Optimization model of water supply networks design
|
|
- Nelson Ward
- 5 years ago
- Views:
Transcription
1 Opimizaion model of wae upply newok deign Pof. d. eng. IOAN SÂRBU Depamen of Building Sevice Poliehnica Univeiy of imioaa Piaa Bieicii, no. 4A, 333 imioaa ROMANIA Abac: he pape appoache he opimizaion of wae diibuion newok upplied fom one o moe node ouce, accoding o demand vaiaion. adiionally, in pipe opimizaion, he obecive funcion i alway focued on he co cieia of newok componen. In hi udy an impoved linea model i developed, which ha he advanage of uing no only co cieia, bu alo enegy conumpion, conumpion of cace eouce, opeaing expene ec. he pape ea looped newok wich have concenaed ouflow o unifom ouflow along he lengh of each pipe. An impoved model i developed fo opimal deing of new o paially exended wae diibuion newok, which opeae eihe by mean of gaviy o a pump yem.he model i baed on he mehod of linea pogamming and allow he deeminaion of an opimal diibuion of commecial diamee fo each pipe in he newok and he lengh of he pipe which coepond o hee diamee. Alo, i i poible o ake ino accoun he vaiou funcional iuaion chaaceiic found duing opeaion. hi pape compae linea opimizaion model o he ome ohe, uch a he claic model of aveage economical velociie and Mohnin opimizaion model. hi how he good pefomance of he new model. Fo diffeen analyzed newok, he aving of elecical enegy, due o diminihing peue loe and opeaion co when applying he developed model, epeen abou 35 %. Key-Wod: Wae upply, Diibuion, Looped newok, Opimal deign, Linea opimizaion model. Inoducion Diibuion newok ae an eenial pa of all wae upply yem. he eliabiliy of upply i much geae in he cae of looped newok. Diibuion yem co wihin any wae upply cheme may be equal o o geae han 6 % of he enie co of he poec. Alo, he enegy conumed in a diibuion newok upplied by pumping may exceed 6 % of he oal enegy conumpion of he yem [6]. Aemp hould be made o educe he co and enegy conumpion of he diibuion yem hough opimizaion in analyi and deign. A wae diibuion newok ha include pump mouned in he pipe, peue educing valve, and check-valve can be analyzed by eveal common mehod uch a Hady Co, linea heoy, and Newon Raphon []. adiionally, pipe diamee ae choen accoding o he aveage economical velociie (Hady Co mehod) [3]. hi pocedue i cumbeome, uneconomical, and equie ial, eldom leading o an economical and echnical opimum. hi pape develop a linea model fo opimal deign of new and paially exended diibuion yem upplied by pumping o gaviaion. I i baed on linea pogamming and allow fo he deeminaion of opimal diibuion of commecial diamee along he lengh of each pipe and he lengh of pipe eco coeponding o hee diamee. I i poible o ake ino accoun vaiou funcional iuaion chaaceiic found duing opeaion and unifom ouflow along he lengh of each pipe. Bai of hydaulic calculaion A diibuion newok may be epeened by oienaion compiing a finie numbe of ac (pipe, pump, fiing) and a e of node a well a eevoi and pump o pipe ineecion. In he cae of a complex opology, wih eevoi and pump a he node, he numbe of open loop (peudoloop) N RP i added o he numbe of cloed loop, o ha he oal numbe M of independen loop i deemined fom he equaion: M N + N RP () whee: i numbe of pipe; N numbe of node; N RP numbe of peue geneaing faciliie. he hydaulic calculaion of a diibuion newok involve in deemining he diamee, dichage and head loe in pipe, in ode o guaanee a each node he neceay dichage and peue. When pefoming he hydaulic calculaion of a diibuion newo he law of wae flow in all he pipe mu be epeced: dichage coninuiy a node: ISSN: ISBN:
2 f N i i i + q (,..., N N ) () in which: f i he eidual dichage a he node ; i dichage hough pipe i, wih he ign (+) when eneing node and ( ) when leaving i; q conumpion dichage (demand) a node wih he ign (+) fo node inflow and ( ) fo node ouflow. enegy conevaion in loop: h m i m i RP ε h f ( m,..., M ) (3) i i m in which: h m i he eidual head lo (divegence) in he loop m; h i head lo of he pipe i; ε i oienaion of flow hough he pipe, having he value (+) o ( ) a he wae flow ene i he ame o opoie o he pah ene of he loop m, and () value if i m; f m peue head inoduced by he poenial elemen of he loop m, given by: imple cloed loop: f m (4) cloed loop conaining boe pmp inalled in he pipe: f m ε H (5) i m i i p, i open loop wih pump and/o eevoi a node: f m Z I Z E (6) whee: Z I, Z E ae piezomeic head a peue device a he enance o exi fom he loop; H p,i pump head of he pump inegaed on he pipe i, fo he dichage i, appoximaed by paabolic inepolaion on he pump cuve given by poin [6]. 3 Newok deign opimizaion cieia Opimizaion of diibuion newok diamee conide a mono o mulicieial obecive funcion. Co o enegy cieia may be ued, imple o complex, which conide he newok co, pumping enegy co, opeaing expene, included enegy, conumed enegy, oal expene ec. hee cieia can be expeed in a complex obecive mulicieial funcion [7], wih he geneal fom: F ξ c in which: NP α ( a + bdi ) Li + ψp, ( hi + H ) i a ( + β ) (8) β ( + β ) a p + ; ξ a p (7) ξ + (9) ψ 9.8 ( f σξ 73 τ ) η + Φ a e () k whee: i he numbe of pipe in a newok; a, b, α co/enegy paamee depending on pipe maeial [9]; D i, L i diamee and lengh of pipe i; NP numbe of pump aion; p, pumped dichage of pump aion ; Σh i um of head loe along a pah beween he pump aion and he ciical node; H geodezic and uilizaion componen of he pumping oal dynamic head; β / amoizaion pa fo he opeaion peiod ; p, p epai, mainenance and peiodic eing pa fo newok pipe and pump aion, epecively; peiod fo which he opimizaion cieion expeed by he obecive funcion i applied, having he value o ; η efficiency of pump aion; f inallaion co of uni powe; σ a faco geae han one which ake ino accoun he inalled eeve powe; e co of elecical enegy; τ p /876 pumping coefficien, which ake ino accoun he effecive numbe p of pumping hou pe yea; Φ κ aio beween he aveage monhly dichage and he pumped dichage [6]. Fo newok upplied by pumping, he lieaue [], [], [] ugge he ue of minimum annual oal expene cieion (CAN), bu chooing he opimal diamee obained in hi way, he newok become uneconomical a ome ime afe conucion, due o inflaion. heefoe, i i ecommended he foe menioned cieion be ubec o dynamizaion by uing he cieion of oal updaed minimum expene (CA), he fome being in fac a pecific cae of he lae when he invemen i ealied wihin a yea; he opeaing expene ae he ame fom one yea o anohe and he expeced life-ime of he diibuion yem i high. In paicula, he ue of enegeical cieia diffeen fom co cieia i ecommendable. hu, anohe way o appoach he poblem, wih ha a bee validiy in ime and he homogenizaion of he obecive funcion i newok deign accoding o minimum enegeic conumpion (W). he geneal funcion (7) enable u o obain a paicula obecive funcion by paiculaizaion of he ime paamee and of he ohe economic and enegeic paamee, chaaceiic of he diibuion yem. Fo example, fom, a, e, f he minimum enegeic conumpion cieion i obained. 4 Developmen of opimizaion model Uing following nondimenional paamee: ISSN: ISBN:
3 fo ouflow: fo pipe: θ c i () ω i α Di, () λ L i he expeion of head lo h i, fo pipe wih unifom ouflow along hei lengh, ake he fom: Ω i h i hi Θ i (3) Li whee: 4 θi 3θi + 3 Θ i (4) 3 ( θ ) i i 4α Dk, i Ω i (5) λ ( θ ) i in which: h i i he head lo fo pipe i wih concenaed ouflow; c ouflow along he lengh of he pipe i; inflow in he iniial ecion of he pipe i; α nonunifomiy coefficien of velociy diibuion in he co ecion of he pipe; λ i ficion faco of pipe i. he oal lengh of a pipe i, wih he dichage i, may be divided ino i paial lengh (eco), of D i diamee and X i lengh. aking ino accoun he Dacy Weibach funcional equaion, he ficion lope J i fo each eco k of he pipe i can be calculaed, in he hypohei of concenaed ouflow, wih he equaion: hk, i 8 i J i λ i (6) X π g D i i i whee: i an exponen having he value 5.; g gaviaional acceleaion; λ i ficion faco of eco k in pipe i, can be calculaed uing he Colebook Whie fomula. Since in eal condiion he dichage deceae fom one co ecion o anohe in he ene of ouflow, an inceae of peue i accomplihed a he oule of he pipe, by a phenomenon imila o ebound, which ha a he effec of diminihing he head lo. hu, he expeion of ficion lope in each eco k of he pipe i, fo he unifom ouflow along he lengh of he pipe, i ewien a: h Ω i i J Θ i J i i (7) X i X i Specific conumpion of enegy fo diibuion of wae w d, in kwh/m 3, i obained by efeing he hydaulic powe diipaed in pipe o he um of dichage: w d i R q< β +.7 (8), whee q i he ouflow a he node. Compuaion of he opimal deign of looped newok mu be pefomed in wo age: eablihmen of opimal diibuion fo dichage hough pipe, i, accoding o he minimum bulk anpo cieion [8], which ake ino accoun he newok eliabiliy; compuaion of opimal pipe diamee, D i, aking ino accoun he opimized dichage. he eie of commecial diamee which can be ued D i [D max,i, D min,i ] fo each pipe i ae eablihed uing he limi value of opimal diamee D max,i and D min,i, compued by opimizaion elaion (9) fo pumping opeaion newok o elaion () fo gaviy newok: in which: D D max min), i N i α+ max(min) q i, α+ p β α+ i ( E (9) max( min), i 4i () πv min( max), i.33 n' ψ E () abξ whee: i i he dichage of he pipe i; p Σ p, pumped dichage; V min, V max limi of he economic velociie; n Manning oughne coefficien of he pipe; E economy-enegy faco of he pipe, which ha a maximum value and a minimum value [9], coeponding o he limi value of he vaiaion of economy-enegy paamee (p, p, η, f, σ, e, τ, Φ k ) fo he diibuion yem, included in ψ and ξ. A penaly coefficien p i i ued when opimizing diamee in he cae of exending a newo which ha he value equal o he value of coeponding impoed diamee, fo pipe wih fixed diamee, euling in D i p i. Admiing ha a pipe i of lengh L i of a pumping opeaion newok made up of pipe, can be divided ino i eco k of diamee D i and lengh X i and aking ino accoun he noaion: α c i ξ( a + bdk, i ) () Z IPP, ( hi + H ) (3) he obecive funcion (7) ake he fom: ISSN: ISBN:
4 F c i i k k i NP c, X, + ψ, Z, min (4) k i p IPP he unknown of he obecive funcion ae vaiable X i and Z IPP,. When he peue device i compied of one o moe eevoi (ψ ), he expeion (4) of he obecive funcion become: i F c X min, (5) c i k i i minimizing he included enegy o he newok co and having a unknown he vaiable X i. Hence, he value of he vaiable mu be deemined in ode o minimize he obecive funcion F c, povided he following conain ae aified: conucive conain: i k X k, i Li ( i,..., ) (6) funcional conain which ae wien fo each opeaing iuaion, and which mu povide he neceay peue HN o a he ciical node, aing on diffeen pah fom he peue device IPP (fig. ): Z IPP N i, ε i Θi J i X i Zo + HN i k N i ( ε i Ω k i J i + H p, i k, i ) o (7) whee: N i he pipe numbe of a pah IPP O; Z o elevaion head a he ciical node O; Z IPP, available piezomeic head a he peue device ; H p,i pumping head of he boe pump mouned in he pipe i. Fig. Scheme of a pah IPP ciical node O hydaulic conain chaaceiic only fo looped newok, expeing he enegy conevaion in loop: ε i Θi J k i k i i k i k i m i m i i m m, X, ε Ω, J, + f ( m,..., M ) (8) in which he peue head f m i given by he elaion (4), (5), (6) and ε i i he oienaion of he pipe. In he cae ha he available piezomeic head Z IPP, ae known, and i being unneceay o deemine hem by opimizaion, he obecive funcion (4) ake he fom (5), while value Z IPP, ae conained in he fee em of conain (7) and (8). A he obecive funcion (4) o (5) and conain (6), (7), (8) ae linea wih epec o he unknown of yem he opimal oluion i deemined accoding o he linea pogamming mehod, uing he Simplex algoyhm. Compuing he unknown Z IPP, by opimizaion, fo pumping opeaion newok eul in he coeponding pumping head: Z Z (9) H p, IPP, SP, whee Z SP, i he wae level in he ucion bain of IPP. aking ino accoun head lo SH n on he pah IPP n: SH n N i N i Θi J i X i ( Ω i J i + H p, i ) i k i k (3) he piezomeic head Z n and he eidual peue head H n a he node n ae deemined fom he elaion: Z n Z IPP, SH n (3) H n Z n Zn (3) whee Z n i he elevaion head a he node n. Fo an opimal deign, he piezomeic line of a pah of N pipe, iuaed in he ame peue zone, mu epeen a polygonal line which eemble a cloely a poible he opimal fom expeed by he equaion: βα + α+ N d Z Z h (33) IPP, - N n i i Li i in which: Z n i he piezomeic head a he node n; d diance beween node n and he peue device. he compue pogam OPLIRA ha been elaboaed baed on he linea opimizaion model, in he FORRAN pogamming language fo IBM PC compaible micoyem. 5 Numeical applicaion he looped diibuion newok wih he opology fom Figue i conideed. I i made of ca ion and i upplied by pumping wih a dichage of.3 m 3 /. he following daa i known: pipe lengh L i, in m, elevaion head Z, in m, and neceay peue HN 4 m H O. ISSN: ISBN:
5 A compaaive udy of newok dimenioning i pefomed uing he claic model of aveage economical velociie (MVE), Mohnin opimizaion model (MOM) [] and he linea opimizaion model (MOL) developed above, he la being applied in he hypohei of concenaed ouflow (MOL N), a well a of unifom ouflow along he lengh of he pipe (MOL D). able. Hydaulic chaaceiic of he pipe deemined wih he model MOL N and MOL D Fig. Scheme of he deigned diibuion newok Calculu wa pefomed conideing a anioy ubulence egime of wae flow and he opimizaion cieion ued wa ha of minimum enegeic conumpion. Reul of he numeical oluion pefomed by mean of an IBM PC compue, efeing o he hydaulic chaaceiic of he pipe ae peened in able and. able. Hydaulic chaaceiic of he pipe deemined wih he model MVE and MOM Pipe L MVE MOM i D i h i V i i D i h i V i [m 3 /] [mm] [m] [m/] [m 3 /] [mm] [m] [m/] MOL-N MOL-D Pipe i - i k X i D i h i V i i k X i D i h i V i [m 3 /] [m] [mm] [m] [m/] [m 3 /] [m] [mm] [m] [m/] , he ignificance of ( ) ign of dichage and head loe in able and i he change of flow ene in he epecive pipe wih epec o he iniial ene conideed in he Figue. In Figue 3 hee i a gaphic epeenaion, aing fom he node ouce 8 o he ciical node, on he pah 8 5, he piezomeic line being obained uing he hee menioned model of compuaion, evidencing hei deviaion fom he opimal heoeical fom. Figue 3 alo include he coeponding value of he obecive funcion F c, he newok included enegy W c, pumping enegy W e, a well a pecific enegy conumpion fo wae diibuion w d. Accoding o he pefomed udy i wa eablihed ha: all he pipe of he newok ae opeaing in a anioy ubulence egime of wae flow; hee i a geneal inceae of pipe diamee obained by opimizaion model (MOM, MOL) wih epec o MVE, becaue he claical model doe no ake ino accoun he minimum conumpion of enegy and he diveiy of economical paamee; ISSN: ISBN:
6 Fig. 3 Piezomeic line along he pah 8 5 in compaion wih he eul obained by MVE, he one obained by opimizaion model ae moe economical, a ubanial educion of pecific enegy conumpion fo wae diibuion i achieved (MOM.3 %, MOL-N 4.3 %, MOL-D 45.3 %) a well a a educion of pumping enegy (MOM 6,4%, MOL-N.3%, MOL-D.6%), a he ame ime he obecive funcion ha alo malle value (MOM.3 %, MOL-N 4.5 %, MOL-D 4.8 %); he opimal eul obained uing MOL ae upeio enegeically o hoe offeed by MOM, leading o pumping enegy aving of 5 %; alo, he applicaion of MOL fo unifom ouflow along he lengh of he pipe, ha led o he minimum deviaion fom he opimal fom of he piezomeic line, epecially o a moe unifom diibuion of he pumping enegy, by eliminaion of a high level of available peue a ome node even a maximum conumpion. he malle value of he pecific enegeic conumpion, namely ha of.4 kwh/m 3, alo uppo hi aeion; educion of he peue in he diibuion newok achieved in hi way, i of mao pacical impo, conibuing o he diminihing of wae loe fom he yem. 6. Concluion he popoed opimizaion model, a vey geneal and pacical one, offe he poibiliy of opimal deign of wae upply newok uing muliple opimizaion cieia and conide he anioy o quadaic ubulence flow. I ha he advanage of uing no only co cieia, bu alo enegy conumpion, conumpion of cace eouce, and ohe cieia can be expeed by imple opion in he obecive funcion (7). he model of linea opimizaion could be applied o any looped o ee haped newo eihe when piezomeic head a peue device (pump aion o ank) mu be deemined o when hee head ae given. I pemi he deeminaion of an opimal diibuion of comecial diamee along he lengh of each pipe of he newok and he lengh of pipe eco coeponding o hee diamee. Alo, hi faciliae he conideaion of unifom ouflow along he lengh of he pipe newok. A moe unifom diibuion of pumping enegy i achieved o ha head loe and paamee of pump aion can be deemined moe peciely. Fo diffeen analized newok, he aving of elecical enegy due o diminihing peue loe and opeaion co when applying he model of linea opimizaion epeen abou...35%, which i of gea impoance, conideing he geneal e- negy iue. Refeence: [] Abamov, N.N. eoia i meodica acea iem podaci i apedelenia vodî, Soizda, Mokva, 97. [] Cenedee, A. Mele, P. Opimal deign of wae diibuion newok, Jounal of he Hydaulic Diviion, ASCE, no. HY, 978. [3] Co, H. Analyi of flow in newok of condui o conduco, Bullein no. 86, Univ. of Illinoi Engg. Expeimen Saion, III, 936. [4] Jame M. e al. Opimal oluion fo diic heaing pipe newok, Poc. of he 5 h IASME/ WSEAS In. Conf. on Enegy & Envionmen, Cambidge, Febuay 3-5,, pp [5] Kope, J. Dobee D. Goicanec, D. Vaiaion of pipe diamee and i influence on he flowpeue condiion, WSEAS anacion on Fluid Mechanic, vol., no., 6, pp [6] Sâbu, I. Enegeical opimizaion of wae diibuion yem, Publihing Houe of he Romanian Academy, Buchae, 997. [7] Sâbu, I. Kalmà, F. Opimizaion of looped wae upply newok, Peiodica Polyechnica, Budape, vol 46, no.,, pp [8] Sâbu, I. Opimizaion of he dichage diibuion in wae upply newok, Hydoechnic, no. 6, 5, pp [9] Sâbu, I. Kalma, F. Compue aided deign of building equipmen, Publihing Houe Mion, imioaa,. [] Sephenon, D. Pipe flow analyi, Elevie Science Publihe B.V., 984. [] hawa, W. Lea co deign of wae diibuion yem, Jounal of he Hydaulic Diviion, ASCE, no. HY9, 973. ISSN: ISBN:
Molecular Evolution and Phylogeny. Based on: Durbin et al Chapter 8
Molecula Evoluion and hylogeny Baed on: Dubin e al Chape 8. hylogeneic Tee umpion banch inenal node leaf Topology T : bifucaing Leave - N Inenal node N+ N- Lengh { i } fo each banch hylogeneic ee Topology
More informationThe Production of Well-Being: Conventional Goods, Relational Goods and Status Goods
The Poducion of Well-Bein: Convenional Good, Relaional Good and Sau Good Aloy Pinz Iniue of Public Economic II Univeiy of Müne, Gemany New Diecion in Welfae II, OECD Pai July 06 08, 2011 Conen 1. Inoducion
More informationSTUDY OF THE STRESS-STRENGTH RELIABILITY AMONG THE PARAMETERS OF GENERALIZED INVERSE WEIBULL DISTRIBUTION
Inenaional Jounal of Science, Technology & Managemen Volume No 04, Special Issue No. 0, Mach 205 ISSN (online): 2394-537 STUDY OF THE STRESS-STRENGTH RELIABILITY AMONG THE PARAMETERS OF GENERALIZED INVERSE
More informationSupport Vector Machines
Suppo Veco Machine CSL 3 ARIFICIAL INELLIGENCE SPRING 4 Suppo Veco Machine O, Kenel Machine Diciminan-baed mehod olean cla boundaie Suppo veco coni of eample cloe o bounday Kenel compue imilaiy beeen eample
More informationGeneral Non-Arbitrage Model. I. Partial Differential Equation for Pricing A. Traded Underlying Security
1 Geneal Non-Abiage Model I. Paial Diffeenial Equaion fo Picing A. aded Undelying Secuiy 1. Dynamics of he Asse Given by: a. ds = µ (S, )d + σ (S, )dz b. he asse can be eihe a sock, o a cuency, an index,
More informationWORK POWER AND ENERGY Consevaive foce a) A foce is said o be consevaive if he wok done by i is independen of pah followed by he body b) Wok done by a consevaive foce fo a closed pah is zeo c) Wok done
More informationDEVELOPMENT OF A DESIGN AND PERFORMANCE PREDICTION TOOL FOR THE GROUND SOURCE HEAT PUMP SYSTEM
DEVELOPMEN OF A DESIGN AND PERFORMANCE PREDICION OOL FOR HE GROUND SOURCE HEA PUMP SYSEM. INRODUCION. Kaua K. Nagano S. akeda. Ibamoo S.Naia Gaduae School of Engineeing Hokkaido Univeiy Sappoo 060-868
More informationLow-complexity Algorithms for MIMO Multiplexing Systems
Low-complexiy Algoihms fo MIMO Muliplexing Sysems Ouline Inoducion QRD-M M algoihm Algoihm I: : o educe he numbe of suviving pahs. Algoihm II: : o educe he numbe of candidaes fo each ansmied signal. :
More informationTransmit Beamforming with Reduced Channel State Information in MIMO-OFDM Wireless Systems
anmi Beamfoming wih Reduced Channel Sae Infomaion in MIMO-OFDM Wiele Syem Seung-Hyeon Yang, Jae-Yun Ko, and Yong-Hwan Lee School of Elecical Engineeing and INMC Seoul Naional Univeiy Seoul, Koea Email:
More informationMATHEMATICAL FOUNDATIONS FOR APPROXIMATING PARTICLE BEHAVIOUR AT RADIUS OF THE PLANCK LENGTH
Fundamenal Jounal of Mahemaical Phsics Vol 3 Issue 013 Pages 55-6 Published online a hp://wwwfdincom/ MATHEMATICAL FOUNDATIONS FOR APPROXIMATING PARTICLE BEHAVIOUR AT RADIUS OF THE PLANCK LENGTH Univesias
More informationRepresenting Knowledge. CS 188: Artificial Intelligence Fall Properties of BNs. Independence? Reachability (the Bayes Ball) Example
C 188: Aificial Inelligence Fall 2007 epesening Knowledge ecue 17: ayes Nes III 10/25/2007 an Klein UC ekeley Popeies of Ns Independence? ayes nes: pecify complex join disibuions using simple local condiional
More informationRandomized Perfect Bipartite Matching
Inenive Algorihm Lecure 24 Randomized Perfec Biparie Maching Lecurer: Daniel A. Spielman April 9, 208 24. Inroducion We explain a randomized algorihm by Ahih Goel, Michael Kapralov and Sanjeev Khanna for
More informationDegree of Approximation of a Class of Function by (C, 1) (E, q) Means of Fourier Series
IAENG Inenaional Jounal of Applied Mahemaic, 4:, IJAM_4 7 Degee of Appoximaion of a Cla of Funcion by C, E, q Mean of Fouie Seie Hae Kihna Nigam and Kuum Shama Abac In hi pape, fo he fi ime, we inoduce
More informationTopic 3. Single factor ANOVA: Introduction [ST&D Chapter 7] 3.1. The F distribution [ST&D p. 99]
Topic 3. Single faco ANOVA: Inoducion [ST&D Chape 7] "The analyi of vaiance i moe han a echnique fo aiical analyi. Once i i undeood, ANOVA i a ool ha can povide an inigh ino he naue of vaiaion of naual
More informationLecture 26: Leapers and Creepers
Lecue 6: Leape and Ceepe Scibe: Geain Jone (and Main Z. Bazan) Depamen of Economic, MIT May, 5 Inoducion Thi lecue conide he analyi of he non-epaable CTRW in which he diibuion of ep ize and ime beween
More informationThe sudden release of a large amount of energy E into a background fluid of density
10 Poin explosion The sudden elease of a lage amoun of enegy E ino a backgound fluid of densiy ceaes a song explosion, chaaceized by a song shock wave (a blas wave ) emanaing fom he poin whee he enegy
More informationr P + '% 2 r v(r) End pressures P 1 (high) and P 2 (low) P 1 , which must be independent of z, so # dz dz = P 2 " P 1 = " #P L L,
Lecue 36 Pipe Flow and Low-eynolds numbe hydodynamics 36.1 eading fo Lecues 34-35: PKT Chape 12. Will y fo Monday?: new daa shee and daf fomula shee fo final exam. Ou saing poin fo hydodynamics ae wo equaions:
More informationOn The Estimation of Two Missing Values in Randomized Complete Block Designs
Mahemaical Theoy and Modeling ISSN 45804 (Pape ISSN 505 (Online Vol.6, No.7, 06 www.iise.og On The Esimaion of Two Missing Values in Randomized Complee Bloc Designs EFFANGA, EFFANGA OKON AND BASSE, E.
More informationSections 3.1 and 3.4 Exponential Functions (Growth and Decay)
Secions 3.1 and 3.4 Eponenial Funcions (Gowh and Decay) Chape 3. Secions 1 and 4 Page 1 of 5 Wha Would You Rahe Have... $1million, o double you money evey day fo 31 days saing wih 1cen? Day Cens Day Cens
More informationOn Control Problem Described by Infinite System of First-Order Differential Equations
Ausalian Jounal of Basic and Applied Sciences 5(): 736-74 ISS 99-878 On Conol Poblem Descibed by Infinie Sysem of Fis-Ode Diffeenial Equaions Gafujan Ibagimov and Abbas Badaaya J'afau Insiue fo Mahemaical
More informationMonochromatic Wave over One and Two Bars
Applied Mahemaical Sciences, Vol. 8, 204, no. 6, 307-3025 HIKARI Ld, www.m-hikai.com hp://dx.doi.og/0.2988/ams.204.44245 Monochomaic Wave ove One and Two Bas L.H. Wiyano Faculy of Mahemaics and Naual Sciences,
More informationLecture 17: Kinetics of Phase Growth in a Two-component System:
Lecue 17: Kineics of Phase Gowh in a Two-componen Sysem: descipion of diffusion flux acoss he α/ ineface Today s opics Majo asks of oday s Lecue: how o deive he diffusion flux of aoms. Once an incipien
More informationRevisited the Mathematical Derivation Wall Thickness Measurement of Pipe for Radiography
DI 007 - Inenaional Sympoium on Digial induial adiology and Compued Tomogaphy, June 5-7, 007, Lyon, Fance eviied he Mahemaical Deivaion all Thickne Meauemen o Pipe o adiogaphy Ab.. Hamzah and Sii M. M.
More information, the. L and the L. x x. max. i n. It is easy to show that these two norms satisfy the following relation: x x n x = (17.3) max
ecure 8 7. Sabiliy Analyi For an n dimenional vecor R n, he and he vecor norm are defined a: = T = i n i (7.) I i eay o how ha hee wo norm aify he following relaion: n (7.) If a vecor i ime-dependen, hen
More informationChapter 7: Inverse-Response Systems
Chaper 7: Invere-Repone Syem Normal Syem Invere-Repone Syem Baic Sar ou in he wrong direcion End up in he original eady-ae gain value Two or more yem wih differen magniude and cale in parallel Main yem
More informationDERIVATION OF LORENTZ TRANSFORMATION EQUATIONS AND THE EXACT EQUATION OF PLANETARY MOTION FROM MAXWELL AND NEWTON Sankar Hajra
PHYSICAL INTERPRETATION OF RELATIVITY THEORY CONFERENCE, LONDON, 4 DERIVATION OF LORENTZ TRANSFORMATION EQUATIONS AND THE EXACT EQUATION OF PLANETARY MOTION FROM MAXWELL AND NEWTON Sanka Haja CALCUTTA
More informationMacroeconomics Fiscal and Monetary Policy Interdependence
acoeconomic Fical and oneay olicy Inedependence Nicola Viegi Sepembe 207 oneay Economic Lecue 0 Inoducion Fical olicy back a he cene of policy dicuion Theoy of Fical olicy no well developed Ricadian Equivalence
More informationu(t) Figure 1. Open loop control system
Open loop conrol v cloed loop feedbac conrol The nex wo figure preen he rucure of open loop and feedbac conrol yem Figure how an open loop conrol yem whoe funcion i o caue he oupu y o follow he reference
More information7 Wave Equation in Higher Dimensions
7 Wave Equaion in Highe Dimensions We now conside he iniial-value poblem fo he wave equaion in n dimensions, u c u x R n u(x, φ(x u (x, ψ(x whee u n i u x i x i. (7. 7. Mehod of Spheical Means Ref: Evans,
More informationExponential and Logarithmic Equations and Properties of Logarithms. Properties. Properties. log. Exponential. Logarithmic.
Eponenial and Logaihmic Equaions and Popeies of Logaihms Popeies Eponenial a a s = a +s a /a s = a -s (a ) s = a s a b = (ab) Logaihmic log s = log + logs log/s = log - logs log s = s log log a b = loga
More informationWhat is maximum Likelihood? History Features of ML method Tools used Advantages Disadvantages Evolutionary models
Wha i maximum Likelihood? Hiory Feaure of ML mehod Tool ued Advanage Diadvanage Evoluionary model Maximum likelihood mehod creae all he poible ree conaining he e of organim conidered, and hen ue he aiic
More informationLecture 22 Electromagnetic Waves
Lecue Elecomagneic Waves Pogam: 1. Enegy caied by he wave (Poyning veco).. Maxwell s equaions and Bounday condiions a inefaces. 3. Maeials boundaies: eflecion and efacion. Snell s Law. Quesions you should
More informationPricing Credit Card Loans with Default Risks
Picing Cedi Cad Loan wih Defaul Rik Chuang-Chang Chang, Hi-Chi Chen, Ra-Jian Ho and Hong-Wen Lin * ABSTRACT Thi pape exend he Jaow and Devene (1998) model o faciliae he conideaion of defaul ik wihin he
More informationCHAPTER 7: SECOND-ORDER CIRCUITS
EEE5: CI RCUI T THEORY CHAPTER 7: SECOND-ORDER CIRCUITS 7. Inroducion Thi chaper conider circui wih wo orage elemen. Known a econd-order circui becaue heir repone are decribed by differenial equaion ha
More information5.2 GRAPHICAL VELOCITY ANALYSIS Polygon Method
ME 352 GRHICL VELCITY NLYSIS 52 GRHICL VELCITY NLYSIS olygon Mehod Velociy analyi form he hear of kinemaic and dynamic of mechanical yem Velociy analyi i uually performed following a poiion analyi; ie,
More informationIntroduction to SLE Lecture Notes
Inroducion o SLE Lecure Noe May 13, 16 - The goal of hi ecion i o find a ufficien condiion of λ for he hull K o be generaed by a imple cure. I urn ou if λ 1 < 4 hen K i generaed by a imple curve. We will
More informationParameter Determination of an Induction Machine for Integrated Starter Alternator
Paamee Deeminaion of an Inducion fo Inegaed ae Alenao C. P. Mudannayake and M. F. Rahman chool of Elecical Engineeing and Telecommunicaion Univeiy of New ouh Wale, ydney, Aualia chahua@uden.unw.edu.au
More informationMultibody Dynamics 2015
2015 ECCOAS THEATIC CONERENCE ON ULTIBODY DYNAICS ulibody Dynamic 2015 Bacelona, June 29 July 2 Bacelona School of Induial Engineeing Unieia Poliècnica de Caalunya mulibody2015.og 1 ECCOAS Themaic Confeence
More informationKINEMATICS OF RIGID BODIES
KINEMTICS OF RIGID ODIES In igid body kinemaics, we use he elaionships govening he displacemen, velociy and acceleaion, bu mus also accoun fo he oaional moion of he body. Descipion of he moion of igid
More informationLecture 18: Kinetics of Phase Growth in a Two-component System: general kinetics analysis based on the dilute-solution approximation
Lecue 8: Kineics of Phase Gowh in a Two-componen Sysem: geneal kineics analysis based on he dilue-soluion appoximaion Today s opics: In he las Lecues, we leaned hee diffeen ways o descibe he diffusion
More informationLecture-V Stochastic Processes and the Basic Term-Structure Equation 1 Stochastic Processes Any variable whose value changes over time in an uncertain
Lecue-V Sochasic Pocesses and he Basic Tem-Sucue Equaion 1 Sochasic Pocesses Any vaiable whose value changes ove ime in an unceain way is called a Sochasic Pocess. Sochasic Pocesses can be classied as
More informationPHYS GENERAL RELATIVITY AND COSMOLOGY PROBLEM SET 7 - SOLUTIONS
PHYS 54 - GENERAL RELATIVITY AND COSMOLOGY - 07 - PROBLEM SET 7 - SOLUTIONS TA: Jeome Quinin Mach, 07 Noe ha houghou hee oluion, we wok in uni whee c, and we chooe he meic ignaue (,,, ) a ou convenion..
More informationConsider a Binary antipodal system which produces data of δ (t)
Modulaion Polem PSK: (inay Phae-hi keying) Conide a inay anipodal yem whih podue daa o δ ( o + δ ( o inay and epeively. Thi daa i paed o pule haping ile and he oupu o he pule haping ile i muliplied y o(
More informationResearch on the Algorithm of Evaluating and Analyzing Stationary Operational Availability Based on Mission Requirement
Reseach on he Algoihm of Evaluaing and Analyzing Saionay Opeaional Availabiliy Based on ission Requiemen Wang Naichao, Jia Zhiyu, Wang Yan, ao Yilan, Depamen of Sysem Engineeing of Engineeing Technology,
More informationA New Method for Directional Control of a Tractor Semi-trailer
Aualian Jounal of Baic and Applied Science, 6(12): 396-49, 212 ISSN 1991-8178 A New Mehod fo Diecional Conol of a Taco Semi-aile 1 S.H. Tabaabaei Oeh, 1 R. Kazemi, 1 S. Azadi, 2 A. Zahedi 1 Depamen of
More informationRelative Positioning Method of Using Single-frequency Model for Formation Flying Missions
Inenaional Induial Infomaic and Compue Engineeing Confeence (IIICEC 205) Relaive Poiioning Mehod of Uing Single-fequency Model fo Fomaion Flying Miion Hanyi Shi, Qizi Huangpeng2,a, Yuanyuan Qiao3,4, Yong
More informationAdmin MAX FLOW APPLICATIONS. Flow graph/networks. Flow constraints 4/30/13. CS lunch today Grading. in-flow = out-flow for every vertex (except s, t)
/0/ dmin lunch oday rading MX LOW PPLIION 0, pring avid Kauchak low graph/nework low nework direced, weighed graph (V, ) poiive edge weigh indicaing he capaciy (generally, aume ineger) conain a ingle ource
More informationÖRNEK 1: THE LINEAR IMPULSE-MOMENTUM RELATION Calculate the linear momentum of a particle of mass m=10 kg which has a. kg m s
MÜHENDİSLİK MEKANİĞİ. HAFTA İMPULS- MMENTUM-ÇARPIŞMA Linea oenu of a paicle: The sybol L denoes he linea oenu and is defined as he ass ies he elociy of a paicle. L ÖRNEK : THE LINEAR IMPULSE-MMENTUM RELATIN
More information6.8 Laplace Transform: General Formulas
48 HAP. 6 Laplace Tranform 6.8 Laplace Tranform: General Formula Formula Name, ommen Sec. F() l{ f ()} e f () d f () l {F()} Definiion of Tranform Invere Tranform 6. l{af () bg()} al{f ()} bl{g()} Lineariy
More informationPHYS PRACTICE EXAM 2
PHYS 1800 PRACTICE EXAM Pa I Muliple Choice Quesions [ ps each] Diecions: Cicle he one alenaive ha bes complees he saemen o answes he quesion. Unless ohewise saed, assume ideal condiions (no ai esisance,
More informationTo become more mathematically correct, Circuit equations are Algebraic Differential equations. from KVL, KCL from the constitutive relationship
Laplace Tranform (Lin & DeCarlo: Ch 3) ENSC30 Elecric Circui II The Laplace ranform i an inegral ranformaion. I ranform: f ( ) F( ) ime variable complex variable From Euler > Lagrange > Laplace. Hence,
More informationCombinatorial Approach to M/M/1 Queues. Using Hypergeometric Functions
Inenaional Mahemaical Foum, Vol 8, 03, no 0, 463-47 HIKARI Ld, wwwm-hikaicom Combinaoial Appoach o M/M/ Queues Using Hypegeomeic Funcions Jagdish Saan and Kamal Nain Depamen of Saisics, Univesiy of Delhi,
More informationAn Automatic Door Sensor Using Image Processing
An Auomaic Doo Senso Using Image Pocessing Depamen o Elecical and Eleconic Engineeing Faculy o Engineeing Tooi Univesiy MENDEL 2004 -Insiue o Auomaion and Compue Science- in BRNO CZECH REPUBLIC 1. Inoducion
More informationEFFECT OF PERMISSIBLE DELAY ON TWO-WAREHOUSE INVENTORY MODEL FOR DETERIORATING ITEMS WITH SHORTAGES
Volume, ssue 3, Mach 03 SSN 39-4847 EFFEC OF PERMSSBLE DELAY ON WO-WAREHOUSE NVENORY MODEL FOR DEERORANG EMS WH SHORAGES D. Ajay Singh Yadav, Ms. Anupam Swami Assisan Pofesso, Depamen of Mahemaics, SRM
More informationAB for hydrogen in steel is What is the molar flux of the hydrogen through the steel? Δx Wall. s kmole
ignen 6 Soluion - Hydogen ga i oed a high peue in a ecangula conaine (--hick wall). Hydogen concenaion a he inide wall i kole / and eenially negligible on he ouide wall. The B fo hydogen in eel i.6 / ec
More informationOPTIMIZATION OF LOOPED WATER SUPPLY NETWORKS
PERIODICA POLYTECHNICA SER. MECH. ENG. VOL. 46, NO. 1, PP. 75 90 (2002) OPTIMIZATION OF LOOPED WATER SUPPLY NETWORKS Ioan SÂRBU and Fancisc KALMÁR The Politehnica Univesity of Timişoaa 1900 Timişoaa, Piaţa
More informationReinforcement learning
Lecue 3 Reinfocemen leaning Milos Hauskech milos@cs.pi.edu 539 Senno Squae Reinfocemen leaning We wan o lean he conol policy: : X A We see examples of x (bu oupus a ae no given) Insead of a we ge a feedback
More informationAn assessment of ring seine fishery in Kerala through surplus production model
Indian J. Fish., 54() : 35-40, Ap.-Jun., 007 35 An assessmen of ing seine fishey in Keala hough suplus poducion model K. ALAN AND T. V. SATHIANANDAN* Cenal Maine Fisheies Reseach Insiue, Cochin - 68 08,
More information, on the power of the transmitter P t fed to it, and on the distance R between the antenna and the observation point as. r r t
Lecue 6: Fiis Tansmission Equaion and Rada Range Equaion (Fiis equaion. Maximum ange of a wieless link. Rada coss secion. Rada equaion. Maximum ange of a ada. 1. Fiis ansmission equaion Fiis ansmission
More informationEECE 301 Signals & Systems Prof. Mark Fowler
EECE 31 Signal & Syem Prof. Mark Fowler Noe Se #27 C-T Syem: Laplace Tranform Power Tool for yem analyi Reading Aignmen: Secion 6.1 6.3 of Kamen and Heck 1/18 Coure Flow Diagram The arrow here how concepual
More informationThe International Diversification Puzzle when Goods Prices are Sticky: It s Really about Exchange-Rate Hedging, not Equity Portfolios
The Inenaional Diveificaion Puzzle when Good Pice ae Sicky: I eally abou Exchange-ae edging, no Equiy Pofolio by CALES ENGEL AND AKITO MATSUMOTO Appendix A. Soluion of he Dynamic Model An equilibium aifie
More informationApproximating solutions of backward doubly stochastic differential equations with measurable coefficients using a time discretization scheme
Loughboough Univeiy Iniuional Repoioy Appoximaing oluion of backwad doubly ochaic diffeenial equaion wih meauable coefficien uing a ime diceizaion cheme Thi iem wa ubmied o Loughboough Univeiy' Iniuional
More informationA Numerical Simulation of Adsorption Using Non-Standard Isotherm Equations in COMSOL
Excep fom he Poceeding of he COSOL Confeence 2008 Boon A Numeical Simulaion of Adopion Uing Non-Sandad Iohem Equaion in COSOL A. Oiz-Tapia *1, D. A. Lopez-Falcon 1,. A. Diaz-Viea 1, S. Lopez-Ramiez 1,
More informationAn Open cycle and Closed cycle Gas Turbine Engines. Methods to improve the performance of simple gas turbine plants
An Open cycle and losed cycle Gas ubine Engines Mehods o impove he pefomance of simple gas ubine plans I egeneaive Gas ubine ycle: he empeaue of he exhaus gases in a simple gas ubine is highe han he empeaue
More informationLaplace Transform. Inverse Laplace Transform. e st f(t)dt. (2)
Laplace Tranform Maoud Malek The Laplace ranform i an inegral ranform named in honor of mahemaician and aronomer Pierre-Simon Laplace, who ued he ranform in hi work on probabiliy heory. I i a powerful
More informationIdentification of Fault Locations using Transient State Estimation
denificaion of Faul Locaion uing Tanien Sae Eimaion K. K.C. Yu, Suden Membe, EEE and N. R. Waon, Senio Membe, EEE Abac n a lage cale elecical powe yem, idenificaion of yem faul can be a ediou ak. Unexpeced
More informationMATHEMATICS PAPER 121/2 K.C.S.E QUESTIONS SECTION 1 ( 52 MARKS) 3. Simplify as far as possible, leaving your answer in the form of surd
f MATHEMATICS PAPER 2/2 K.C.S.E. 998 QUESTIONS CTION ( 52 MARKS) Answe he enie queion in his cion /5. U logaihms o evaluae 55.9 (262.77) e F 2. Simplify he epeson - 2 + 3 Hence solve he equaion - - 2 +
More information156 There are 9 books stacked on a shelf. The thickness of each book is either 1 inch or 2
156 Thee ae 9 books sacked on a shelf. The hickness of each book is eihe 1 inch o 2 F inches. The heigh of he sack of 9 books is 14 inches. Which sysem of equaions can be used o deemine x, he numbe of
More informationSelling at the ultimate maximum in a regime-switching model
Selling a he ulimae maximum in a egime-wiching model axiv:158.677v2 mah.pr 24 Jun 216 Yue Liu Nicola Pivaul School of Phyical and Mahemaical Science Diviion of Mahemaical Science Nanyang Technological
More informationPressure Vessels Thin and Thick-Walled Stress Analysis
Pessue Vessels Thin and Thick-Walled Sess Analysis y James Doane, PhD, PE Conens 1.0 Couse Oveview... 3.0 Thin-Walled Pessue Vessels... 3.1 Inoducion... 3. Sesses in Cylindical Conaines... 4..1 Hoop Sess...
More informationAN EVOLUTIONARY APPROACH FOR SOLVING DIFFERENTIAL EQUATIONS
AN EVOLUTIONARY APPROACH FOR SOLVING DIFFERENTIAL EQUATIONS M. KAMESWAR RAO AND K.P. RAVINDRAN Depamen of Mechanical Engineeing, Calicu Regional Engineeing College, Keala-67 6, INDIA. Absac:- We eploe
More informationProblem Set If all directed edges in a network have distinct capacities, then there is a unique maximum flow.
CSE 202: Deign and Analyi of Algorihm Winer 2013 Problem Se 3 Inrucor: Kamalika Chaudhuri Due on: Tue. Feb 26, 2013 Inrucion For your proof, you may ue any lower bound, algorihm or daa rucure from he ex
More informationTwo-dimensional Effects on the CSR Interaction Forces for an Energy-Chirped Bunch. Rui Li, J. Bisognano, R. Legg, and R. Bosch
Two-dimensional Effecs on he CS Ineacion Foces fo an Enegy-Chiped Bunch ui Li, J. Bisognano,. Legg, and. Bosch Ouline 1. Inoducion 2. Pevious 1D and 2D esuls fo Effecive CS Foce 3. Bunch Disibuion Vaiaion
More informationÜber die Fortpanzung ebener Luftwellen von endlicher Schwingungsweite The Propagation of Planar Air Waves of Finite Amplitude
Übe ie Fopanzung ebene Lufwellen von enliche Schwingungweie The Popagaion of Plana Ai Wave of Finie Ampliue Benha Riemann Abhanlungen e Geellchaf e Wienchafen zu Göingen 8 pp 43-65 860 Even hough he iffeenial
More informationThe Production of Polarization
Physics 36: Waves Lecue 13 3/31/211 The Poducion of Polaizaion Today we will alk abou he poducion of polaized ligh. We aleady inoduced he concep of he polaizaion of ligh, a ansvese EM wave. To biefly eview
More informationChapter 7. Interference
Chape 7 Inefeence Pa I Geneal Consideaions Pinciple of Supeposiion Pinciple of Supeposiion When wo o moe opical waves mee in he same locaion, hey follow supeposiion pinciple Mos opical sensos deec opical
More informationEE202 Circuit Theory II
EE202 Circui Theory II 2017-2018, Spring Dr. Yılmaz KALKAN I. Inroducion & eview of Fir Order Circui (Chaper 7 of Nilon - 3 Hr. Inroducion, C and L Circui, Naural and Sep epone of Serie and Parallel L/C
More information( ) exp i ω b ( ) [ III-1 ] exp( i ω ab. exp( i ω ba
THE INTEACTION OF ADIATION AND MATTE: SEMICLASSICAL THEOY PAGE 26 III. EVIEW OF BASIC QUANTUM MECHANICS : TWO -LEVEL QUANTUM SYSTEMS : The lieaue of quanum opics and lase specoscop abounds wih discussions
More informationToday - Lecture 13. Today s lecture continue with rotations, torque, Note that chapters 11, 12, 13 all involve rotations
Today - Lecue 13 Today s lecue coninue wih oaions, oque, Noe ha chapes 11, 1, 13 all inole oaions slide 1 eiew Roaions Chapes 11 & 1 Viewed fom aboe (+z) Roaional, o angula elociy, gies angenial elociy
More information[ ] 0. = (2) = a q dimensional vector of observable instrumental variables that are in the information set m constituents of u
Genealized Mehods of Momens he genealized mehod momens (GMM) appoach of Hansen (98) can be hough of a geneal pocedue fo esing economics and financial models. he GMM is especially appopiae fo models ha
More informationChapter 19 Webassign Help Problems
Chapte 9 Webaign Help Poblem 4 5 6 7 8 9 0 Poblem 4: The pictue fo thi poblem i a bit mileading. They eally jut give you the pictue fo Pat b. So let fix that. Hee i the pictue fo Pat (a): Pat (a) imply
More informationCS 188: Artificial Intelligence Fall Probabilistic Models
CS 188: Aificial Inelligence Fall 2007 Lecue 15: Bayes Nes 10/18/2007 Dan Klein UC Bekeley Pobabilisic Models A pobabilisic model is a join disibuion ove a se of vaiables Given a join disibuion, we can
More informationElastic-Plastic Deformation of a Rotating Solid Disk of Exponentially Varying Thickness and Exponentially Varying Density
Poceedings of he Inenaional MuliConfeence of Enginees Compue Scieniss 6 Vol II, IMECS 6, Mach 6-8, 6, Hong Kong Elasic-Plasic Defomaion of a Roaing Solid Dis of Exponenially Vaying hicness Exponenially
More informationOptimal Decentralized State-Feedback Control with Sparsity and Delays
Opimal Decenalized Sae-Feedback Conol wih Spaiy and Delay ndew Lampeki Lauen Lead uomaica, vol. 58, pp. 43 5, ug. 5 bac Thi wok peen he oluion o a cla of decenalized linea quadaic ae-feedback conol poblem,
More informationControl Volume Derivation
School of eospace Engineeing Conol Volume -1 Copyigh 1 by Jey M. Seizman. ll ighs esee. Conol Volume Deiaion How o cone ou elaionships fo a close sysem (conol mass) o an open sysem (conol olume) Fo mass
More informationMEEN 617 Handout #11 MODAL ANALYSIS OF MDOF Systems with VISCOUS DAMPING
MEEN 67 Handou # MODAL ANALYSIS OF MDOF Sysems wih VISCOS DAMPING ^ Symmeic Moion of a n-dof linea sysem is descibed by he second ode diffeenial equaions M+C+K=F whee () and F () ae n ows vecos of displacemens
More informationWide Area Based Precise Point Positioning
Wide Aea Baed Pecie Poin Poiioning Rodigo F. Leando and Macelo C. Sano Geodeic Reeach Laboaoy, Depamen of Geodey and Geomaic Engineeing Univeiy of ew Bunwick, Fedeicon, Canada BIOGRAPHIES Rodigo Leando
More informationThi aicle wa oiginally publihed in a jounal publihed by levie, and he aached copy i povided by levie fo he auho benefi and fo he benefi of he auho iniuion, fo non-commecial eeach and educaional ue including
More informationTheorem 2: Proof: Note 1: Proof: Note 2:
A New 3-Dimenional Polynomial Intepolation Method: An Algoithmic Appoach Amitava Chattejee* and Rupak Bhattachayya** A new 3-dimenional intepolation method i intoduced in thi pape. Coeponding to the method
More informationOrthotropic Materials
Kapiel 2 Ohoopic Maeials 2. Elasic Sain maix Elasic sains ae elaed o sesses by Hooke's law, as saed below. The sesssain elaionship is in each maeial poin fomulaed in he local caesian coodinae sysem. ε
More informationEngineering Accreditation. Heat Transfer Basics. Assessment Results II. Assessment Results. Review Definitions. Outline
Hea ansfe asis Febua 7, 7 Hea ansfe asis a Caeo Mehanial Engineeing 375 Hea ansfe Febua 7, 7 Engineeing ediaion CSUN has aedied pogams in Civil, Eleial, Manufauing and Mehanial Engineeing Naional aediing
More informationENGI 4430 Advanced Calculus for Engineering Faculty of Engineering and Applied Science Problem Set 9 Solutions [Theorems of Gauss and Stokes]
ENGI 44 Avance alculus fo Engineeing Faculy of Engineeing an Applie cience Poblem e 9 oluions [Theoems of Gauss an okes]. A fla aea A is boune by he iangle whose veices ae he poins P(,, ), Q(,, ) an R(,,
More informationDiscussion Session 2 Constant Acceleration/Relative Motion Week 03
PHYS 100 Dicuion Seion Conan Acceleraion/Relaive Moion Week 03 The Plan Today you will work wih your group explore he idea of reference frame (i.e. relaive moion) and moion wih conan acceleraion. You ll
More informationΣr2=0. Σ Br. Σ br. Σ r=0. br = Σ. Σa r-s b s (1.2) s=0. Σa r-s b s-t c t (1.3) t=0. cr = Σ. dr = Σ. Σa r-s b s-t c t-u d u (1.4) u =0.
0 Powe of Infinite Seie. Multiple Cauchy Poduct The multinomial theoem i uele fo the powe calculation of infinite eie. Thi i becaue the polynomial theoem depend on the numbe of tem, o it can not be applied
More informationLecture 5. Chapter 3. Electromagnetic Theory, Photons, and Light
Lecue 5 Chape 3 lecomagneic Theo, Phoons, and Ligh Gauss s Gauss s Faada s Ampèe- Mawell s + Loen foce: S C ds ds S C F dl dl q Mawell equaions d d qv A q A J ds ds In mae fields ae defined hough ineacion
More informationNuclear Inst. and Methods in Physics Research B
Conen li available a Scienceiec Nuclea n. and Mehod in Phyic Reeach B jounal homepage: www.elevie.com/locae/nimb Localied aniion model in luminecence: A eappaial Geoge Kii a,, Vaili Pagoni b a Aiole Univeiy
More informationSelling at the ultimate maximum in a regime-switching model
Selling a he ulimae maximum in a egime-wiching model Yue Liu School of Finance and Economic Jiangu Univeiy Zhenjiang 21213 P.R. China Nicola Pivaul School of Phyical and Mahemaical Science Nanyang Technological
More informationReminder: Flow Networks
0/0/204 Ma/CS 6a Cla 4: Variou (Flow) Execie Reminder: Flow Nework A flow nework i a digraph G = V, E, ogeher wih a ource verex V, a ink verex V, and a capaciy funcion c: E N. Capaciy Source 7 a b c d
More informationJoint Workshop of Russian Acoustical Society (RAS) and French Acoustical Society (SFA)
. Symko, O. G., Abdel-Rahman, E., Kon, Y. S., Emmi, M., and Behunin, R., 004, Deign and developmen of high-fequency hemoacouic engine fo hemal managemen in micoeleconic, Micoeleconic Jounal, 35, pp. 85-9.
More informationThe k-filtering Applied to Wave Electric and Magnetic Field Measurements from Cluster
The -fileing pplied o Wave lecic and Magneic Field Measuemens fom Cluse Jean-Louis PINÇON and ndes TJULIN LPC-CNRS 3 av. de la Recheche Scienifique 4507 Oléans Fance jlpincon@cns-oleans.f OUTLINS The -fileing
More information