A Fuzzy Satisfactory Optimization Method Based on Stress Analysis for a Hybrid Composite Flywheel

Size: px
Start display at page:

Download "A Fuzzy Satisfactory Optimization Method Based on Stress Analysis for a Hybrid Composite Flywheel"

Transcription

1 Wold Academy of Science, Engineeing and Technology Intenational Jounal of Mateials and Metallugical Engineeing A Fuzzy Satisfactoy Optimization Method Based on Stess Analysis fo a Hybid Composite Flywheel Liping Yang, Cuan Cawfod, J. Ren, Zhengyi Ren Intenational Science Index, Mateials and Metallugical Engineeing waset.og/publication/ Abstact Consideing the cost evaluation and the stess analysis, a fuzzy satisfactoy optimization (FSO) method has been developed fo a hybid composite flywheel. To evaluate the cost, the cost coefficients of the flywheel components ae obtained though calculating the weighted sum of the scoes of the mateial manufactuability, the stuctue chaacte, and the mateial pice. To expess the satisfactoy degee of the enegy, the cost, and the mass, the satisfactoy functions ae poposed by using the decline function and intoducing a satisfactoy coefficient. To imply the diffeent significance of the objectives, the object weight coefficients ae defined. Based on the stess analysis of composite mateial, the cicumfeential and adial stesses ae consideed into the optimization fomulation. The simulations of the FSO method with diffeent weight coefficients and stoage enegy density optimization (SEDO) method of a flywheel ae contasted. The analysis esults show that the FSO method can satisfy diffeent equiements of the designe and the FSO method with suitable weight coefficients can eplace the SEDO method. Keywods Flywheel enegy stoage, fuzzy, optimization, stess analysis. I. INTRODUCTION OMPARED with chemical enegy stoage, Flywheel C Enegy Stoage (FES) has the advantages of no pollution, no equiement of stict envionmental tempeatue, etc. Theefoe, along with the envionment potection being paid moe attention, FES technology has eceived moe and moe attention within the ecent yeas. As the coe components of a FES System (FESS), the flywheel stuctue is vey impotant not only fo stoage capacity, but also fo safety and manufactuing cost of the FESS. Since the accuate data of the cost ae not available in cost optimization design, Kack et al. poposed that the cost could be nomalized by the pice of composite mateial [1], []. Yan designed pe unit mass pice of glass fibe as 1 so that othe mateial pice could be calculated by efeing to the pice of glass fibe []. Howeve, when consideing the total manufactuing pocess of a flywheel, it can be found that the cost of a flywheel is also affected by the stuctue and manufactuing pocess. Hence, how to evaluate the cost of a flywheel should be deeply eseached. As the stuctue of the flywheel decides how much kinetic Liping Yang is with Reseach Institute of Enegy Stoage Technology and Application, the Habin Engineeing Univesity, Habin, China (coesponding autho, phone: , fax: , yanglipingylp0@ 16.com). Cuan Cawfod, J., was with Depatment of Mechanical Engineeing, Univesity of Victoia, Victoia, Bitish Columbia, Canada. Zhengyi Ren is with Reseach Institute of Enegy Stoage Technology and Application, the Habin Engineeing Univesity, Habin, China. enegy can be stoed by the whole system, many eseaches used the kinetic enegy as the optimization object to design a flywheel [], [5]. Howeve, too much mass will bing inconvenience to the assembly and tanspotation of the flywheel especially fo the application in mobile machine. Hence, Stoage enegy density (SED) is used as anothe optimization object [6]-[8]. Along with the development of the composite mateial and the magnetic suspended beaing technologies, the cost of flywheel becomes an impotant facto affecting the application of the FESS. Hence, how to obtain big SED and low cost simultaneously is becoming moe and moe impotant. On the othe hand, the safety of a high velocity flywheel is vey impotant. In ode to avoid the failue of the flywheel, Cutiss et al. eseached and deived an equation which expesses the elationship between the stesses and flywheel paametes, such as the oute adii, inne adii, Poisson s atio, imum disk im velocity, adial and cicumfeential elastic modulus, etc. [9]. Kack et al. used the equation of stesses to veify the numeical tess esults, and used as a constaint fo the optimization design to calculate the imum angula velocity [1]. Ha et al. also consideed the stess into the design optimization to calculate the optimum adii unde the condition of the imum angula velocity being fixed [10]. But, all the eseaches did not use the stess equation fo calculating the imum angula velocity and the imum oute adii simultaneously. In this study, a flywheel cost evaluation method is developed. Then, to expess the satisfactoy degees fo diffeent objectives easonably, the FSO method based on fuzzy satisfactoy function and the object weight coefficients is poposed. Moeove, to guaantee the safety of the high velocity flywheel, based on the analysis of the elationship between the imum angula velocity, imum oute adii and stesses, FSO method based on the calculation of stesses is poposed. At last, the compaison of simulation esults fom diffeent optimization design methods shows the effective of the poposed method. II. COST EVALUATION FOR FLYWHEELS The taditional cost is calculated only accoding to the pice of mateials, it is clea that this evaluation method has geat limitations. We know that although being made by same mateial, the flywheels with diffeent stuctue have diffeent costs. It is also obvious that some mateials ae easy to be machined, but some ae not. Hence, we poposed that the cost of a flywheel is influenced not only by the mateial pice, but also by the manufactuing pocess and the mateial machinability. Intenational Scholaly and Scientific Reseach & Innovation 11(8) schola.waset.og/ /

2 Wold Academy of Science, Engineeing and Technology Intenational Jounal of Mateials and Metallugical Engineeing Intenational Science Index, Mateials and Metallugical Engineeing waset.og/publication/ To evaluate the cost moe easonably, the flywheel is divided into m components accoding to the mateial chaacte and the flywheel stuctue. Fo evey component, thee ae some main indicatos being used to evaluate the flywheel cost, such as mateial manufactuability, stuctue chaacte, and mateial pice. Mateial manufactuability indicates that the mateial is easy o not to be fomed and machined. Stuctue chaacte means that the stuctue is easy o not to be manufactued. Theefoe, the evaluation indicato set of the i th (i=1,,,m) component of a flywheel is descibed as follows: ψ i ={f i 1, f i, f i }={mateial manufactuability, stuctue chaacte, mateial pice}. To evaluate the pefomance of each element f i j, the scoe of xij [0,100](i=1,,,m; j=1,,) is given to f i j. The i highe the scoe fo f 1 is, the moe difficulty the mateial manufactuing pocess is. On the othe hand, the highe the scoe fo f i is, the moe complicated the stuctue is. Similaly, the highe the scoe fo f i is, the moe expensive the mateial pice is. Accoding to the expet evaluation, the weight vecto is W ( w1, w, w), wj 1, 0 w j 1. Theefoe, the cost j1 coefficient of the i th (i=1,,,m ) component is: C w x j ij di (1) j1 100 Accoding to the cost coefficient and mass distibution, the flywheel equivalent cost can be calculated as: m D C V( d, h) () di i i i i i1 whee i is the density of the i th component, d i and h i ae the oute diamete and the height of the i th component, Vi( di, h i) is the volume of the i th component, which is the function about d i and h i. III. MULTI-OBJECTIVE OPTIMIZATION BASED ON FSO METHOD High stoage enegy and low cost usually ae the pupose of the flywheel optimization poblem. Moeove, less mass will make the tanspotation moe convenient and will decease the otational inetia which will makes the flywheel otate moe stable. Theefoe, the imum stoage enegy, the cost, and the mass ae the optimization objects of the flywheel. In ode to expess the optimization objects, M ( X ), D ( X ) and ( X ), espectively, ae defined as the imum kinetic enegy, the equivalent cost and the mass of the flywheel. X (, di, hi) ( i=1,,,m) is the decision vecto, whee is the imum angula velocity of the flywheel, d i and h i ae oute diamete and height of the i th component. Accoding to the flywheel woking pinciple, M ( X ), D ( X ), and ( X ) can be epesented as: m M ( X) V ( d, h) () i i i i i1 m D ( X) C V( d, h) () di i i i i i1 1 ( X) J (5) whee J is the otational inetia which is the function of d i and h i. Fo diffeent designes, thei satisfactoy degees fo the objective values ae diffeent. Fo this eason, the fuzzy satisfactoy degee functions ae intoduced. Fo multi-objective optimization poblem in fuzzy envionment, thee ae vaious kinds of membeship functions such as linea, hypebolic, and exponential functions [11]. To simplify the calculation and epesent the desiability of designes, the tiangle-like membeship functions ae used as the fuzzy satisfactoy degee functions fo the flywheel optimization objectives [1]. In ode to adjust the tiangle-like membeship functions easily, a satisfactoy coefficient of (0.5 1) is used to descibe membeship functions. Hence, the satisfactoy degee functions of the optimization objects ae epesented as: 1 M M ( X) ( 1) M M min min ( X ) M M ( X) ( 1) M M (6) min ( 1 ) M M M ( X) M min ( M M ) min 1 D D ( X) ( 1) D D ( X ) D D ( X) ( 1) D D min ( 1 ) D D D ( X) D ( D D ) min min min min (7) Intenational Scholaly and Scientific Reseach & Innovation 11(8) schola.waset.og/ /

3 Wold Academy of Science, Engineeing and Technology Intenational Jounal of Mateials and Metallugical Engineeing E ( X)-E k kmin E E ( X) E ( 1) E kmin k k kmin ( X ) ( - ) E E E k kmin 1 E ( 1 ) E E ( X) E k kmin k k (8) Intenational Science Index, Mateials and Metallugical Engineeing waset.og/publication/ whee M and M min, D and D min, E k and E k min ae uppe and lowe bounds of M ( X ), D ( X ) and ( X ), espectively. As an example, the fuzzy satisfactoy degee function of flywheel mass is shown in Fig. 1. To ealize the multi-objective optimization along with the diffeent significance of the objectives, the weight coefficients of ε (0<ε 1) and γ (0<ε+εγ 1) ae defined. ε is the coefficient of the enegy significance, and γ is the coefficient of the cost significance elative to the enegy. Accodingly, the multi-objective optimization fomulation based on the satisfactoy function is epesented as follows: Maximize: [ E( X ) D ( X)] [1 (1 ) ] M ( X) Subject To: X min X X (1 ) 1 Fig. 1 Fuzzy satisfactoy membeship function of mass IV. STRESS ANALYSIS FOR FLYWHEEL OPTIMIZATION DESIGN Compaed with metal mateial, the composite mateial has the chaacteistics of light weight and high stength, which is the pefeed mateial fo the high velocity flywheel. As the safety of the flywheel is vey impotant, the influence of the composite mateial stess should be fully consideed. Othewise, the flywheel failue will esult in disastous consequences. Since the stesses on the oute ing have the geatest influence on the flywheel safety, the elationship between the stess and the mateial paametes and the size of this component is analyzed. The oute ing is a kind of axisymmetic constant thickness spinning disk, so the adial stess σ and cicumfeential stess σ θ ae epesented as follows [9]: (9) v 1 v / R R / R R 1 1 o i o i 1 v ( e v R i Ro Ro Ri v / R / 1 v / i Ro Ri R o v R i Ro Ro Ri v R o v R R / R R 1 1 o i o i 1 v ( e Ri Ro Ro Ri 1 1 Ri Ro Ri / Ro 1 ) Ri Ro Ro Ri Ro v ) (10) (11) whee is the mateial density, is the Poisson s atio of contaction in adial diection due to cicumfeential θ tension, ve is the imum disk im velocity, Ri and R o ae the disk inne and oute adii, E0 E, E0 and E ae adial elastic moduli, and cicumfeential elastic modulus, ( Ri Ro) is the adius of select point. Defining Ri Ro and x Ro, the σ θ and σ can be deived as: whee v ( cx c x c x ) (1) 1 1 e 1 v ( c x c x c x ) (1) v 1 1 c, c 9 1 c v e 1 v, 9 1, c v. 9 Assume that in and in ae the cicumfeential stess coefficient and adial stess coefficient, espectively. As ve Ro and the stesses should be less than the allowable stesses, fom (1) and (1), the following fomulas ae deived as: Ro [ ]/ in (1) R o [ ]/ in (15) whee Intenational Scholaly and Scientific Reseach & Innovation 11(8) schola.waset.og/ /

4 Wold Academy of Science, Engineeing and Technology Intenational Jounal of Mateials and Metallugical Engineeing Intenational Science Index, Mateials and Metallugical Engineeing waset.og/publication/ in cx c x c x in cx cx cx The imum of in and in can be calculated fo a kind of composite mateial. Theefoe, fo a fixed value of α, the multi-objective optimization fomulation consideing stesses constaints is epesented as follows: Maximize: [ E( X) D ( X)] [1 (1 ) ] M( X) Xmin X X 0 1 (16) Subject To: 0 (1 ) 1 Ro min{ [ ] / in, [ ] / in } R / R = i o whee X min and X ae the minimum value and imum value of X, in and in ae the imum of in and, espectively. in V. COMPARISON OF SIMULATION RESULTS In ode to analyze the pesented multi-objective FSO, a composite mateial flywheel stuctue is designed which is shown in Fig.. Fig. A flywheel stuctue Accoding to the mateial and the stuctue, the flywheel is divided into fou components: shaft, im1, im, and im. The mateial of shaft is steel. The mateial of im1 and im is aluminium alloy. The mateial of im is cabon fibe. Because oute ing of this flywheel is im, thee ae Ri = d /, Ro = d /. The vaiables include diametes of the fou components d, d, d, d (m) and the imum angula velocity (ad/s). 1 Setting =0.5, thee ae X (, d, d, d ) 1. Accoding to the design equiement, thee ae X min (00,0.06, 0.15, 0.6) and X ( 000, 0.08, 0.5, 0.8).Othe stuctue paametes of the flywheel ae h1 0.5 m, h 0.1 m, h h = 0. m. The densities of steel, aluminium alloy and cabon fibe ae 7800 kg/m, 700 kg/ m, and 1780 kg/ m, espectively. Fo mateial manufactuability, the manufactuing pocesses of the steel and aluminium alloy ae obviously diffeent fom the pocess of the cabon fibe. Because the aluminum alloy mateial belongs to the non-feous metal, the hadness is infeio to the steel, and the pocessing difficulty must be smalle than the steel. Due to the high equiement of the winding technology of cabon fibe flywheel, the technology matuity is not as good as the metal manufactuing pocess. Theefoe, the mateial manufactuability scoes of the fou components ae: x 0 11, x 0 1, x 0 1, x 80 1 On the othe hand, the stuctue chaacte of the shaft is elatively complex. It not only equies stict dimensional accuacy, igoous suface oughness, and suface hadness but also equies high shock esistance. On contast, the stuctue chaacte of im1 and im mainly eflects in the complex shape. Additionally, the demands on dimensional accuacy and suface oughness of the inne hole suface of im1 ae moe igoous than the oute cicle suface of im. The im is winded by cabon fibe which has egulaly shape and lowe dimensional accuacy. Hence, the scoe of stuctue chaacte of im is lowest in the scoes of the fou components. Theefoe, the scoe of the stuctue chaacte of the fou components ae: x 90 1, x 50, x 0, x 10 Based on the maket pices of steel, aluminium alloy and cabon fibe, the scoes of the mateial pice ae: x 5, x 1, x 1, x Accoding to the impotance degee, the weight set of the evaluation indicatos is: W= (0., 0., 0.5). The cost coefficient of the i th (i=1,,,m) component is calculated espectively as: C d C d C d Intenational Scholaly and Scientific Reseach & Innovation 11(8) schola.waset.og/ /

5 Wold Academy of Science, Engineeing and Technology Intenational Jounal of Mateials and Metallugical Engineeing Intenational Science Index, Mateials and Metallugical Engineeing waset.og/publication/ C d Accoding to the mass distibution of each component, the equivalent cost of the flywheel is: D (.V 0.59V 0.5V 1.5 V ) 10 1 Accoding to the (), (), (5), the M ( X ), D ( X ) and ( X) can be epesented as follows: 10 ( X ) (.6d1 0.5d 0.8d 0.5 d) 10 D ( X) (1.091d 0.1d 0.d 0. d ) 1 10 M ( X) (.6d 0.5d 0.8d 0.5 d ) 1 Hence, when the β=0.8, the fuzzy satisfactoy degee functions ae as follows: 6 ( X) ( X) E( X) E ( X) D( X) 11.5 ( X) D D( X) D( X) M ( X) 5.6 ( X) M M ( X) M ( X) when β=1, the fuzzy satisfactoy degee functions ae as follows: 6 ( X) E( X). ( X) D ( X) 95. D( X) D( X) M ( X) 1.8 M( X) M( X) The paametes of the cabon fibe ae v =0., E GPa, E 56 GPa, 1780 kg/m [1]. Hence, can be deived as: k E0 E Accoding to (1) and (1), the values of c 1, c, c, and c can be calculated as follows: and c1-0.6, c , c -.085, c 0.6 Hence, using the MATLAB optimization tool box, in ae calculated as: 0.617, inamx in inamx Since the longitudinal and tansvese tensile stengths of cabon fibe ae [ ] =500MPa and [ ] =56MPa [11], we can obtain: in, in [ ]/( ) 1786 [ ] / ( ) 79.5 Theefoe, fom (16) the epesentation of the optimization fomula is ewitten as follows: Maximize: [ E( X) D ( X)] (1 ) M( X) Xmin X X 0 1 Subject To: 0 (1 ) 1 d/ 79.5 d / d =1/ (17) A. Compaison of FSO with Diffeent β, ε and γ To veify the FSO method, the optimum esults of diffeent β, ε, and γ ae listed in Table I. TABLE I THE OPTIMUM RESULTS OF FSO WITH DIFFERENT COEFFICIENTS ε =0.8, γ=0. ε=0., γ=1 ε=0., γ= Indicatos β=0.8 β=1 β=0.8 β=1 β=0.8 β=1 ω (ad/s) d 1 (mm) d (mm) D (mm) E k(mj) D M (kg) μ E μ D μ M In ode to analyze the optimization effect, the values of the object which has the imum weight among the thee objects ae compaed. In the case of ε =0.8 and γ=0., the optimum value of enegy of β=1 is 5.6% highe than the value of β=0.8. In the case of ε =0. and γ=1, the optimum value of mass of β=1 is 18.5% lowe than the value of β=0.8. Moeove, in the case of ε =0. and γ=, the optimum value of cost of β=1 is 15.6% lowe than the value of β=0.8. All these show that when β=1, Intenational Scholaly and Scientific Reseach & Innovation 11(8) schola.waset.og/ /

6 Wold Academy of Science, Engineeing and Technology Intenational Jounal of Mateials and Metallugical Engineeing Intenational Science Index, Mateials and Metallugical Engineeing waset.og/publication/ the design equiements of the satisfaction degee ae moe stingent. On the othe hand, in Table I, when ε=0. and β=1, the optimum esults with diffeent γ ae same. But when ε =0. and β=0.8, the optimum cost of γ=1 is 0.6% bigge than the cost of γ=, and μ D of γ=1 is 0.5% smalle than μ D of γ=. It is obvious that the impotance of cost inceases with the incease of β. B. Compaison of FSO with and without the Stess Constaints When β=1, the optimum esults of FSO with o without the stess constaints ae listed in Table II. Consideing the stess constaints, the values of ωd / unde diffeent ε and γ is smalle than the allowable value of 79.5 ad m/s, as shown in (17). On contast, the optimum esults of ωd / without stess constaints ae all bigge than 79.5 ad m/s. It is obvious that the optimization with the stess constaints can guaantee the safety of the flywheel. TABLE Ⅱ THE OPTIMUM RESULTS WITH OR WITHOUT STRESS CONSTRAINTS Indicatos ε =0.8, γ=0. ε =0.6, γ=0.5 With without with without ω(ad/s) d 1 (mm) d (mm) d (mm) E k(mj) D M (kg) ωd /(ad m/s) C. Simulation Contast of FSO and SEDO In ode to povide futhe insight on the FSO, the optimum esults of FSO of β=1 and SEDO with same constaints ae listed in Table III. Indicatos TABLE Ⅲ THE OPTIMUM RESULTS OF FSO AND SEDO. ε =0.8, γ=0. FSO ε =0.5, γ=0.5 SEDO ω(ad/s) d 1 (mm) d (mm) d (mm) E k(mj) D M (kg) SED(MJ/kg) Fo the optimum E k and M of FSO, the SED of ε =0.8 and γ=0. is 0.08% smalle than that of SEDO. But, on the contay, the SED of ε =0.5 and γ=0.5 is 0.% bigge than that of SEDO. It can be seen that the optimum ESD can be acquied by the FSO method when the values of the weight coefficients ae suitable. VI. CONCLUSION An equivalent cost evaluation method was poposed. To evaluate the cost moe easonably, the flywheel is divided into seveal components accoding to the mateial chaacte and the flywheel stuctue. Fo evey component, mateial manufactuability, stuctue chaacte and mateial pice wee consideed as the main indicatos evaluating the flywheel cost. Based on intoducing the fuzzy satisfactoy degee functions, the enegy coefficient and the cost coefficient, the FSO method was poposed. The tiangle-like membeship functions ae used as the fuzzy satisfactoy degee functions fo the flywheel optimization objectives. A satisfactoy coefficient was used to adjust the tiangle-like membeship functions. On the basis of the stess analysis, the elativity between the oute diamete, imum velocity and the flywheel stesses wee calculated. Using the imum of the cicumfeential stess and adial stess as the constaints, the FSO method consideing the stesses constaints was poposed. To veify the effect of FSO, the FSO methods with diffeent satisfactoy coefficient and weight coefficients wee simulated. The esult analysis demonstated that the FSO could ealize the diffeent design taget. The contast of FSO simulation with/without stess constaint showed that only the calculated adial stess with stess constaint was smalle than the allowance adial stess. Additionally, the contast of SEDO and the FSO indicated that the FSO could each a highe SED when the values of paametes ae suitable. REFERENCES [1] M. Kack, M. Secanell, P. Metiny, Cost Optimization of Hybid Composite Flywheel Rotos fo Enegy Stoage, Stuct Multidisc Optim, vol.1, 010, pp [] M. Kack, M. Secanell, P. Metiny, Cost Optimization of a Hybid Composite Flywheel Roto with a Split-type Hub Using Combined Analytical/numeical Models, Stuct Multidisc Optim, vol., 011, pp [] X. l. Yan, Cost Optimization Design of Hybid Composite Flywheel Roto, Jounal of mechanical engineeing, vol.. n1, 01, pp [] J. Huang, G. Fadel, Heteogeneous Flywheel Modeling and Optimization, Mateials and Design, vol.1. n, 000, pp [5] D. Kzyszt, T. Jan, Two Methods fo Optimization of Flywheel, Engineeing Optimization, vol.1. n, 009, pp [6] S. Ha, H. Jeong, Y. Cho, Optimum Design of Thick-walled Composite Rings fo an Enegy Stoage System, Jounal of Composite Mateials, vol.. n9, 1998, pp [7] S. K. Ha, J. H. Kim, Y. H. Han, Design of a hybid composite flywheel multi-im oto system using geometic scaling factos, Compos Mate, vol.. n8, 008, pp [8] J. D. Kwon, S. J. Kim, S. U. Nasi, S. K. Ha, Design and Fabication of Hybid Composite Flywheel Roto, Wold Academy of Science, Engineeing and Technology, vol.60, 011, pp [9] D. H. Cutiss, P P Mongeau, R L Putebaugh, Advanced Composite Flywheel Stuctual Design fo a Pulsed Disk Altenato, IEEE Tansactions On Magnetics, vol.1. n1, 1995, pp [10] S.K. Ha, S. J. Kim, S. U. Nasi, S. C. Han. Design optimization and fabication of a hybid composite flywheel oto, composite stuctue, vol.9, 01, pp [11] M. Sakawa, K. Kosuke, K. Hideki, An Inteactive Fuzzy Satisficing Method fo Multiobjective Linea Pogamming Poblems with Random Vaiable Coefficients Though a Pobability Maximization Model, Fuzzy Sets and Systems, vol.16, 00, pp [1] R. N. Tiwai, S. Dhama, J. R. Rao, Fuzzy Goal Pogamming-An Additive Model, Fuzzy Sets and Systems, vol., 1987, pp. 7-. [1] S. K. Ha, H. I. Yang, D. J. Kim, Optimal Design of a Hybid Composite Flywheel with a Pemanent Magnet Roto, Jounal of Composite Mateials, vol.. n16, 1999, pp Intenational Scholaly and Scientific Reseach & Innovation 11(8) schola.waset.og/ /

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

Appraisal of Logistics Enterprise Competitiveness on the Basis of Fuzzy Analysis Algorithm

Appraisal of Logistics Enterprise Competitiveness on the Basis of Fuzzy Analysis Algorithm Appaisal of Logistics Entepise Competitiveness on the Basis of Fuzzy Analysis Algoithm Yan Zhao, Fengge Yao, Minming She Habin Univesity of Commece, Habin, Heilongjiang 150028, China, zhaoyan2000@yahoo.com.cn

More information

Materials selection The materials index

Materials selection The materials index MME445: Lectue 20 Mateials selection The mateials index A. K. M. B. Rashid Pofesso, Depatment of MME BUET, Dhaka Leaning Objectives Knowledge & Undestanding Elementay knowledge of how to expess design

More information

ELASTIC ANALYSIS OF CIRCULAR SANDWICH PLATES WITH FGM FACE-SHEETS

ELASTIC ANALYSIS OF CIRCULAR SANDWICH PLATES WITH FGM FACE-SHEETS THE 9 TH INTERNATIONAL CONFERENCE ON COMPOSITE MATERIALS ELASTIC ANALYSIS OF CIRCULAR SANDWICH PLATES WITH FGM FACE-SHEETS R. Sbulati *, S. R. Atashipou Depatment of Civil, Chemical and Envionmental Engineeing,

More information

COMPUTATIONS OF ELECTROMAGNETIC FIELDS RADIATED FROM COMPLEX LIGHTNING CHANNELS

COMPUTATIONS OF ELECTROMAGNETIC FIELDS RADIATED FROM COMPLEX LIGHTNING CHANNELS Pogess In Electomagnetics Reseach, PIER 73, 93 105, 2007 COMPUTATIONS OF ELECTROMAGNETIC FIELDS RADIATED FROM COMPLEX LIGHTNING CHANNELS T.-X. Song, Y.-H. Liu, and J.-M. Xiong School of Mechanical Engineeing

More information

Safety variations in steel designed using Eurocode 3

Safety variations in steel designed using Eurocode 3 JCSS Wokshop on eliability Based Code Calibation Safety vaiations in steel designed using Euocode 3 Mike Byfield Canfield Univesity Swindon, SN6 8LA, UK David Nethecot Impeial College London SW7 2BU, UK

More information

Levitation force analysis of ring and disk shaped permanent magnet-high temperature superconductor

Levitation force analysis of ring and disk shaped permanent magnet-high temperature superconductor Inn Jounal of Pue & Applied Physics Vol. 55, Apil 017, pp. 61-68 Levitation foce analysis of ing and disk shaped pemanent magnet-high tempeatue supeconducto Sinan Basaan & Selim Sivioglu* Depatment of

More information

A NEW VARIABLE STIFFNESS SPRING USING A PRESTRESSED MECHANISM

A NEW VARIABLE STIFFNESS SPRING USING A PRESTRESSED MECHANISM Poceedings of the ASME 2010 Intenational Design Engineeing Technical Confeences & Computes and Infomation in Engineeing Confeence IDETC/CIE 2010 August 15-18, 2010, Monteal, Quebec, Canada DETC2010-28496

More information

Analysis of high speed machining center spindle dynamic unit structure performance Yuan guowei

Analysis of high speed machining center spindle dynamic unit structure performance Yuan guowei Intenational Confeence on Intelligent Systems Reseach and Mechatonics Engineeing (ISRME 0) Analysis of high speed machining cente spindle dynamic unit stuctue pefomance Yuan guowei Liaoning jidian polytechnic,dan

More information

Duality between Statical and Kinematical Engineering Systems

Duality between Statical and Kinematical Engineering Systems Pape 00, Civil-Comp Ltd., Stiling, Scotland Poceedings of the Sixth Intenational Confeence on Computational Stuctues Technology, B.H.V. Topping and Z. Bittna (Editos), Civil-Comp Pess, Stiling, Scotland.

More information

MAGNETIC FIELD AROUND TWO SEPARATED MAGNETIZING COILS

MAGNETIC FIELD AROUND TWO SEPARATED MAGNETIZING COILS The 8 th Intenational Confeence of the Slovenian Society fo Non-Destuctive Testing»pplication of Contempoay Non-Destuctive Testing in Engineeing«Septembe 1-3, 5, Potoož, Slovenia, pp. 17-1 MGNETIC FIELD

More information

A Three-Dimensional Magnetic Force Solution Between Axially-Polarized Permanent-Magnet Cylinders for Different Magnetic Arrangements

A Three-Dimensional Magnetic Force Solution Between Axially-Polarized Permanent-Magnet Cylinders for Different Magnetic Arrangements Poceedings of the 213 Intenational Confeence on echanics, Fluids, Heat, Elasticity Electomagnetic Fields A Thee-Dimensional agnetic Foce Solution Between Axially-Polaied Pemanent-agnet Cylindes fo Diffeent

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

THE INFLUENCE OF THE MAGNETIC NON-LINEARITY ON THE MAGNETOSTATIC SHIELDS DESIGN

THE INFLUENCE OF THE MAGNETIC NON-LINEARITY ON THE MAGNETOSTATIC SHIELDS DESIGN THE INFLUENCE OF THE MAGNETIC NON-LINEARITY ON THE MAGNETOSTATIC SHIELDS DESIGN LIVIU NEAMŢ 1, ALINA NEAMŢ, MIRCEA HORGOŞ 1 Key wods: Magnetostatic shields, Magnetic non-lineaity, Finite element method.

More information

Long-range stress re-distribution resulting from damage in heterogeneous media

Long-range stress re-distribution resulting from damage in heterogeneous media Long-ange stess e-distibution esulting fom damage in heteogeneous media Y.L.Bai (1), F.J.Ke (1,2), M.F.Xia (1,3) X.H.Zhang (1) and Z.K. Jia (1) (1) State Key Laboatoy fo Non-linea Mechanics (LNM), Institute

More information

A scaling-up methodology for co-rotating twin-screw extruders

A scaling-up methodology for co-rotating twin-screw extruders A scaling-up methodology fo co-otating twin-scew extudes A. Gaspa-Cunha, J. A. Covas Institute fo Polymes and Composites/I3N, Univesity of Minho, Guimaães 4800-058, Potugal Abstact. Scaling-up of co-otating

More information

Web-based Supplementary Materials for. Controlling False Discoveries in Multidimensional Directional Decisions, with

Web-based Supplementary Materials for. Controlling False Discoveries in Multidimensional Directional Decisions, with Web-based Supplementay Mateials fo Contolling False Discoveies in Multidimensional Diectional Decisions, with Applications to Gene Expession Data on Odeed Categoies Wenge Guo Biostatistics Banch, National

More information

SIMULAITION AND ANALYSIS OF PROCESS-INDUCED DISTORTIONS FOR COMPOSITE STRUCTURES

SIMULAITION AND ANALYSIS OF PROCESS-INDUCED DISTORTIONS FOR COMPOSITE STRUCTURES 21 st Intenational Confeence on Composite Mateials Xi an, 20-25 th August 2017 SIMULAITION AND ANALYSIS OF PROCESS-INDUCED DISTORTIONS FOR COMPOSITE STRUCTURES LIU Kai *1, ZHANG Boming 1, YE Jinui 1, Tang

More information

Shape optimization of a flywheel

Shape optimization of a flywheel Stuct Multidisc Optim 19, 74 81 Spinge-Velag 000 Shape optimization of a flywheel G.R. Kess Abstact This pape deals with finding the best thickness distibution along the adius of a centally boed flywheel

More information

Liquid gas interface under hydrostatic pressure

Liquid gas interface under hydrostatic pressure Advances in Fluid Mechanics IX 5 Liquid gas inteface unde hydostatic pessue A. Gajewski Bialystok Univesity of Technology, Faculty of Civil Engineeing and Envionmental Engineeing, Depatment of Heat Engineeing,

More information

Rotor Blade Performance Analysis with Blade Element Momentum Theory

Rotor Blade Performance Analysis with Blade Element Momentum Theory Available online at www.sciencediect.com ScienceDiect Enegy Pocedia 5 (7 ) 3 9 The 8 th Intenational Confeence on Applied Enegy ICAE6 Roto Blade Pefomance Analysis with Blade Element Momentum Theoy Faisal

More information

2 Governing Equations

2 Governing Equations 2 Govening Equations This chapte develops the govening equations of motion fo a homogeneous isotopic elastic solid, using the linea thee-dimensional theoy of elasticity in cylindical coodinates. At fist,

More information

Chapter Introduction to Finite Element Methods

Chapter Introduction to Finite Element Methods Chapte 1.4 Intoduction to Finite Element Methods Afte eading this chapte, you should e ale to: 1. Undestand the asics of finite element methods using a one-dimensional polem. In the last fifty yeas, the

More information

General Railgun Function

General Railgun Function Geneal ailgun Function An electomagnetic ail gun uses a lage Loentz foce to fie a pojectile. The classic configuation uses two conducting ails with amatue that fits between and closes the cicuit between

More information

Coupled Electromagnetic and Heat Transfer Simulations for RF Applicator Design for Efficient Heating of Materials

Coupled Electromagnetic and Heat Transfer Simulations for RF Applicator Design for Efficient Heating of Materials Coupled Electomagnetic and Heat Tansfe Simulations fo RF Applicato Design fo Efficient Heating of Mateials Jeni Anto 1 and Raj C Thiagaajan 2 * 1 Reseache, Anna Univesity, Chennai, 2 ATOA Scientific Technologies

More information

An Application of Fuzzy Linear System of Equations in Economic Sciences

An Application of Fuzzy Linear System of Equations in Economic Sciences Austalian Jounal of Basic and Applied Sciences, 5(7): 7-14, 2011 ISSN 1991-8178 An Application of Fuzzy Linea System of Equations in Economic Sciences 1 S.H. Nassei, 2 M. Abdi and 3 B. Khabii 1 Depatment

More information

Computational Methods of Solid Mechanics. Project report

Computational Methods of Solid Mechanics. Project report Computational Methods of Solid Mechanics Poject epot Due on Dec. 6, 25 Pof. Allan F. Bowe Weilin Deng Simulation of adhesive contact with molecula potential Poject desciption In the poject, we will investigate

More information

EFFECTS OF GFRP REINFORCING REBARS ON SHRINKAGE AND THERMAL STRESSES IN CONCRETE

EFFECTS OF GFRP REINFORCING REBARS ON SHRINKAGE AND THERMAL STRESSES IN CONCRETE EFFECTS OF GFRP REINFORCING REBARS ON SHRINKAGE AND THERMAL STRESSES IN CONCRETE Roge H. L. Chen 1 and Jeong-Hoon Choi 2 ABSTRACT The use of Glass Fibe Reinfoced Polyme (GFRP) ebas instead of conventional

More information

Reliability analysis examples

Reliability analysis examples Reliability analysis examples Engineeing Risk Analysis Goup, Technische Univesität München. Acisst., 80 Munich, Gemany. May 8, 08 Intoduction In the context of eliability analysis and ae event estimation,

More information

Magneto-Elastic Analysis of an Annular FGM Plate Based on Classical Plate Theory Using GDQ Method

Magneto-Elastic Analysis of an Annular FGM Plate Based on Classical Plate Theory Using GDQ Method 736 Magneto-Elastic Analysis of an Annula FGM Plate Based on Classical Plate Theoy Using GDQ Method Abstact Using GDQ method, the adial and cicumfeential stesses in an annula FGM plate with a unifom thickness

More information

Chapter 7-8 Rotational Motion

Chapter 7-8 Rotational Motion Chapte 7-8 Rotational Motion What is a Rigid Body? Rotational Kinematics Angula Velocity ω and Acceleation α Unifom Rotational Motion: Kinematics Unifom Cicula Motion: Kinematics and Dynamics The Toque,

More information

Solution of a Spherically Symmetric Static Problem of General Relativity for an Elastic Solid Sphere

Solution of a Spherically Symmetric Static Problem of General Relativity for an Elastic Solid Sphere Applied Physics eseach; Vol. 9, No. 6; 7 ISSN 96-969 E-ISSN 96-9647 Published by Canadian Cente of Science and Education Solution of a Spheically Symmetic Static Poblem of Geneal elativity fo an Elastic

More information

CHALLENGES IN THE DESIGN OF HIGH ENERGY STORAGE FLYWHEELS MADE OF COMPOSITE MATERIAL

CHALLENGES IN THE DESIGN OF HIGH ENERGY STORAGE FLYWHEELS MADE OF COMPOSITE MATERIAL 8 TH INTERNATIONAL CONFERENCE ON COMPOSITE MATERIALS CHALLENGES IN THE DESIGN OF HIGH ENERGY STORAGE V.Antonelli, P. He *, H. Baie Institute of Ligtweigt Stuctues, Tecnisce Univesität Müncen, Munic, Gemany

More information

Identification of the degradation of railway ballast under a concrete sleeper

Identification of the degradation of railway ballast under a concrete sleeper Identification of the degadation of ailway ballast unde a concete sleepe Qin Hu 1) and Heung Fai Lam ) 1), ) Depatment of Civil and Achitectual Engineeing, City Univesity of Hong Kong, Hong Kong SAR, China.

More information

International Journal of Mathematical Archive-3(12), 2012, Available online through ISSN

International Journal of Mathematical Archive-3(12), 2012, Available online through  ISSN Intenational Jounal of Mathematical Achive-3(), 0, 480-4805 Available online though www.ijma.info ISSN 9 504 STATISTICAL QUALITY CONTROL OF MULTI-ITEM EOQ MOEL WITH VARYING LEAING TIME VIA LAGRANGE METHO

More information

Kunming, , R.P. China. Kunming, , R.P. China. *Corresponding author: Jianing He

Kunming, , R.P. China. Kunming, , R.P. China. *Corresponding author: Jianing He Applied Mechanics and Mateials Online: 2014-04-28 ISSN: 1662-7482, Vol. 540, pp 92-95 doi:10.4028/www.scientific.net/amm.540.92 2014 Tans Tech Publications, Switzeland Reseach on Involute Gea Undecutting

More information

Physics 2A Chapter 10 - Moment of Inertia Fall 2018

Physics 2A Chapter 10 - Moment of Inertia Fall 2018 Physics Chapte 0 - oment of netia Fall 08 The moment of inetia of a otating object is a measue of its otational inetia in the same way that the mass of an object is a measue of its inetia fo linea motion.

More information

Pearson s Chi-Square Test Modifications for Comparison of Unweighted and Weighted Histograms and Two Weighted Histograms

Pearson s Chi-Square Test Modifications for Comparison of Unweighted and Weighted Histograms and Two Weighted Histograms Peason s Chi-Squae Test Modifications fo Compaison of Unweighted and Weighted Histogams and Two Weighted Histogams Univesity of Akueyi, Bogi, v/noduslód, IS-6 Akueyi, Iceland E-mail: nikolai@unak.is Two

More information

EVOLUTIONARY COMPUTING FOR METALS PROPERTIES MODELLING

EVOLUTIONARY COMPUTING FOR METALS PROPERTIES MODELLING EVOLUTIONARY COMPUTING FOR METALS PROPERTIES MODELLING M.F. Abbod*, M. Mahfouf, D.A. Linkens and Sellas, C.M. IMMPETUS Institute fo Micostuctue and Mechanical Popeties Engineeing, The Univesity of Sheffield

More information

Implicit Constraint Enforcement for Rigid Body Dynamic Simulation

Implicit Constraint Enforcement for Rigid Body Dynamic Simulation Implicit Constaint Enfocement fo Rigid Body Dynamic Simulation Min Hong 1, Samuel Welch, John app, and Min-Hyung Choi 3 1 Division of Compute Science and Engineeing, Soonchunhyang Univesity, 646 Eupnae-i

More information

THE INFLUENCE OF TEMPERATURE S CHANGE ALONG THE RADIUS ON THE MEMBRANE STRESSES FIELD AT ROTATING DISKS

THE INFLUENCE OF TEMPERATURE S CHANGE ALONG THE RADIUS ON THE MEMBRANE STRESSES FIELD AT ROTATING DISKS 6 th Intenational Confeence Computational Mechanics and Vitual Engineeing COMEC 015 15-16 Octobe 015, Başov, Romania HE INFLUENCE OF EMPERAURE S CHANGE ALONG HE RADIUS ON HE MEMBRANE SRESSES FIELD A ROAING

More information

DESIGN OF INTERMEDIATE RING STIFFENERS FOR COLUMN-SUPPORTED CYLINDRICAL STEEL SHELLS

DESIGN OF INTERMEDIATE RING STIFFENERS FOR COLUMN-SUPPORTED CYLINDRICAL STEEL SHELLS DESIGN OF INTERMEDIATE RING STIFFENERS FOR COLUMN-SUPPORTED CYLINDRICAL STEEL SHELLS Öze Zeybek Reseach Assistant Depatment of Civil Engineeing, Middle East Technical Univesity, Ankaa, Tukey E-mail: ozeybek@metu.edu.t

More information

APPLICATION OF MAC IN THE FREQUENCY DOMAIN

APPLICATION OF MAC IN THE FREQUENCY DOMAIN PPLICION OF MC IN HE FREQUENCY DOMIN D. Fotsch and D. J. Ewins Dynamics Section, Mechanical Engineeing Depatment Impeial College of Science, echnology and Medicine London SW7 2B, United Kingdom BSRC he

More information

Steady State and Transient Performance Analysis of Three Phase Induction Machine using MATLAB Simulations

Steady State and Transient Performance Analysis of Three Phase Induction Machine using MATLAB Simulations Intenational Jounal of Recent Tends in Engineeing, Vol, No., May 9 Steady State and Tansient Pefomance Analysis of Thee Phase Induction Machine using MATAB Simulations Pof. Himanshu K. Patel Assistant

More information

Surveillance Points in High Dimensional Spaces

Surveillance Points in High Dimensional Spaces Société de Calcul Mathématique SA Tools fo decision help since 995 Suveillance Points in High Dimensional Spaces by Benad Beauzamy Januay 06 Abstact Let us conside any compute softwae, elying upon a lage

More information

R dt 2. INDIRECT FIELD ORIENTED CONTROL OF INDUCTION MOTOR

R dt 2. INDIRECT FIELD ORIENTED CONTROL OF INDUCTION MOTOR Indiect Field Oiented Contol of Induction Moto Using Fuzzy Logic Aun Kuma R PG Schola, PED, SELECT, VIT Univesity, Chennai Campus aunkumalmc@gmail.com Abstact: This pape pesents a fuzzy logic based speed

More information

Computers and Mathematics with Applications

Computers and Mathematics with Applications Computes and Mathematics with Applications 58 (009) 9 7 Contents lists available at ScienceDiect Computes and Mathematics with Applications jounal homepage: www.elsevie.com/locate/camwa Bi-citeia single

More information

High precision computer simulation of cyclotrons KARAMYSHEVA T., AMIRKHANOV I. MALININ V., POPOV D.

High precision computer simulation of cyclotrons KARAMYSHEVA T., AMIRKHANOV I. MALININ V., POPOV D. High pecision compute simulation of cyclotons KARAMYSHEVA T., AMIRKHANOV I. MALININ V., POPOV D. Abstact Effective and accuate compute simulations ae highly impotant in acceleatos design and poduction.

More information

Title. Author(s)Y. IMAI; T. TSUJII; S. MOROOKA; K. NOMURA. Issue Date Doc URL. Type. Note. File Information

Title. Author(s)Y. IMAI; T. TSUJII; S. MOROOKA; K. NOMURA. Issue Date Doc URL. Type. Note. File Information Title CALCULATION FORULAS OF DESIGN BENDING OENTS ON TH APPLICATION OF THE SAFETY-ARGIN FRO RC STANDARD TO Autho(s)Y. IAI; T. TSUJII; S. OROOKA; K. NOURA Issue Date 013-09-1 Doc URL http://hdl.handle.net/115/538

More information

ASTR415: Problem Set #6

ASTR415: Problem Set #6 ASTR45: Poblem Set #6 Cuan D. Muhlbege Univesity of Mayland (Dated: May 7, 27) Using existing implementations of the leapfog and Runge-Kutta methods fo solving coupled odinay diffeential equations, seveal

More information

The Substring Search Problem

The Substring Search Problem The Substing Seach Poblem One algoithm which is used in a vaiety of applications is the family of substing seach algoithms. These algoithms allow a use to detemine if, given two chaacte stings, one is

More information

Absorption Rate into a Small Sphere for a Diffusing Particle Confined in a Large Sphere

Absorption Rate into a Small Sphere for a Diffusing Particle Confined in a Large Sphere Applied Mathematics, 06, 7, 709-70 Published Online Apil 06 in SciRes. http://www.scip.og/jounal/am http://dx.doi.og/0.46/am.06.77065 Absoption Rate into a Small Sphee fo a Diffusing Paticle Confined in

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

Rotational Motion. Every quantity that we have studied with translational motion has a rotational counterpart

Rotational Motion. Every quantity that we have studied with translational motion has a rotational counterpart Rotational Motion & Angula Momentum Rotational Motion Evey quantity that we have studied with tanslational motion has a otational countepat TRANSLATIONAL ROTATIONAL Displacement x Angula Position Velocity

More information

COUPLED MODELS OF ROLLING, SLIDING AND WHIRLING FRICTION

COUPLED MODELS OF ROLLING, SLIDING AND WHIRLING FRICTION ENOC 008 Saint Petesbug Russia June 30-July 4 008 COUPLED MODELS OF ROLLING SLIDING AND WHIRLING FRICTION Alexey Kieenkov Ins ti tu te fo P ob le ms in Me ch an ic s Ru ss ia n Ac ad em y of Sc ie nc es

More information

Designing a Sine-Coil for Measurement of Plasma Displacements in IR-T1 Tokamak

Designing a Sine-Coil for Measurement of Plasma Displacements in IR-T1 Tokamak Designing a Sine-Coil fo Measuement of Plasma Displacements in IR-T Tokamak Pejman Khoshid, M. Razavi, M. Ghoanneviss, M. Molaii, A. TalebiTahe, R. Avin, S. Mohammadi and A. NikMohammadi Dept. of Physics,

More information

Research Article EXPERIMENTAL STUDY OF HEAT TRANSFER CHARACTERISTICS OF STAINLESS STEEL FIBROUS FLOW INSULATOR

Research Article EXPERIMENTAL STUDY OF HEAT TRANSFER CHARACTERISTICS OF STAINLESS STEEL FIBROUS FLOW INSULATOR Tansactions of the TSME (16) Vol. 4, No. 2, 148 155 Jounal of seach and Applications in Mechanical Engineeing Copyight 16 by TSME ISSN 2229-2152 pint DOI: 1.14456/jame.16.15 seach Aticle EXPERIMENTAL STUDY

More information

A Comparative Study of Exponential Time between Events Charts

A Comparative Study of Exponential Time between Events Charts Quality Technology & Quantitative Management Vol. 3, No. 3, pp. 347-359, 26 QTQM ICAQM 26 A Compaative Study of Exponential Time between Events Chats J. Y. Liu 1, M. Xie 1, T. N. Goh 1 and P. R. Shama

More information

Electrodynamic Forces in Steel Strip during Induction Heating

Electrodynamic Forces in Steel Strip during Induction Heating Intenational Scientific Colloquium Modelling fo Electomagnetic Pocessing Hannove, Mach 4-6, 3 Electodynamic Foces in Steel Stip duing Induction Heating H. Kasjanow, H. Schülbe,. Nikanoov bstact Tangential

More information

COLD STRANGLING HOLLOW PARTS FORCES CALCULATION OF CONICAL AND CONICAL WITH CYLINDRICAL COLLAR

COLD STRANGLING HOLLOW PARTS FORCES CALCULATION OF CONICAL AND CONICAL WITH CYLINDRICAL COLLAR COLD STANGLING HOLLOW PATS OCES CALCULATION O CONICAL AND CONICAL WITH CYLINDICAL COLLA Lucian V. Sevein, Taian Lucian Sevein,, Stefan cel Mae Univesity of Suceava, aculty of Mechanical Engineeing, Mechatonics

More information

Swissmetro: design methods for ironless linear transformer

Swissmetro: design methods for ironless linear transformer Swissmeto: design methods fo ionless linea tansfome Nicolas Macabey GESTE Engineeing SA Scientific Pak PSE-C, CH-05 Lausanne, Switzeland Tel (+4) 2 693 83 60, Fax. (+4) 2 693 83 6, nicolas.macabey@geste.ch

More information

Three-dimensional Quantum Cellular Neural Network and Its Application to Image Processing *

Three-dimensional Quantum Cellular Neural Network and Its Application to Image Processing * Thee-dimensional Quantum Cellula Neual Netwok and Its Application to Image Pocessing * Sen Wang, Li Cai, Huanqing Cui, Chaowen Feng, Xiaokuo Yang Science College, Ai Foce Engineeing Univesity Xi an 701,

More information

MODULE 5 ADVANCED MECHANICS GRAVITATIONAL FIELD: MOTION OF PLANETS AND SATELLITES VISUAL PHYSICS ONLINE

MODULE 5 ADVANCED MECHANICS GRAVITATIONAL FIELD: MOTION OF PLANETS AND SATELLITES VISUAL PHYSICS ONLINE VISUAL PHYSICS ONLIN MODUL 5 ADVANCD MCHANICS GRAVITATIONAL FILD: MOTION OF PLANTS AND SATLLITS SATLLITS: Obital motion of object of mass m about a massive object of mass M (m

More information

Fuzzy Adaptive Neural-Network Model-Following Speed Control for PMSM Drives

Fuzzy Adaptive Neural-Network Model-Following Speed Control for PMSM Drives Fuzzy Adaptive Neual-Netwok Model-Following Speed Contol fo PMSM Dives FAYEZ F. M. EL-SOUSY MAGED N. F. NASHED Powe Electonics & Enegy Convesion Depatment Electonics Reseach Institute (ERI) Al-Tahi Steet,

More information

Chem 453/544 Fall /08/03. Exam #1 Solutions

Chem 453/544 Fall /08/03. Exam #1 Solutions Chem 453/544 Fall 3 /8/3 Exam # Solutions. ( points) Use the genealized compessibility diagam povided on the last page to estimate ove what ange of pessues A at oom tempeatue confoms to the ideal gas law

More information

Molecular dynamics simulation of ultrafast laser ablation of fused silica

Molecular dynamics simulation of ultrafast laser ablation of fused silica IOP Publishing Jounal of Physics: Confeence Seies 59 (27) 1 14 doi:1.188/1742-6596/59/1/22 Eighth Intenational Confeence on Lase Ablation Molecula dynamics simulation of ultafast lase ablation of fused

More information

B. Spherical Wave Propagation

B. Spherical Wave Propagation 11/8/007 Spheical Wave Popagation notes 1/1 B. Spheical Wave Popagation Evey antenna launches a spheical wave, thus its powe density educes as a function of 1, whee is the distance fom the antenna. We

More information

A dual-reciprocity boundary element method for axisymmetric thermoelastodynamic deformations in functionally graded solids

A dual-reciprocity boundary element method for axisymmetric thermoelastodynamic deformations in functionally graded solids APCOM & ISCM 11-14 th Decembe, 013, Singapoe A dual-ecipocity bounday element method fo axisymmetic themoelastodynamic defomations in functionally gaded solids *W. T. Ang and B. I. Yun Division of Engineeing

More information

School of Electrical and Computer Engineering, Cornell University. ECE 303: Electromagnetic Fields and Waves. Fall 2007

School of Electrical and Computer Engineering, Cornell University. ECE 303: Electromagnetic Fields and Waves. Fall 2007 School of Electical and Compute Engineeing, Conell Univesity ECE 303: Electomagnetic Fields and Waves Fall 007 Homewok 8 Due on Oct. 19, 007 by 5:00 PM Reading Assignments: i) Review the lectue notes.

More information

Determining solar characteristics using planetary data

Determining solar characteristics using planetary data Detemining sola chaacteistics using planetay data Intoduction The Sun is a G-type main sequence sta at the cente of the Sola System aound which the planets, including ou Eath, obit. In this investigation

More information

Field emission of Electrons from Negatively Charged Cylindrical Particles with Nonlinear Screening in a Dusty Plasma

Field emission of Electrons from Negatively Charged Cylindrical Particles with Nonlinear Screening in a Dusty Plasma Reseach & Reviews: Jounal of Pue and Applied Physics Field emission of Electons fom Negatively Chaged Cylindical Paticles with Nonlinea Sceening in a Dusty Plasma Gyan Pakash* Amity School of Engineeing

More information

A HYBRID DEA/AHP MODEL OF R&D PROJECT SELECTION CONSIDERING ORDINAL EVALUATION FACTORS

A HYBRID DEA/AHP MODEL OF R&D PROJECT SELECTION CONSIDERING ORDINAL EVALUATION FACTORS A HYBRID DA/AHP MDL F R&D PRJCT SLCTIN CNSIDRING RDINAL VALUATIN FACTRS Deok-Joo Lee College of Advanced ngineeing, Kyunghee Univesity, ldj@khu.ac.k Sungsik Bae Depatment of Industial ngineeing, Seoul

More information

Stiff, strong zero thermal expansion lattices via the Poisson effect

Stiff, strong zero thermal expansion lattices via the Poisson effect Stiff, stong zeo themal expansion lattices via the Poisson effect Jeemy Lehman Depatment of Engineeing Physics, Engineeing Mechanics Pogam, Univesity of Wisconsin Madison, Madison, Wisconsin 53706-1687

More information

CHAPTER 25 ELECTRIC POTENTIAL

CHAPTER 25 ELECTRIC POTENTIAL CHPTE 5 ELECTIC POTENTIL Potential Diffeence and Electic Potential Conside a chaged paticle of chage in a egion of an electic field E. This filed exets an electic foce on the paticle given by F=E. When

More information

Analytical Solutions for Confined Aquifers with non constant Pumping using Computer Algebra

Analytical Solutions for Confined Aquifers with non constant Pumping using Computer Algebra Poceedings of the 006 IASME/SEAS Int. Conf. on ate Resouces, Hydaulics & Hydology, Chalkida, Geece, May -3, 006 (pp7-) Analytical Solutions fo Confined Aquifes with non constant Pumping using Compute Algeba

More information

J. Electrical Systems 1-3 (2005): Regular paper

J. Electrical Systems 1-3 (2005): Regular paper K. Saii D. Rahem S. Saii A Miaoui Regula pape Coupled Analytical-Finite Element Methods fo Linea Electomagnetic Actuato Analysis JES Jounal of Electical Systems In this pape, a linea electomagnetic actuato

More information

ON THE TWO-BODY PROBLEM IN QUANTUM MECHANICS

ON THE TWO-BODY PROBLEM IN QUANTUM MECHANICS ON THE TWO-BODY PROBLEM IN QUANTUM MECHANICS L. MICU Hoia Hulubei National Institute fo Physics and Nuclea Engineeing, P.O. Box MG-6, RO-0775 Buchaest-Maguele, Romania, E-mail: lmicu@theoy.nipne.o (Received

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

Chapter 13 Gravitation

Chapter 13 Gravitation Chapte 13 Gavitation In this chapte we will exploe the following topics: -Newton s law of gavitation, which descibes the attactive foce between two point masses and its application to extended objects

More information

arxiv: v1 [physics.pop-ph] 3 Jun 2013

arxiv: v1 [physics.pop-ph] 3 Jun 2013 A note on the electostatic enegy of two point chages axiv:1306.0401v1 [physics.pop-ph] 3 Jun 013 A C Tot Instituto de Física Univesidade Fedeal do io de Janeio Caixa Postal 68.58; CEP 1941-97 io de Janeio,

More information

Solving Problems of Advance of Mercury s Perihelion and Deflection of. Photon Around the Sun with New Newton s Formula of Gravity

Solving Problems of Advance of Mercury s Perihelion and Deflection of. Photon Around the Sun with New Newton s Formula of Gravity Solving Poblems of Advance of Mecuy s Peihelion and Deflection of Photon Aound the Sun with New Newton s Fomula of Gavity Fu Yuhua (CNOOC Reseach Institute, E-mail:fuyh945@sina.com) Abstact: Accoding to

More information

Conservative Averaging Method and its Application for One Heat Conduction Problem

Conservative Averaging Method and its Application for One Heat Conduction Problem Poceedings of the 4th WSEAS Int. Conf. on HEAT TRANSFER THERMAL ENGINEERING and ENVIRONMENT Elounda Geece August - 6 (pp6-) Consevative Aveaging Method and its Application fo One Heat Conduction Poblem

More information

Ultrafast effects in 3D Metamaterials

Ultrafast effects in 3D Metamaterials Ultafast effects in 3D Metamateials Nkoni Katte,2 and Philip G.Evans 3 Electical Engineeing Wilbefoce Univesity, 2 Sensos Laboatoy Wight State Univesity and 3 Oak idge National Laboatoy *Coesponding autho:

More information

Aalborg Universitet. Load Estimation from Natural input Modal Analysis Aenlle, Manuel López; Brincker, Rune; Canteli, Alfonso Fernández

Aalborg Universitet. Load Estimation from Natural input Modal Analysis Aenlle, Manuel López; Brincker, Rune; Canteli, Alfonso Fernández Aalbog Univesitet Load Estimation fom atual input Modal Analysis Aenlle, Manuel López; Bincke, Rune; Canteli, Alfonso Fenández Published in: Confeence Poceedings Publication date: 005 Document Vesion Publishe's

More information

Calculation of Temperature Rise in Dry-type Air-core Reactors Using Strong Coupling of Fluid-Temperature Field

Calculation of Temperature Rise in Dry-type Air-core Reactors Using Strong Coupling of Fluid-Temperature Field Reseach Jounal of Applied Sciences, Engineeing and Technology 5(10: 941-945, 013 ISSN: 040-7459; e-issn: 040-7467 Maxwell Scientific Oganization, 013 Submitted: Septembe 15, 01 Accepted: Octobe 4, 01 Published:

More information

Recent Advances in Chemical Engineering, Biochemistry and Computational Chemistry

Recent Advances in Chemical Engineering, Biochemistry and Computational Chemistry Themal Conductivity of Oganic Liquids: a New Equation DI NICOLA GIOVANNI*, CIARROCCHI ELEONORA, PIERANTOZZI ARIANO, STRYJEK ROAN 1 DIIS, Univesità Politecnica delle ache, 60131 Ancona, ITALY *coesponding

More information

IOP Conference Series: Materials Science and Engineering. Related content PAPER OPEN ACCESS

IOP Conference Series: Materials Science and Engineering. Related content PAPER OPEN ACCESS IOP Confeence Seies: Mateials Science and Engineeing PAPER OPE ACCESS A genealized self-consistent method fo estimating ective shea popeties of unidiectional composites compising cylindical othotopic constituents

More information

Physics 2212 GH Quiz #2 Solutions Spring 2016

Physics 2212 GH Quiz #2 Solutions Spring 2016 Physics 2212 GH Quiz #2 Solutions Sping 216 I. 17 points) Thee point chages, each caying a chage Q = +6. nc, ae placed on an equilateal tiangle of side length = 3. mm. An additional point chage, caying

More information

Rigid Body Dynamics 2. CSE169: Computer Animation Instructor: Steve Rotenberg UCSD, Winter 2018

Rigid Body Dynamics 2. CSE169: Computer Animation Instructor: Steve Rotenberg UCSD, Winter 2018 Rigid Body Dynamics 2 CSE169: Compute Animation nstucto: Steve Rotenbeg UCSD, Winte 2018 Coss Poduct & Hat Opeato Deivative of a Rotating Vecto Let s say that vecto is otating aound the oigin, maintaining

More information

Fourier decomposition of segmented magnets with radial magnetization in surface-mounted PM machines

Fourier decomposition of segmented magnets with radial magnetization in surface-mounted PM machines Jounal of ELECTRICAL ENGINEERING, VOL 68 (217), NO6, 47 475 Fouie decomposition of segmented magnets with adial magnetization in suface-mounted PM machines Tow Leong Tiang, Dahaman Ishak, Chee Peng Lim

More information

FORMULA FOR SPIRAL CLOUD-RAIN BANDS OF A TROPICAL CYCLONE. Boris S. Yurchak* University of Maryland, Baltimore County, Greenbelt, Maryland =, (2)

FORMULA FOR SPIRAL CLOUD-RAIN BANDS OF A TROPICAL CYCLONE. Boris S. Yurchak* University of Maryland, Baltimore County, Greenbelt, Maryland =, (2) PF.3 FORMULA FOR SPIRAL CLOUD-RAIN BANDS OF A TROPICAL CYCLONE Bois S. Yuchak* Univesity of Mayland, Baltimoe County, Geenbelt, Mayland. INTRODUCTION Spial cloud-ain bands (SCRB) ae some of the most distinguishing

More information

Yuvraj B. Jadhava, Abhijeet P. Shahb IJSER

Yuvraj B. Jadhava, Abhijeet P. Shahb IJSER Intenational Jounal of Scientific & Engineeing Reseach, Volume 8, Issue 4, Apil-07 ISSN 9-558 Mathematical modeling & design of wom and wom gea pai fo detemining the suface stess acting on the tooth of

More information

Research Article On Alzer and Qiu s Conjecture for Complete Elliptic Integral and Inverse Hyperbolic Tangent Function

Research Article On Alzer and Qiu s Conjecture for Complete Elliptic Integral and Inverse Hyperbolic Tangent Function Abstact and Applied Analysis Volume 011, Aticle ID 697547, 7 pages doi:10.1155/011/697547 Reseach Aticle On Alze and Qiu s Conjectue fo Complete Elliptic Integal and Invese Hypebolic Tangent Function Yu-Ming

More information

[2007] IEEE. Reprinted, with permission, from [Jiaxin Chen, Jianguo Zhu, Youguang Guo, A 2-D nonlinear FEA tool embedded in Matlab/Simulink

[2007] IEEE. Reprinted, with permission, from [Jiaxin Chen, Jianguo Zhu, Youguang Guo, A 2-D nonlinear FEA tool embedded in Matlab/Simulink [2007] IEEE. Repinted, with pemission, fom [Jiaxin Chen, Jianguo Zhu, Youguang Guo, A 2-D nonlinea FEA tool embedded in Matlab/Simulin suounding fo application of electomagnetic field analysis in powe

More information

An Adaptive Neural-Network Model-Following Speed Control of PMSM Drives for Electric Vehicle Applications

An Adaptive Neural-Network Model-Following Speed Control of PMSM Drives for Electric Vehicle Applications Poceedings of the 9th WSEAS Intenational Confeence on Applied Mathematics, Istanbul, Tuey, May 27-29, 2006 (pp412-417) An Adaptive Neual-Netwo Model-Following Speed Contol of PMSM Dives fo Electic Vehicle

More information

STABILITY AND PARAMETER SENSITIVITY ANALYSES OF AN INDUCTION MOTOR

STABILITY AND PARAMETER SENSITIVITY ANALYSES OF AN INDUCTION MOTOR HUNGARIAN JOURNAL OF INDUSTRY AND CHEMISTRY VESZPRÉM Vol. 42(2) pp. 109 113 (2014) STABILITY AND PARAMETER SENSITIVITY ANALYSES OF AN INDUCTION MOTOR ATTILA FODOR 1, ROLAND BÁLINT 1, ATTILA MAGYAR 1, AND

More information

JIEMS Journal of Industrial Engineering and Management Studies

JIEMS Journal of Industrial Engineering and Management Studies JIEMS Jounal of Industial Engineeing and Management Studies Vol. 4, No. 2, 2017, pp. 19-34 DOI: 10.22116/JIEMS.2017.54603 www.jiems.icms.ac.i Pefomance of CCC- contol chat with vaiable sampling intevals

More information

Modelling Vortex Fields in Metal Smelting Furnaces

Modelling Vortex Fields in Metal Smelting Furnaces Int. Jnl. of Multiphysics Volume 4 Numbe 4 00 35 Modelling Votex Fields in Metal Smelting Funaces Oleg Kazak, Oleksand Semko Depatment Of Physics, Donetsk National Univesity, Donetsk, Ukaine Email: olegkazak@yandex.u;

More information

Relating Branching Program Size and. Formula Size over the Full Binary Basis. FB Informatik, LS II, Univ. Dortmund, Dortmund, Germany

Relating Branching Program Size and. Formula Size over the Full Binary Basis. FB Informatik, LS II, Univ. Dortmund, Dortmund, Germany Relating Banching Pogam Size and omula Size ove the ull Binay Basis Matin Saueho y Ingo Wegene y Ralph Wechne z y B Infomatik, LS II, Univ. Dotmund, 44 Dotmund, Gemany z ankfut, Gemany sauehof/wegene@ls.cs.uni-dotmund.de

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