Conducting fuzzy division by using linear programming
|
|
- Amberlynn Riley
- 5 years ago
- Views:
Transcription
1 WSES TRNSCTIONS on INFORMTION SCIENCE & PPLICTIONS Muat pe Basaan, Cagdas Hakan adag, Cem Kadia Conducting fuzzy division by using inea pogamming MURT LPER BSRN Depatment of Mathematics Nigde Univesity Nigde TURKEY CGDS HKN LDG Depatment of Statistics Hacettepe Univesity Beytepe, nkaa TURKEY CEM KDILR Depatment of Statistics Hacettepe Univesity Beytepe, nkaa TURKEY bstact: Some appoimation methods have been poposed fo fuzzy mutipication and division in the iteatue. Instead of doing aithmetic opeations using fuzzy membeship functions fo fuzzy numbes, paameteized epesentation of fuzzy numbes have been used in aithmetic opeations. The most appied paameteized fuzzy numbes used in many of the eseach papes ae symmetic and asymmetic tiangua and tapezoida fuzzy numbes. In this study, we popose a new appoimation method based on inea pogamming fo fuzzy division. In ode to show the appicabiity of the poposed method, some eampes ae soved using the poposed method and the esuts ae compaed with those geneated by othe methods in the iteatue. The poposed method has poduced bette esuts than those geneated by the othes. Key-wods: ppoimation method; Fuzzy aithmetic; Fuzzy division; Linea pogamming; Tiangua fuzzy numbe 1 Intoduction Instead of using membeship functions in fuzzy aithmetic, paameteized fom of fuzzy numbes have been used fo aithmetic opeations. Despite of the fact that the addition and subtaction of the paameteized fuzzy numbes esut in cosed fom, the same does not hod fo mutipication and division. Howeve, fuzzy mutipication in cosed fom can be done unde the weakest T nom as an eception [4]. Theefoe, some appoimation methods ae poposed fo mutipication and division of the paameteized fuzzy numbes [1,,3,4]. The most appied paameteized fuzzy numbes ae symmetic and asymmetic tiangua and tapezoida fuzzy numbes since they ae simpe and easy to impement fo many puposes [8]. Dubois and Pade [1] fist intoduced aithmetic opeations on paameteized fuzzy numbes. Then, Giachetti and Young [,3] poposed a new method fo fuzzy mutipication and division. nothe method fo fuzzy aithmetic opeation is the weakest T nom [4]. In these studies, eseaches have focused on deceasing the fuzziness of the esuting fuzzy numbe. It is assumed that two paameteized tiangua fuzzy numbes ae mutipied o divided. This computation can be done using one of the methods mentioned above [1,,3,4]. Howeve, the esuts obtained fom these methods have diffeent fuzzy end points o spead vaues ecept cente vaue. Instead of using paameteized fom of fuzzy numbes that consist of ea numbes, the aea and the popotions of cente vaue to eft and to ight end points ae used to do mutipication o division of two fuzzy numbes. We poposed a new method based on inea pogamming fo paameteized fuzzy division. The paameteized fuzzy numbes ae imited to symmetic and asymmetic and tapezoida fuzzy numbes because of thei simpicity and ease of use. In this pape, new fuzzy division method is appied to tiangua fuzzy numbes. The essence of poposed method depends on utiizing geometic featues and definition of tiangua fuzzy numbes [5,7]. In the net section, some peiminay knowedge eated to fuzzy set is given. Section 3 gives bief infomation about eisting appoaches avaiabe in the iteatue fo fuzzy division. The new poposed method is intoduced in Section 4. Section 5 contains the impementation of the poposed method and the compaisons with othe avaiabe methods in the iteatue. Last section is discussion and concusion. Peiminaies fuzzy set [6] of the ea ine R with membeship function : R [ 0,1] μ is caed a fuzzy numbe if 1. is noma, namey, thee eist an eement such that μ ( = 1. is fuzzy conve, that is, μ ( λ1 + (1 λ μ ( 1 μ ( 1, R, λ [0,1] 3. μ is semi continuous 4. supp is bounded whee supp = R : μ ( > 0 { } ISSN: Issue 6, Voume 5, June 008
2 WSES TRNSCTIONS on INFORMTION SCIENCE & PPLICTIONS Muat pe Basaan, Cagdas Hakan adag, Cem Kadia The α cut of a fuzzy set is a non- fuzzy set defined as α = { R : μ ( α}. ccoding to the definition of a fuzzy numbe, evey α cut of a fuzzy numbe is a cosed inteva. Thus, α = [ L ( α, U ( α ] can be witten, whee L ( α = inf{ R : μ ( α} U ( α = sup{ R : μ ( α} The membeship function fo tiangua fuzzy numbe is [7] defined as 0 fo < a a fo a b b a μ ( = c fo b c c b 0 fo > c Thee ae two ways of denoting paameteized fuzzy numbes. The fist one denotes eft end point, cente vaue and the ight end point. On the othe hand, the second one shows eft spead vaue, cente vaue, and the ight spead vaue. Thoughout the pape, two ways of denoting fuzzy numbes ae adopted in fuzzy aithmetic opeations. 3 Review of Eisting ppoaches The fist way of doing paameteized fuzzy aithmetic was intoduced by Dubois and Pade [1]. The esuting fuzzy numbe is just an appoimation. Howeve, the usage of them is easy and simpe in appications. Let M and N be two tiangua fuzzy numbes denoted by M = ( m, α, β, N = ( n, γ, δ. Dubois and Pade [1] intoduced fuzzy division with the epession given beow. M m m n m n X δ + α γ + β = = (,, N n n n In Tabe 1, thee iustations ae given utiizing the epession given by [1]. Giachetti and Young [,3] intoduced a new appoimation method fo fuzzy mutipication and division. Whie a new appoimation method fo mutipication was intoduced in [], [3] incuded a new appoach fo fuzzy division. The motivation behind those papes is that the esuting fuzzy numbe shoud be obtained with ess eo which means that the fuzziness of the esuting fuzzy numbe is epected to gow ess. the mathematica epessions fo the new appoimation method fo fuzzy division [3] was given as foows: QN( L = DL+ G( α, n τl( n, λ( b a QN( R = DR+ G( α, n τr( n, ρ( c b whee D L is the actua division using α -cut, G( α, n is the coection tem which is witten in tems of α. The inea fit between the geometic mean of the spead atios and the numbe incuded in division is denoted by τ ( n L, λ. ( b a is the eft spead vaue. The same tems can be witten fo the ight side of the esuting fuzzy numbe. Heein, we ae not going into the detaied epanations about how the method poposed by [,3] is appied to tiangua fuzzy numbes. The moe detaied epanations can be found in [,3]. 4 The Poposed Method Instead of using numbes given in paameteized fom of the fuzzy numbes to pefom fuzzy aithmetic, we popose a new method based on inea pogamming utiizing the geometic featues and definition of fuzzy numbes. It is assumed that two asymmetic fuzzy numbes ae divided. The paameteized fom of these fuzzy numbes ae denoted by ( 1,, 1 and (,,, whee 1 and, c 1 and c, and, 1 and denote eft end points, cente points and, ight end points, espectivey. Let = ( 1,, 1 and B = (,, be two fuzzy numbes. The esuting fuzzy numbe obtained fom the division of these fuzzy numbes can be witten as foows. X = (1 B whee X = (,, is a fuzzy numbe. c The constaints and the objective function of the inea pogamming pobem fo the fuzzy division given in (1 ae defined as foows: The fist constaint is based on the aea of fuzzy numbes. The aea of the esuting fuzzy numbe X shoud be equa to o ess than the aea obtained fom the division of two aeas of fuzzy numbes and B. Thus, the mathematica epession fo the fist constaint is witten as foows: ( 1 1 ( ( ( ISSN: Issue 6, Voume 5, June 008
3 WSES TRNSCTIONS on INFORMTION SCIENCE & PPLICTIONS Muat pe Basaan, Cagdas Hakan adag, Cem Kadia whee the aeas of fuzzy numbe and B ae computed ( 1 as 1 ( and espectivey and the aea of fuzzy numbe X ( is computed as. Epession ( can be ewitten as foows: ( 1 1 (3 ( The second and the thid constaints ae defined using the atios of cente vaues to eft and ight speads espectivey. The second constaint is constucted based on the eft speads. The eft spead vaue ove cente vaue fo X shoud be equa to o ess than the division of the same atios cacuated fo and B. Thus, the mathematica epession of the second constaint is witten as foows: ( 1 ( c (4 ( c c The cente vaue of X is equa to the division of the cente vaues of and B since a the avaiabe methods in the iteatue [1,,3] have used this notion. Thus, the epession given in (4 is ewitten as foows: ( 1 (5 ( In a simia manne, the thid constaint is constucted as foows: ( 1 + (6 ( The fouth and fifth constaints can be defined based on the definition of fuzzy numbe. The eft end point of a fuzzy numbe shoud be ess than the cente vaue. Then, the mathematica epession fo the fouth constaint is given beow. < (7 The ight end point of a fuzzy numbe shoud be geate than the cente vaue. Then, the mathematica epession fo the fifth constaint is given beow. > (8 When taking the second (5, thid (6, fouth (7, and the fifth (8 constaints into account, the uppe and owe bounds fo and can be witten as given beow. ( 1 < c ( c c ( 1 < + ( In the objective function, what we ae ooking fo is a fuzzy numbe X which contains the fuzziness esuted fom dividing two fuzzy numbes. Theefoe, the diffeence between the end points and shoud be maimized. Then, the objective function is given beow. f ( = (9 Instead of maimizing the objective function in (9, if the diffeence between and wee tied to be minimized, the vaue of f ( woud take zeo. This means that the esuting fuzzy numbe becomes having zeo speads, that is, it is a degeneated fuzzy numbe. Finay, the defined inea pogamming pobem is given beow. Ma f ( = ( 1 1 ( ( 1 ( ( 1 + (9 ( < > In the fomuation of the pobem, thee ae two unknown vaiabes and. In the esut of soving the inea pogamming pobem, the eft and ight end points of X, whose cente vaue known as in advance, ae obtained. 5 Impementation Let and B be two fuzzy numbes which ae denoted by = ( 1,, 1 and B = (,, whee 1 and, and c, and, 1 and denote eft end points, cente points and, ight end points, espectivey. Fo eampe, et = (70,100,130 and B = (4,10,16 be two asymmetic fuzzy numbes. The poposed method is used in ode to divide these two fuzzy ISSN: Issue 6, Voume 5, June 008
4 WSES TRNSCTIONS on INFORMTION SCIENCE & PPLICTIONS Muat pe Basaan, Cagdas Hakan adag, Cem Kadia numbes. Then, the inea pogamming pobem is given beow. Ma f ( = < 10 > 10 If the pobem is ewitten, the new fomuation is given beow. Ma f ( = < 10 > 10 When the pobem is soved, the soution gives = 15 and = 5. Thus, the esut of division is X = (5,10,15. When the fuzzy numbes having diffeent featues such as geate cente vaues o wide spead vaues ae divided, esuts ae given in ode to show the appicabiity of the poposed method. Fo compaison, the esuts of the soved eampes based on the poposed method and othe methods avaiabe in the iteatue ae summaized in Tabe 1. The ea numbe unde the esuting fuzzy numbe denotes the diffeence between the end points. Fo eampe, when = (1,5,7 is divided by B = (5,0,3, using the poposed method gives X = ( ,0.5, Then the diffeence between end points of this esut is When the esuts ae eamined, the poposed method has esuting fuzzy numbe whose fuzziness is ess than the fuzziness of the method poposed by Dubois and Pade [1]. The fist two eampes poduce appoimatey the same fuzziness fo the methods poposed by Giachetti and Young [3] and the poposed method. Howeve, when the thid eampe is eaimed, the poposed method has poduced much naowe fuzziness than the method poposed by Giachetti and Young [3] since the paametes used in thei method ae out of the ange specified by Giachetti and Young [3]. Theefoe, the poposed method shoud be pefeed to the Giachetti and Young s method since the poposed method does not impose any imitation on any paametes. Tabe 1. The esuts of the diffeent fuzzy division methods (1,5,7 / (5,0,3 esuts ange The poposed method (0.0,0.5, Dubois and Pade (-0.05,0.5, Giachetti and Young (0.01,0.5, (70,110,130 / (4,10,16 esuts ange The poposed method (5,10,15 10 Dubois and Pade (1,10,19 18 Giachetti and Young (6.7,10, (18,147,178 / (3,4,87 esuts ange The poposed method (0.19,3.500, Dubois and Pade (-3.33,3.5, Giachetti and Young (0.765,3.5, It is a known fact that the vaiabes in inea pogamming take positive vaues. Howeve, the components of the esuting fuzzy numbe can take positive and negative vaues at the same time. In ode to sove this pobem in fuzzy division, the inea pogamming pobem is modified. This modification enabes the poposed method to geneate negative end points just as doing aithmetic opeations in ea ines. Theefoe, the imitation of the inea pogamming can be eiminated. When the cente vaue of the esuting fuzzy numbe neas to zeo o the diffeence between eft spead vaues of dividend fuzzy numbe and of diviso fuzzy numbe is age, the eft end point of the esuting fuzzy numbe can be a negative numbe. The constaint given beow can point that might have negative vaue. ( 1 ( Thus, when the condition ( 1 < (10 ( is eaized, the domain of contains negative vaues. This is the mathematica epession of the veba epanation given above. Howeve, the esuts obtained fom soving the inea pogamming pobem fo fuzzy division can not be negative. In ode to ovecome this issue, the vaiabe can be edefined as foows: = 1 whee 1 and ae positive numbes. When the new epession given above is witten in the pobem ISSN: Issue 6, Voume 5, June 008
5 WSES TRNSCTIONS on INFORMTION SCIENCE & PPLICTIONS Muat pe Basaan, Cagdas Hakan adag, Cem Kadia constucted fo fuzzy division, the new inea pogamming pobem is obtained as foows: Ma f ( = 1 + ( ( ( 1 1 ( ( 1 + (11 ( 1 < > The fomuation constucted above shoud be soved in ode to obtain the paametes of the esuting fuzzy numbe fo fuzzy division. Thee ae thee unknown vaiabes, and 1.Then, the eft and ight end points of X, whose cente vaue is known as in advance, ae obtained. The eft end point of the esuting fuzzy numbe is obtained by subtacting fom 1. Fo eampe, et = (1,5,7 and B = (5,0,3 be two asymmetic fuzzy numbes. When the vaues ae witten as in (10, the inequaity given beow is obtained. 5 (5 1 < 0 (0 5 Then 0.50 < 0.67 is obtained. It is seen that the condition is satisfied so the eft end point of the esuting fuzzy numbe wi be a negative numbe. Theefoe, the poposed method is used in ode to divide these two fuzzy numbes. Then, the modified inea pogamming pobem is given beow. Ma f ( = < 0.50 > 0.50 When the pobem is soved, the soution gives = and = Thus, the esut of division is X = ( 0.017, 0.50, It shoud be noted that checking the condition given in (9 is not necessay when fuzzy division is conducted since the modified vesion of inea pogamming fomuation eiminates finding just positive numbes. Even though the condition given in (9 is not satisfied, esuts obtained fom the soution of the fomuation (9 ae same as those obtained fom the fomuation (11. Theefoe, the fomuation (11 can be used evey time without checking the condition given in (9. In shot, the fomuation given in (9 is a specia type of the fomuation given in (11 that can poduce positive and negative end points. 6 Concusion Thee have been vaious methods avaiabe in the iteatue in ode to do fuzzy paameteized aithmetic since using membeship functions in fuzzy aithmetic is a compe pocess. Howeve, utiizing paameteized fuzzy aithmetic just poduces appoimated esuts and using paameteized fuzzy aithmetic epeatedy causes to incease the fuzziness of the esuting fuzzy numbe, which is obtained at end of the fuzzy opeations. In this pape, we poposed a new method based on inea pogamming fo fuzzy division of tiangua fuzzy numbes. When the constaints of the inea pogamming pobem ae constucted, we epoit the geometic featues and definition of a fuzzy numbe. The poposed method cacuates the cente vaue of the esuting fuzzy numbe just as the othe methods [1,,3] avaiabe in the iteatue. Thus, the eft and ight end points of the esuting fuzzy numbe ae unknowns. Then, these vaues ae caed decision vaiabes fo the inea pogamming pobem. The esuting fuzzy numbe is obtained by soving this inea pogamming pobem consisting of five constaints. In ode to show the appicabiity of the poposed method, vaious eampes ae soved. The esuts of the poposed method ae compaed with the esuts of the othe methods in the iteatue [1,,3]. It is ceay seen that the poposed method poduces much naowe fuzziness than those poduced by the othe methods. nothe advantage of the poposed method is no dependencies fo any paametes. Fo instance, Giachetti and Young [,3] caimed that thei method woks we fo paametes in specified anges. They caed these paametes as eft and ight side atios. Refeences: [1] D. Dubois and H. Pade, Fuzzy Sets and Systems: Theoy and ppications, cademic Pess, New Yok, [] R.E. Giachetti and R.E. Young, naysis of the eo in the standad appoimation used fo mutipication ISSN: Issue 6, Voume 5, June 008
6 WSES TRNSCTIONS on INFORMTION SCIENCE & PPLICTIONS Muat pe Basaan, Cagdas Hakan adag, Cem Kadia of tiangua and tapezoida fuzzy numbes and the deveopment of a new appoimation, Fuzzy Sets and Systems, Vo. 91, 1997, pp [3] R.E. Giachetti and R.E. Young, paametic epesentation of fuzzy numbes and thei aithmetic opeatos, Fuzzy Sets and Systems, Vo. 91, 1997, pp [4] D.H. Hong, Shape peseving mutipications of fuzzy numbes, Fuzzy Sets and Systems, Vo. 13, 001, pp [5] D. Dubois and H. Pade, Possibiity Theoy n ppoach to Computeized Pocessing of Uncetainity, Penun Pess, [6] Fuzzy Sets and ppications: Seected Papes by L.. Zadeh, Edited by R.R Yage, S. Ovchinnikov, R.M Tong, H.T Nguyen, [7] D. Dubois, H. Pade, Opeations on fuzzy numbes, ntenat. J. Systems Science, Vo. 9(6, 1978, pp [8] W. Pedycz, Why tiangua membeship functions?, Fuzzy Sets and Systems, Vo. 64, 1994, pp ISSN: Issue 6, Voume 5, June 008
Seidel s Trapezoidal Partitioning Algorithm
CS68: Geometic Agoithms Handout #6 Design and Anaysis Oigina Handout #6 Stanfod Univesity Tuesday, 5 Febuay 99 Oigina Lectue #7: 30 Januay 99 Topics: Seide s Tapezoida Patitioning Agoithm Scibe: Michae
More informationObjectives. We will also get to know about the wavefunction and its use in developing the concept of the structure of atoms.
Modue "Atomic physics and atomic stuctue" Lectue 7 Quantum Mechanica teatment of One-eecton atoms Page 1 Objectives In this ectue, we wi appy the Schodinge Equation to the simpe system Hydogen and compae
More informationHomework 1 Solutions CSE 101 Summer 2017
Homewok 1 Soutions CSE 101 Summe 2017 1 Waming Up 1.1 Pobem and Pobem Instance Find the smaest numbe in an aay of n integes a 1, a 2,..., a n. What is the input? What is the output? Is this a pobem o a
More informationMerging to ordered sequences. Efficient (Parallel) Sorting. Merging (cont.)
Efficient (Paae) Soting One of the most fequent opeations pefomed by computes is oganising (soting) data The access to soted data is moe convenient/faste Thee is a constant need fo good soting agoithms
More informationThe Solutions of the Classical Relativistic Two-Body Equation
T. J. of Physics (998), 07 4. c TÜBİTAK The Soutions of the Cassica Reativistic Two-Body Equation Coşkun ÖNEM Eciyes Univesity, Physics Depatment, 38039, Kaysei - TURKEY Received 3.08.996 Abstact With
More informationEntropy Operator for Membership Function of Uncertain Set
Entopy Opeato fo Membeship Function of Uncetain Set Kai Yao 1, Hua Ke 1. Schoo of Management, Univesity of Chinese Academy of Sciences, Beijing 119, China. Schoo of Economics and Management, Tongji Univesity,
More informationProbability Estimation with Maximum Entropy Principle
Pape 0,CCG Annua Repot, 00 ( c 00) Pobabiity Estimation with Maximum Entopy Pincipe Yupeng Li and Cayton V. Deutsch The pincipe of Maximum Entopy is a powefu and vesatie too fo infeing a pobabiity distibution
More informationFunctions Defined on Fuzzy Real Numbers According to Zadeh s Extension
Intenational Mathematical Foum, 3, 2008, no. 16, 763-776 Functions Defined on Fuzzy Real Numbes Accoding to Zadeh s Extension Oma A. AbuAaqob, Nabil T. Shawagfeh and Oma A. AbuGhneim 1 Mathematics Depatment,
More informationLecture 1. time, say t=0, to find the wavefunction at any subsequent time t. This can be carried out by
Lectue The Schödinge equation In quantum mechanics, the fundamenta quantity that descibes both the patice-ike and waveike chaacteistics of patices is wavefunction, Ψ(. The pobabiity of finding a patice
More informationJackson 3.3 Homework Problem Solution Dr. Christopher S. Baird University of Massachusetts Lowell
Jackson 3.3 Homewok Pobem Soution D. Chistophe S. Baid Univesity of Massachusetts Lowe POBLEM: A thin, fat, conducting, cicua disc of adius is ocated in the x-y pane with its cente at the oigin, and is
More information= ρ. Since this equation is applied to an arbitrary point in space, we can use it to determine the charge density once we know the field.
Gauss s Law In diffeentia fom D = ρ. ince this equation is appied to an abita point in space, we can use it to detemine the chage densit once we know the fied. (We can use this equation to ve fo the fied
More informationA STUDY OF HAMMING CODES AS ERROR CORRECTING CODES
AGU Intenational Jounal of Science and Technology A STUDY OF HAMMING CODES AS ERROR CORRECTING CODES Ritu Ahuja Depatment of Mathematics Khalsa College fo Women, Civil Lines, Ludhiana-141001, Punjab, (India)
More informationInternational 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 informationON INDEPENDENT SETS IN PURELY ATOMIC PROBABILITY SPACES WITH GEOMETRIC DISTRIBUTION. 1. Introduction. 1 r r. r k for every set E A, E \ {0},
ON INDEPENDENT SETS IN PURELY ATOMIC PROBABILITY SPACES WITH GEOMETRIC DISTRIBUTION E. J. IONASCU and A. A. STANCU Abstact. We ae inteested in constucting concete independent events in puely atomic pobability
More information7.2. Coulomb s Law. The Electric Force
Coulomb s aw Recall that chaged objects attact some objects and epel othes at a distance, without making any contact with those objects Electic foce,, o the foce acting between two chaged objects, is somewhat
More informationLET a random variable x follows the two - parameter
INTERNATIONAL JOURNAL OF MATHEMATICS AND SCIENTIFIC COMPUTING ISSN: 2231-5330, VOL. 5, NO. 1, 2015 19 Shinkage Bayesian Appoach in Item - Failue Gamma Data In Pesence of Pio Point Guess Value Gyan Pakash
More informationKR- 21 FOR FORMULA SCORED TESTS WITH. Robert L. Linn, Robert F. Boldt, Ronald L. Flaugher, and Donald A. Rock
RB-66-4D ~ E S [ B A U R L C L Ii E TI KR- 21 FOR FORMULA SCORED TESTS WITH OMITS SCORED AS WRONG Robet L. Linn, Robet F. Boldt, Ronald L. Flaughe, and Donald A. Rock N This Bulletin is a daft fo inteoffice
More informationDo Managers Do Good With Other People s Money? Online Appendix
Do Manages Do Good With Othe People s Money? Online Appendix Ing-Haw Cheng Haison Hong Kelly Shue Abstact This is the Online Appendix fo Cheng, Hong and Shue 2013) containing details of the model. Datmouth
More informationEncapsulation theory: the transformation equations of absolute information hiding.
1 Encapsulation theoy: the tansfomation equations of absolute infomation hiding. Edmund Kiwan * www.edmundkiwan.com Abstact This pape descibes how the potential coupling of a set vaies as the set is tansfomed,
More informationMarkscheme May 2017 Calculus Higher level Paper 3
M7/5/MATHL/HP3/ENG/TZ0/SE/M Makscheme May 07 Calculus Highe level Pape 3 pages M7/5/MATHL/HP3/ENG/TZ0/SE/M This makscheme is the popety of the Intenational Baccalaueate and must not be epoduced o distibuted
More informationTHE JEU DE TAQUIN ON THE SHIFTED RIM HOOK TABLEAUX. Jaejin Lee
Koean J. Math. 23 (2015), No. 3, pp. 427 438 http://dx.doi.og/10.11568/kjm.2015.23.3.427 THE JEU DE TAQUIN ON THE SHIFTED RIM HOOK TABLEAUX Jaejin Lee Abstact. The Schensted algoithm fist descibed by Robinson
More informationProblems with Mannheim s conformal gravity program
Poblems with Mannheim s confomal gavity pogam June 4, 18 Youngsub Yoon axiv:135.163v6 [g-qc] 7 Jul 13 Depatment of Physics and Astonomy Seoul National Univesity, Seoul 151-747, Koea Abstact We show that
More informationAbsorption 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 informationCoordinate Geometry. = k2 e 2. 1 e + x. 1 e. ke ) 2. We now write = a, and shift the origin to the point (a, 0). Referred to
Coodinate Geomet Conic sections These ae pane cuves which can be descibed as the intesection of a cone with panes oiented in vaious diections. It can be demonstated that the ocus of a point which moves
More informationGradient-based Neural Network for Online Solution of Lyapunov Matrix Equation with Li Activation Function
Intenational Confeence on Infomation echnology and Management Innovation (ICIMI 05) Gadient-based Neual Netwok fo Online Solution of Lyapunov Matix Equation with Li Activation unction Shiheng Wang, Shidong
More informationPHYS 705: Classical Mechanics. Central Force Problems I
1 PHYS 705: Cassica Mechanics Centa Foce Pobems I Two-Body Centa Foce Pobem Histoica Backgound: Kepe s Laws on ceestia bodies (~1605) - Based his 3 aws on obsevationa data fom Tycho Bahe - Fomuate his
More informationSteady 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 informationSTUDY 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 informationMutual Inductance. If current i 1 is time varying, then the Φ B2 flux is varying and this induces an emf ε 2 in coil 2, the emf is
Mutua Inductance If we have a constant cuent i in coi, a constant magnetic fied is ceated and this poduces a constant magnetic fux in coi. Since the Φ B is constant, thee O induced cuent in coi. If cuent
More informationDuality 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 informationProblem set 6. Solution. The problem of firm 3 is. The FOC is: 2 =0. The reaction function of firm 3 is: = 2
Pobem set 6 ) Thee oigopoists opeate in a maket with invese demand function given by = whee = + + and is the quantity poduced by fim i. Each fim has constant magina cost of poduction, c, and no fixed cost.
More informationMATH 415, WEEK 3: Parameter-Dependence and Bifurcations
MATH 415, WEEK 3: Paamete-Dependence and Bifucations 1 A Note on Paamete Dependence We should pause to make a bief note about the ole played in the study of dynamical systems by the system s paametes.
More informationComplex Intuitionistic Fuzzy Group
Global Jounal of Pue and pplied Mathematics. ISSN 0973-1768 Volume 1, Numbe 6 (016, pp. 499-4949 Reseach India Publications http://www.ipublication.com/gjpam.htm Comple Intuitionistic Fuzzy Goup Rima l-husban
More informationAn Application of Bessel Functions: Study of Transient Flow in a Cylindrical Pipe
Jouna of Mathematics and System Science 6 (16) 7-79 doi: 1.1765/159-591/16..4 D DAVID PUBLISHING An Appication of Besse Functions: Study of Tansient Fow in a Cyindica Pipe A. E. Gacía, Lu Maía Gacía Cu
More informationTheorem on the differentiation of a composite function with a vector argument
Poceedings of the Estonian Academy of Sciences 59 3 95 doi:.376/poc..3. Avaiae onine at www.eap.ee/poceedings Theoem on the diffeentiation of a composite function with a vecto agument Vadim Kapain and
More informationPhysics 235 Chapter 5. Chapter 5 Gravitation
Chapte 5 Gavitation In this Chapte we will eview the popeties of the gavitational foce. The gavitational foce has been discussed in geat detail in you intoductoy physics couses, and we will pimaily focus
More informationApplication of homotopy perturbation method to the Navier-Stokes equations in cylindrical coordinates
Computational Ecology and Softwae 5 5(): 9-5 Aticle Application of homotopy petubation method to the Navie-Stokes equations in cylindical coodinates H. A. Wahab Anwa Jamal Saia Bhatti Muhammad Naeem Muhammad
More informationMEASURES OF BLOCK DESIGN EFFICIENCY RECOVERING INTERBLOCK INFORMATION
MEASURES OF BLOCK DESIGN EFFICIENCY RECOVERING INTERBLOCK INFORMATION Walte T. Fedee 337 Waen Hall, Biometics Unit Conell Univesity Ithaca, NY 4853 and Tey P. Speed Division of Mathematics & Statistics,
More informationThree-dimensional systems with spherical symmetry
Thee-dimensiona systems with spheica symmety Thee-dimensiona systems with spheica symmety 006 Quantum Mechanics Pof. Y. F. Chen Thee-dimensiona systems with spheica symmety We conside a patice moving in
More informationDetermining 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 informationGeneralized net model of the process of ordering of university subjects
eventh Int. okshop on Gs, ofia, 4- Juy 006, -9 Geneaized net mode of the pocess of odeing of univesity subjects A. hannon, E. otiova, K. Atanassov 3, M. Kawczak 4, P. Meo-Pinto,. otiov, T. Kim 6 KvB Institute
More informationPearson 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 informationASTR415: 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 informationA Sardinas-Patterson Characterization Theorem for SE-codes
A Sadinas-Patteson Chaacteization Theoem fo SE-codes Ionuţ Popa,Bogdan Paşaniuc Facuty of Compute Science, A.I.Cuza Univesity of Iaşi, 6600 Iaşi, Romania May 0, 2004 Abstact The aim of this pape is to
More informationNo. 6 Cell image ecognition with adial hamonic Fouie moments 611 ecognition expeiment is pefomed. Results show that as good image featues, RHFMs ae su
Vol 12 No 6, June 23 cfl 23 Chin. Phys. Soc. 19-1963/23/12(6)/61-5 Chinese Physics and IOP Publishing Ltd Cell image ecognition with adial hamonic Fouie moments * Ren Hai-Ping(Φ ±) a)y, Ping Zi-Liang(
More informationAn 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 informationMechanics Physics 151
Mechanics Physics 5 Lectue 5 Centa Foce Pobem (Chapte 3) What We Did Last Time Intoduced Hamiton s Pincipe Action intega is stationay fo the actua path Deived Lagange s Equations Used cacuus of vaiation
More informationRelating Scattering Amplitudes to Bound States
Reating Scatteing Ampitudes to Bound States Michae Fowe UVa. 1/17/8 Low Enegy Appoximations fo the S Matix In this section we examine the popeties of the patia-wave scatteing matix ( ) = 1+ ( ) S k ikf
More informationA 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 informationMiskolc Mathematical Notes HU e-issn Tribonacci numbers with indices in arithmetic progression and their sums. Nurettin Irmak and Murat Alp
Miskolc Mathematical Notes HU e-issn 8- Vol. (0), No, pp. 5- DOI 0.85/MMN.0.5 Tibonacci numbes with indices in aithmetic pogession and thei sums Nuettin Imak and Muat Alp Miskolc Mathematical Notes HU
More informationWhen two numbers are written as the product of their prime factors, they are in factored form.
10 1 Study Guide Pages 420 425 Factos Because 3 4 12, we say that 3 and 4 ae factos of 12. In othe wods, factos ae the numbes you multiply to get a poduct. Since 2 6 12, 2 and 6 ae also factos of 12. The
More informationA Simultaneous Routing Tree Construction and Fanout Optimization Algorithm *
A Simutaneous Routing Tee Constuction and Fanout Optimization Agoithm * Ami H. Saek, Jinan Lou, Massoud Pedam Depatment of Eectica Engineeing - Systems Univesity of Southen Caifonia Los Angees, CA 90089
More informationEncapsulation theory: radial encapsulation. Edmund Kirwan *
Encapsulation theoy: adial encapsulation. Edmund Kiwan * www.edmundkiwan.com Abstact This pape intoduces the concept of adial encapsulation, wheeby dependencies ae constained to act fom subsets towads
More informationAbsolute Specifications: A typical absolute specification of a lowpass filter is shown in figure 1 where:
FIR FILTER DESIGN The design of an digital filte is caied out in thee steps: ) Specification: Befoe we can design a filte we must have some specifications. These ae detemined by the application. ) Appoximations
More informationComputing selected eigenvalues of sparse unsymmetric matrices using subspace iteration
RAL-91-056 Computing seected eigenvaues of spase unsymmetic matices using subspace iteation by I. S. Duff and J. A. Scott ABSRAC his pape discusses the design and deveopment of a code to cacuate the eigenvaues
More informationCourse Updates. Reminders: 1) Assignment #10 due next Wednesday. 2) Midterm #2 take-home Friday. 3) Quiz # 5 next week. 4) Inductance, Inductors, RLC
Couse Updates http://www.phys.hawaii.edu/~vane/phys7-sp10/physics7.htm Remindes: 1) Assignment #10 due next Wednesday ) Midtem # take-home Fiday 3) Quiz # 5 next week 4) Inductance, Inductos, RLC Mutua
More informationBayesian Analysis of Topp-Leone Distribution under Different Loss Functions and Different Priors
J. tat. Appl. Po. Lett. 3, No. 3, 9-8 (6) 9 http://dx.doi.og/.8576/jsapl/33 Bayesian Analysis of Topp-Leone Distibution unde Diffeent Loss Functions and Diffeent Pios Hummaa ultan * and. P. Ahmad Depatment
More informationStanford University CS259Q: Quantum Computing Handout 8 Luca Trevisan October 18, 2012
Stanfod Univesity CS59Q: Quantum Computing Handout 8 Luca Tevisan Octobe 8, 0 Lectue 8 In which we use the quantum Fouie tansfom to solve the peiod-finding poblem. The Peiod Finding Poblem Let f : {0,...,
More informationHua Xu 3 and Hiroaki Mukaidani 33. The University of Tsukuba, Otsuka. Hiroshima City University, 3-4-1, Ozuka-Higashi
he inea Quadatic Dynamic Game fo Discete-ime Descipto Systems Hua Xu 3 and Hioai Muaidani 33 3 Gaduate School of Systems Management he Univesity of suuba, 3-9- Otsua Bunyo-u, oyo -0, Japan xuhua@gssm.otsua.tsuuba.ac.jp
More informationAPPLICATION 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 informationPhysics 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 informationPressure in the Average-Atom Model
Pessue in the Aveage-Atom Moe W.. Johnson Depatment of Physics, 225 Nieuwan Science Ha Note Dame Univesity, Note Dame, IN 46556 Febuay 28, 2002 Abstact The (we-known) quantum mechanica expession fo the
More informationA matrix method based on the Fibonacci polynomials to the generalized pantograph equations with functional arguments
A mati method based on the Fibonacci polynomials to the genealized pantogaph equations with functional aguments Ayşe Betül Koç*,a, Musa Çama b, Aydın Kunaz a * Coespondence: aysebetuloc @ selcu.edu.t a
More informationDepartment of Applied Mathematics, National Chiao Tung University, Hsinchu 30050, Taiwan.
Gaphs and Cobinatoics (1999) 15 : 95±301 Gaphs and Cobinatoics ( Spinge-Veag 1999 T-Cooings and T-Edge Spans of Gaphs* Shin-Jie Hu, Su-Tzu Juan, and Gead J Chang Depatent of Appied Matheatics, Nationa
More informationEstimation of the Correlation Coefficient for a Bivariate Normal Distribution with Missing Data
Kasetsat J. (Nat. Sci. 45 : 736-74 ( Estimation of the Coelation Coefficient fo a Bivaiate Nomal Distibution with Missing Data Juthaphon Sinsomboonthong* ABSTRACT This study poposes an estimato of the
More informationCOMPARISON OF METHODS FOR SOLVING THE HEAT TRANSFER IN ELECTRICAL MACHINES
POZNAN UNIVE RSITY OF TE CHNOLOGY ACADE MIC JOURNALS No 75 Electical Engineeing 2013 Zbynek MAKKI* Macel JANDA* Ramia DEEB* COMPARISON OF METHODS FOR SOLVING THE HEAT TRANSFER IN ELECTRICAL MACHINES This
More informationExperiment I Voltage Variation and Control
ELE303 Electicity Netwoks Expeiment I oltage aiation and ontol Objective To demonstate that the voltage diffeence between the sending end of a tansmission line and the load o eceiving end depends mainly
More informationRigid 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 informationMechanics Physics 151
Mechanics Physics 5 Lectue 5 Centa Foce Pobem (Chapte 3) What We Did Last Time Intoduced Hamiton s Pincipe Action intega is stationay fo the actua path Deived Lagange s Equations Used cacuus of vaiation
More information15.081J/6.251J Introduction to Mathematical Programming. Lecture 6: The Simplex Method II
15081J/6251J Intoduction to Mathematical Pogamming ectue 6: The Simplex Method II 1 Outline Revised Simplex method Slide 1 The full tableau implementation Anticycling 2 Revised Simplex Initial data: A,
More informationChapter 5 Force and Motion
Chapte 5 Foce and Motion In Chaptes 2 and 4 we have studied kinematics, i.e., we descibed the motion of objects using paametes such as the position vecto, velocity, and acceleation without any insights
More informationInteraction of Feedforward and Feedback Streams in Visual Cortex in a Firing-Rate Model of Columnar Computations. ( r)
Supplementay mateial fo Inteaction of Feedfowad and Feedback Steams in Visual Cotex in a Fiing-Rate Model of Columna Computations Tobias Bosch and Heiko Neumann Institute fo Neual Infomation Pocessing
More informationThis brief note explains why the Michel-Levy colour chart for birefringence looks like this...
This bief note explains why the Michel-Levy colou chat fo biefingence looks like this... Theoy of Levy Colou Chat fo Biefingent Mateials Between Cossed Polas Biefingence = n n, the diffeence of the efactive
More informationChapter 5 Force and Motion
Chapte 5 Foce and Motion In chaptes 2 and 4 we have studied kinematics i.e. descibed the motion of objects using paametes such as the position vecto, velocity and acceleation without any insights as to
More informationThe American Community Survey Sample Design: An Experimental Springboard
The Ameican Communit Suve Sampe Design: An Epeimenta Spingboad Megha Joshipua, Steven Hefte U.S. Census Bueau 4600 Sive Hi Road Washington, D.C., 033 Megha..Joshipua@census.gov Steven..Hefte@census.gov
More informationTESTING THE VALIDITY OF THE EXPONENTIAL MODEL BASED ON TYPE II CENSORED DATA USING TRANSFORMED SAMPLE DATA
STATISTICA, anno LXXVI, n. 3, 2016 TESTING THE VALIDITY OF THE EXPONENTIAL MODEL BASED ON TYPE II CENSORED DATA USING TRANSFORMED SAMPLE DATA Hadi Alizadeh Noughabi 1 Depatment of Statistics, Univesity
More informationAdvanced Quantum Mechanics
Advanced Quantum Mechanics Rajdeep Sensama sensama@theoy.tif.es.in Scatteing Theoy Ref : Sakuai, Moden Quantum Mechanics Tayo, Quantum Theoy of Non-Reativistic Coisions Landau and Lifshitz, Quantum Mechanics
More informationCALCULUS II Vectors. Paul Dawkins
CALCULUS II Vectos Paul Dawkins Table of Contents Peface... ii Vectos... 3 Intoduction... 3 Vectos The Basics... 4 Vecto Aithmetic... 8 Dot Poduct... 13 Coss Poduct... 21 2007 Paul Dawkins i http://tutoial.math.lama.edu/tems.aspx
More informationSOME SOLVABILITY THEOREMS FOR NONLINEAR EQUATIONS
Fixed Point Theoy, Volume 5, No. 1, 2004, 71-80 http://www.math.ubbcluj.o/ nodeacj/sfptcj.htm SOME SOLVABILITY THEOREMS FOR NONLINEAR EQUATIONS G. ISAC 1 AND C. AVRAMESCU 2 1 Depatment of Mathematics Royal
More informationHOW TO TEACH THE FUNDAMENTALS OF INFORMATION SCIENCE, CODING, DECODING AND NUMBER SYSTEMS?
6th INTERNATIONAL MULTIDISCIPLINARY CONFERENCE HOW TO TEACH THE FUNDAMENTALS OF INFORMATION SCIENCE, CODING, DECODING AND NUMBER SYSTEMS? Cecília Sitkuné Göömbei College of Nyíegyháza Hungay Abstact: The
More informationTopic 4a Introduction to Root Finding & Bracketing Methods
/8/18 Couse Instucto D. Raymond C. Rumpf Office: A 337 Phone: (915) 747 6958 E Mail: cumpf@utep.edu Topic 4a Intoduction to Root Finding & Backeting Methods EE 4386/531 Computational Methods in EE Outline
More informationImplicit 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 informationAlternative Tests for the Poisson Distribution
Chiang Mai J Sci 015; 4() : 774-78 http://epgsciencecmuacth/ejounal/ Contibuted Pape Altenative Tests fo the Poisson Distibution Manad Khamkong*[a] and Pachitjianut Siipanich [b] [a] Depatment of Statistics,
More informationKOEBE DOMAINS FOR THE CLASSES OF FUNCTIONS WITH RANGES INCLUDED IN GIVEN SETS
Jounal of Applied Analysis Vol. 14, No. 1 2008), pp. 43 52 KOEBE DOMAINS FOR THE CLASSES OF FUNCTIONS WITH RANGES INCLUDED IN GIVEN SETS L. KOCZAN and P. ZAPRAWA Received Mach 12, 2007 and, in evised fom,
More information6 Matrix Concentration Bounds
6 Matix Concentation Bounds Concentation bounds ae inequalities that bound pobabilities of deviations by a andom vaiable fom some value, often its mean. Infomally, they show the pobability that a andom
More informationSupplementary 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 informationFI 2201 Electromagnetism
F Eectomagnetism exane. skana, Ph.D. Physics of Magnetism an Photonics Reseach Goup Magnetostatics MGNET VETOR POTENTL, MULTPOLE EXPNSON Vecto Potentia Just as E pemitte us to intouce a scaa potentia V
More informationUnobserved Correlation in Ascending Auctions: Example And Extensions
Unobseved Coelation in Ascending Auctions: Example And Extensions Daniel Quint Univesity of Wisconsin Novembe 2009 Intoduction In pivate-value ascending auctions, the winning bidde s willingness to pay
More informationControl Chart Analysis of E k /M/1 Queueing Model
Intenational OPEN ACCESS Jounal Of Moden Engineeing Reseach (IJMER Contol Chat Analysis of E /M/1 Queueing Model T.Poongodi 1, D. (Ms. S. Muthulashmi 1, (Assistant Pofesso, Faculty of Engineeing, Pofesso,
More informationMATH 172: CONVERGENCE OF THE FOURIER SERIES
MATH 72: CONVEGENCE OF THE FOUIE SEIES ANDÁS VASY We now discuss convegence of the Fouie seies on compact intevas I. Convegence depends on the notion of convegence we use, such as (i L 2 : u j u in L 2
More informationJournal of Inequalities in Pure and Applied Mathematics
Jounal of Inequalities in Pue and Applied Mathematics COEFFICIENT INEQUALITY FOR A FUNCTION WHOSE DERIVATIVE HAS A POSITIVE REAL PART S. ABRAMOVICH, M. KLARIČIĆ BAKULA AND S. BANIĆ Depatment of Mathematics
More informationOn intersecting a set of parallel line segments with a convex polygon of minimum area
On intesecting a set of aae ine segments with a convex oygon of minimum aea Asish Mukhoadhyay Schoo of Comute Science Univesity of Windso, Canada Eugene Geene Schoo of Comute Science Univesity of Windso,
More information1D2G - Numerical solution of the neutron diffusion equation
DG - Numeical solution of the neuton diffusion equation Y. Danon Daft: /6/09 Oveview A simple numeical solution of the neuton diffusion equation in one dimension and two enegy goups was implemented. Both
More informationBifurcation Analysis for the Delay Logistic Equation with Two Delays
IOSR Jounal of Mathematics (IOSR-JM) e-issn: 78-578, p-issn: 39-765X. Volume, Issue 5 Ve. IV (Sep. - Oct. 05), PP 53-58 www.iosjounals.og Bifucation Analysis fo the Delay Logistic Equation with Two Delays
More informationTHE 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 informationTo Feel a Force Chapter 7 Static equilibrium - torque and friction
To eel a oce Chapte 7 Chapte 7: Static fiction, toque and static equilibium A. Review of foce vectos Between the eath and a small mass, gavitational foces of equal magnitude and opposite diection act on
More informationLight Time Delay and Apparent Position
Light Time Delay and ppaent Position nalytical Gaphics, Inc. www.agi.com info@agi.com 610.981.8000 800.220.4785 Contents Intoduction... 3 Computing Light Time Delay... 3 Tansmission fom to... 4 Reception
More informationComputers 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 informationHydroelastic 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 informationChapter 5 Linear Equations: Basic Theory and Practice
Chapte 5 inea Equations: Basic Theoy and actice In this chapte and the next, we ae inteested in the linea algebaic equation AX = b, (5-1) whee A is an m n matix, X is an n 1 vecto to be solved fo, and
More information