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Layout of spillway aerator air vents and its effect on air supply PDF

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DEGREE PROJECT IN VEHICLE ENGINEERING, SECOND CYCLE, 30 CREDITS STOCKHOLM, SWEDEN 2017 Layout of spillway aerator air vents and its effect on air supply GUSTAV DAGGENFELT KTH ROYAL INSTITUTE OF TECHNOLOGY SCHOOL OF ENGINEERING SCIENCES Layout of spillway aerator air vents and its effect on air supply Gustav Daggenfelt June 12, 2017 Abstract Chute aerators are constructed to protect spillways from cavitation dam- age. They function by launching the water flow as a jet and supplying air underneath since having air entrained into the water is an effective way to mitigate cavitation. This report looks at Bergeforsen, a dam in northern Sweden, and its spillway as a basis for investigating how altering the aer- ator’s outlet alters its performance. Five different designs are tested using CFDwithANSYSFluent17. Thedesignsareevaluatedwithregardtototal air flow, air flow distribution, duct pressure distribution, cavity length, and air concentration in water jet. Itwasfoundthatdesignswithmoreevenductpressuredistribution,that transported air further toward the spillway center, had somewhat reduced total air supply compared to designs that released more of its air in the early part of the duct. Consequently there appear to be a trade off between effectively distributing the air and providing more air flow. The current design used by Bergeforsen strikes this balance quite well, better than the other tested designs. Luftinblandare byggs f¨or att skydda utskov fr˚an kavitationsskador. De fungerar genom att l˚ata vattenstr¨ommen bli en str˚ale under vilken luft tills¨attseftersomattblandainluftivattenstr¨ommen¨aretteffektivts¨attatt motverkakavitation. Denh¨arrapportenunders¨okerBergeforsen, endammi norraSverige,ochdessutskovf¨orattunders¨okahurluftinblandarensutsl¨app p˚averkar dess prestanda. Fem olika designer testas med hj¨alp av CFD i ANSYS Fluent 17. Designerna utv¨arderas med avsikt p˚atotalt luftfl¨ode, f¨ordelning av luftfl¨ode, tryckf¨ordelning i luftg˚angen, l¨angd p˚alufth˚alrum, samt luftkoncentration i vattenstr˚alen. Det uppt¨acktes att designer med mer j¨amn tryckf¨ordelning i luftg˚angen, som transporterade mer luft till utskovets mitt, hade n˚agot mindre total lufttillf¨orsel j¨amf¨ort med designer som sl¨appte ut mer av luften tidigare ur luftg˚angen. Det ser d¨arf¨or ut att kr¨avas en kompromiss mellan effektiv f¨ordelning och totalt luft fl¨ode. Den design som anv¨ands i Bergeforsen idag uppfyller den kompromissen ganska v¨al, b¨attre ¨an de andra som testades. Acknowledgements This work was done at the department for Hydraulic Engineering at Kung- ligaTekniskaH¨ogskolanonbehalfofVattenfallABandsupervisedbyJames Yang. Particular thanks to Penghua Teng for providing grids for CFD and for plenty of help and advice along the way. 1 Contents 1 Background 3 2 Theory 5 2.1 Spillway . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 5 2.2 Cavitation . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 5 2.3 Aeration . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 6 2.4 Bergeforsen . . . . . . . . . . . . . . . . . . . . . . . . . . . . 7 3 Method 9 3.1 Numerical model . . . . . . . . . . . . . . . . . . . . . . . . . 9 3.2 Air vent designs. . . . . . . . . . . . . . . . . . . . . . . . . . 10 4 Results 12 4.1 Duct pressure . . . . . . . . . . . . . . . . . . . . . . . . . . . 12 4.2 Air Volume Flow . . . . . . . . . . . . . . . . . . . . . . . . . 13 4.3 Air Cavity . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 14 5 Conclusion & Discussion 17 6 Appendix 18 6.1 Graphics . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 18 2 Chapter 1 Background Spillwaysareimportantstructures partsoftheflowadjacenttothewalls servingasoutletsforexcesswaterfrom or bottom. A chute aerator is a de- hydroelectric dams. In steeper and signthatusearampdeflectortolaunch longer spillways, so more commonly thewaterintoajetunderneathwhich in large dams, the streaming water there is an air duct outlet. The free can reach high velocities that cause surface of the jet then has air en- cavitation damage which erode the trained into it [2]. concrete along the spillway floor and Bergeforsen power station is lo- walls. cated on Indals¨alven outside Timr˚a. Cavitation damage has been ob- The dam began its service in 1955 servedinspillwaysworldwidethrough-andiscurrentlyunderongoingmain- out the 20th century. A dam fail- tenanceandmodernizationforfuture ure at the Madden Dam in Panama use. Primarily a new spillway was 1935 first prompted research into the constructedin2014[8]. Thenewspill- phenomenon [2]. Some of the most way has an aerator to reduce erosion standoutcaseshavebeeninpipespill- caused by cavitation. The aerator wayssuchasGlenCanyonDam1983 has 13 square outlets along a ramp [1]whereinitialcavitiationdamageis spanning the width of the spillway. lesslikelytobespottedearly. Inthat Potentially the aerator could be im- case the erosion eventually led to vi- proved by changing the design of the brations breaking apart large pieces outlet, and as a result improve the ofconcreteandpullingoutmetalbars, protection against erosion. opening up an 11 m deep hole. Due to the spillway’s unusually Cavitationinspillwayscanbemit- large width the flow characteristics igated in several ways; redesigning differ somewhat compared to other the spillway for reduced flow veloci- smaller Swedish dams. The size also ties, smoothing out the concrete sur- make experiments with small scale face and removing edges or other ir- models less reliable. Therefor CFD- regularities, andinstallinganaerator simulation will be the method used upstream of the critical region. to investigate. Aerators are devices that mix air into the water, most importantly the 3 Figure 1.1: Bergeforsen’s new spillway, air vents from the aerator can been seen along the bottom. 4 Chapter 2 Theory 2.1 Spillway process will cause small shock waves and micro jets of water that can cre- Aspillwayisanessentialpartofdam ate large pressure spikes on nearby constructionasitistheoutletforex- surfaces such as the concrete floor or cess water from the reservoir to the walls resulting in erosion and mate- river beneath. Typically it can be rial fatigue.[1, chapter 1] In hydro- separated into three sections; a gate, engineeringthisentirechainofevents achannelorchute,andanenergydis- is usually included in the term cav- sipator. Thegateregulatesthewater itation due to the temporary nature flow from the reservoir into the chute of the vapor bubbles. where it flows down into the dissipa- The collapse of a vapor bubble torwherethewaterhasitskineticen- is cyclical; the bubble is first com- ergy reduced before it’s released into pressed before it collapses into two the river. smaller bubbles and releases a wa- ter micro jet, the two then combine 2.2 Cavitation back into a single bubble and the cy- cle begins again. After each cycle Inhighvelocitywaterflowoveranir- the resulting bubble is smaller than regular or rough surface there will be it was at the start.[1, page 8-10] If pockets of flow separation resulting the collapse happens in the vicinity in low pressure areas. If these pres- of a boundary the microjet tends to sure drops are large enough the wa- be directed towards it, as shown in terwillstarttotransitionintovapor, figure 2.1. essentiallyaboilingphenomenondue When the two bubbles recombine to decreased pressure rather than in- they generate shock waves and it is creased temperature. The formation these and the micro jets that cause of these vapor bubbles in the water cavitation damage. Which factor is is called cavitation. moreimportantishardtodetermine, Asthevaporreturnstothehigher partiallybecausetheshockwavesfrom pressurelevelsofthesurroundingflow onebubblecollapsecantriggerachain the bubbles will collapse back into reactioninothernearbybubbles. Such water. As they do so the collapsing achainreactioncanresultinanultra 5 shock waves and the jets during bub- ble collapse.[1, pages 11-12 & 34] 2.3 Aeration Figure 2.1: Bubble collapse and re- As early as 1953 it was found that bound cycle close to a boundary. [1, cavitation damage can be effectively page 9] mitigated if there is between 6-8% air entrainment in the water[5]. In truth the air concentration required jet whenmultiplemicrojetsfromdif- is poorly understood as it is difficult ferent bubbles combine into a larger to measure air concentration at the single jet with velocity in the order area where damage occurs. It also ofabouthalfthesonicvelocityofthe depends on surface roughness, flow liquid.[1, page 9-10] velocity, depth and other unknown Cavitationdamageisprogressive, factors. The findings from several which means that erosion of a sur- studieshoweveragreethatonlysmall face is going to increase the inten- amounts of air are needed to signif- sityofcavitationonthatsurface,and icantly reduce cavitation damage[2]. it’s therefore important to use pre- In order to increase the air entrain- ventive measures as damage can go ment,particularlyinthecrucialparts from being unnoticed to being dan- of the flow close to the spillway floor, gerous quickly.[3, page 95] aeratorsarecommonlyinstalled. Aer- Theriskofcavitationcanbeesti- ators are airducts that suck in out- mated using the cavitation index K side air and distribute it from under- h +h −h neath the water flow. p a v K = (2.1) V2/2g whereh isthebottompressurehead, p h is the atmospheric pressure head, a h is the vapor pressure head, V is v the water flow velocity and g is grav- itational acceleration. A K-value at 0.2 or less indicates critical risk of cavitation requiring aeration.[7] Aerationreducescavitionbyhav- ing air entrained in the flow. The Figure2.2: Exampleofageneralaer- main reason for this appears to be ator design. Sideview crossection. thefactthatanair-watermixturewith more than 1% undissolved air, some- Aerators typically use an offset what counter-intuitively, can have a andadeflectororrampinorderachieve muchlowersonicvelocitythaneither a water jet with an air cavity under- fluidhasonitsown. Thisreducesthe neath in which air can be supplied, pressurespikesgeneratedbyboththe 6 air entrainment coefficient: Q A β = (2.2) Q W where Q and Q are the respective A W volume flows of air and water at the aerator. Another similar parameter is the localaverageairconcentrationatthe Figure 2.3: Water flow over an aera- aerator defined as tor with P and L defined. C = Q /(Q +Q ) (2.3) a A A W howeverbothoftheseparametershave as shown in figure 2.2. The flow can the weakness of not considering the thereforbesaidtohavethreegeneral bottomairconcentrationinthedown- flowzones; thejetzone,thereattach- stream region.[7] ment and spray zone, and the far- Whendoinginitialdesignofavent fieldzone.[6]Thejetreattachmentpoint aerator there are several important is denoted P and its distance from steps to take, the dimensions of the the deflector and/or offset is the jet ramp and offset are of primary im- length L. The flow zones can then portance but those will not be cov- be defined as jet zone at 0 < x/L < ered in this report. Instead focus is 1, reattachment and spray zone at on the vent and duct design. 1 < x/L < 3, and far-field zone at The air duct should be designed x/L > 3. The reattachment point P to avoid so called choked flow which can be defined in various ways but iswhereasonicflowregimeisreached. in this report is defined by the point A duct flow velocity limited to under of peak pressure on the spillway bot- 100 m/s is therefor recommended as tom. Figure 2.3 shows a possible ex- well as a maximum pressure drop in ample based on one of the CFD sim- the duct of roughly 2-6% depending ulations. ontheamountoffrictionlossesinthe Very little of the air entrained in duct. The vent outlet area is recom- thejetzoneremaininthelowerparts mended to be less than the area of of the flow after reattachment point the duct intake.[1, page 70] P,insteadmostoftheairisdetrained bybeingtransportedupandreleased fromthewatersurface. Aeratorscon- 2.4 Bergeforsen sequently have only a small effect on the bottom air concentration in the ThespillwayatBergeforsendam,shown far-field zone [6]. Luckily not much infigure1.1, hasanopeningwidthof air is required. 25mwhichmakesitthelargestspill- A common ratio used to evaluate way in Sweden. It’s crest is at an el- the effectiveness of an aerator is the evation 112.75 m and the aerator is located 24.72 m downstream, more measurements are given in table 2.1. 7

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They function by launching the water flow as a jet and supplying air underneath Det ser därför ut att krävas en kompromiss mellan effektiv fördelning
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