MULTIDIMENSIONAL EXTENICS THEORY
|
|
- Alexia Hubbard
- 5 years ago
- Views:
Transcription
1 U.P.B. Sci. Bull., Series A, Vl. 75, Iss. 1, 213 ISSN MULTIDIMENSIONAL EXTENICS THEORY Ovidiu Ilie ŞANDRU 1, Luige VLǍDAREANU 2, Paul ŞCHIOPU 3, Victr VLǍDAREANU 4, Alexadra ŞANDRU 5 Î această lucrare vm extide teria Exteics de la cazul uidimesial cuscut î prezet la cazul -dimesial, > 1. Datritǎ imprtaţei pe care aceastǎ terie are î rezlvarea multr prbleme practice, extesia pe care realizǎm î acest articl ferǎ dmeiului aplicativ maximul de csisteţǎ tehicǎ pe care aceasta îl pate feri. This paper will exted Exteics Thery frm the e-dimesial case kw at preset t the -dimesial case, > 1. Due t the imprtace f this thery i slvig multiple practical prblems, the extesi preseted i this paper brigs a maximum f techical csistecy t the applicative field. Keywrds: Exteics thery, We idicatrs, dyamic systems with status idicatrs. 1. Itrducti Fr slvig certai paradxical prblems which are fte met i daily practice, Prf. Cai We develped a efficiet mathematical thery which he geerically amed Exteics, amely the sciece f extedig the meas f ivestigati used i classical mathematics 6. The results btaied up t the preset by Prf. Cai deal exclusively with prblems expressable by uidimesial mathematical mdels. Sice this restricts the area f applicability f a meas f ivestigati which eve uder these cditis prved t have widespread 1 Departmet f Mathematical Mdels ad Methds, Uiversity POLITEHNICA f Bucharest, 313 Splaiul Idepedeţei, 642 Bucharest, Rmaia, isadru@yah.cm. 2 Istitute f Slid Mechaics f Rmaia Academy, C-ti Mille 15, Bucharest 1, Rmaia, e- mail: luigiv@arexim.r. 3 Departmet f Electric Techlgy ad Reliability, Uiversity POLITEHNICA f Bucharest, Bd. Iuliu Maiu 1-3, Bucharest 6, Rmaia, schipu@tehfi.pub.r. 4 Departmet f Electric Techlgy ad Reliability, Uiversity POLITEHNICA f Bucharest, Bd. Iuliu Maiu 1-3, Bucharest 6, Rmaia, vladareauv@gmail.cm. 5 Departmet f Electric Techlgy ad Reliability, Uiversity POLITEHNICA f Bucharest, Bd. Iuliu Maiu 1-3, Bucharest 6, Rmaia, alexadra_sadru@yah.cm. 6 Fr further details this matter see papers [4, 9, 1, 11], where [9] represets the early wrk f prf. Cai We t which we shall refer expressly withi ur article ad [4, 1, 11] represet develpmets f the pits f view frmulated i [9] fllwed by umerus applicative examples particularly fr the egieerig field.
2 4 O. I. Şadru, L. Vlǎdareau, P. Şchipu, V. Vlǎdareau, A. Şadru applicatis 7 it is ly atural that e becmes ccered with its develpmet i a way that allws a geeralizati f the existig thery which wuld cmprise the practical prblems that eed t be mathematically expressed by multidimesial mdels 8. This paper attempts t d just that. As ca be see frm the ctet, the trasiti frm the uidimesial case t the multidimesial is either direct, as ituitive aspects d t fucti well withi the geeralizati prcess, r immediate, sice reachig the geeral cadre f the thery ecessitates a much mre sphisticated mathematical apparatus. 2. Maximal extesi f the ti f distace i Exteics Thery By d we dete the euclidea distace, i.e. 1/2 2 d( x, y) = ( yk xk), where x = ( x1 2 ) k = 1, x,.., x, ad y = ( y ) 1, y2,.., y represet tw pits frm. This thig allws us t csider the relati δ ( x, A) if d( x, y) =, y A which, as is kw, represets the distace frm pit x t the set A. I classical mathematics the ti f distace frm a give pit t a certai set f pits is sufficiet t express whether that pit belgs r t t the set csidered. I Exteics thery, the relati that ca exist betwee a pit x ad a set A is t be exteded, with the iteti f expressig mre tha the simple idea that x A r x A. I rder t btai this result we prpse replacig the idicatr δ defied earlier with the idicatr s defied as fllws: 7 See i this respect papers [1-7], [1-12]. 8 Preccupatis i this directi d t represet a tpic itrduced by us exclusively. The first iitiative f this kid belgs t prf. Freti Smaradache (see paper [8]) wh was able t develp prf Cai We s thery i tw particular directis: e referrig t the situati i which the sets f the csidered mathematical mdel have cetral symmetry ad the secd i which the prblems beig studied admit the s-called attracti pit priciple. Hwever, the thery preseted by us i this paper fudametally differs frm the apprach f prf. Smaradache ad the results that we btaied are i geeral, distict. Whe cmpared t the thery f prf. Smaradache, ur thery represets ather variat f geeralizig the thery f prf. Cai We, which leads t ther implicatis up the applicative field.
3 Multidimesial exteics thery 5 (, ), ( ) δ x A x A s ( xa, ) =, (1) δ x, A, x A where by A we deted the abslute cmplemet f A, i.e. A = \ A. We shall w shw that this ew idicatr keeps all the prperties f the idicatr ρ ( x, [ a, b] ) a+ b b a = x, (2) 2 2 itrduced by Cai We i [9] fr the particular case where x ad set A is a iterval f the real umbers set f the frm [ a, b ], with a< b, which it als geeralizes, i the sese that the restricti applied t ur idicatr, t the case studied by Prf. Cai, cicides with ρ. Ideed, the idicatr s verifies the prperties detailed belw: Prpsiti 1. Fr ay pit x ad ay set A, if x A, where with A is deted the iterir f the set A i tplgy iduced by the metric d fixed earlier the space s xa<,, ad reciprcally., the ( ) The prf f this setece results directly frm the defiiti f the idicatr s. Prpsiti 2. Fr ay pit ( ) x ad ay set A, we have x A s x, A >, where with A is ted the clsure f set A i tplgy iduced by metric d space. As earlier the prf f this setece results directly frm the defiiti f idicatr s. Prpsiti 3. Fr ay pit s xa, > s xb,, x. ( ) ( ) x ad ay sets A ad B i Prf. We eed t aalyze three distict cases., if A B the
4 6 O. I. Şadru, L. Vlǎdareau, P. Şchipu, V. Vlǎdareau, A. Şadru Case l. x A. Let x '' B s that δ ( x, B) = d( x, x'' ) ad x ' A s that the pits x, x', x '' be clliear, ad x ' be betwee x ad x '', see Figure 1 9. Uder δ x, A d x, x' < d x, x'' = δ x, B. It fllws these cditis ( ) ( ) ( ) ( ) s( x, A) > s ( x, B). Nte. The symbls A ad B used abve dete the budaries f sets A ad B respectively, meaig A = A\ A, respectively, B= B\ B. Case 2. x B\ A Fig. 1.. I this case we have δ ( x, A) δ ( x, B) ( x, A) > ( x, B) s s. See Fig. 2. >, r equivaletly, Fig Please te that bth figure 1 ad ther figures, t which we shall refer t hereiafter, d t exhaustively cver the multitude f all situatis evisaged by the demstrati (fr example sets A ad B must t ecessarily be f dmai type). The purpse f these figures is limited t ly prvidig a ituitive visual framewrk meat t help fix the ideas withi that demstrati.
5 Multidimesial exteics thery 7 Case 3. x B. Let x '' A s that d( x, x'' ) δ ( x, A) = ad x ' [ xx, ''] B, where [ x, x ''] represets the set f all pist f the straight lie determied by pits x ad x '' situated betwee x ad x ''. See Fig. 3. With this preamble we ca write δ ( x, A) = d( x, x'' ) > d( x, x' ) δ ( x, B), which meas s x, A > s x, B. ( ) ( ) Fig. 3. Prpsiti 4. I the particular case x, A [ a, b] idicatrs ρ ( x, A) ad s ( x, A) cicide. The prf t this affirmati results directly frm calculati. 3. Maximal extesi f the Cai We idicatr =, a, b, a < b, the With the help f the s idicatr we defied i the previus paragraph it is pssible t build a ew vital idicatr fr Exteics Thery, amely s( xa, ) S ( xab,, ) =, (3) s x, B s x, A ( ) ( ) defied fr ay x ad fr ay sets A ad B i fr which A B. This idicatr geeralizes the idicatr ρ ( xa, ) K( x, A, B) =, (4) ρ x, B ρ x, A ( ) ( )
6 8 O. I. Şadru, L. Vlǎdareau, P. Şchipu, V. Vlǎdareau, A. Şadru itrduced by Prf. Cai i [9] fr the case x, x, A = [ a, b ], B ( a, b) =, a, b, a, b, a< a < b < b. The idicatr S has all the prperties detailed belw. Prpsiti 5. Fr ay tw sets A ad B i fr which A B we have S x, AB, < 1, if x B 1 S xab,, <, if x B\ A S xab,,, if ( ) x A, ad reciprcally. ; ( ) ; ( ) Prf. Usig the prperties f the idicatr s detailed i the previus seteces it is easy t deduce that: I the first case where x B, we have s ( xa, ) > ad s ( xb, ) >. It s x, B + s x, A < s x, A. Takig it accut that fllws that ( ) ( ) ( ) ( xb, ) ( xa, ) < S ( xab,, ) < 1; I the secd case where x B\ A, we have s ( xb, ) ad ( ) Csequetly, ( x, B) + ( x, A) ( x, A) s( xb, ) s ( xa, ) <, we ca usually deduce that 1 S ( xab,, ) <. I the last case where x A, we have ( xa, ) s( xb, ) s ( xa, ) <, it ca be see immediately that S ( xab,, ). s s, (see Prpsiti 3) we btai the iequality s xa>,. s s s. Sice additially Prpsiti 6. I the particular case x, A [ a, b] ( a, b) < < <, the idicatrs K ( xab,, ) ad ( x, AB, ) a a b b s. Sice =, a, b, a, b, S cicide. Prf. I the hyptheses abve the idicatrs ρ ad s cicide (see Prpsiti 4). 4. Aplicati May f the state f the art techical istallatis such as thse which emit high itesity radiati brig abut areas which are dagerus fr humas. We shall assume that we wish t secure such a istallati thrugh a cetralized system usig electric sesrs which versees the dager areas ad depedig the gravity f the situati ca sed warig sigals fr users r eve stp the system. Fr this we shall te with X the area i the surrudig space
7 Multidimesial exteics thery 9 (mathematically mdeled thrugh 3 ) iside which the radiati is ver the admitted safety level ad with X, ( X X ) that area iside X i which the level f radiati is uacceptable (fatal) fr humas. The sesrs muted i the areas 3 \ X, X \ X ad X sed t the cetral mitrig ad ctrl uity the spatial crdiates f all perss implicated i the activity. The sftware applicati which iterprets the data received frm the sesrs must accmplish the fllwig fuctis: 1) Whe the spatial crdiates x = ( x1, x2 x3) f a user belg t the area 3 \ X, the istallati is allwed t fucti uimpeded; 2) Whe the spatial crdiates x = ( x1, x2 x3) f a user belg t the area X \ X, the verseer system must sed warig sigals; 3) Whe the spatial crdiates x = ( x1, x2 x3) f a user belg t the area X, the verseer system must stp the istallati. Prducig such a sftware applicati is much simplified by usig the idicatr S ( x, X, X) which was defied earlier i relati (3) i which A = X ad B X S x t, X, X < 1, fr ay =. Ideed, accrdig t Prpsiti 5, if ( a ( ) ) a A, where by A we have deted the set f emplyees servig the istallati which we refer t ad by xa ( t ) the spatial crdiates f the emplyee a at the mmet t, the mitrig ad ctrl system will t sed ut a warig sigal the istallati is left t fucti at rmal capacity; if S ( xa ( t), X, X) [ 1,) fr at least a a A, the the mitrig ad ctrl system seds ut warig sigals fr the istallati users, but the istallati is allwed t ctiue fuctiig; if S ( xa ( t), X, X) fr at least a a A, the the cetralized cmmad system stps the istallati ucditially. The prblem aalyzed previusly referred t the simple case f a techlgical istallati with ly e risk factr. The sluti preseted ca be exteded t the geeral case f istallatis ctaiig multiple risk factrs. T exemplify this we shall aalyze the case f a similar istallati, but with > 1 surces f radiati. The iteded gal is the same as i the case previusly studied: desigig a mitrig system which will war f apprach it dagerus areas ad if ecessary iterrupt the use f thse radiati surces which culd edager humas. I rder t fix the ideas we shall suppse X1, X2,.., X t be the dager areas distributed fr each f the surces f the istallati which emit radiati ad X1, X2,.., X ( X1 X1, X2 X 2,.., X X ) t be the areas i their immediate veciity f their surces, where the dager fr persel
8 1 O. I. Şadru, L. Vlǎdareau, P. Şchipu, V. Vlǎdareau, A. Şadru is maximum. Oce these zes are established, we may the csider, fr each f the alarms systems f the istallati, a idicatr ( ) s( xx, k ) ( xx, ) s( xx, ) S x, Xk, Xk =, k = 1,2,..,, (5) s k f the frm csidered earlier i the case f a e-surce istallati. The alarm systems are desiged t fucti accrdig t the same priciple as i the case f ly e alarm system, but idepedetly frm e ather, thus, if at a certai amut f time t all idicatrs S ( xa( t), Xk, Xk), k = 1, 2,..,, are strictly smaller tha 1 fr ay a A, where A is the set f persel, ad xa () t are the spatial crdiates f emplyee a at time t, the the techlgical prcess is left uimpeded; if at a certai time t there is a A fr which e r mre f the idicatrs S ( xa( t), Xk, Xk), k = 1,2,..,, have values betwee 1, iclusively, ad, exclusively, the the mitrig system r systems i that area will sed ut warig sigals; ad if at a certai time t there is a A fr which e r mre f the idicatrs S ( xa( t), Xk, Xk), k = 1,2,..,, have values greater r equal t the the mitrig ad ctrl system r systems i thse areas will autmatically stp this r these surces f radiati emissi. I the case f the system with mre degrees f freedm i regards t the pssibility f prducig a uwated icidet, situatis may arise which are yet mre cmplicated t mitr. Fr example, i a istallati with, > 1 risk factrs, if stppig a certai subsystem f the istallati is impssible (fr techical reass r thse relatig t disaster preveti) uless the etire istallati is stpped, the the mitrig ad ctrl systems f the istallati, which supervise (each f them) the surces f ptetial dager, will have t dispse f a relative idepedece f acti ly, a cetral uit fr ctrl ad mitrig beig required t sythesize the ifrmati frm the lcal mitrig systems. Mrever, this cetral uit must have the pwer t verride the lcal systems whe the situati requires a verall iterrupti f the istallati. I rder t realize such a mitrig system we wuld prpse that the lcal mitrig ad ctrl systems are equipped with a idicatr f the frm (5), ad the cetral uit with a tempral idicatr f the frm: () ( () ) k { a k k k, a } S t = sup S x t, X, X 1 A. Parameter t appearig abve desigates the mmet i time at which the mitrig is made.
9 Multidimesial exteics thery 11 The fuctiig priciple f the prtecti system: As lg as idicatr S() t is strictly egative, the lcal mitrig systems are allwed t act idepedetly (meaig they will sigal, wheever ecessary, the presece f persel i the mderate risk areas Xk \ Xk, k = 1,2,.., ). Hwever, whe a critical situati arises, where the idicatr S( t ) wuld have a value greater r equal t, the cetralized safety system wuld cmmad the iterrupti f the etire istallati. 5. Cmmets The applicable examples f the idicatrs ( x, X, X) ( xa() t X k Xk) k, a { } S ad S() t = = sup S,, 1 A respectively, give i the previus paragraph suggest the itrducti f a ew ccept i the thery f dyamic systems, that f dyamic system with status idicatr 1. By this ti a imprtat class f systems ca be delimitated withi dyamic systems, which, by the status idicatrs they are edwed with, ca beefit frm special methds t slve a great umber f specific issues, such as thse related t the real-time quality ctrl prcess regardig their w fuctiig. R E F E R E N C E S [1] He Bi, Zhu Xuefeg, Hybrid Extesi ad Adaptive Ctrl, Ctrl Thery & Applicatis,25,22 (2), [2] Zhi Che, Ygqua Yu, T Fid the Key Matter-Elemet Research f Extesi Detectig, It. Cf. Cmputer, Cmmuicati ad Ctrl Techlgies (CCCT), Flrida, USA, 23, 7. [3] Wg Chigchag,Che Jeyag, Adaptive Extesi Ctrller Desig fr Nliear Systems, Egieerig Sciece, 21,3(7), [4] Yag Chuya, Cai We, Extesi Egieerig, Sciece Press, Beijig, 22. [5] Yag Chuya, Li Weihua, Li Xiamei, Recet Research Prgress i Theries ad Methds fr the Itelliget Dispsal f Ctradictry Prblems, Jural f Guagdg Uiversity f Techlgy,211, 28 (1), [6] Gua Feg-Xu, Wag Ke-Ju, Study Extesi Ctrl Strategy f Pedulum System, Jural f Harbi Istitute f Techlgy, 26,38 (7), I a very abstract maer the ti f dyamic system edwed with status idicatr assumes, by defiiti, the existece f a set ( ), Σ I made up f a dyamic system Σ ad a idicatr I f the states which the system Σ passes thrugh durig its fuctiig.
10 12 O. I. Şadru, L. Vlǎdareau, P. Şchipu, V. Vlǎdareau, A. Şadru [7] Che Jeyag, Wg Chigchag, Extesi Ctrller Desig via Slidig Mde Ctrl, Egieerig Sciece, 21,3 (7), [8] Flreti Smaradache, Geeralizatis f the Distace ad Depedet Fucti i Exteics t 2D, 3D, ad -D, vixra.rg, [9] Cai We, Extesi Set ad N-Cmpatible Prblems, Advaces i Applied Mathematics ad Mechaics i Chia, Pekig: Iteratial Academic Publishers, 199,1-21. [1] Cai We, Extesi Thery ad Its Applicati, Chiese Sciece Bulleti,1999, 44 (17), [11] Cai We, Shi Yg, Exteics, its Sigificace i Sciece ad Prspects i Applicati, Jural Of Harbi Istitute f Techlgy, 26, 38 (7): [12] Zha Yawei, Study f Cceptual Desig f Extesi fr Mechaical Prducts, Egieerig Sciece,21, 18 (6),
Multi-objective Programming Approach for. Fuzzy Linear Programming Problems
Applied Mathematical Scieces Vl. 7 03. 37 8-87 HIKARI Ltd www.m-hikari.cm Multi-bective Prgrammig Apprach fr Fuzzy Liear Prgrammig Prblems P. Padia Departmet f Mathematics Schl f Advaced Scieces VIT Uiversity
More informationChapter 3.1: Polynomial Functions
Ntes 3.1: Ply Fucs Chapter 3.1: Plymial Fuctis I Algebra I ad Algebra II, yu ecutered sme very famus plymial fuctis. I this secti, yu will meet may ther members f the plymial family, what sets them apart
More informationBIO752: Advanced Methods in Biostatistics, II TERM 2, 2010 T. A. Louis. BIO 752: MIDTERM EXAMINATION: ANSWERS 30 November 2010
BIO752: Advaced Methds i Bistatistics, II TERM 2, 2010 T. A. Luis BIO 752: MIDTERM EXAMINATION: ANSWERS 30 Nvember 2010 Questi #1 (15 pits): Let X ad Y be radm variables with a jit distributi ad assume
More informationSolutions. Definitions pertaining to solutions
Slutis Defiitis pertaiig t slutis Slute is the substace that is disslved. It is usually preset i the smaller amut. Slvet is the substace that des the disslvig. It is usually preset i the larger amut. Slubility
More informationENGI 4421 Central Limit Theorem Page Central Limit Theorem [Navidi, section 4.11; Devore sections ]
ENGI 441 Cetral Limit Therem Page 11-01 Cetral Limit Therem [Navidi, secti 4.11; Devre sectis 5.3-5.4] If X i is t rmally distributed, but E X i, V X i ad is large (apprximately 30 r mre), the, t a gd
More informationIntermediate Division Solutions
Itermediate Divisi Slutis 1. Cmpute the largest 4-digit umber f the frm ABBA which is exactly divisible by 7. Sluti ABBA 1000A + 100B +10B+A 1001A + 110B 1001 is divisible by 7 (1001 7 143), s 1001A is
More informationA New Method for Finding an Optimal Solution. of Fully Interval Integer Transportation Problems
Applied Matheatical Scieces, Vl. 4, 200,. 37, 89-830 A New Methd fr Fidig a Optial Sluti f Fully Iterval Iteger Trasprtati Prbles P. Padia ad G. Nataraja Departet f Matheatics, Schl f Advaced Scieces,
More informationQuantum Mechanics for Scientists and Engineers. David Miller
Quatum Mechaics fr Scietists ad Egieers David Miller Time-depedet perturbati thery Time-depedet perturbati thery Time-depedet perturbati basics Time-depedet perturbati thery Fr time-depedet prblems csider
More informationGrade 3 Mathematics Course Syllabus Prince George s County Public Schools
Ctet Grade 3 Mathematics Curse Syllabus Price Gerge s Cuty Public Schls Prerequisites: Ne Curse Descripti: I Grade 3, istructial time shuld fcus fur critical areas: (1) develpig uderstadig f multiplicati
More informationD.S.G. POLLOCK: TOPICS IN TIME-SERIES ANALYSIS STATISTICAL FOURIER ANALYSIS
STATISTICAL FOURIER ANALYSIS The Furier Represetati f a Sequece Accrdig t the basic result f Furier aalysis, it is always pssible t apprximate a arbitrary aalytic fucti defied ver a fiite iterval f the
More informationENGI 4421 Central Limit Theorem Page Central Limit Theorem [Navidi, section 4.11; Devore sections ]
ENGI 441 Cetral Limit Therem Page 11-01 Cetral Limit Therem [Navidi, secti 4.11; Devre sectis 5.3-5.4] If X i is t rmally distributed, but E X i, V X i ad is large (apprximately 30 r mre), the, t a gd
More informationFourier Method for Solving Transportation. Problems with Mixed Constraints
It. J. Ctemp. Math. Scieces, Vl. 5, 200,. 28, 385-395 Furier Methd fr Slvig Trasprtati Prblems with Mixed Cstraits P. Padia ad G. Nataraja Departmet f Mathematics, Schl f Advaced Scieces V I T Uiversity,
More informationMATH Midterm Examination Victor Matveev October 26, 2016
MATH 33- Midterm Examiati Victr Matveev Octber 6, 6. (5pts, mi) Suppse f(x) equals si x the iterval < x < (=), ad is a eve peridic extesi f this fucti t the rest f the real lie. Fid the csie series fr
More informationAxial Temperature Distribution in W-Tailored Optical Fibers
Axial Temperature Distributi i W-Tailred Optical ibers Mhamed I. Shehata (m.ismail34@yah.cm), Mustafa H. Aly(drmsaly@gmail.cm) OSA Member, ad M. B. Saleh (Basheer@aast.edu) Arab Academy fr Sciece, Techlgy
More informationESWW-2. Israeli semi-underground great plastic scintillation multidirectional muon telescope (ISRAMUTE) for space weather monitoring and forecasting
ESWW-2 Israeli semi-udergrud great plastic scitillati multidirectial mu telescpe (ISRAMUTE) fr space weather mitrig ad frecastig L.I. Drma a,b, L.A. Pustil'ik a, A. Sterlieb a, I.G. Zukerma a (a) Israel
More informationActive redundancy allocation in systems. R. Romera; J. Valdés; R. Zequeira*
Wrkig Paper -6 (3) Statistics ad Ecmetrics Series March Departamet de Estadística y Ecmetría Uiversidad Carls III de Madrid Calle Madrid, 6 893 Getafe (Spai) Fax (34) 9 64-98-49 Active redudacy allcati
More informationK [f(t)] 2 [ (st) /2 K A GENERALIZED MEIJER TRANSFORMATION. Ku(z) ()x) t -)-I e. K(z) r( + ) () (t 2 I) -1/2 e -zt dt, G. L. N. RAO L.
Iterat. J. Math. & Math. Scl. Vl. 8 N. 2 (1985) 359-365 359 A GENERALIZED MEIJER TRANSFORMATION G. L. N. RAO Departmet f Mathematics Jamshedpur C-perative Cllege f the Rachi Uiversity Jamshedpur, Idia
More informationComparative analysis of bayesian control chart estimation and conventional multivariate control chart
America Jural f Theretical ad Applied Statistics 3; ( : 7- ublished lie Jauary, 3 (http://www.sciecepublishiggrup.cm//atas di:.648/.atas.3. Cmparative aalysis f bayesia ctrl chart estimati ad cvetial multivariate
More informationCh. 1 Introduction to Estimation 1/15
Ch. Itrducti t stimati /5 ample stimati Prblem: DSB R S f M f s f f f ; f, φ m tcsπf t + φ t f lectrics dds ise wt usually white BPF & mp t s t + w t st. lg. f & φ X udi mp cs π f + φ t Oscillatr w/ f
More informationMean residual life of coherent systems consisting of multiple types of dependent components
Mea residual life f cheret systems csistig f multiple types f depedet cmpets Serka Eryilmaz, Frak P.A. Cle y ad Tahai Cle-Maturi z February 20, 208 Abstract Mea residual life is a useful dyamic characteristic
More information5.1 Two-Step Conditional Density Estimator
5.1 Tw-Step Cditial Desity Estimatr We ca write y = g(x) + e where g(x) is the cditial mea fucti ad e is the regressi errr. Let f e (e j x) be the cditial desity f e give X = x: The the cditial desity
More informationClaude Elysée Lobry Université de Nice, Faculté des Sciences, parc Valrose, NICE, France.
CHAOS AND CELLULAR AUTOMATA Claude Elysée Lbry Uiversité de Nice, Faculté des Scieces, parc Valrse, 06000 NICE, Frace. Keywrds: Chas, bifurcati, cellularautmata, cmputersimulatis, dyamical system, ifectius
More informationIJISET - International Journal of Innovative Science, Engineering & Technology, Vol. 2 Issue 12, December
IJISET - Iteratial Jural f Ivative Sciece, Egieerig & Techlgy, Vl Issue, December 5 wwwijisetcm ISSN 48 7968 Psirmal ad * Pararmal mpsiti Operatrs the Fc Space Abstract Dr N Sivamai Departmet f athematics,
More informationThe Molecular Diffusion of Heat and Mass from Two Spheres
Iteratial Jural f Mder Studies i Mechaical Egieerig (IJMSME) Vlume 4, Issue 1, 018, PP 4-8 ISSN 454-9711 (Olie) DOI: http://dx.di.rg/10.0431/454-9711.0401004 www.arcjurals.rg The Mlecular Diffusi f Heat
More information[1 & α(t & T 1. ' ρ 1
NAME 89.304 - IGNEOUS & METAMORPHIC PETROLOGY DENSITY & VISCOSITY OF MAGMAS I. Desity The desity (mass/vlume) f a magma is a imprtat parameter which plays a rle i a umber f aspects f magma behavir ad evluti.
More informationEvery gas consists of a large number of small particles called molecules moving with very high velocities in all possible directions.
Kietic thery f gases ( Kietic thery was develped by Berlli, Jle, Clasis, axwell ad Bltzma etc. ad represets dyamic particle r micrscpic mdel fr differet gases sice it thrws light the behir f the particles
More informationStudy of Energy Eigenvalues of Three Dimensional. Quantum Wires with Variable Cross Section
Adv. Studies Ther. Phys. Vl. 3 009. 5 3-0 Study f Eergy Eigevalues f Three Dimesial Quatum Wires with Variale Crss Secti M.. Sltai Erde Msa Departmet f physics Islamic Aad Uiversity Share-ey rach Ira alrevahidi@yah.cm
More informationON FREE RING EXTENSIONS OF DEGREE N
I terat. J. Math. & Mah. Sci. Vl. 4 N. 4 (1981) 703-709 703 ON FREE RING EXTENSIONS OF DEGREE N GEORGE SZETO Mathematics Departmet Bradley Uiversity Peria, Illiis 61625 U.S.A. (Received Jue 25, 1980) ABSTRACT.
More informationAuthor. Introduction. Author. o Asmir Tobudic. ISE 599 Computational Modeling of Expressive Performance
ISE 599 Cmputatial Mdelig f Expressive Perfrmace Playig Mzart by Aalgy: Learig Multi-level Timig ad Dyamics Strategies by Gerhard Widmer ad Asmir Tbudic Preseted by Tsug-Ha (Rbert) Chiag April 5, 2006
More informationFourier Series & Fourier Transforms
Experimet 1 Furier Series & Furier Trasfrms MATLAB Simulati Objectives Furier aalysis plays a imprtat rle i cmmuicati thery. The mai bjectives f this experimet are: 1) T gai a gd uderstadig ad practice
More informationMATHEMATICS 9740/01 Paper 1 14 Sep hours
Cadidate Name: Class: JC PRELIMINARY EXAM Higher MATHEMATICS 9740/0 Paper 4 Sep 06 3 hurs Additial Materials: Cver page Aswer papers List f Frmulae (MF5) READ THESE INSTRUCTIONS FIRST Write yur full ame
More informationStudy in Cylindrical Coordinates of the Heat Transfer Through a Tow Material-Thermal Impedance
Research ural f Applied Scieces, Egieerig ad echlgy (): 9-63, 3 ISSN: 4-749; e-issn: 4-7467 Maxwell Scietific Orgaiati, 3 Submitted: uly 4, Accepted: September 8, Published: May, 3 Study i Cylidrical Crdiates
More information5.80 Small-Molecule Spectroscopy and Dynamics
MIT OpeCurseWare http://cw.mit.edu 5.8 Small-Mlecule Spectrscpy ad Dyamics Fall 8 Fr ifrmati abut citig these materials r ur Terms f Use, visit: http://cw.mit.edu/terms. 5.8 Lecture #33 Fall, 8 Page f
More informationThe generalized marginal rate of substitution
Jural f Mathematical Ecmics 31 1999 553 560 The geeralized margial rate f substituti M Besada, C Vazuez ) Facultade de Ecmicas, UiÕersidade de Vig, Aptd 874, 3600 Vig, Spai Received 31 May 1995; accepted
More informationMarkov processes and the Kolmogorov equations
Chapter 6 Markv prcesses ad the Klmgrv equatis 6. Stchastic Differetial Equatis Csider the stchastic differetial equati: dx(t) =a(t X(t)) dt + (t X(t)) db(t): (SDE) Here a(t x) ad (t x) are give fuctis,
More informationUnifying the Derivations for. the Akaike and Corrected Akaike. Information Criteria. from Statistics & Probability Letters,
Uifyig the Derivatis fr the Akaike ad Crrected Akaike Ifrmati Criteria frm Statistics & Prbability Letters, Vlume 33, 1997, pages 201{208. by Jseph E. Cavaaugh Departmet f Statistics, Uiversity f Missuri,
More informationA Hartree-Fock Calculation of the Water Molecule
Chemistry 460 Fall 2017 Dr. Jea M. Stadard Nvember 29, 2017 A Hartree-Fck Calculati f the Water Mlecule Itrducti A example Hartree-Fck calculati f the water mlecule will be preseted. I this case, the water
More informationThe Excel FFT Function v1.1 P. T. Debevec February 12, The discrete Fourier transform may be used to identify periodic structures in time ht.
The Excel FFT Fucti v P T Debevec February 2, 26 The discrete Furier trasfrm may be used t idetify peridic structures i time ht series data Suppse that a physical prcess is represeted by the fucti f time,
More informationE o and the equilibrium constant, K
lectrchemical measuremets (Ch -5 t 6). T state the relati betwee ad K. (D x -b, -). Frm galvaic cell vltage measuremet (a) K sp (D xercise -8, -) (b) K sp ad γ (D xercise -9) (c) K a (D xercise -G, -6)
More informationEfficient Processing of Continuous Reverse k Nearest Neighbor on Moving Objects in Road Networks
Iteratial Jural f Ge-Ifrmati Article Efficiet Prcessig f Ctiuus Reverse k Nearest Neighbr Mvig Objects i Rad Netwrks Muhammad Attique, Hyug-Ju Ch, Rize Ji ad Tae-Su Chug, * Departmet f Cmputer Egieerig,
More informationFunction representation of a noncommutative uniform algebra
Fucti represetati f a cmmutative uifrm algebra Krzysztf Jarsz Abstract. We cstruct a Gelfad type represetati f a real cmmutative Baach algebra A satisfyig f 2 = kfk 2, fr all f 2 A:. Itrducti A uifrm algebra
More informationA unified brittle fracture criterion for structures with sharp V-notches under mixed mode loading
Jural f Mechaical Sciece ad Techlgy Jural f Mechaical Sciece ad Techlgy 22 (2008) 269~278 www.sprigerlik.cm/ctet/738-494x A uified brittle fracture criteri fr structures with sharp V-tches uder mixed mde
More informationWEST VIRGINIA UNIVERSITY
WEST VIRGINIA UNIVERSITY PLASMA PHYSICS GROUP INTERNAL REPORT PL - 045 Mea Optical epth ad Optical Escape Factr fr Helium Trasitis i Helic Plasmas R.F. Bivi Nvember 000 Revised March 00 TABLE OF CONTENT.0
More information, the random variable. and a sample size over the y-values 0:1:10.
Lecture 3 (4//9) 000 HW PROBLEM 3(5pts) The estimatr i (c) f PROBLEM, p 000, where { } ~ iid bimial(,, is 000 e f the mst ppular statistics It is the estimatr f the ppulati prprti I PROBLEM we used simulatis
More informationDirectional Duality Theory
Suther Illiis Uiversity Carbdale OpeSIUC Discussi Papers Departmet f Ecmics 2004 Directial Duality Thery Daiel Primt Suther Illiis Uiversity Carbdale Rlf Fare Oreg State Uiversity Fllw this ad additial
More informationOn the affine nonlinearity in circuit theory
O the affie liearity i circuit thery Emauel Gluski The Kieret Cllege the Sea f Galilee; ad Ort Braude Cllege (Carmiel), Israel. gluski@ee.bgu.ac.il; http://www.ee.bgu.ac.il/~gluski/ E. Gluski, O the affie
More informationDistributed Trajectory Generation for Cooperative Multi-Arm Robots via Virtual Force Interactions
862 IEEE TRANSACTIONS ON SYSTEMS, MAN, AND CYBERNETICS PART B: CYBERNETICS, VOL. 27, NO. 5, OCTOBER 1997 Distributed Trajectry Geerati fr Cperative Multi-Arm Rbts via Virtual Frce Iteractis Tshi Tsuji,
More informationSuper-efficiency Models, Part II
Super-efficiec Mdels, Part II Emilia Niskae The 4th f Nvember S steemiaalsi Ctets. Etesis t Variable Returs-t-Scale (0.4) S steemiaalsi Radial Super-efficiec Case Prblems with Radial Super-efficiec Case
More informationPhysical Chemistry Laboratory I CHEM 445 Experiment 2 Partial Molar Volume (Revised, 01/13/03)
Physical Chemistry Labratry I CHEM 445 Experimet Partial Mlar lume (Revised, 0/3/03) lume is, t a gd apprximati, a additive prperty. Certaily this apprximati is used i preparig slutis whse ccetratis are
More informationare specified , are linearly independent Otherwise, they are linearly dependent, and one is expressed by a linear combination of the others
Chater 3. Higher Order Liear ODEs Kreyszig by YHLee;4; 3-3. Hmgeeus Liear ODEs The stadard frm f the th rder liear ODE ( ) ( ) = : hmgeeus if r( ) = y y y y r Hmgeeus Liear ODE: Suersiti Pricile, Geeral
More informationSound Absorption Characteristics of Membrane- Based Sound Absorbers
Purdue e-pubs Publicatis f the Ray W. Schl f Mechaical Egieerig 8-28-2003 Sud Absrpti Characteristics f Membrae- Based Sud Absrbers J Stuart Blt, blt@purdue.edu Jih Sg Fllw this ad additial wrks at: http://dcs.lib.purdue.edu/herrick
More informationALE 26. Equilibria for Cell Reactions. What happens to the cell potential as the reaction proceeds over time?
Name Chem 163 Secti: Team Number: AL 26. quilibria fr Cell Reactis (Referece: 21.4 Silberberg 5 th editi) What happes t the ptetial as the reacti prceeds ver time? The Mdel: Basis fr the Nerst quati Previusly,
More informationUNIVERSITY OF TECHNOLOGY. Department of Mathematics PROBABILITY THEORY, STATISTICS AND OPERATIONS RESEARCH GROUP. Memorandum COSOR 76-10
EI~~HOVEN UNIVERSITY OF TECHNOLOGY Departmet f Mathematics PROBABILITY THEORY, STATISTICS AND OPERATIONS RESEARCH GROUP Memradum COSOR 76-10 O a class f embedded Markv prcesses ad recurrece by F.H. Sims
More informationA Study on Estimation of Lifetime Distribution with Covariates Under Misspecification
Prceedigs f the Wrld Cgress Egieerig ad Cmputer Sciece 2015 Vl II, Octber 21-23, 2015, Sa Fracisc, USA A Study Estimati f Lifetime Distributi with Cvariates Uder Misspecificati Masahir Ykyama, Member,
More informationUnit -2 THEORY OF DILUTE SOLUTIONS
Uit - THEORY OF DILUTE SOLUTIONS 1) hat is sluti? : It is a hmgeus mixture f tw r mre cmpuds. ) hat is dilute sluti? : It is a sluti i which slute ccetrati is very less. 3) Give a example fr slid- slid
More informationExamination No. 3 - Tuesday, Nov. 15
NAME (lease rit) SOLUTIONS ECE 35 - DEVICE ELECTRONICS Fall Semester 005 Examiati N 3 - Tuesday, Nv 5 3 4 5 The time fr examiati is hr 5 mi Studets are allwed t use 3 sheets f tes Please shw yur wrk, artial
More informationChapter 5. Root Locus Techniques
Chapter 5 Rt Lcu Techique Itrducti Sytem perfrmace ad tability dt determied dby cled-lp l ple Typical cled-lp feedback ctrl ytem G Ope-lp TF KG H Zer -, - Ple 0, -, - K Lcati f ple eaily fud Variati f
More informationCold mirror based on High-Low-High refractive index dielectric materials
Cld mirrr based High-Lw-High refractive idex dielectric materials V.V. Elyuti.A. Butt S.N. Khia Samara Natial Research Uiversity 34 skvske Shsse 443086 Samara Russia Image Prcessig Systems Istitute Brach
More informationx 2 x 3 x b 0, then a, b, c log x 1 log z log x log y 1 logb log a dy 4. dx As tangent is perpendicular to the x axis, slope
The agle betwee the tagets draw t the parabla y = frm the pit (-,) 5 9 6 Here give pit lies the directri, hece the agle betwee the tagets frm that pit right agle Ratig :EASY The umber f values f c such
More informationGeneral Chemistry 1 (CHEM1141) Shawnee State University Fall 2016
Geeral Chemistry 1 (CHEM1141) Shawee State Uiversity Fall 2016 September 23, 2016 Name E x a m # I C Please write yur full ame, ad the exam versi (IC) that yu have the scatr sheet! Please 0 check the bx
More informationFrequency-Domain Study of Lock Range of Injection-Locked Non- Harmonic Oscillators
0 teratial Cferece mage Visi ad Cmputig CVC 0 PCST vl. 50 0 0 ACST Press Sigapre DO: 0.776/PCST.0.V50.6 Frequecy-Dmai Study f Lck Rage f jecti-lcked N- armic Oscillatrs Yushi Zhu ad Fei Yua Departmet f
More informationWavelet Video with Unequal Error Protection Codes in W-CDMA System and Fading Channels
Wavelet Vide with Uequal Errr Prtecti Cdes i W-CDMA System ad Fadig Chaels MINH HUNG LE ad RANJITH LIYANA-PATHIRANA Schl f Egieerig ad Idustrial Desig Cllege f Sciece, Techlgy ad Evirmet Uiversity f Wester
More informationA Simplified Nonlinear Generalized Maxwell Model for Predicting the Time Dependent Behavior of Viscoelastic Materials
Wrld Jural f Mechaics, 20,, 58-67 di:0.4236/wj.20.302 Published Olie Jue 20 (http://www.scirp.rg/jural/wj) A Siplified Nliear Geeralized Maxwell Mdel fr Predictig the Tie Depedet Behavir f Viscelastic
More informationLecture 21: Signal Subspaces and Sparsity
ECE 830 Fall 00 Statistical Sigal Prcessig istructr: R. Nwak Lecture : Sigal Subspaces ad Sparsity Sigal Subspaces ad Sparsity Recall the classical liear sigal mdel: X = H + w, w N(0, where S = H, is a
More informationAn S-type upper bound for the largest singular value of nonnegative rectangular tensors
Ope Mat. 06 4 95 933 Ope Matematics Ope Access Researc Article Jiaxig Za* ad Caili Sag A S-type upper bud r te largest sigular value egative rectagular tesrs DOI 0.55/mat-06-0085 Received August 3, 06
More informationFull algebra of generalized functions and non-standard asymptotic analysis
Full algebra f geeralized fuctis ad -stadard asympttic aalysis Tdr D. Tdrv Has Veraeve Abstract We cstruct a algebra f geeralized fuctis edwed with a caical embeddig f the space f Schwartz distributis.
More informationDeclarative approach to cyclic steady state space refinement: periodic process scheduling
It J Adv Mauf Techl DOI 10.1007/s00170-013-4760-0 ORIGINAL ARTICLE Declarative apprach t cyclic steady state space refiemet: peridic prcess schedulig Grzegrz Bcewicz Zbigiew A. Baaszak Received: 16 April
More informationAP Statistics Notes Unit Eight: Introduction to Inference
AP Statistics Ntes Uit Eight: Itrducti t Iferece Syllabus Objectives: 4.1 The studet will estimate ppulati parameters ad margis f errrs fr meas. 4.2 The studet will discuss the prperties f pit estimatrs,
More informationThe Acoustical Physics of a Standing Wave Tube
UIUC Physics 93POM/Physics 406POM The Physics f Music/Physics f Musical Istrumets The Acustical Physics f a Stadig Wave Tube A typical cylidrical-shaped stadig wave tube (SWT) {aa impedace tube} f legth
More informationThe Simple Linear Regression Model: Theory
Chapter 3 The mple Lear Regress Mdel: Ther 3. The mdel 3.. The data bservats respse varable eplaatr varable : : Plttg the data.. Fgure 3.: Dsplag the cable data csdered b Che at al (993). There are 79
More informationControl Systems. Controllability and Observability (Chapter 6)
6.53 trl Systems trllaility ad Oservaility (hapter 6) Geeral Framewrk i State-Spae pprah Give a LTI system: x x u; y x (*) The system might e ustale r des t meet the required perfrmae spe. Hw a we imprve
More informationPartial-Sum Queries in OLAP Data Cubes Using Covering Codes
326 IEEE TRANSACTIONS ON COMPUTERS, VOL. 47, NO. 2, DECEMBER 998 Partial-Sum Queries i OLAP Data Cubes Usig Cverig Cdes Chig-Tie H, Member, IEEE, Jehshua Bruck, Seir Member, IEEE, ad Rakesh Agrawal, Seir
More informationModern Physics. Unit 15: Nuclear Structure and Decay Lecture 15.2: The Strong Force. Ron Reifenberger Professor of Physics Purdue University
Mder Physics Uit 15: Nuclear Structure ad Decay Lecture 15.: The Strg Frce R Reifeberger Prfessr f Physics Purdue Uiversity 1 Bidig eergy er ucle - the deuter Eergy (MeV) ~0.4fm B.E. A =.MeV/ = 1.1 MeV/ucle.
More informationNUROP CONGRESS PAPER CHINESE PINYIN TO CHINESE CHARACTER CONVERSION
NUROP Chinese Pinyin T Chinese Character Cnversin NUROP CONGRESS PAPER CHINESE PINYIN TO CHINESE CHARACTER CONVERSION CHIA LI SHI 1 AND LUA KIM TENG 2 Schl f Cmputing, Natinal University f Singapre 3 Science
More informationON THE M 3 M 1 QUESTION
Vlume 5, 1980 Pages 77 104 http://tplgy.aubur.edu/tp/ ON THE M 3 M 1 QUESTION by Gary Gruehage Tplgy Prceedigs Web: http://tplgy.aubur.edu/tp/ Mail: Tplgy Prceedigs Departmet f Mathematics & Statistics
More informationDYNAMICAL SYSTEMS DETERMINABLE BY DISCRETE SAMPLES
SISOM ad Sessio of the Commissio of Acoustics Bucharest 5-6 May DYNAMICAL SYSTEMS DETERMINABLE BY DISCRETE SAMPLES Ovidiu Ilie ŞANDRU Luige VLĂDĂREANU Alexadra ŞANDRU 3 Departmet of Mathematics II Politehica
More informationPipe Networks - Hardy Cross Method Page 1. Pipe Networks
Pie Netwrks - Hardy Crss etd Page Pie Netwrks Itrducti A ie etwrk is a itercected set f ies likig e r mre surces t e r mre demad (delivery) its, ad ca ivlve ay umber f ies i series, bracig ies, ad arallel
More informationIdentical Particles. We would like to move from the quantum theory of hydrogen to that for the rest of the periodic table
We wuld like t ve fr the quatu thery f hydrge t that fr the rest f the peridic table Oe electr at t ultielectr ats This is cplicated by the iteracti f the electrs with each ther ad by the fact that the
More informationCopyright 1978, by the author(s). All rights reserved.
Cpyright 1978, by the authr(s). All rights reserved. Permissi t make digital r hard cpies f all r part f this wrk fr persal r classrm use is grated withut fee prvided that cpies are t made r distributed
More information(A sequence also can be thought of as the list of function values attained for a function f :ℵ X, where f (n) = x n for n 1.) x 1 x N +k x N +4 x 3
MATH 337 Sequeces Dr. Neal, WKU Let X be a metric space with distace fuctio d. We shall defie the geeral cocept of sequece ad limit i a metric space, the apply the results i particular to some special
More informationAn Electrostatic Catastrophe Machine as an Attosecond Pulse Generator
Optics ad Phtics Jural, 014, 4, 337-345 Published Olie December 014 i SciRes. http://www.scirp.rg/jural/pj http://dx.di.rg/10.436/pj.014.41034 A Electrstatic Catastrphe Machie as a Attsecd Pulse Geeratr
More informationRMO Sample Paper 1 Solutions :
RMO Sample Paper Slutis :. The umber f arragemets withut ay restricti = 9! 3!3!3! The umber f arragemets with ly e set f the csecutive 3 letters = The umber f arragemets with ly tw sets f the csecutive
More informationReview of Important Concepts
Appedix 1 Review f Imprtat Ccepts I 1 AI.I Liear ad Matrix Algebra Imprtat results frm liear ad matrix algebra thery are reviewed i this secti. I the discussis t fllw it is assumed that the reader already
More informationElectrostatics. . where,.(1.1) Maxwell Eqn. Total Charge. Two point charges r 12 distance apart in space
Maxwell Eq. E ρ Electrstatics e. where,.(.) first term is the permittivity i vacuum 8.854x0 C /Nm secd term is electrical field stregth, frce/charge, v/m r N/C third term is the charge desity, C/m 3 E
More information1 Introduction to reducing variance in Monte Carlo simulations
Copyright c 010 by Karl Sigma 1 Itroductio to reducig variace i Mote Carlo simulatios 11 Review of cofidece itervals for estimatig a mea I statistics, we estimate a ukow mea µ = E(X) of a distributio by
More informationThe generation of successive approximation methods for Markov decision processes by using stopping times
The geerati f successive apprximati methds fr Markv decisi prcesses by usig stppig times Citati fr published versi (APA): va Nue, J. A. E. E., & Wessels, J. (1976). The geerati f successive apprximati
More informationExperimental and Theoretical Investigations of PAN Molecular Weight Increase in Precipitation Polymerization as a Function of H 2 O/DMSO Ratio
Carb Letters Vl., N. March 00 pp. -7 Experimetal ad Theretical Ivestigatis f PAN Mlecular Weight Icrease i Precipitati Plymerizati as a ucti f H O/DMSO Rati Jig Zhag, egjig Bu, Ygqiag Dai, Liwei Xue, Zhixia
More informationSTRUCTURES IN MIKE 21. Flow over sluice gates A-1
A-1 STRUCTURES IN MIKE 1 Fl ver luice gate Fr a give gemetry f the luice gate ad k ater level uptream ad dtream f the tructure, the fl rate, ca be determied thrugh the equati f eergy ad mmetum - ee B Pedere,
More informationAlternative Approaches to Default Logic. Fachgebiet Intellektik. Technische Hochschule Darmstadt. Alexanderstrae 10. W. Ken Jackson. Burnaby, B.C.
Alterative Appraches t Default Lgic James P. Delgrade Schl f Cmputig Sciece Sim Fraser Uiversity Buraby, B.C. Caada V5A 1S6 Trste Schaub Fachgebiet Itellektik Techische Hchschule Darmstadt Alexaderstrae
More informationAn epsilon-based measure of efficiency in DEA revisited -A third pole of technical efficiency-
GRIPS Plicy Ifrmati Ceter Discussi Paper : 09-2 A epsil-based measure f efficiecy i DEA revisited -A third ple f techical efficiecy- Karu Te Natial Graduate Istitute fr Plicy Studies 7-22- Rppgi, Miat-ku,
More informationResult on the Convergence Behavior of Solutions of Certain System of Third-Order Nonlinear Differential Equations
Iteratial Jural f Mer Nliear Thery a Applicati, 6, 5, 8-58 Publishe Olie March 6 i SciRes http://wwwscirprg/jural/ijmta http://xirg/6/ijmta655 Result the Cvergece Behavir f Slutis f Certai System f Thir-Orer
More informationAbstract: The asympttically ptimal hypthesis testig prblem with the geeral surces as the ull ad alterative hyptheses is studied uder expetial-type err
Hypthesis Testig with the Geeral Surce y Te Su HAN z April 26, 2000 y This paper is a exteded ad revised versi f Sectis 4.4 4.7 i Chapter 4 f the Japaese bk f Ha [8]. z Te Su Ha is with the Graduate Schl
More informationChemistry 20 Lesson 11 Electronegativity, Polarity and Shapes
Chemistry 20 Lessn 11 Electrnegativity, Plarity and Shapes In ur previus wrk we learned why atms frm cvalent bnds and hw t draw the resulting rganizatin f atms. In this lessn we will learn (a) hw the cmbinatin
More informationPortfolio Performance Evaluation in a Modified Mean-Variance-Skewness Framework with Negative Data
Available lie at http://idea.srbiau.ac.ir It. J. Data Evelpmet Aalysis (ISSN 345-458X) Vl., N.3, Year 04 Article ID IJDEA-003,3 pages Research Article Iteratial Jural f Data Evelpmet Aalysis Sciece ad
More informationSeed and Sieve of Odd Composite Numbers with Applications in Factorization of Integers
IOSR Joural of Mathematics (IOSR-JM) e-issn: 78-578, p-issn: 319-75X. Volume 1, Issue 5 Ver. VIII (Sep. - Oct.01), PP 01-07 www.iosrjourals.org Seed ad Sieve of Odd Composite Numbers with Applicatios i
More informationJournal of Applied and Computational Mechanics, Vol. 3, No. 1, (2017), DOI: /jacm
Jural f Applied ad Cmputatial echaics, Vl., N., (7), -79 DOI:.55/jacm.7. Therm-mechaical liear vibrati aalysis f fluidcveyig structures subjected t differet budary cditis usig Galerki-Newt-Harmic balacig
More informationBC Calculus Review Sheet. converges. Use the integral: L 1
BC Clculus Review Sheet Whe yu see the wrds.. Fid the re f the uuded regi represeted y the itegrl (smetimes f ( ) clled hriztl imprper itegrl).. Fid the re f differet uuded regi uder f() frm (,], where
More informationCharacteristics of helical flow in slim holes and calculation of hydraulics for ultra-deep wells
6 Pet.Sci.(00)7:6-3 DOI 0.007/s8-00-006-8 Characteristics f helical flw i slim hles ad calculati f hydraulics fr ultra-deep wells Fu Jiahg, Yag Yu, Che Pig ad Zha Jihai 3 State Key Labratry f Oil ad Gas
More informationPreliminary Test Single Stage Shrinkage Estimator for the Scale Parameter of Gamma Distribution
America Jural f Mathematics ad Statistics, (3): 3-3 DOI:.593/j.ajms.3. Prelimiary Test Sigle Stage Shrikage Estimatr fr the Scale Parameter f Gamma Distributi Abbas Najim Salma,*, Aseel Hussei Ali, Mua
More informationSymmetric Two-User Gaussian Interference Channel with Common Messages
Symmetric Two-User Gaussia Iterferece Chael with Commo Messages Qua Geg CSL ad Dept. of ECE UIUC, IL 680 Email: geg5@illiois.edu Tie Liu Dept. of Electrical ad Computer Egieerig Texas A&M Uiversity, TX
More information