TWO-PHASE REACTION TURBINE
Technical Progress ReportFor the Period July-December 1999
FAS Engineering, inc.2039 Dublin Drive, Glendale, CA9102
Tel (818) 952-0217, (818) 95243915Email: gfabris@earthlink. net
Principal Investigator, Dr. Gracio Fabris,
Prepared for theINVENTIONS AND INNOVATION SECTION OF
THE UNITED STATES DEPARTMENT OF ENERGYUnder contract
DE-FG36-98G01 0317
During the initial part of this period the concentrated effort was placed on gettingcomprehensive analysis and design of the turbine prototype. This was in order tobe able to initiate its fabrication as needed for its building, assembling and timelytesting.
In the second part of this period the effort was placed on design and otherconsiderations needed to acquire the test rig within the limited budget based onsubsequent grant from the DOE. This certainly is very challenging undertaking.
1} Analyze Other Mechanical Enqineerinq Turbine Desiqn Issues
Design of any turbine prototype is very challenging task in itself. Repeatediteration and extended reconsideration are needed.
Due to large volume of steam at the turbine exhaust a large flow cross-section isnecessary. For this reason the stationary housing is designed in form of domewith its open end facing downwards. This dome, i.e. the turbine housing, is goingto be placed on the top of a separator tank.
We have decided to avoid cantilever shaft-rotor design. Two stainless steelbearing are placed on each side of the impeller and at a short distance from it. In
DISCLAIMER
This report was,,prepared as an account of work sponsoredby an agency of the United States Government. Neitherthe United States Government nor any agency thereof, norany of their employees, make any warranty, express orimplied, or assumes any legal liability or responsibility forthe accuracy, completeness, or usefulness of anyinformation, apparatus, product, or process disclosed, orrepresents that its use would not infringe privately ownedrights. Reference herein to any specific commercialproduct, process, or service by trade name, trademark,manufacturer, or otherwise does not necessarily constituteor imply its endorsement, recommendation, or favoring bythe United States Government or any agency thereof. Theviews and opinions of authors expressed herein do notnecessarily state or reflect those of the United StatesGovernment or any agency thereof.
DISCLAIMER
Po~’ons of this document may be illegiblein e~ectronic image products. Images areproduced from thedocument.
best available original
this way the critical speed of rotation will be much higher avoiding a possibility ofthe rotor vibrations.
Hot high-pressure water will be introduced in to the impeller through a hollowshaft. Two soft brass labyrinth seals inserts will be placed at two ends of theshaft. At the lower side, the differential pressure across the labyrinth seal is muchhigher. We were also concerned about leaking of some of the incoming hot waterflow through the labyrinth seal. For this reason we have designed introduction ofsmall amount of pressurized steam or air into the middle of the lower labyrinthseal. This should completely stop leaks of the main hot water supply.
The impeller itself is sandwich-like being split into two pieces horizontally throughthe middle of the curved nozzles. Curving of the reaction nozzles is calculatedusing a computer code written by us. A thin sheet of soft copper of thickness of0.004 inches will be placed between two impeller halves. The two halves of theimpeller halves will be held and be sandwiched together with about twentyrecessed alien type screws. Perfect tight alignment of the two impeller halves willbe accomplished by a push fit on the push fit on the shaft plus a push fit on oneor two dowel pins. These dowel pins will also go through the large 3.5-inchdiameter part of the shaft. In such a way torque will be completely securelytransferred from the impeller to the shaft. The maximum torque would occurwhen the shaft is jammed shut and the maximum flow is passing through thecurved nozzles. Assuming maximum momentum no separation jets dischargingthe nozzles we get the maximum torque of 36.7 Nm. Further calculations showthat two dowel pins of 1/8 inches in diameter placed at radii of 1.5 inches cancarry six times larger torque than the maximum predicted.
Calculation of stress for a flat rotating disc of uniform thickness and diameter of8.6 inches and with a hole at its centerline shows that for rotational speed of20,000 RPM the maximum stress will be 330 MPa and located at the innerradius. Based on this and various other considerations we have chosen the rotorto be made out of stainless steel 17-PH4 which has the tensile strength of 1,310MPa.
In addition to the above stress calculation, our design has further substantiallydecreased the maximum stress by more than a factor of two. This is achieved bytwo design modifications. First, the thickness of the rotor at the inner radius,where it attaches to the shaft, is about two times larger than at the outer radius.This considerable decreased the maximum stress.
Second, when there is no central hole in a rotating disc of uniform thickness therithe maximum stress is only half as high compared to the case with a hole at thedisc center? In our case for no-hole design the maximum stress would be only165 MPa. We have taken advantage of this feature by observing that the upperpart of the shaft has no hole in the center. For this reason we will machine theupper shaft from 3.5 inch diameter stock steel with an internal recess which will
Ihelp ‘hold’ the impeller (which has much larger outer diameter) as shown on theenclosed Figures. This will reduce the maximum stress in the impeller. Weexpect the actual maximum stress for the rotational speed of 20,000 RPM to beat about 160 MPa, i.e. eight times lower than the maximum strength of thechosen stainless steel.
IEarlier we intended to make rotor 16 inches in diameter so that it would have thesame diameter as the rotor of the LLL two-phase turbine. This turned our to betoo costly and too bulky to manufacture. Accordingly we have decreased therotor to eight inches. The housing has also decreased in diameter by factor ofapproximately two. The weight and the manufacturing costs are basicallyproportional to the square of the diameter. This means that we have reduced theactual manufacturing costs by factor of close to four.
One negative consequence of the two times smaller radius is two times higherrotational speed. The biggest inconvenience that this has caused was thedifficulty of finding commercially available dynamometer. However even for10,000 RPM and 30kW power the dynamometer would cost about $25,000. Wehave resolved this issue by using high-speed electtid generator with resistiveload banks as a dynamometer. In order to increase the accuracy of measuringthe power output, the stator of the electrical generator will be held by a flangetype torque cell. In such a way exiting torque of the turbine shaft will bemeasured very accurately. The RPM-s will also be measured very accurately byusing optical tachometer.
Manufacturing issues for the turbine and the whole test rig are continuously beingreexamined and solutions improved? It is very hard and overly time consumingand ineffective to in written form explain many many issues and aspects of thedesign considerations. Just for an example we were given bids for appropriatedynamometers by two well established companies in Southern California, ofabout $80,000 each. This was of course financially completely not possible withinthe project’s budget. We have done very intensive and wide consideration anddesign of alternative dynamometer. We are satisfied that we have come up withmuch more economical and effective device to measure the power output of theturbine.
We also had to choose thermodynamic and flow parameters at and for which todesign the first turbine prototype. Many important factors had to be weighted inchoosing the key parameters. One of the key ones being available funds forbuilding and testing the turbine prototype. Some of these considerations areactually covered by our next project, which are the building and the testing of theturbine prototype.
2) Develop the Enqineerinq Drawims of the Turbhe
The initial most innovative part of the design of the prototype turbine is design ofits curved 100% reaction nozzles. Based on the governing equations we havedeveloped a computer code, which calculates the curvature of the nozzles inapproximately 1500 incremental finite difference steps along the nozzles. Cross-sectional flow areas of the nozzles were calculated using the governingequations as well as thermodynamic properties of state.
Two nozzles, rather than four, were used. In this way the cross-sectional areasare twice as large than in the LLL nozzles. We believe that this will be beneficialsince the boundary layers would occupy smaller fraction of the total cross-sectional areas.
The assembly drawing explains the most about the design of this turbine. Itwould be way too extensive to start to elaborate on details of design of theturbine. Drawings of various parts are enclosed.
3) Desire Test Facility
We have undertaken, within a modest budget, to design and (subsequently) builda test rig needed to verify the performance from our turbine. Instead of acontinuously running facility we have chosen a blow down test rig, which isshown on an enclosed figure. This facility will have 200 GL high temperature(400F) and pressure (250 PSIA) hot water tank connected to appropriated gasburning heating coils (tubes) of heating capacity of about 300,000 BTU/hr. Thetank and the heating coils replace usual much more expensive high temperateand pressure boiler. Using this system we will first have to heat the water forabout 5 hours to 400F, then we should be able to achieve high flow steady stateoperation of our turbine for at least 10 minutes. During the steady state operationtime we will take all needed data to calculate the performance of the turbine.
The other large saving in the cost of the facility we are achieving by having anatmospheric separation tank downstream of the two-phase turbine instead oflow-pressure condenser. About 85%, by mass, of the turbine discharge flow, iswater. it will be contained into 300 GL separator tank. The steam is 15!40of thedischarge flow. The steam cannot be saved but it will be continuously dischargedfor the separator tank via one-foot diameter duct, which will exit through the roofof the building.
Drawings of the high temperature, and of the separator, tanks are enclosed.
Third very large savings will be accomplished in terms of equipment to measurethe power output of the turbine. We have received two bids from establishedSouthern California companies to such supply such equipment. Each of thesetwo bids is for about $80,000 just to measure the power output of the turbine.Subsequently we have made our own design of the assembly of equipment
,.,.
needed to measure the power output of the turbine.
The main part of the dynamometer will be electrical generator. We have alreadypurchased an electric generator capable of delivering 30kW or more. It is asurplus generator of an aircraft bomber. It is designed to operate at 6,000 RPMbut also it can run at 9,000 RPM. We expect that the turbine impeller will rotate atup to 20,000RPM. Accordingly it is necessary to have a transmission RPMreduction system from the turbine shaft to the generator shaft. We have doneextensive considerations of transmission systems and have selected sprocketand chain system as the most appropriate. We have already purchased a chainand two sprockets. Drawing showing the turbine assembly, the electricalgenerator and the transmission system. Please note that the turbine andgenerator shafts and the transmission are completely enclosed by thick steeishrouds. This is done in order to achieve high degree of safety.
The output of the electric generator will be taken to and electrical load bank. Theload bank has various resistors so the loading in the generator, i.e.simultaneously on the turbine, can be changed at any particular constant RPM.
4] Analyze Potential Amlications of the FAS Two-Phase Reaction Turbine
We were asked to compare performance of geothermal power plants that do notor do employ our turbine in various thermal cycles possible. There are manymany considerations that need to be taken in account. The main considerationsand comparisons of improvements in performance have been given in our earlierproposais and answers to questions submitted to the DOE.
in order to be able to more directly compare the thermodynamic and poweroutput performance we have assumed the same state parameters of the brineentering the assumed piant and the same condensation temperature of theworking fluid. If geothermal fluid now entering the plant is 90% in iiquid and 10%in steam state, this that there is flashing of the iiquid oniy brine within iast topparts of the upcoming well in the ground. This can be rectified and appreciablebenefit gained by using larger diameter hole for the upcoming flow, or by using adown-hoie pump, which, in this case, wouid require a relatively small powerinput.
his known that the throttling is constant enthaipy process in which the avaiiablemechanical energy is wasted. Based on the parameters given to us (335F, 10!kOsteam quaiity) we have calculated the more appropriate input (the sameenthalpy, and 0!!40quaiity) to be saturated brine at temperature of214C. Thecondensation temperature we have taken to be the same in ail cases, at 25C.Based on these basic assumptions, and a brine flow rate of 100 kg/s, we havecalculated the foiiowing resuits:
‘<I “1-u
a)
b)
c)
d)
e)
f)
9)
.-
Single Flash Conventional Plant
Assuming the efficiency of the steam turbine is 0.85 the plant power output is7,733WV.
Single Flash Plant Retrofitted with Two Two-Phase Flow Turbines.
Assuming the efficiency of the two-phase flow turbines is 0.75 the plant poweroutput is 12,727kW.
Dual Flash Conventional Plant
Assuming the efficiency of steam turbine to be 0.85 the plant power output is9,775kw.
Dual Flash Plant Retrofitted with Three Two-Phase Fiow Turbines.
Assuming the efficiency of the two-phase flow turbines is 0.75 the plant poweroutput is 13,009kW.
Open Brine Trilateral Cycle
Assuming the condensation temperature at 40C and the efficiency of the two-phase flow turbine of 0.75, the plant power output is 11 ,782kW.
Open Brine Trilateral Cycle
Assuming the condensation temperature at 26.67C and the efficiency of thetwo-phase flow turbine of 0.75, the plant power output is 13,770kW.
Trilateral Cycle with Binary Fluid
Assuming the temperature difference in the receiving heat exchanger of 5C,the condensation temperature of 40C, efficiency of the two-phase flow turbineof 0.75, the plant power output is 12,053kW.
*
TEST RIG SET UP
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232.319 4.114
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0.290 0,725
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. . NAVAIR 0~-5AS-5
Technical Manual
Overhaul Instructions
PLCGENERATOR
(IlcIILli:i)
.“,..
THIS PU’il!_!CATION SUPERSEDES NAV’:i’E?S G3-5AS-5
DATEZI 15 NO VE;,f BER 1S64
PUBlkHED BY THE DIRECTION OF THE “COhl MANDER. NAVAL AIR SYSTEF4S COMMAND
i.. .~~~’”=s
“.L--’ J Sq)Im’ks 1967.. ,. .-,,. .
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xtlv~un 03-5:\s-5 Section 1paragraphs 1-] to 1-7
. -~,
SECTIOX I
INTRODUCTION
1-1. G~NER:\L.
1-2. This manual contains ovcrhwl instructions ant!* test procedure for type 28 B54- 1-A, Alternating Cur-
rent Gencr3tor, manufactured by The Bendix Corpo -ration, Electric Power Division, Eatontown, hkwJersey, and is prepared unc!er contract NO0383-67-C-2571.
1-3. PURPOSE OF EQUIPhiENT. The ~C generator(figure l-l) is used to provide an output voltage forthe alternating current, aircraft ekctric systcm.
.,.* -’””
1-4. LEADfSG PARTICULARS. The leading pzrticu -ktrs of the alterni~tin: current generator are listedin tab!c L
1-5.
1-6.lmui
1-A AC Ger.c Yztor. Ovcrku! ir.str~ctions ~nci testprocedure for xlciition~l t}Tes are provided in SectionIV by the usc of Difference Datz Sheets. The adc!i-tionzI types covered in Section IV are listed in Sec-tion IV.
1-7. Overhaul instructions and test procedure for thetypes covered in Section IV are the szme as thosegiven in Sections II and III, except for the specificc!iffc rences noted by the appliczblc Difference D-tzSheet.
Note
“Llany pints for equi!m:cnt ccwercd in this pJb-Iication are Drovided in the form of kits. (Seeapp[icablc IIlustrztcd Parts BrcAdowr. for
DfT’FIZi&NCE DATA SHEETS. dctziis. ) Iiov;cvcr, c!canin:, ixpcction, test-ing and repair inform~tion is inc!uc?cd for a!i
Stctions U and If I of this kndbook cor,:lin oi’cr - parts w!~ich cm bc rc@recf to cclvcr anyinst~~ctions ant! test procedure for type 2SD5+- emcrgencies czusccf by skarwgcs in supply. ‘*
R~tcd ~O]h.:C (Li!!c to mw:n!) . . . . . . . . . . . . . . . . . 1~~ ‘.’.
Ratcc! Vol:c.:e (iine to line}. . . . . . . . . . . . . . . . . . . . . 203 \-
Rmec{Loac! . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . ..30k.3
Power F~ctor . . . . . . . . . . . . . . . . . . . . . . . . . . . . . ...0.75
Frequency . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . ..400 c.1s
Phase . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . ...3
Rated SIwcd . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . ..57001YNz1
hkxin?um Speed for Regulation. . . . . . . . . . . . . . ...7000 rprn
Rotation (lricwing drive end) . . . . . . . . . . . . . . . . . . . Counterclocl-w’ise
We i:ht (Mxis) . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 70 lb
Bolt Circlc Diameter. . . . . . . . . . . . . . . . . . . . . ...10.000 in.
Drive Si>line . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . ..l~-tooth
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‘.- NAVAIR03-5AS-6.... .,‘T\
Technical Manual
Illustrated Parts Breakdown
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AC GENERATOR
TYPE NO.~gB54.~.A 28 B54-$)-A28 B54-1-B 2SBjfL~-~
(Benciix)
TH{S PUBLICATION SUPERSEDES NAVWEPS 03-5AS-6DATED 1 AUGUST 1964
PUBLISHEDBY THE DIRECTIONOF THECOMMANDER. NAVAL AIR SYSTEMS COMMAND
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NAVAli: 03-5.G-j“.
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Figure 4-4. AC Gencz-alor Type 28 B54-9-B
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1. Generator to airduct adapter
2. (3. :4. 15. 1
6. ‘7. !8. ‘9.
10.11.12.13.1’4.
15.16.17.18.19.20.21.22.23.24.25.26.~~ .
28.29.30.31.32.33.34.35.36.37.38.39.40.41.
:aplugScrewLi3ckwasherVasherTermimd block coverScrewWasherSelf -locking nutWasherRound nutWasherBeveled retaining ringPermanent magnetrotor coreI%Xor shaftWmxkuff keyDrive shait assemblyS&f-locking nutWasherSpringFront plateLack ringFan assemblyWmxiruff keyStator and panei assemblySc Z?’.VLackwzsherWa~he rScrewLoclcwasherWasherService linerScrewEnd bellDirt slingerBail bearingBearing retainerCuter bearing retainerScrewBushingBearing spacer
42.43.44.45.46.47.48.49.50.51.52.53.54.55.56.57.58.59.
60.61.62.63.64.
65.66.67.sa.69.70.‘il.72.73.74.75.76.77.78.79.80.al.82.
)irt slingerMl bearinglelf-locking nut.ockwasherVasher;crewZlectricd leadtlastic stop nutRectifierShimVasherNutInsulating washerResistorRotor assemblyInner bearing retainerDust capElectrical receptacleconnector assembiyScrewLockwasherWasherConnector adapterMotor generatorexciter statorsc~~w
Square washerTerminal blockSC~~w
LockvmherWasherJumper strapJumper strapAC stator assemblyScrewIdentification plateScrewService linerScrewScreenScrewSpacerHousing
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80-?01
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Figure 2-1. Type 28B54- l-~ AC Generator, Main Assembly
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