t nozzle means, as for example no~zle box 32, is associated with fixed structure 19, and is supplied with wet steam for 0 expansion in the box. As also shown in ~igs. 2 and 3, the .. ., . .. ., ... . . ,.. ,, . ,. ... , . , , -~ ....
3 ~ 6 5 nozzle box 32 typically includes a series of nozzle segments 32a spaced about axis 22 and located between parallel walls 33 which extend in planes which are normal to that axis. The nozzles define venturis, including convergent portion 34 throat 35 and divertent portion 36.
Walls 33 are integral wi~h fixed structure 19. Wet steam may be supplied from boiler BB along pa~hs B 5 and 136 to the nozzle box. Figs. 2 and 3 shows the provision of fluid injectors 37 operable to inject fluid such as water into the wet steam path as defined by annular manifold 39, immediately upstream of the nozzles 32. Such fluid may be supplied via a fluid inlet 38 to a ring-shaped manifold 39 to which the injectors are connected. Such in~ectors provide good droplet distribution in the wet steam, for optimum turbine operating efficiency, expansion of the steam through the nozzles accelerating the water droplets for maximum impulse delivery to the turbine vanes 42. A steam inlet is shown at 136a.
Rotary turbine structure 24 provides first vanes, as for example at 42 spaced about axis 22, to receive and pass the water droplets in the steam .in the nozzle means 32. In this regard, the steam fraction increases when expanding. Such first vanes may extend in a~ial radial planes, and are typically spaced about axis 22 in circular 2S sequence. They extend between annular walls 44 and 45 of structure 24, to which an outer closure wall 46 is joined. Wall may fo~m one or more nozzles, two being shown at 47 in Fig. 3. Nozzles 47 are directed generally counterclockwise in Fig. 3, whereas noæzles 32 are directed generally clockwise, 50 that turbine structure 24 ~ 5- -rotates clockwise in Fig. 3. The turbine structure is basically a drum that contains a ring of liquid (i.e.
water ring indicated at 50 in Fig. 3), which is collected from the droplets issuin~ from nozzles 32. Such water -5a-.. . . . ,.. ..... ,.. ., ... , ~ . . ~ .. .. , .. ,; .. .. " , . .
issuing as jets from nozzles ~7 is under pressurization generated hy the rotation of the solid ring of water 50.
In this manner, the static pressure in the region 51 outwardly of the turbine structure need not be lower than the pressure of the nozzle 32 discharge to assure proper liquid acceleration across such nozzles 47. Tne radi~l vanes 42 ensure solid body rotation of ~he rins of liquid at the speed of the structure 24. The vanes are also useful in assuring a rapid acceleration of the turbine from standstill or idle condition.
Water collecting in region 51 impinges on the freely rotating rotor 55 extending about turbine rotor structure 24, and tends to rotate that ro~or with a rotating ring of water collecting at 56. A non-rotating scoop 57 extending into zone 51 collects water at the inner surface of the ring 56, the scoop communicating with second nozzle means 58 to be described, as via ducts or paths 1~9-1~63.Accordingly, expanded first stage 1.iquid (captured by free-wheeling drum or rotor 55 and scooped up ~ pitot opening 5-7) may be supplied in pressuri~ed state to the inlet of second stage nozzle 58~
Also shown in Fig. 1 is what may be referxed to as rotary means to receive feed water and to centrifugally pressurize same. Such means may take the for~ of a centrifugal rotarY pump 60 mounted as by bearings 61 to -fixed structure 19. The pump may include a series of discs 62 which are normal to axis 22, and which are located within and rotate with pump casing 63 rotating at the same speed as the turbine structure 24. ~or that purpose, _~;_ . .
~ 160~
a connection 64 may extena ~etween casing 63 and the turbine 24. The discs of such a pump ~as for example a Tesla pump) are olosely spaced apart so as to allow the liquid or water discharge from inlet spout 65 to "
distribute generally uniformly among the individual slots between the plates and to flow radially outwardly, while gaining pressure. - .
A recuperative zone 66 is provided inwardly of the turbine wall structure 24a,to communicate with the discharge 60a of rotating pump 60, and with the nozzle box 32 via a series of steam passing vanes 68.
The latter are connected to the turbine rotor wall 24b to receive and pass steam discharging from nozzles 32, imparting further torque to the turbine rotor. After passage be~een vanes 68, the ~team is drawn into direct heat exchange contact with the water droplets spun-off fxom the pump 60, in heat exchange, or recuperative zone 66. Both liquid droplets and steam have equal swirl velocity and are at equal static pressure in rotating zone 66~ as they mix therein~
The mix is ~ontinuously withdrawn for further heating and supply to the first nozzle means 32. For the puxpose, a scoop 70 may be associated with fixed structure 19, and extend into zone 6~ to withdraw the fluid mix for supply via fixed ducts 71 and 72 to boiler or heater BB, ~rom which the ~luid mix is returned via path 135 to the nozzle means 32.
The second stage nozzle me~ns 58 receives . water from scoop 57, as previously descri~ed, and also steam spill-over from ~pace 66, as via pakhs 74 and 75 Trade Mark adjacent tur~ine wall 24c. Such pressurized steam mixed with liquid ~rom scoop 57 is expanded in the second nozzle means 58 producing vapor and waterl the vapor being ducted via paths 78 and 79 to condenser CC. Fourth vanes 81 attached to rotating turbine wall 24d receive pressure application rom the flowing steam to extract energy from the steam and to develop additional torque.
The condensate from the condenser is returned via path 83 to the inlet 65 of pump 60. The water from nozzle L0 means 58 collects in a rotating ring in region 84, imparting torque to vanes 85 in that region bounded by turbine rotor walls 86 and 87, and outer wall 88. ~or that purpose, the construction may be the same as tha~ o the first nozzle means 32, water ring 50, vanes 42 and L5 walls 44-46. Nozzles 89 discharge water from the rotating ring in region 84, and correspond to nozzles 41. Free wheeling rotor 55 extends at 55a about nozzles 47, and collects water discharging from the latter, ~orming a riny in zone 91 due to centrifugal effect. Won-rotary 5COOp 90 collects water in the ring formed by rotor extent 55a, and ducts it at 92 to path 83 for return to the TESLA
pump 60.
The cylic operation of the engine will now be described by reference to the temperature-entropy diagram of Fig. 5, wherein state points are shown ln capital letters~ Arabic numerals refer to the compon~nts already referred to in Figs. 1-3.
Wet steam of condition ~ is delivered from the boiler to nozzle box 32 (Fig. 1). The special two-phase nozzles use the expanding vapor for the acceleration of . , . ~ , .... . . ..
46~
the liquid droplets so tha-t the mixtur~ of wet steam will enter the turbine rin~ 42 (Fig. 3) at nearly uniform velocity, at the thermoaynamic condition ~ .
The liquid will then separate from the vapor and issue through the nozzles 47 (Fig. 3) and collect in a rotating ring in the drum 55 (Fig. 1). The scoop 57 will deliver collected liquid to the nozzle box 58 at condition ~ .
The saturated expanded stea~ from nozzle 32 at a condition ~ (not shown) in the meantime will drive vanes 68 and enter the recuperator 66.
In the recuperator the vapor will be partially condensed by direct contact with feed-water originally at condition ~ from scoop 90 in Fig. 1, mixed with condensate as it is returned from the condenser CC. Both streams of liquid ~at condition ~ ) whether supplied by scoop 90 or that returning f~om the condenser CC is pumped up at 60 to the sta~ic pressure of the steam entering zone 66 (Fig. 1). The heat exchange by direc-t contact occurs across the surfaces of spherical droplets that are spun~off from the rotating discs of the TESLA pump, and into zone-66.
The heated li~uid of condition ~ that is derived ~rom preheating by the steam and augmented by condensate formed at condition ~ , is scooped up at 70 and returned to the boiler BB by stationery lines 71 and 72.
The steam which was not fully condensed in the recuperator 66 will pass on at 74 to nozzle box 58 where it is mixed with the liquid that was returned by scoop 57.
The ~ixture will be at a condition ~ I corresponding to the total amount of preheated liquid of condition ~ and _~9~
.
o ~ ~
saturated vapor of condition ~ .
The subsequent nozzle expansion at 58 from condition ~ to ~results in similar velocities as produced S
. -9a~ . - -- -. . , . , ~ , _ ,~ ., .. , . ,.. ~ .. - , . . . .
-3 ~60~5 in the expansion ~ to ~ in nozzle 32. The issuing jet can therefore drive the second liquid turbine efficiently at the speed of the first turhine, so that direct coupling of the two stages is possible.
The path of the liquid collected in dr~m 25 (Fig.l) a~
the condition E was already described as it is passed on to the inlet 65 of pump 60. The satura~ed vapor at condition ~ tnot shown) is ducted at 78 and 79 ~o the -condenser CC, which is cooled by a separate coolant. The condensate at condition E is then also returned at 83 to the pump inlet 65.
Alternate ways of condensing the steam of condition ~ may be envisioned ~hat are similar to the method employed herein to condense steam of condition ~
; at intermediatè pressure in the recuperator. The difference is that a direct contact low pressure condenser will require clean water to be used for the coolant, so that mixing with the internal working medium is possible. Such a liquid coolant will probabl~ best be cooled itself in a separate conventional li~uid-to-liquid or liquid-to-air heat exchanger"so that it may be re-circulated continuously in a closed, clean system.
The turbine engine described in FigO 1 is a two-stage unit with only one intermediate recu~rator.
An analysis of the efficiency of the thermodynamic cycle shows that the performance i5 improved amony others by two factors~
13 increased vapor quality of the steam trelative mass fractionof saturated steam) -- ~
1 lB0465
BACKGROI~ND OF THE - INVENTION
This invention is concerned with a new class of heat engines where the working fluid, for example steam, is used in its two-phase region with vapor and liquid occurring simultaneously for at least part of the cycle, in particular the nozzle expansion. The fields of use are primarily those where lower speeds and high torques are required, for example~ as a prime mover driving an electric generator, an engine ~or marine and ~o land propulsion, and generally as units of small power output. No restrictions are imposea on the heat source, which may be utilizing ~ossil fuels burned in air, waste heat, solar heat, or nuclear reaction heat etc.
The proposed engine is related to existing steam tu.rbine engines; however, as a consequence of using large fractions of liquid in the expanding part of the cycle, a much smaller number of stages may usually be required, and the tuxbine ma.y handle liquid only. Also, the thermodyn.amic cycle ~ay be altered considera~ly from the usual Rankine cycle, inasmuch as the expansion is taking place near the liquid line of $he temperature~
entropy diapgram, and essentially parallel to that line, as described below. In contrast to other proposed two-phase engines with two components (a high-~apor pressure component and a low-vapor pressure component, see U.S. Patents Nos.3,879,949 and 3,972,195), the present engine is limited to a single-component fluid, as for example water, the intent being to simplify the working ~ .~
04¢5 fluid storage and handling, and to improve engine reliability by employing well proven working medla of high chemical stability.
SUMMARY OF TE~E INVENTION
It is a major object of the invention to provide an economical engine of low capital cost due to simple construction, low fuel consum~tion, high reliability, and minimum maintenance requirements.
The ob]ective of low fuel consumption is achieved by "Carnotizi~g"the,leat engine cycle in a fashion similar to regenerative feed-water preheating, which consists in extracting ~xpanding steam from the turbine in order to preheat feed-water by condensation of the ext~acted steam. Since the pressure of the heat emitting condensing vapor and the heat absorbing feed-water can be made the same, a direct-contact heat exchanger may he used, which is of high effectiveness and typically of very small size.
Further, and in contrast to the co~ventional regenerative feed-water heating scheme~ the expanding steam is of low quality, typically o~ lO to 20~ mass fraction o vapor in the total wet mixture flow. As a result, the enthalpy change across the nozzle is reduced to such a degree that a two-stage turbine, for example, is able to handle the entire expansion head at moderate stress levels.
By way of contrast, a comparable conventional im~ulse steam turbines would require about ~ifteen stages. The turbine itself may consist of a liquid turbine that may be combined with a rotary separator in the manner to be described.
1 lB0465 These and other objects and advantages oE the inven-tion, as well as the details of an illustrative embodiment, will be more fully understood from the following description and drawings, in which:
i DRAWING DESCRIPTION
Fig. 1 is an axial vertical elevation, in section, schematically showing a two-stage liquid turbine, with recuperator;
Fig. 2 is a vertical section showing details of the Fig. 1 apparatus, and taken along the axis;
Fig. 3 is an axial view of the Fi~. 2 apparatus;
Fig. 4 is a flow diagram;
Fig. 5 is a temperature-entropy diagram; and Fig. 6 is a side elevation of a nozzle, taken in section.
~ETAILED DE5CRIPTION
Referring first to Fig. 1, the ~rime mover apparatus shown includeslfixed, non-rotating structure 19 including a casing 20,1 an output shaft 21 rotatable about axis 22 to drive and do work upon external device 23;
rotary structure 24 with~h the casing and direc~ly connected to shaft 21; and a free w~eeling rotor 25 within the casing.
A bearing 26 mounts the ~otor 25 to a casing flange 20a;
a bearing 27 enters sha~t 21 in the casing bore 20bi ~5 bearings 28 and 29 mount ~-tructure 24 on fixed structure 19; and bearing 30 cente~s rotor 25 relative to structure 24.
In accordance ~ith the invention, firs-t nozzle means, as for example no~zle box 32, is associated with fixed structure 19, and is supplied with wet steam for 0 expansion in the box. As also shown in ~igs. 2 and 3, the .. ., . .. ., ... . . ,.. ,, . ,. ... , . , , -~ ....
3 ~ 6 5 nozzle box 32 typically includes a series of nozzle segments 32a spaced about axis 22 and located between parallel walls 33 which extend in planes which are normal to that axis. The nozzles define venturis, including convergent portion 34 throat 35 and divertent portion 36.
Walls 33 are integral wi~h fixed structure 19. Wet steam may be supplied from boiler BB along pa~hs B 5 and 136 to the nozzle box. Figs. 2 and 3 shows the provision of fluid injectors 37 operable to inject fluid such as water into the wet steam path as defined by annular manifold 39, immediately upstream of the nozzles 32. Such fluid may be supplied via a fluid inlet 38 to a ring-shaped manifold 39 to which the injectors are connected. Such in~ectors provide good droplet distribution in the wet steam, for optimum turbine operating efficiency, expansion of the steam through the nozzles accelerating the water droplets for maximum impulse delivery to the turbine vanes 42. A steam inlet is shown at 136a.
Rotary turbine structure 24 provides first vanes, as for example at 42 spaced about axis 22, to receive and pass the water droplets in the steam .in the nozzle means 32. In this regard, the steam fraction increases when expanding. Such first vanes may extend in a~ial radial planes, and are typically spaced about axis 22 in circular 2S sequence. They extend between annular walls 44 and 45 of structure 24, to which an outer closure wall 46 is joined. Wall may fo~m one or more nozzles, two being shown at 47 in Fig. 3. Nozzles 47 are directed generally counterclockwise in Fig. 3, whereas noæzles 32 are directed generally clockwise, 50 that turbine structure 24 ~ 5- -rotates clockwise in Fig. 3. The turbine structure is basically a drum that contains a ring of liquid (i.e.
water ring indicated at 50 in Fig. 3), which is collected from the droplets issuin~ from nozzles 32. Such water -5a-.. . . . ,.. ..... ,.. ., ... , ~ . . ~ .. .. , .. ,; .. .. " , . .
issuing as jets from nozzles ~7 is under pressurization generated hy the rotation of the solid ring of water 50.
In this manner, the static pressure in the region 51 outwardly of the turbine structure need not be lower than the pressure of the nozzle 32 discharge to assure proper liquid acceleration across such nozzles 47. Tne radi~l vanes 42 ensure solid body rotation of ~he rins of liquid at the speed of the structure 24. The vanes are also useful in assuring a rapid acceleration of the turbine from standstill or idle condition.
Water collecting in region 51 impinges on the freely rotating rotor 55 extending about turbine rotor structure 24, and tends to rotate that ro~or with a rotating ring of water collecting at 56. A non-rotating scoop 57 extending into zone 51 collects water at the inner surface of the ring 56, the scoop communicating with second nozzle means 58 to be described, as via ducts or paths 1~9-1~63.Accordingly, expanded first stage 1.iquid (captured by free-wheeling drum or rotor 55 and scooped up ~ pitot opening 5-7) may be supplied in pressuri~ed state to the inlet of second stage nozzle 58~
Also shown in Fig. 1 is what may be referxed to as rotary means to receive feed water and to centrifugally pressurize same. Such means may take the for~ of a centrifugal rotarY pump 60 mounted as by bearings 61 to -fixed structure 19. The pump may include a series of discs 62 which are normal to axis 22, and which are located within and rotate with pump casing 63 rotating at the same speed as the turbine structure 24. ~or that purpose, _~;_ . .
~ 160~
a connection 64 may extena ~etween casing 63 and the turbine 24. The discs of such a pump ~as for example a Tesla pump) are olosely spaced apart so as to allow the liquid or water discharge from inlet spout 65 to "
distribute generally uniformly among the individual slots between the plates and to flow radially outwardly, while gaining pressure. - .
A recuperative zone 66 is provided inwardly of the turbine wall structure 24a,to communicate with the discharge 60a of rotating pump 60, and with the nozzle box 32 via a series of steam passing vanes 68.
The latter are connected to the turbine rotor wall 24b to receive and pass steam discharging from nozzles 32, imparting further torque to the turbine rotor. After passage be~een vanes 68, the ~team is drawn into direct heat exchange contact with the water droplets spun-off fxom the pump 60, in heat exchange, or recuperative zone 66. Both liquid droplets and steam have equal swirl velocity and are at equal static pressure in rotating zone 66~ as they mix therein~
The mix is ~ontinuously withdrawn for further heating and supply to the first nozzle means 32. For the puxpose, a scoop 70 may be associated with fixed structure 19, and extend into zone 6~ to withdraw the fluid mix for supply via fixed ducts 71 and 72 to boiler or heater BB, ~rom which the ~luid mix is returned via path 135 to the nozzle means 32.
The second stage nozzle me~ns 58 receives . water from scoop 57, as previously descri~ed, and also steam spill-over from ~pace 66, as via pakhs 74 and 75 Trade Mark adjacent tur~ine wall 24c. Such pressurized steam mixed with liquid ~rom scoop 57 is expanded in the second nozzle means 58 producing vapor and waterl the vapor being ducted via paths 78 and 79 to condenser CC. Fourth vanes 81 attached to rotating turbine wall 24d receive pressure application rom the flowing steam to extract energy from the steam and to develop additional torque.
The condensate from the condenser is returned via path 83 to the inlet 65 of pump 60. The water from nozzle L0 means 58 collects in a rotating ring in region 84, imparting torque to vanes 85 in that region bounded by turbine rotor walls 86 and 87, and outer wall 88. ~or that purpose, the construction may be the same as tha~ o the first nozzle means 32, water ring 50, vanes 42 and L5 walls 44-46. Nozzles 89 discharge water from the rotating ring in region 84, and correspond to nozzles 41. Free wheeling rotor 55 extends at 55a about nozzles 47, and collects water discharging from the latter, ~orming a riny in zone 91 due to centrifugal effect. Won-rotary 5COOp 90 collects water in the ring formed by rotor extent 55a, and ducts it at 92 to path 83 for return to the TESLA
pump 60.
The cylic operation of the engine will now be described by reference to the temperature-entropy diagram of Fig. 5, wherein state points are shown ln capital letters~ Arabic numerals refer to the compon~nts already referred to in Figs. 1-3.
Wet steam of condition ~ is delivered from the boiler to nozzle box 32 (Fig. 1). The special two-phase nozzles use the expanding vapor for the acceleration of . , . ~ , .... . . ..
46~
the liquid droplets so tha-t the mixtur~ of wet steam will enter the turbine rin~ 42 (Fig. 3) at nearly uniform velocity, at the thermoaynamic condition ~ .
The liquid will then separate from the vapor and issue through the nozzles 47 (Fig. 3) and collect in a rotating ring in the drum 55 (Fig. 1). The scoop 57 will deliver collected liquid to the nozzle box 58 at condition ~ .
The saturated expanded stea~ from nozzle 32 at a condition ~ (not shown) in the meantime will drive vanes 68 and enter the recuperator 66.
In the recuperator the vapor will be partially condensed by direct contact with feed-water originally at condition ~ from scoop 90 in Fig. 1, mixed with condensate as it is returned from the condenser CC. Both streams of liquid ~at condition ~ ) whether supplied by scoop 90 or that returning f~om the condenser CC is pumped up at 60 to the sta~ic pressure of the steam entering zone 66 (Fig. 1). The heat exchange by direc-t contact occurs across the surfaces of spherical droplets that are spun~off from the rotating discs of the TESLA pump, and into zone-66.
The heated li~uid of condition ~ that is derived ~rom preheating by the steam and augmented by condensate formed at condition ~ , is scooped up at 70 and returned to the boiler BB by stationery lines 71 and 72.
The steam which was not fully condensed in the recuperator 66 will pass on at 74 to nozzle box 58 where it is mixed with the liquid that was returned by scoop 57.
The ~ixture will be at a condition ~ I corresponding to the total amount of preheated liquid of condition ~ and _~9~
.
o ~ ~
saturated vapor of condition ~ .
The subsequent nozzle expansion at 58 from condition ~ to ~results in similar velocities as produced S
. -9a~ . - -- -. . , . , ~ , _ ,~ ., .. , . ,.. ~ .. - , . . . .
-3 ~60~5 in the expansion ~ to ~ in nozzle 32. The issuing jet can therefore drive the second liquid turbine efficiently at the speed of the first turhine, so that direct coupling of the two stages is possible.
The path of the liquid collected in dr~m 25 (Fig.l) a~
the condition E was already described as it is passed on to the inlet 65 of pump 60. The satura~ed vapor at condition ~ tnot shown) is ducted at 78 and 79 ~o the -condenser CC, which is cooled by a separate coolant. The condensate at condition E is then also returned at 83 to the pump inlet 65.
Alternate ways of condensing the steam of condition ~ may be envisioned ~hat are similar to the method employed herein to condense steam of condition ~
; at intermediatè pressure in the recuperator. The difference is that a direct contact low pressure condenser will require clean water to be used for the coolant, so that mixing with the internal working medium is possible. Such a liquid coolant will probabl~ best be cooled itself in a separate conventional li~uid-to-liquid or liquid-to-air heat exchanger"so that it may be re-circulated continuously in a closed, clean system.
The turbine engine described in FigO 1 is a two-stage unit with only one intermediate recu~rator.
An analysis of the efficiency of the thermodynamic cycle shows that the performance i5 improved amony others by two factors~
13 increased vapor quality of the steam trelative mass fractionof saturated steam) -- ~
1 lB0465
2) An increased number of intermediary recuperators. Since an increase in vapor quality raises the magnitude o~ the nozzle discharge velocity, a compromise is called for between number of pxessure stages, allowed rotor tip speed, and num~er of recuperators. Note that sa~urated steam may be extracted at equal increments along the nozzlei at least two recuperators operating at intermediate pressure levels may be arranged per stage in order to improve the cycle efficlency without increasing o the nozzle velocity.
Other types o~ liquid turbines may be used instead of the particular turbine shown in Fig. 1 and Pig. 2. See for example U.S. Patents 3,8?9,949 and 3~972,195.
Alsor a more conventional turbine with buckets .5 around the periphery may be employed and which admits a homogeneous mixture of saturated steam and satùrated water droplets.
Good ef~iciencies for such turbines are obtainable if the droplet size of the mixture emerging from the nozzle !0 is kept at a few microns or less.
To achieve the latter, the con~erging-diverging nozzle may ~e designed with a sharp-edged throat as a transition from a straight converging cone 200 to a straig~.t divera,~ng cone 201. See Fig. 6 showing such a ~5 noz~le 202.
Fig. 1 also shows annular partition 95 integral with xotor 55, and separating rotary ring of water 56 from rotary ring 91 o~ water.
,o ' .~ ,
Other types o~ liquid turbines may be used instead of the particular turbine shown in Fig. 1 and Pig. 2. See for example U.S. Patents 3,8?9,949 and 3~972,195.
Alsor a more conventional turbine with buckets .5 around the periphery may be employed and which admits a homogeneous mixture of saturated steam and satùrated water droplets.
Good ef~iciencies for such turbines are obtainable if the droplet size of the mixture emerging from the nozzle !0 is kept at a few microns or less.
To achieve the latter, the con~erging-diverging nozzle may ~e designed with a sharp-edged throat as a transition from a straight converging cone 200 to a straig~.t divera,~ng cone 201. See Fig. 6 showing such a ~5 noz~le 202.
Fig. 1 also shows annular partition 95 integral with xotor 55, and separating rotary ring of water 56 from rotary ring 91 o~ water.
,o ' .~ ,
Claims (9)
1. A gas/liquid separator comprising a housing, a rotor mounted for rotation about an axis in the housing, the rotor having an inside surface, means for directing a gas/liquid mixture toward the inside surface of the rotor for rotating the rotor, and a plurality of fan blades on the rotor to rotate therewith for passing gas separated from the liquid that rotates the rotor, said blades located closer to said axis than said inside surface.
2. The separator of claim 1 wherein said means includes nozzle structure.
3. The separator of claim l including other means to receive liquid from said inside surface of the rotor.
4. A gas/liquid separator comprising a housing having an inlet for a gas/liquid mixture to be separated, a rotor mounted for rotation about an axis in the housing, the rotor having an inside peripheral surface, a plurality of turbine blades on the rotor and located closer to said axis than said inside surface and directed toward the inside peripheral surface of the rotor, means between the inlet and the turbine blades for directing a gas/liquid mixture toward the turbine blades for rotating the rotor and for causing liquid to collect on the inside peripheral surface of the rotor, with gas separating from the liquid, and other blades on the rotor to rotate therewith for discharging gas separated from said liquid.
The separator of claim 4 wherein said means includes nozzle structure.
6. The separator of claim 4 including means to receive collected liquid flowing from said inside surface of the rotor
The separator of claim 4 wherein said other blades are axially spaced from said turbine blades.
8. The separator of claim l including nozzle means on said rotor and located to receive liquid from said inside surface of the rotor.
9. The separator of claim 8 wherein said nozzles are angled to jet liquid therefrom for producing torque to rotate the rotor.
Priority Applications (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
CA000412808A CA1160465A (en) | 1979-03-05 | 1982-10-04 | Multi-stage, wet steam turbine |
Applications Claiming Priority (4)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
US17,456 | 1979-03-05 | ||
US06/017,456 US4258551A (en) | 1979-03-05 | 1979-03-05 | Multi-stage, wet steam turbine |
CA000346953A CA1159264A (en) | 1979-03-05 | 1980-03-04 | Multi-stage, wet steam turbine |
CA000412808A CA1160465A (en) | 1979-03-05 | 1982-10-04 | Multi-stage, wet steam turbine |
Publications (1)
Publication Number | Publication Date |
---|---|
CA1160465A true CA1160465A (en) | 1984-01-17 |
Family
ID=27166606
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
CA000412808A Expired CA1160465A (en) | 1979-03-05 | 1982-10-04 | Multi-stage, wet steam turbine |
Country Status (1)
Country | Link |
---|---|
CA (1) | CA1160465A (en) |
-
1982
- 1982-10-04 CA CA000412808A patent/CA1160465A/en not_active Expired
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