Optimal Design of Transonic Fan Blade Leading Edge Shape Using CFD and Simultaneous Perturbation Stochastic Approximation Method

Size: px
Start display at page:

Download "Optimal Design of Transonic Fan Blade Leading Edge Shape Using CFD and Simultaneous Perturbation Stochastic Approximation Method"

Transcription

1 1 Optimal Design f Tansnic Fan Blade Leading Edge Shape Using CFD and Simultaneus Petubatin Stchastic Appximatin Methd X.Q.Xing and M.Damdaan Abstact Simultaneus Petubatin Stchastic Appximatin methd has attacted cnsideable applicatin in many diffeent aeas such as statistical paamete estimatin, feedbac cntl, simulatin-based ptimizatin, signal & image pcessing, and expeimental design. In this pape, its pefmance as a viable ptimizatin tl is demnstated by applying it fist t a simple wing gemety design pblem f which the bjective functin is descibed by an empiical fmula fm aicaft design pactice and then it is used in a tansnic fan blade design pblem in which the bjective functin is nt epesented by any explicit functin but is estimated at each design iteatin by a cmputatinal fluid dynamics algithm f slving the Navie-Stes equatins Keywds glbal ptimizatin; simultaneus petubatin stchastic appximatin methd, simulated annealing, tansnic fan design I. INTRODUCTION he need f slving multivaiate ptimizatin pblems is T pevasive in engineeing, the physical and scial sciences. The chaacteistic featues f such pblems ae the pesence f a lage numbe f design vaiables, cmplex cnstaints, and even discete design paamete values. A numbe f ptimizatin algithms, bth lcal and glbal ptimizatin algithms have been develped f ptimizing such pblems. Besides deteministic methds, stchastic methds such as genetic algithm (GA) and simulated annealing (SA) algithm etc have ecently fund applicatins in pactical engineeing design ptimizatin pblems. These algithms ae all stchastic in natue and easily implemented in bust cmpute cdes as cmpaed with deteministic methds. Hweve, SA and GA methds equie lage numbe f functin evaluatins and elative lng cmputatin time especially in the case f cmplex design pblems. One X.Q. Xing, SMA Reseach Fellw, Cente f Advanced Numeical Engineeing Simulatins, Nanyang Technlgical Univesity, Nanyang Avenue, Singape, (telephne: , xqxing@ ntu.edu.sg). M.Damdaan, Assciate Pfess f Nanyang Technlgical Univesity and SMA Faculty Fellw, Schl f Mechanical and Pductin Engineeing Simulatins, Nanyang Technlgical Univesity, Nanyang Avenue, Singape, (telephne: , mdamdaan@ ntu.edu.sg). appach t educe cmputatinal time wuld be t use paallel GA and paallel SA as utlined in Wang and Damdaan 1. An attactive altenative t SA and GA culd be the Simultaneus Petubatin Stchastic Appximatin (SPSA) methd descibed by Spall 2-4 and which has been applied t difficult multivaiate ptimizatin pblems. The SPSA methd has attacted cnsideable applicatin in many diffeent aeas such as statistical paamete estimatin, feedbac cntl, simulatin-based ptimizatin, signal & image pcessing, and expeimental design. The essential featue f SPSA, which accunts f its pwe and elative ease f implementatin, is the undelying gadient appximatin which equies nly tw measuements f the bjective functin egadless f the dimensin f the ptimizatin pblem. This featue allws f a significant decease in the cst f ptimizatin, especially in pblems with a lage numbe f vaiables t be ptimized. SPSA methds ae biefly utlined and its pefmance as a viable ptimizatin tl is demnstated by applying it fist t a simple wing gemety design pblem f which the bjective functin is descibed by an empiical fmula fm aicaft design pactice and then it is used in a tansnic fan blade design pblem in which the bjective functin is nt epesented by any explicit functin but is estimated at each design iteatin by a cmputatinal fluid dynamics algithm f slving the Navie-Stes equatins. II. SPSA METHOD SPSA is elatively easy t implement and des nt equie gadient infmatin. It is a faily bust methd and has the ability t find a glbal minimum in the pesence f multiple minima. SPSA is an algithm that is based n a simultaneus petubatin gadient appximatin. The simultaneus petubatin appximatin uses nly tw functin measuements independent f the numbe f paametes (say, p) being ptimized. The SPSA algithm ws by iteating fm an initial guess f the ptimal vect X 0. Fist, the cunte index is initialized t a value f 0, an initial guess f the design vaiable vect X and nn-negative empiical cefficients ae set. Next a p-dimensinal andm

2 2 simultaneus petubatin vect is cnstucted and tw measuements f the bjective functin, namely y( X + c ) and y( X c ) ae btained based n the simultaneus petubatin aund the given vect X. Then geneate the simultaneus petubatin appximatin t m the gadient g ( X ). The paamete c = c0 /( ) whee c 0 is a small psitive numbe taen as 0.01 in this study, is the lp index and m is a cefficient taen as 1/6 in this study. The tem epesents the andm petubatin vect geneated by Mnte-Cal appaches and the cmpnents f this petubatin ae independently geneated fm a zemean pbability distibutin and a simple distibutin that has been used in this study is the Benulli ± 1 distibutin with pbability f ½ f each ± 1 utcme. This is fllwed immediately by the calculatin f the gadient appximatin based n tw measuements f the functin based n the simultaneus petubatin aund the cuent value f the design vaiable vect and the updating f the design vect X t a new value X + 1 using standad SA fm, i.e. X + 1 = X a g( X ). The value f a can be chsen t ensue effective pactical pefmance f the algithm. Finally the algithm is teminated if thee ae insignificant changes in seveal successive iteatins if the maximum allwable numbe f iteatins has been eached. The details f the step-by-step implementatin f the SPSA algithm ae utlined in Spall 2,4. III. WING DESIGN OPTIMIZATION A. Wing Design Pblem The design pblem cncens the design f wing shape such that the aedynamic efficiency f the wing eaches a maximum value duing cuise with the wing weight acting as a cnstaint, i.e. the gal is t detemine the shape f the wing f minimizing D/L (dag-t-lift) maximizing L/D with the wing weight as a cnstaint. Explicit empiical functin f D/L which fm the bjective functin f the ptimizatin pblem and empiical expessins used hee ae defined in Rayme 6. The bjective functin t be ptimized is defined as fllws: Minimize F( x) = D / L (1) Subject t six cnstaints n the design vaiables defined as fllw: 1.0 α 10.0, 10.0 b 50. 0, 3.5 c 10.0, 0.0 λ 35.0, 0.5 A R 15.0, W wing 2473( lb) Whee.0 15 λis the angle f attac, b is the wing span, c is the mean aedynamic chd, λ is the wing sweep, AR is the wing aspect ati and W wing is the wing weight. The cnstaints ae incpated in int a cmpsite bjective functin by way f penalty functins. B. Optimizatin Results and Cmpaisn Table 1 shws the ptimum values f the bjective functin and design vaiables eached by diffeent ptimizatin algithms. It can be seen that the esults f bjective functin and vaiables fm SPSA ae vey simila t thse f Simulated Annealing (SA). Fig. 1 cmpaes the evaluatins f functin t each the ptimal values based n the specified cnvegence citein using SPSA with thse attained by SA methd. It can be seen that SPSA eaches ptimal values abut 9 times faste than SA theeby suggesting that SPSA is a viable and a me efficient stchastic design methd. TABLE I COMPARING OPTIMAL DESIGN RESULTS USING SPSA AND SA OPTIMIZATION METHODS Algithm α ( ) b ( ft ) c ( ft ) λ ( ) Wing Weight ( lb ) bjective Functin D/L SPSA SA SA SPSA Evaluatins f Objective Functin Fig. 1. Evaluatins f Objective Functins IV. TRANSONIC FAN BLADE LEADING EDGE DESIGN PROBLEM Tansnic fan blade design pblems include the design f the blade aifil sectins at diffeent adial psitins and the stacing f these aifils t fm a thee dimensinal blade. Many studies have fcused n the aifil ptimizatin using the Navie-Stes and adjint equatins as in ptimized design f shc-fee aifils and wings epted in Sung and Kwn 8. Catalan 9 pesented an invese design f a thee-dimensinal tub-machiney blade in which bjective functins wee based n inviscid tansnic flw mdel and Tng 10 ppsed a multi-bjective simulated annealing algithm t impve the initial design f tubine blade. Studies f swept ts ae mtivated by the fact that swept wings educed shc wave stength, and the shape f the

3 3 leading edge f a swept blade can be alteed t cntl the shc stuctue and the migatin f the lw-mmentum flw fluid, which cnsequently decease the lsses induced by the inteactin between shc and bunday laye as well as the inteactin between shc and secnday flw. This mtivates the cuent applicatin pblem dealing with the design f the leading edge cuve t meet design bjectives. The flw fields aund swept wings can be assumed as twdimensinal in which case it is sufficient t descibe the wing leading edge using a sweep angle α s as shwn in Fig. 2(a). Hweve, the leading edges f tansnic fan blades ae theedimensinal as shwn in Fig. 2(b). Ás (a) (b) Fig.2. Diffeence between (a) wing and (b)blade leading edge The design pblem cncens the design f the leading edge cuve such that the adiabatic efficiency f a tansnic fan s t eaches a maximum value duing 100% f the design speed, with the t s stall magin acting as a cnstaint. At the same time, the pessue ati must satisfy a given value. As the stall magin and the pessue ati cannt be expessed by the design vaiables, these wee nt integated int the design pblem as cnstaints but wee nly checed thugh numeical simulatin f the pesent study. A. Blade design pblem The t s leading edge cuve defined hee is same t that f efeence 11 by a cubic thee-dimensinal cuve as fllws: 2 3 R ( t) = a + bt + ct + dt (2) Whee, a = a, a, ], b = b, b, ], a3 b3 c = c, c, ], d = d, d, ] (3) c3 d 3 If the stating pint vect R (0), the cespnding tangent ' vect R (0), the end pint vect R(1) and the cespnding ' tangent vect R (1) ae given, the cuve can be detemined. The equatin f the cubic cuve defined in catesian cdinates is as fllws: x(0) y(0) z(0) 2 3 = x(1) y(1) z(1) x( t), y( t), z( t)] 1, t, t, t ] M x '(0) y '(0) z '(0) x' (1) y' (1) z '(1) (4) Whee, M = (5) In de t educe design vaiables and t cntl the evlving shape, the ends f the leading edge i.e. x(0), y (0), z(0), x(1), y(1), z(1) ae fixed accding t a baseline design cnfiguatin which is chsen t stat this design ptimizatin study. The gadients at the ends f the leading edge cuve, i.e.. x ' (0), y ' (0), z ' (0), x ' (1), y ' (1), z ' (1) ae alteed duing design iteatin t fm new leading edge cuves s that thee ae the six ptimizatin vaiables. The bjective functin t be maximized is defined as: F = Max ( η ) (6) O the pblem can be cast as a minimizatin pblem as fllws: F = Min( 1./ η ) (7) Whee η is the t's adiabatic efficiency which is estimated using a cmpessible cmputatinal fluid dynamics slve slving the Navie-Stes equatins and this is biefly utlined in the next sectin. B. Numeical Simulatin and Optimizatin The numeical simulatin cde that was used t test the adiabatic efficiency f the t, pessue ati and stall magin is utlined in Wang and Zha 12. F the cuent study, the Navie-Stes equatins ae slved with a finite-vlume, fustep Runge-Kutta, time maching methd, withut cnsideing tip-cleaance effects. The tubulence mdel used hee is a simple algebaic mdel and the gid cnsists f 62 ndes in axial diectin, 25 ndes in the adial diectin and 25 ndes in the blade-t-blade diectin. The whle design pcess is shwn in Fig. 3.

4 4 Thugh-flw cmputatin Set a baseline leading edge cuve 3D CFD Simulatin Abitay blading Max( η ) NO O satisfied the design demand? YES end Fig. 3. Design Pcess Flw Chat Optimizing the leading edge cuve Based n an initial guess f a cuve defining the shape f the leading edge, it is pssible t design a thee-dimensinal blade pfile using the semi-empiical thugh-flw analysis methd f Wennestm and Putehaugh 13 and the abitay blading methd t detemine the lcal blade cambe in the spanwise diectin and t distibute the thicness aund the cambe. The lcal thicness distibutin at the spanwise statins f the blade is assumed t emain fixed f the cuent study. Afte btaining the appximate blade gemety with lcal spanwise cambe and thicness the flw field f the t can be estimated using CFD. Based n the estimated values f ttal tempeatue and ttal pessue fm CFD analysis, the efficiency η f the t defined as whee in γ 1 γ ut Pin Tut Tin ( P / ) 1 η = / 1 P and P ae the ttal pessues and T and ut in (8) T ut ae the ttal tempeatues at the inflw and utflw bundaies f the t flw field cmputatinal dmain and γ is the ati specific heat f the gas, can be cmputed. This is fllwed by the ptimizatin steps t find a new blade leading edge cuve using the ptimizatin methd and the pcess is cntinued till desied cnvegence is achieved. design iteatins, is fist cnsideed. Figues 4(a)-(c) shws the cnvegence f the design iteatins cespnding t values f the paamete a set t 30, 50 and 100 espectively. The esults shw that the ate f cnvegence is the mst fastest when a =30. When the value f a is inceased, the ate f cnvegence is educed, while if the value f a is deceased t less than 30, thee is a pssibility that the design iteatins may divege duing the initial stages f the ptimizatin. F the case when a=30 the ptimal value is eached in abut 60 iteatins which equies abut 180 functin evaluatins. F the case when a=100 ptimal esult is eached in abut 200 iteatins equiing abut 600 functin evaluatin. The ptimal value f t s efficiency η attained can be baceted between 2 and 5 f all values f a in view f the scillaty manne in which the ptimal value is eached by the SPSA methd. Rt Efficiency (1./bjective functin) Rt's Efficiency (1./Objective Functin) SPSA methd Iteatins (a) a= N. f Iteatins (b) a=50 SPSA methd C. Results and Discussin F pupse f illustating the applicatin f SPSA methd a swept 3D blade shape with a staight wing leading edge is cnsideed as the baseline cnfiguatin t initiate the ptimizatin pcess. The effect f the paamete a appeaing in the fmulatin f the SPSA methd as discussed in Sectin II n the cnvegence f the bjective functin i.e. the cmputed/ptimized t adiabatic efficiency vs. numbe f

5 5 Rt's Efficiency (1./Objectin Functin) N. f Iteatins SPSA methd (c) a=100 Fig. 4. Effect f SPSA paamete a n cnvegence f bjective functin Fm Fig. 4, it can be seen that the adiabatic efficiency f the t des nt cnvege t a fixed value in view f the scillaty natue f the vaiatin f the bjective functin t the ptimal value. Based n the tends f the bjective functin vaiatin, it is pssible t appximately fit a mean cuve thugh the band f the scillating egin. One easn f this ind f scillaty behavi culd be the manne in which the teatment f the design paametes is dne. It is well nwn that duing the design pcess f a tub-machiney blade, distibutin f lsses and the design paametes within the famew f the empiical methd f abitay blading distibutin shuld be adjusted caefully t get a easnably gd design. In the pesent study the distibutin f the lsses and the design paametes had been limited f all blade shapes t pduce the autmatic seach pcess. The impact f this will be analyzed in a sepaate study as the fcus f this execise is t gauge the feasibility f SPSA methd in shape design. Figues 5 and 6 cmpae the blade shape and the leading edge cuve shape cespnding t baseline and ptimal shape btained by the SPSA methd. (a) (b ) (c) Fig.6. (a) Initial blade shape (b) Optimized blade shape (c) Cmpaisn between (a) and (b) A deteministic methd based n the Byden-Fletche- Gldfab-Shann vaiable metic methd and a stchastic methd based n Simulated Annealing (SA) wee als used t aive at ptimal shape designs f the blade unde the same cnditins cnsideed using the SPSA methd f pupses f cmpaing the utcmes with that f the SPSA methd. Fig. 7 shws the cnvegence f the bjective functin with design iteatins btained by using deteministic methd while Fig. 8 shws the cnvegence f the bjective functin using the simulated annealing ptimizatin methd. Objective Functin GB methd Iteatin Numbes Fig. 7. Cnvegence f Objective functin Using Deteministic Methd The teminatin citein used t stp the design ptimizatin pcess is 6 f ( x 1) f ( x ) Fig.5. Cmpaisn f the leading edge shape cespnding t baseline (staight leading edge)and ptimal design (cuved leading edge)

6 6 Rt's Efficiency (1./Objectin Functin) SA methd N. f Functin Evaluatins Fig.8. Results f SA methd Fm Fig. 7 it appeas that afte 25 design iteatins the deteministic ptimizatin methd appeas t have been tapped in a lcal minimum as thee des nt appea t be any significant vaiatins in the bjective functin. Fm Fig. 8, it can be seen that cnvegence f the bjective functin using SA methd is vey simila t that f SPSA but the SA methd equies abut 320 t 400 functin evaluatins t achieve a value f η lying between 4 and 6. It is vey clea fm this peliminay investigatin that the SPSA methd is a bust methd f btaining glbal ptimizatin. It is cetainly faste than the SA methd while the gadient-based methd GB methd seems t be tapped in a lcal ptima. REFERENCES 1] X. Wang, M.Damdaan, Cmpaisn f Deteministic and Stchastic Optimizatin Algithms f Geneic Wing Design Pblems, Junal f Aicaft, AIAA, Vl. 37, N.5, ] J. C. Spall, Multivaiate Stchastic Appximatin Using a Simultaneus Petubatin Gadient Appximatin, IEEE Tansactin n Autmatic Cntl, Vl.37, N. 3, ] J. C. Spall, An Oveview f the Simultaneus Petubatin Methd f Efficient Optimizatin, Jhns Hpins APL Technical Digest, Vl.19, N.4, ] J. C. Spall, Implementatin f the Simultaneus Petubatin Algithm f Stchastic Optimizatin, IEEE Tansactins n Aespace and Electnic Systems, Vl. 34, N.3, July ] K. Deb, Optimizatin f Engineeing Design, Algithms and Examples, Pentice-Hall f India pivate Limited, New Delhi, ] D. P. Rayme, Aicaft Design: A Cnceptual Appach, AIAA Educatin Seies, Seies Edit-in-chief: J.S. Pzemienieci, Published by AIAA, Inc, 370 L Enfant Pmenade, S.W., Washingtn, D.C., 20024, ] D. E.Gldbeg, Genetic Algithms in Seach, Optimizatin and Machine Leaning, Addisn Wesley, ] C. Sung, J.H. Kwn, Aedynamic Design Optimizatin Using the Navie-Stes and Adjint Equatins, AIAA Pape , ] L.A. Catalan, A. Dadne, Pgessive Optimizatin f the Efficient Design f 3D Cascades, AIAA Pape , ] T. Tng, Z. P. Feng, Multi-bjective Optimizatin Design f Tansnic Tubine Cascades Using Simulated Annealing Algithm, Submitted t Junal f Xi an Jiatng Univesity. 11] X.Q. Xing, Pbing Int the Cnntatin f Sweep Aedynamics f Tansnic Fans and Cmpesss, ASME Pape 2001-GT-352, ] W. Wang and X.L. Zha, Unsteady Numeical Simulatin f the Inteactin between Wae and Dwnsteam Blade Rw, Junal f Engineeing Themphysics, Chinese Academy f Sciences, Vl.17, N. 2, ] Wennestm, A. J. and Putehaugh, S. L., A Thee-Dimensinal Mdel f the Pedictin f Shc Lsses in Cmpess Blade Rws, Tans. ASME J. Eng f Gas Tubines and Pwe Vl 106 (1984), pp V. CONCLUSIONS Fm this study fcusing n the design ptimizatin f the blade leading edge cuve, it can be seen that it quite difficult t attain glbal ptimum using deteministic methd. Bth SA and SPSA methd ae able t each ptimal values and that SPSA has the ptential f achieving ptimal esults in much less cmputatinal efft than SA methd. It can be cncluded that SPSA methd is a suitable feasible ptimizatin methd which can be used t handle cmplex design pblems such as the fan blade shape designs. It is als elatively easy t implement. SPSA equies nly tw measuements f the bjective functin egadless f the dimensins f the design space cespnding t the ptimizatin pblem and the cst f ptimizatin deceases. The pesent investigatin fms the basis f futhe study t l at vaius aspects such as eplacing the abitay blading step with a me sphisticated suface gemety epesentatin incpating blade twist, sweep etc theeby inceasing the numbe f design vaiables using paameteic epesentatin f blade suface patches, the impact f the vaius pssible altenative methds f geneating the andm petubatin vect in the SPSA methd and the impact f that n the design f cmplex 3D shape designs.

OBJECTIVE To investigate the parallel connection of R, L, and C. 1 Electricity & Electronics Constructor EEC470

OBJECTIVE To investigate the parallel connection of R, L, and C. 1 Electricity & Electronics Constructor EEC470 Assignment 7 Paallel Resnance OBJECTIVE T investigate the paallel cnnectin f R,, and C. EQUIPMENT REQUIRED Qty Appaatus 1 Electicity & Electnics Cnstuct EEC470 1 Basic Electicity and Electnics Kit EEC471-1

More information

5/20/2011. HITT An electron moves from point i to point f, in the direction of a uniform electric field. During this displacement:

5/20/2011. HITT An electron moves from point i to point f, in the direction of a uniform electric field. During this displacement: 5/0/011 Chapte 5 In the last lectue: CapacitanceII we calculated the capacitance C f a system f tw islated cnducts. We als calculated the capacitance f sme simple gemeties. In this chapte we will cve the

More information

Announcements Candidates Visiting Next Monday 11 12:20 Class 4pm Research Talk Opportunity to learn a little about what physicists do

Announcements Candidates Visiting Next Monday 11 12:20 Class 4pm Research Talk Opportunity to learn a little about what physicists do Wed., /11 Thus., /1 Fi., /13 Mn., /16 Tues., /17 Wed., /18 Thus., /19 Fi., / 17.7-9 Magnetic Field F Distibutins Lab 5: Bit-Savat B fields f mving chages (n quiz) 17.1-11 Pemanent Magnets 18.1-3 Mic. View

More information

ME 3600 Control Systems Frequency Domain Analysis

ME 3600 Control Systems Frequency Domain Analysis ME 3600 Cntl Systems Fequency Dmain Analysis The fequency espnse f a system is defined as the steady-state espnse f the system t a sinusidal (hamnic) input. F linea systems, the esulting utput is itself

More information

Example

Example hapte Exaple.6-3. ---------------------------------------------------------------------------------- 5 A single hllw fibe is placed within a vey lage glass tube. he hllw fibe is 0 c in length and has a

More information

Outline. Steady Heat Transfer with Conduction and Convection. Review Steady, 1-D, Review Heat Generation. Review Heat Generation II

Outline. Steady Heat Transfer with Conduction and Convection. Review Steady, 1-D, Review Heat Generation. Review Heat Generation II Steady Heat ansfe ebuay, 7 Steady Heat ansfe wit Cnductin and Cnvectin ay Caett Mecanical Engineeing 375 Heat ansfe ebuay, 7 Outline eview last lectue Equivalent cicuit analyses eview basic cncept pplicatin

More information

Summary chapter 4. Electric field s can distort charge distributions in atoms and molecules by stretching and rotating:

Summary chapter 4. Electric field s can distort charge distributions in atoms and molecules by stretching and rotating: Summa chapte 4. In chapte 4 dielectics ae discussed. In thse mateials the electns ae nded t the atms mlecules and cannt am fee thugh the mateial: the electns in insulats ae n a tight leash and all the

More information

Example 11: The man shown in Figure (a) pulls on the cord with a force of 70

Example 11: The man shown in Figure (a) pulls on the cord with a force of 70 Chapte Tw ce System 35.4 α α 100 Rx cs 0.354 R 69.3 35.4 β β 100 Ry cs 0.354 R 111 Example 11: The man shwn in igue (a) pulls n the cd with a fce f 70 lb. Repesent this fce actin n the suppt A as Catesian

More information

CHAPTER GAUSS'S LAW

CHAPTER GAUSS'S LAW lutins--ch 14 (Gauss's Law CHAPTE 14 -- GAU' LAW 141 This pblem is ticky An electic field line that flws int, then ut f the cap (see Figue I pduces a negative flux when enteing and an equal psitive flux

More information

WYSE Academic Challenge Sectional Mathematics 2006 Solution Set

WYSE Academic Challenge Sectional Mathematics 2006 Solution Set WYSE Academic Challenge Sectinal 006 Slutin Set. Cect answe: e. mph is 76 feet pe minute, and 4 mph is 35 feet pe minute. The tip up the hill takes 600/76, 3.4 minutes, and the tip dwn takes 600/35,.70

More information

CHAPTER 24 GAUSS LAW

CHAPTER 24 GAUSS LAW CHAPTR 4 GAUSS LAW LCTRIC FLUX lectic flux is a measue f the numbe f electic filed lines penetating sme suface in a diectin pependicula t that suface. Φ = A = A csθ with θ is the angle between the and

More information

Steady State Analysis of Squirrel-Cage Induction Machine with Skin-Effect

Steady State Analysis of Squirrel-Cage Induction Machine with Skin-Effect Steady State Analysis f Squiel-Cage Inductin Machine with Skin-Effect D.-Ing. O. I. Ok Depatment f Electical Engineeing Univesity f Nigeia, Nsukka Enugu State, Nigeia. Email: gnnayak@htmail.cm ABSTACT

More information

Electric Charge. Electric charge is quantized. Electric charge is conserved

Electric Charge. Electric charge is quantized. Electric charge is conserved lectstatics lectic Chage lectic chage is uantized Chage cmes in incements f the elementay chage e = ne, whee n is an intege, and e =.6 x 0-9 C lectic chage is cnseved Chage (electns) can be mved fm ne

More information

Hotelling s Rule. Therefore arbitrage forces P(t) = P o e rt.

Hotelling s Rule. Therefore arbitrage forces P(t) = P o e rt. Htelling s Rule In what fllws I will use the tem pice t dente unit pfit. hat is, the nminal mney pice minus the aveage cst f pductin. We begin with cmpetitin. Suppse that a fim wns a small pa, a, f the

More information

The Gradient and Applications This unit is based on Sections 9.5 and 9.6, Chapter 9. All assigned readings and exercises are from the textbook

The Gradient and Applications This unit is based on Sections 9.5 and 9.6, Chapter 9. All assigned readings and exercises are from the textbook The Gadient and Applicatins This unit is based n Sectins 9.5 and 9.6 Chapte 9. All assigned eadings and eecises ae fm the tetbk Objectives: Make cetain that u can define and use in cntet the tems cncepts

More information

Journal of Theoretics

Journal of Theoretics Junal f Theetics Junal Hme Page The Classical Pblem f a Bdy Falling in a Tube Thugh the Cente f the Eath in the Dynamic They f Gavity Iannis Iaklis Haanas Yk Univesity Depatment f Physics and Astnmy A

More information

MEM202 Engineering Mechanics Statics Course Web site:

MEM202 Engineering Mechanics Statics Course Web site: 0 Engineeing Mechanics - Statics 0 Engineeing Mechanics Statics Cuse Web site: www.pages.dexel.edu/~cac54 COUSE DESCIPTION This cuse cves intemediate static mechanics, an extensin f the fundamental cncepts

More information

Application of Net Radiation Transfer Method for Optimization and Calculation of Reduction Heat Transfer, Using Spherical Radiation Shields

Application of Net Radiation Transfer Method for Optimization and Calculation of Reduction Heat Transfer, Using Spherical Radiation Shields Wld Applied Sciences Junal (4: 457-46, 00 ISSN 88-495 IDOSI Publicatins, 00 Applicatin f Net Radiatin Tansfe Methd f Optimizatin and Calculatin f Reductin Heat Tansfe, Using Spheical Radiatin Shields Seyflah

More information

On the structure of MHD shock waves in a viscous gas

On the structure of MHD shock waves in a viscous gas On the stuctue f MHD shck waves in a viscus gas On the stuctue f MHD shck waves in a viscus gas R. K. Anand and Haish C. Yadav Depatment f Physics, Univesity f Allahabad, Allahabad-, India e-mail: anand.ajkuma@ediffmail.cm

More information

THE SPATIAL CROSS-CORRELATION OF. Mobile and Portable Radio Research Group

THE SPATIAL CROSS-CORRELATION OF. Mobile and Portable Radio Research Group FFCTS OF MULTIPATH AGULAR SPRAD O TH SPATIAL CROSS-CORRLATIO OF RCIVD VOLTAG VLOPS Gegy D. Dugin and Thede S. Rappapt Mbile and Ptable Radi Reseach Gup Badley Depatment f lectical and Cmpute ngineeing

More information

Subjects discussed: Aircraft Engine Noise : Principles; Regulations

Subjects discussed: Aircraft Engine Noise : Principles; Regulations 16.50 Lectue 36 Subjects discussed: Aicaft Engine Nise : Pinciples; Regulatins Nise geneatin in the neighbhds f busy aipts has been a seius pblem since the advent f the jet-pweed tanspt, in the late 1950's.

More information

Consider the simple circuit of Figure 1 in which a load impedance of r is connected to a voltage source. The no load voltage of r

Consider the simple circuit of Figure 1 in which a load impedance of r is connected to a voltage source. The no load voltage of r 1 Intductin t Pe Unit Calculatins Cnside the simple cicuit f Figue 1 in which a lad impedance f L 60 + j70 Ω 9. 49 Ω is cnnected t a vltage suce. The n lad vltage f the suce is E 1000 0. The intenal esistance

More information

A Direct Method for the Evaluation of Lower and Upper Bound Ratchet Limits

A Direct Method for the Evaluation of Lower and Upper Bound Ratchet Limits A Diect Methd f the Evaluatin f Lwe and Uppe Bund Ratchet Limits J. Ue a, H. Chen a, T. Li a, W. Chen a, D. Tipping b, D. Macenzie a a Dept f Mechanical Engineeing, Univesity f Stathclyde, Glasgw, Sctland,

More information

Introduction. Electrostatics

Introduction. Electrostatics UNIVESITY OF TECHNOLOGY, SYDNEY FACULTY OF ENGINEEING 4853 Electmechanical Systems Electstatics Tpics t cve:. Culmb's Law 5. Mateial Ppeties. Electic Field Stength 6. Gauss' Theem 3. Electic Ptential 7.

More information

University of Pisa. N. Zaccari, D. Aquaro. Pebble Beds. - ITALY - Department of Mechanical, Nuclear and Production Engineering

University of Pisa. N. Zaccari, D. Aquaro. Pebble Beds. - ITALY - Department of Mechanical, Nuclear and Production Engineering Univesity f Pisa - ITALY - Depatment f Mechanical, Nuclea and Pductin Engineeing Them-Mechanical Behaviu f Li 4 SO 4 and Li TiO 3 N. Zaccai, D. Aqua Cntents f Pesentatin This pesentatin descibes the them-mechanical

More information

Direct Torque Control of 5-Phase 10/8 Switched Reluctance Motors

Direct Torque Control of 5-Phase 10/8 Switched Reluctance Motors Dwnladed fm ijeee.iust.ac.i at 18:19 IRST n Fiday Septembe 8th 18 Diect Tque Cntl f -Phase 1/8 Switched Reluctance Mts M. R. Feyzi* and Y. Ebahimi* Abstact: A switched Reluctance mt (SRM) has seveal desiable

More information

[1 + (r' )2J (O(eCP**)

[1 + (r' )2J (O(eCP**) Pceedings f the 1966 Linea Acceleat Cnfeence, Ls Alams, New Mexic, USA Intductin THE "PIERCE"-GEOMETRY AN ACCELERATING COLUMN DESIGN* C. Rbet lilnigh Ls Alams Scientific Labaty Ls Alams, New Mexic The

More information

A Direct Method for the Evaluation of Lower and Upper Bound Ratchet Limits

A Direct Method for the Evaluation of Lower and Upper Bound Ratchet Limits Ue, James Michael and Chen, Hafeng and Chen, Weihang and Li, Tianbai and Tipping, James and Macenzie, Dnald (211) A diect methd f the evaluatin f lwe and uppe bund atchet limits. In: 11th Intenatinal Cnfeence

More information

INVERSE QUANTUM STATES OF HYDROGEN

INVERSE QUANTUM STATES OF HYDROGEN INVERSE QUANTUM STATES OF HYDROGEN Rnald C. Bugin Edgecmbe Cmmunity Cllege Rcky Munt, Nth Calina 780 bugin@edgecmbe.edu ABSTRACT The pssible existence f factinal quantum states in the hydgen atm has been

More information

A) N B) 0.0 N C) N D) N E) N

A) N B) 0.0 N C) N D) N E) N Cdinat: H Bahluli Sunday, Nvembe, 015 Page: 1 Q1. Five identical pint chages each with chage =10 nc ae lcated at the cnes f a egula hexagn, as shwn in Figue 1. Find the magnitude f the net electic fce

More information

Analytical Solution to Diffusion-Advection Equation in Spherical Coordinate Based on the Fundamental Bloch NMR Flow Equations

Analytical Solution to Diffusion-Advection Equation in Spherical Coordinate Based on the Fundamental Bloch NMR Flow Equations Intenatinal Junal f heetical and athematical Phsics 5, 5(5: 4-44 OI:.593/j.ijtmp.555.7 Analtical Slutin t iffusin-advectin Equatin in Spheical Cdinate Based n the Fundamental Blch N Flw Equatins anladi

More information

Phys 332 Electricity & Magnetism Day 3. Note: I should have recommended reading section 1.5 (delta function) as well. rˆ rˆ

Phys 332 Electricity & Magnetism Day 3. Note: I should have recommended reading section 1.5 (delta function) as well. rˆ rˆ Phs 33 lecticit & Magnetism Da 3 Mn. 9/9 Wed. 9/ Thus 9/ Fi. 9/3 (C.-.5,.8). &.5;..-.. Gauss & Div, T Numeical Quadatue (C.-.5,.8)..3 Using Gauss (C.-.5,.8)..3-.. Using Gauss HW quipment Bing in ppt s

More information

Effect of Peclet Number on the Dispersion of a Solute in a Blood flowing in Non-Uniform Tube

Effect of Peclet Number on the Dispersion of a Solute in a Blood flowing in Non-Uniform Tube Intenatinal Junal f Cmputatinal and Applied Mathematics. ISSN 1819-4966 Vlume 1, Numbe (017), pp. 449-456 Reseach India Publicatins http://www.ipublicatin.cm Effect f clet Numbe n the Dispesin f a Slute

More information

A) (0.46 î ) N B) (0.17 î ) N

A) (0.46 î ) N B) (0.17 î ) N Phys10 Secnd Maj-14 Ze Vesin Cdinat: xyz Thusday, Apil 3, 015 Page: 1 Q1. Thee chages, 1 = =.0 μc and Q = 4.0 μc, ae fixed in thei places as shwn in Figue 1. Find the net electstatic fce n Q due t 1 and.

More information

Journal of Solid Mechanics and Materials Engineering

Journal of Solid Mechanics and Materials Engineering Junal f Slid Mechanics and Mateials Engineeing Vl. 4, N. 8, 21 Themal Stess and Heat Tansfe Cefficient f Ceamics Stalk Having Ptubeance Dipping int Mlten Metal* Na-ki NOD**, Henda**, Wenbin LI**, Yasushi

More information

Work, Energy, and Power. AP Physics C

Work, Energy, and Power. AP Physics C k, Eneg, and Pwe AP Phsics C Thee ae man diffeent TYPES f Eneg. Eneg is expessed in JOULES (J) 4.19 J = 1 calie Eneg can be expessed me specificall b using the tem ORK() k = The Scala Dt Pduct between

More information

Chapter 2: Estuarine Salinity Structure and Circulation

Chapter 2: Estuarine Salinity Structure and Circulation Chapte : Estuaine Salinity Stuctue and Ciculatin W.R. Geye, Wds Hle Oceangaphic Institutin.. The Hizntal Salinity Gadient Estuaies shw a geat divesity f size, shape, depth, and fcing chaacteistics, but

More information

Magnetism. Chapter 21

Magnetism. Chapter 21 1.1 Magnetic Fields Chapte 1 Magnetism The needle f a cmpass is pemanent magnet that has a nth magnetic ple (N) at ne end and a suth magnetic ple (S) at the the. 1.1 Magnetic Fields 1.1 Magnetic Fields

More information

On the Micropolar Fluid Flow through Porous Media

On the Micropolar Fluid Flow through Porous Media Pceedings f the th WEA Int. Cnf. n MATHEMATICAL METHOD, COMPUTATIONAL TECHNIQUE AND INTELLIGENT YTEM On the Micpla Fluid Flw thugh Pus Media M.T. KAMEL 3, D. ROACH, M.H. HAMDAN,3 Depatment f Mathematical

More information

OPERATIONAL AMPLIFIERS

OPERATIONAL AMPLIFIERS PEATINAL AMPLIFIES Why do we study them at ths pont???. pamps are ery useful electronc components. We hae already the tools to analyze practcal crcuts usng pamps 3. The lnear models for pamps nclude dependent

More information

Relevance feedback and query expansion. Goal: To refine the answer set by involving the user in the retrieval process (feedback/interaction)

Relevance feedback and query expansion. Goal: To refine the answer set by involving the user in the retrieval process (feedback/interaction) Relevance feedback and quey epansin Gal: T efine the answe set by invlving the use in the etieval pcess (feedback/inteactin) Lcal Methds (adust the use queies) Relevance feedback Pseud ( Blind) Relevance

More information

EFFECT OF VARIATION IN LENGTH OF THE CONVENTIONAL HEAT PIPE ON THE THERMAL PERFORMANCE

EFFECT OF VARIATION IN LENGTH OF THE CONVENTIONAL HEAT PIPE ON THE THERMAL PERFORMANCE EFFECT OF VAIATION IN LENGTH OF THE CONVENTIONAL HEAT PIPE ON THE THEMAL PEFOMANCE Yung Min Se, Yng Gap Pak and Man Yeng Ha* *Auth f cespndence Schl f Mechanical Engineeing, Pusan Natinal Uniesity, Suth

More information

Strees Analysis in Elastic Half Space Due To a Thermoelastic Strain

Strees Analysis in Elastic Half Space Due To a Thermoelastic Strain IOSR Junal f Mathematics (IOSRJM) ISSN: 78-578 Vlume, Issue (July-Aug 0), PP 46-54 Stees Analysis in Elastic Half Space Due T a Themelastic Stain Aya Ahmad Depatment f Mathematics NIT Patna Biha India

More information

Physics 111. Exam #1. January 26, 2018

Physics 111. Exam #1. January 26, 2018 Physics xam # Januay 6, 08 ame Please ead and fllw these instuctins caefully: Read all pblems caefully befe attempting t slve them. Yu wk must be legible, and the ganizatin clea. Yu must shw all wk, including

More information

Effect of drag on the performance for an efficient wind turbine blade design

Effect of drag on the performance for an efficient wind turbine blade design Available online at www.sciencediect.com Enegy Pocedia 18 (01 ) 404 415 Abstact Effect of dag on the pefomance fo an efficient wind tubine blade design D. Eng. Ali H. Almukhta Univesity of Technology Email-

More information

March 15. Induction and Inductance Chapter 31

March 15. Induction and Inductance Chapter 31 Mach 15 Inductin and Inductance Chapte 31 > Fces due t B fields Lentz fce τ On a mving chage F B On a cuent F il B Cuent caying cil feels a tque = µ B Review > Cuents geneate B field Bit-Savat law = qv

More information

Distance oracles in edge-labeled graphs

Distance oracles in edge-labeled graphs Distance acles in edge-labeled gaphs Fancesc Bnchi Aistides Ginis Fancesc Gull Antti Ukknen Yah Labs Bacelna, Spain {bnchi,gull}@yah-inc.cm Helsinki Institute f Infmatin Technlgy HIIT Aalt Univesity {aistides.ginis,antti.ukknen}@aalt.fi

More information

Lecture #2 : Impedance matching for narrowband block

Lecture #2 : Impedance matching for narrowband block Lectue # : Ipedance atching f nawband blck ichad Chi-Hsi Li Telephne : 817-788-848 (UA) Cellula phne: 13917441363 (C) Eail : chihsili@yah.c.cn 1. Ipedance atching indiffeent f bandwidth ne pat atching

More information

AIR FORCE RESEARCH LABORATORY

AIR FORCE RESEARCH LABORATORY AIR FORC RSARCH LABORATORY The xtinctin Theem as an xample f Reseach Vistas in Mathematical Optics Mach Richad A. Albanese Infmatin Opeatins and Applied Mathematics Human ffectiveness Diectate Bks City-Base

More information

5.1 Moment of a Force Scalar Formation

5.1 Moment of a Force Scalar Formation Outline ment f a Cuple Equivalent System Resultants f a Fce and Cuple System ment f a fce abut a pint axis a measue f the tendency f the fce t cause a bdy t tate abut the pint axis Case 1 Cnside hizntal

More information

SOURCE MODEL OF THE 2010 ELAZIG KOVANCILAR EARTHQUAKE (M w 6.1) FOR BROADBAND GROUND MOTION SIMULATION

SOURCE MODEL OF THE 2010 ELAZIG KOVANCILAR EARTHQUAKE (M w 6.1) FOR BROADBAND GROUND MOTION SIMULATION SOURCE MODEL OF THE 200 ELAZIG KOVANCILAR EARTHQUAKE (M w 6.) FOR BROADBAND GROUND MOTION SIMULATION Mehmet Baykal MEE0509 Supevis: Hie Miyake ABSTRACT On 8 Mach 200, an eathquake f M w =6. ccued in Elazig

More information

Advanced Computational Tools for Wound Core Distribution Transformer No Load Analysis

Advanced Computational Tools for Wound Core Distribution Transformer No Load Analysis ARWt010 Advanced Reseach Wksh n Tansfmes. 3-6 Octbe 010. Santiag de Cmstela Sain Advanced Cmutatinal Tls f Wund Ce Distibutin Tansfme N Lad Analysis Themistklis D. KEFALAS and Antnis G. KLADAS Schl f Electical

More information

Solutions: Solution. d = 3.0g/cm we can calculate the number of Xe atoms per unit volume, Given m and the given values from Table 7.

Solutions: Solution. d = 3.0g/cm we can calculate the number of Xe atoms per unit volume, Given m and the given values from Table 7. Tutial-09 Tutial - 09 Sectin6: Dielectic Mateials ECE:09 (Electnic and Electical Ppeties f Mateials) Electical and Cmpute Engineeing Depatment Univesity f Watel Tut: Hamid Slutins: 7.3 Electnic plaizatin

More information

Chapter 3: Cluster Analysis

Chapter 3: Cluster Analysis Chapter 3: Cluster Analysis } 3.1 Basic Cncepts f Clustering 3.1.1 Cluster Analysis 3.1. Clustering Categries } 3. Partitining Methds 3..1 The principle 3.. K-Means Methd 3..3 K-Medids Methd 3..4 CLARA

More information

Clean Technol., Vol. 22, No. 1, March 2016, pp

Clean Technol., Vol. 22, No. 1, March 2016, pp lean echnl., Vl., N. 1, Mach 016, pp. 45-5 청정에너지기술 mpaisn between Wate and N-etadecane as Insulatin Mateials thugh Mdeling and Simulatin f Heat ansfe in Pacaging Bx f Vaccine Shipping Van-Dung Da 1, I-Kyu

More information

Classical Chaos on Double Nonlinear Resonances in Diatomic Molecules

Classical Chaos on Double Nonlinear Resonances in Diatomic Molecules Junal f Mden Physics, 05, 6, 496-509 Published Online Mach 05 in SciRes. http://www.scip.g/junal/jmp http://dx.di.g/0.436/jmp.05.64054 Classical Chas n Duble Nnlinea Resnances in Diatmic Mlecules G. V.

More information

Computational modeling techniques

Computational modeling techniques Cmputatinal mdeling techniques Lecture 4: Mdel checing fr ODE mdels In Petre Department f IT, Åb Aademi http://www.users.ab.fi/ipetre/cmpmd/ Cntent Stichimetric matrix Calculating the mass cnservatin relatins

More information

PERFORMANCE OPTIMIZATION OF LINEAR INDUCTION MOTOR BY EDDY CURRENT AND FLUX DENSITY DISTRIBUTION ANALYSIS

PERFORMANCE OPTIMIZATION OF LINEAR INDUCTION MOTOR BY EDDY CURRENT AND FLUX DENSITY DISTRIBUTION ANALYSIS unal f Engineeing Science and Technlg Vl. 6, N. 6 (011) 769-776 Schl f Engineeing, Tal s Univesit PERFORMANCE OPTIMIZATION OF LINEAR INDUCTION MOTOR BY EDDY CURRENT AND FLUX DENSITY DISTRIBUTION ANALYSIS

More information

Exercises for Differential Amplifiers. ECE 102, Fall 2012, F. Najmabadi

Exercises for Differential Amplifiers. ECE 102, Fall 2012, F. Najmabadi Execises f iffeential mplifies ECE 0, Fall 0, F. Najmabai Execise : Cmpute,, an G if m, 00 Ω, O, an ientical Q &Q with µ n C x 8 m, t, λ 0. F G 0 an B F G. epeat the execise f λ 0. -. This execise shws

More information

Surface and Interface Science Physics 627; Chemistry 542. Lecture 10 March 1, 2013

Surface and Interface Science Physics 627; Chemistry 542. Lecture 10 March 1, 2013 Suface and Inteface Science Physics 67; Chemisty 54 Lectue 0 Mach, 03 Int t Electnic Ppeties: Wk Functin,Theminic Electn Emissin, Field Emissin Refeences: ) Wduff & Delcha, Pp. 40-4; 46-484 ) Zangwill

More information

Chapter 4 Motion in Two and Three Dimensions

Chapter 4 Motion in Two and Three Dimensions Chapte 4 Mtin in Tw and Thee Dimensins In this chapte we will cntinue t stud the mtin f bjects withut the estictin we put in chapte t me aln a staiht line. Instead we will cnside mtin in a plane (tw dimensinal

More information

STUDY ON 2-D SHOCK WAVE PRESSURE MODEL IN MICRO SCALE LASER SHOCK PEENING

STUDY ON 2-D SHOCK WAVE PRESSURE MODEL IN MICRO SCALE LASER SHOCK PEENING Study Rev. Adv. on -D Mate. shock Sci. wave 33 (13) pessue 111-118 model in mico scale lase shock peening 111 STUDY ON -D SHOCK WAVE PRESSURE MODEL IN MICRO SCALE LASER SHOCK PEENING Y.J. Fan 1, J.Z. Zhou,

More information

1. State Kay Lab of New Ceramics and Fine Processing, Department of Materials Science and Engineering, Tsinghua University, Beijing , China

1. State Kay Lab of New Ceramics and Fine Processing, Department of Materials Science and Engineering, Tsinghua University, Beijing , China Suppting Infmatin Indefinite by natue: fm ultavilet t teahetz Jingb Sun 1, 2, Natalia M Litchinitse 2, Ji Zhu 1, * 1. State Kay Lab f New Ceamics and Fine Pcessing, Depatment f Mateials Science and Engineeing,

More information

REPORT ITU-R SA Protection of the space VLBI telemetry link

REPORT ITU-R SA Protection of the space VLBI telemetry link Rep. ITU-R SA.65 REPORT ITU-R SA.65 Ptectin f the space VLBI telemety link CONTENTS Page Intductin... Space VLBI system.... Space VLBI telemety signal, nise and intefeence..... Signal... 3.. Nise and intefeence...

More information

THE COUPLING SPECTRUM: A NEW METHOD FOR DETECTING TEMPORAL NONLINEAR CAUSALITY IN FINANCIAL TIME SERIES

THE COUPLING SPECTRUM: A NEW METHOD FOR DETECTING TEMPORAL NONLINEAR CAUSALITY IN FINANCIAL TIME SERIES The 7 th Intenatinal Days f Statisti and Ecnmi, Pague, Septembe 9-2, 23 THE COUPLING SPECTRUM: A NEW METHOD FOR DETECTING TEMPORAL NONLINEAR CAUSALIT IN FINANCIAL TIME SERIES Ami Reza Alizad-Rahva Masud

More information

Central Coverage Bayes Prediction Intervals for the Generalized Pareto Distribution

Central Coverage Bayes Prediction Intervals for the Generalized Pareto Distribution Statistics Reseach Lettes Vol. Iss., Novembe Cental Coveage Bayes Pediction Intevals fo the Genealized Paeto Distibution Gyan Pakash Depatment of Community Medicine S. N. Medical College, Aga, U. P., India

More information

is the instantaneous position vector of any grid point or fluid

is the instantaneous position vector of any grid point or fluid Absolute inetial, elative inetial and non-inetial coodinates fo a moving but non-defoming contol volume Tao Xing, Pablo Caica, and Fed Sten bjective Deive and coelate the govening equations of motion in

More information

ON THE K-FACTOR DISTRIBUTION AND DIFFRACTION FADING FOR SOUTHERN AFRICA

ON THE K-FACTOR DISTRIBUTION AND DIFFRACTION FADING FOR SOUTHERN AFRICA 7 SOUTH AFRICAN INSTITUTE OF ELECTRICAL ENGINEERS Vl.97() June 006 ON THE K-FACTOR DISTRIBUTION AND DIFFRACTION AND DIFFRACTION FADING FOR SOUTHERN AFRICA T.J. Afull and P.K. Odedina Schl f Electical,

More information

NUMERICAL EVALUATION ON FLOOR COOLING CAPACITY IN AN AIRPORT AH, Nijmegen, the Netherlands Tianjin, China

NUMERICAL EVALUATION ON FLOOR COOLING CAPACITY IN AN AIRPORT AH, Nijmegen, the Netherlands Tianjin, China ceedings: Building Simulatin 07 NUMEICAL EVALUATION ON FLOO COOLING CAACITY IN AN AIOT 3,3, Bing Yu, J.. uchti and.g. Luscuee Divisin Building Sevices, yal Haskning Gup, stbx 5 6500 AH, Nijmegen, the Nethelands

More information

A) 100 K B) 150 K C) 200 K D) 250 K E) 350 K

A) 100 K B) 150 K C) 200 K D) 250 K E) 350 K Phys10 Secnd Maj-09 Ze Vesin Cdinat: k Wednesday, May 05, 010 Page: 1 Q1. A ht bject and a cld bject ae placed in themal cntact and the cmbinatin is islated. They tansfe enegy until they each a final equilibium

More information

EPr over F(X} AA+ A+A. For AeF, a generalized inverse. ON POLYNOMIAL EPr MATRICES

EPr over F(X} AA+ A+A. For AeF, a generalized inverse. ON POLYNOMIAL EPr MATRICES Intenat. J. Hath. & Math. S. VOL. 15 NO. 2 (1992) 261-266 ON POLYNOMIAL EP MATRICES 261 AR. MEENAKSHI and N. ANANOAM Depatment f Mathematics, Annamalai Univeslty, Annamalainaga- 68 2, Tamll Nadu, INDIA.

More information

Inflow Control on Expressway Considering Traffic Equilibria

Inflow Control on Expressway Considering Traffic Equilibria Memirs f the Schl f Engineering, Okayama University Vl. 20, N.2, February 1986 Inflw Cntrl n Expressway Cnsidering Traffic Equilibria Hirshi INOUYE* (Received February 14, 1986) SYNOPSIS When expressway

More information

Electric Fields and Electric Forces

Electric Fields and Electric Forces Cpyight, iley 006 (Cutnell & Jhnsn 9. Ptential Enegy Chapte 9 mgh mgh GPE GPE Electic Fields and Electic Fces 9. Ptential Enegy 9. Ptential Enegy 9. The Electic Ptential Diffeence 9. The Electic Ptential

More information

2. Electrostatics. Dr. Rakhesh Singh Kshetrimayum 8/11/ Electromagnetic Field Theory by R. S. Kshetrimayum

2. Electrostatics. Dr. Rakhesh Singh Kshetrimayum 8/11/ Electromagnetic Field Theory by R. S. Kshetrimayum 2. Electostatics D. Rakhesh Singh Kshetimayum 1 2.1 Intoduction In this chapte, we will study how to find the electostatic fields fo vaious cases? fo symmetic known chage distibution fo un-symmetic known

More information

NUMERICAL SIMULATION OF MUD-FILTRATE INVASION IN HORIZONTAL WELLS AND SENSITIVITY ANALYSIS OF ARRAY INDUCTION TOOLS

NUMERICAL SIMULATION OF MUD-FILTRATE INVASION IN HORIZONTAL WELLS AND SENSITIVITY ANALYSIS OF ARRAY INDUCTION TOOLS NUMERICAL SIMULATION OF MUD-FILTRATE INVASION IN HORIZONTAL WELLS AND SENSITIVITY ANALYSIS OF ARRAY INDUCTION TOOLS F. O. Alpak, The Univesity f Texas at Austin, E. B. Dussan V., T. Habashy, Schlumbege-Dll

More information

An Exact Solution of Navier Stokes Equation

An Exact Solution of Navier Stokes Equation An Exact Solution of Navie Stokes Equation A. Salih Depatment of Aeospace Engineeing Indian Institute of Space Science and Technology, Thiuvananthapuam, Keala, India. July 20 The pincipal difficulty in

More information

Fri. 10/23 (C14) Linear Dielectrics (read rest at your discretion) Mon. (C 17) , E to B; Lorentz Force Law: fields

Fri. 10/23 (C14) Linear Dielectrics (read rest at your discretion) Mon. (C 17) , E to B; Lorentz Force Law: fields Fi. 0/23 (C4) 4.4. Linea ielectics (ead est at yu discetin) Mn. (C 7) 2..-..2, 2.3. t B; 5..-..2 Lentz Fce Law: fields Wed. and fces Thus. (C 7) 5..3 Lentz Fce Law: cuents Fi. (C 7) 5.2 Bit-Savat Law HW6

More information

DESIGN OPTIMIZATION OF HIGH-LIFT CONFIGURATIONS USING A VISCOUS ADJOINT-BASED METHOD

DESIGN OPTIMIZATION OF HIGH-LIFT CONFIGURATIONS USING A VISCOUS ADJOINT-BASED METHOD DESIGN OPTIMIZATION OF HIGH-LIFT CONFIGURATIONS USING A VISCOUS ADJOINT-BASED METHOD Sangh Kim Stanfrd University Juan J. Alns Stanfrd University Antny Jamesn Stanfrd University 40th AIAA Aerspace Sciences

More information

Electromagnetic Waves

Electromagnetic Waves Chapte 3 lectmagnetic Waves 3.1 Maxwell s quatins and ectmagnetic Waves A. Gauss s Law: # clsed suface aea " da Q enc lectic fields may be geneated by electic chages. lectic field lines stat at psitive

More information

A perturbation density functional theory for the competition between inter and intramolecular association

A perturbation density functional theory for the competition between inter and intramolecular association petubatin density functinal they f the cpetitin between inte and intalecula assciatin Bennett D. Chapan a leand J. Gacía-Cuélla b and Walte G. Chapan a a Depatent f Cheical and Bilecula Engineeing Rice

More information

torr ~tirru 'V Q Hz N/m 2 EQUIPMENT z a r 1 INTRODUCTION

torr ~tirru 'V Q Hz N/m 2 EQUIPMENT z a r 1 INTRODUCTION l @1~ 8 ~tiu ilf'@m W@~(Q) H~W t N-J ERMEER Delft Univesity f Technlgy, The Nethelands a~ SYNOPSS As a cntinuatin f ealie wk, velcities have been easued in the nea wake f a del t in the wind tunnel By

More information

Properties of Preference Questions: Utility Balance, Choice Balance, Configurators, and M-Efficiency

Properties of Preference Questions: Utility Balance, Choice Balance, Configurators, and M-Efficiency Ppeties f Pefeence Questins: Utility Balance, Chice Balance, Cnfiguats, and M-Efficiency by Jhn R. Hause and Olivie Tubia August, 3 Jhn R. Hause is the iin Pfess f Maketing, Slan Schl f Management, Massachusetts

More information

Hydroelastic Analysis of a 1900 TEU Container Ship Using Finite Element and Boundary Element Methods

Hydroelastic Analysis of a 1900 TEU Container Ship Using Finite Element and Boundary Element Methods TEAM 2007, Sept. 10-13, 2007,Yokohama, Japan Hydoelastic Analysis of a 1900 TEU Containe Ship Using Finite Element and Bounday Element Methods Ahmet Egin 1)*, Levent Kaydıhan 2) and Bahadı Uğulu 3) 1)

More information

Overlapping generation models with housing: impact of the key parameters on the models outcomes

Overlapping generation models with housing: impact of the key parameters on the models outcomes The 11 th Pfess Aleksande Zelias Intenatinal Cnfeence n Mdelling and Fecasting f Sci-Ecnmic Phenmena Ovelapping geneatin mdels with husing: impact f the key paametes n the mdels utcmes Jan Acedański 1

More information

Applied Aerodynamics

Applied Aerodynamics Applied Aeodynamics Def: Mach Numbe (M), M a atio of flow velocity to the speed of sound Compessibility Effects Def: eynolds Numbe (e), e ρ c µ atio of inetial foces to viscous foces iscous Effects If

More information

Understanding Control Charting: Techniques and Assumptions

Understanding Control Charting: Techniques and Assumptions Undestanding Cntl Chating: Techniques and Assumptins Chales H. Daby, Health Sevices Evaluatin, May Clinic, Rcheste, Minnesta Abstact Evey pcess has sme cmpnent f vaiatin, and by measuing that vaiatin diectly

More information

Performance Analysis of Household Refrigerator with Alternate Refrigerants

Performance Analysis of Household Refrigerator with Alternate Refrigerants ISSN: 239-873 Intenatinal Junal f Innvative Reseach in Science, Engineeing and Technlgy (An ISO 3297: 2007 Cetified Oganizatin) Vl. 3, Issue 4, Apil 204 Pefmance Analysis f Husehld Refigeat with Altenate

More information

CHE CHAPTER 11 Spring 2005 GENERAL 2ND ORDER REACTION IN TURBULENT TUBULAR REACTORS

CHE CHAPTER 11 Spring 2005 GENERAL 2ND ORDER REACTION IN TURBULENT TUBULAR REACTORS CHE 52 - CHPTE Sping 2005 GENEL 2ND ODE ECTION IN TUULENT TUUL ECTOS Vassilats & T, IChEJ. (4), 666 (965) Cnside the fllwing stichiety: a + b = P The ass cnsevatin law f species i yields Ci + vci =. Di

More information

Solution: (a) C 4 1 AI IC 4. (b) IBC 4

Solution: (a) C 4 1 AI IC 4. (b) IBC 4 C A C C R A C R C R C sin 9 sin. A cuent f is maintaine in a single cicula lp f cicumfeence C. A magnetic fiel f is iecte paallel t the plane f the lp. (a) Calculate the magnetic mment f the lp. (b) What

More information

Contact impedance of grounded and capacitive electrodes

Contact impedance of grounded and capacitive electrodes Abstact Contact impedance of gounded and capacitive electodes Andeas Hödt Institut fü Geophysik und extateestische Physik, TU Baunschweig The contact impedance of electodes detemines how much cuent can

More information

Sensors and Actuators Introduction to sensors

Sensors and Actuators Introduction to sensors Senss and Actuats Intductin t senss Sande Stuij (s.stuij@tue.nl) Depatment f Electical Engineeing Electnic Systems AMPLIFIES (Chapte 5.) Infmatin pcessing system nncntact sens cntact sens abslute sens

More information

Modified Theory of Laminar Flow Around Rigid and Liquid Cylinders

Modified Theory of Laminar Flow Around Rigid and Liquid Cylinders Pceedings f the 4th WSEAS Intenatinal Cnfeence n Fluid Mechanics and Aednamics, Elunda, Geece, August -3, 6 (pp95-3) Mdified The f Lamina Flw Aund Rigid and Liquid Clindes FRIEDRICH K. BENRA, and SIAVASH

More information

Supplementary Figure 1. Circular parallel lamellae grain size as a function of annealing time at 250 C. Error bars represent the 2σ uncertainty in

Supplementary Figure 1. Circular parallel lamellae grain size as a function of annealing time at 250 C. Error bars represent the 2σ uncertainty in Supplementay Figue 1. Cicula paallel lamellae gain size as a function of annealing time at 50 C. Eo bas epesent the σ uncetainty in the measued adii based on image pixilation and analysis uncetainty contibutions

More information

Section 4.2 Radians, Arc Length, and Area of a Sector

Section 4.2 Radians, Arc Length, and Area of a Sector Sectin 4.2 Radian, Ac Length, and Aea f a Sect An angle i fmed by tw ay that have a cmmn endpint (vetex). One ay i the initial ide and the the i the teminal ide. We typically will daw angle in the cdinate

More information

Chapter 9 Dynamic stability analysis III Lateral motion (Lectures 33 and 34)

Chapter 9 Dynamic stability analysis III Lateral motion (Lectures 33 and 34) Pof. E.G. Tulapukaa Stability and contol Chapte 9 Dynamic stability analysis Lateal motion (Lectues 33 and 34) Keywods : Lateal dynamic stability - state vaiable fom of equations, chaacteistic equation

More information

AT622 Section 15 Radiative Transfer Revisited: Two-Stream Models

AT622 Section 15 Radiative Transfer Revisited: Two-Stream Models AT6 Sectin 5 Radiative Tansfe Revisited: Tw-Steam Mdels The gal f this sectin is t intduce sme elementay cncepts f adiative tansfe that accunts f scatteing, absptin and emissin and intduce simple ways

More information

Water flows through the voids in a soil which are interconnected. This flow may be called seepage, since the velocities are very small.

Water flows through the voids in a soil which are interconnected. This flow may be called seepage, since the velocities are very small. Wate movement Wate flows though the voids in a soil which ae inteconnected. This flow may be called seepage, since the velocities ae vey small. Wate flows fom a highe enegy to a lowe enegy and behaves

More information

SPE p p. Abstract

SPE p p. Abstract SPE 169333 Inflw Pefmance Relatinship Euatin f Slutin Gas-Dive Resevis unde Gavity Segegatin Rbet Padilla-Sixt, SPE, Cnsultant, and Rdlf Camach-Velázuez, SPE, Pemex E&P Cpyight 14, Sciety f Petleum Enginees

More information

The Millikan Experiment: Determining the Elementary Charge

The Millikan Experiment: Determining the Elementary Charge LAB EXERCISE 7.5.1 7.5 The Elementay Chage (p. 374) Can you think of a method that could be used to suggest that an elementay chage exists? Figue 1 Robet Millikan (1868 1953) m + q V b The Millikan Expeiment:

More information

NUMERICAL SIMULATION OF FLUID FLOW IN ENCLOSED ROTATING FILTER AND DISK

NUMERICAL SIMULATION OF FLUID FLOW IN ENCLOSED ROTATING FILTER AND DISK VOL., NO. 9, SEPTEMBER 010 ISSN 1819-6608 ARPN Jounal of Engineeing and Applied Sciences 006-010 Asian Reseach Publishing Netwok (ARPN). All ights eseved. www.apnjounals.com NUMERICAL SIMULATION OF FLUID

More information