A Model of Multi-DOF Microrobot Manipulator Using Artificial Muscle

Size: px
Start display at page:

Download "A Model of Multi-DOF Microrobot Manipulator Using Artificial Muscle"

Transcription

1 st WSEAS ntrnatonal Confrnc on BOMEDCAL ELECTRONCS and BOMEDCAL NFORMATCS (BEB '8 Rhods, Grc, August -, 8 A Modl of Mult-DOF Mcrorobot Manpulator Usng Artfcal Muscl l OA, Adran ZAFU Unvrsty of tst, Elctroncs and Computrs Dpartmnt, Strt Targul dn Val, No., tst, Args, 4, Romana cpopa@upt.ro Abstract: - n ths papr, w dscrbd a nw typ of mult-dof manpulator usng a structur wth thr artfcal muscl (MC sgmnts. W dvlop th knmatc modlng of multlnk motons for th control of th manpulator usng a transposd Jacoban or an nvrs Jacoban usng as snsors lmnts of motons was ralzd by MC flm too, bcaus was usd th spcal actuator-snsor sgmnt (MC flms ar sparatd lctrcally by cuttng groovs and both th snsor and th actuator can b unfd n th sam structur. Th papr contan smulaton rsults of ths modl. Kywords: Elctroactv olymr Artfcal Muscl (EAM; onc olymr-mtal Compost (MC; Dgr- Of-Frdom (DOF, dual actuator-snsor flm; mcrorobot manpulator; mult-lnk knmatcs; transposd Jacoban control. ntroducton A bmorph-typ soft polymr gl actuator, whch w call an lctroactv artfcal muscl, s an onc polymr-mtal compost (MC consstng of a prfluorosulfonc acd mmbran wth chmcally platd gold or platnum as lctrods on both sds [, ]. t has som xcllnt charactrstcs for robotc applcatons compard wth othr soft polymr actuators [3, 4, 5] as follows: Low powr consumpton; Drvn wth low voltag (<3V; Fast rspons (> Hz n watr; Mchancally and chmcally durabl and stabl; Soft and complant; Works n watr (or n wt condtons. Morovr, t has an advantag for mnaturzaton wth ts smpl actuator structur. Wth ths charactrstcs, w xpct to apply t to mcromanpulatons n th bongnrng or mdcal flds. Our goal s to ralz bonsprd soft robots, for xampl a multdgr-of frdom (DOF mcrorobot manpulator [6, 7].t s asy to mnaturz th actuator bcaus of ts smpl structur. n th futur, s possbl to mak robots that can swm n thn tubs or n blood vssls, or varous knds of mcromanpulators n th bomdcal fld. n ths papr, w show som rsults from smulatons of th proposd manpulator control mthod of th mult-dof bndng moton and smulatd rsults for th dual actuator snsor sgmnt structur MC flm (s Fgur b. Bcaus Th MC artfcal muscl s not stabl whn work n ar, bat has a good stablty n aquous mdum [4, 5], hand-arm was sunkn n watr (s Fgur a. Th Mult-DOF Manpulator Structur Mcromanpulatons n bongnrng or n th mdcal fld can b on of th applcatons of th artfcal muscl. Our goal s to nvstgat th possblts to ralz a mult-dof mcrorobot manpulator that s automatcally controlld by a dual systm actuator-snsor, as shown n Fgur [8]. MC flms ar sparatd lctrcally by cuttng groovs and both th snsor and th actuator can b unfd n th sam structur. Ths arrangmnt s mor ffctv to sns moton than th paralll arrangmnt bcaus thr s lss ntrfrnc wth th actuaton by th snsor part [9]. Th sz of th strp s 3 [mm]. Th strp s sparatd nto th two sctons, th snsor part s mm wd, and th actuator part s mm wd. Two coupls of lctrods wr arrangd for th actuator and th snsor [9]. Th lasr dsplacmnt snsor was usd for MC snsor flm calbraton. SSN: SBN:

2 st WSEAS ntrnatonal Confrnc on BOMEDCAL ELECTRONCS and BOMEDCAL NFORMATCS (BEB '8 Rhods, Grc, August -, 8 Th block dagram of th control systm for ths modl of mult-dof composd by thr sgmnts MC actuator-snsor s showd n Fgur a. Th pattrnng of lctrods on an MC nabls th mult- DOF bndng motons of a manpulator wth a smpl structur. Command sgnals Currnt amplfr D/A convrtr Cnmatc modl Actuator controllr Snsors sgnals Currnt amplfr A/D convrtr and sral ntrfac C (Wndows X urfd watr Hand arm wth artfcal muscl and snsors MC a Fgur. a Applcaton of mult-dof artfcal muscls MC; b Structur of MC actuator-snsor flm. b Th proposd fdback control systm showd n Fgur ncluds a snsng systm, a Jacoban and rror stmaton componnt, a control componnt, and a mult-dof pattrnd artfcal muscl (MC. Th manpulator s hung n watr abov th lctrc connctor. 3 Modlng of Mult-Lnk Knmatcs To ralz th mult-dof moton of a manpulator, w can connct svral lnks n srs n th sam way as n convntonal sral-lnk manpulators. n ths study, as a frst stp n our rsarch, w rstrct th moton of th manpulator to a two dmnsonal spac, n whch two DOF for poston and on DOF for th tangntal drcton of th nd pont ar controlld. W can control all thr DOF ndpndntly by controllng th thr lnks of an MC. W now dfn coordnat systms,( = {,,,3 } on at th orgn, on at ach jont of th mult-lnk systm, and on at th nd pont of an arm, as shown n Fgurs and 3. A homognous transfr matrx A+ from + to s: A l cos( sn( ( cos l = sn( + cos( + sn α α (3. + whr th crtan lngth of a lnk s l, th curvatur s = r / l, and f th lnk has a crtan bndng angl ( SSN: SBN:

3 st WSEAS ntrnatonal Confrnc on BOMEDCAL ELECTRONCS and BOMEDCAL NFORMATCS (BEB '8 Rhods, Grc, August -, 8 at th jont, ths angl s rfrrd as α. W consdr that l and α ar known and α =. Fgur. On-lnk knmatc modlng (not that usually α =, as n ths study Fgur 3. Mult-lnk coordnat systm (jonts ar usually not bnt, as n ths study A transfr matrx from th bas to th nd pont s calculatd by multplyng ach matrx of th lnk from th frst to th last usng T 3= A A A3 (3. whch s shown n Fgur 3. From ths quaton, w can obtan th poston vctor and rotaton angl th nd pont n th bas coordnat systm follows xprssons (3.3, of as (whr x = (, = (,, : t t x Y = cos( + + cos( + + cos( + + α cos( + = Y (cos α = sn( + + sn( + + sn( + sn( + sn To control th poston and orntaton of th hand of th manpulator, w hav to solv an nvrs knmatc problm. Mor spcfcally, w hav to solv ˆ = ( by t = (,, from Eq. (3.3, whr ˆ dnots both th objctv poston and orntaton. Howvr, t s qut dffcult to solv Eq. (3.3; thus w us Jacoban mthods for controllng and dfn control varabls to convrg to objctv valus. Th Jacoban of wth s dfnd by followng xprssons: J J = [ J J J ] =, ( = {,,} (3.4 Usng th Jacoban, th followng control, whch s an nvrs Jacoban mthod, wll nduc th control varabl to convrg to an objctv valu ˆ xponntally: ' ' λ ˆ = J ( = λ J ε (3.5 whr λ, n ths xprsson, s a gvn constant. Usng th transposd Jacoban mthod, wll also nduc convrgnc to an objctv: (3.6 ' t ' t = λ J ( ˆ = λ Jε Ths s possbl f an approprat valu of a constant ' λ s chosn. J can b calculatd xplctly, but w omt such calculatons. SSN: SBN:

4 st WSEAS ntrnatonal Confrnc on BOMEDCAL ELECTRONCS and BOMEDCAL NFORMATCS (BEB '8 Rhods, Grc, August -, 8 4 Smulatons W prformd som smulatons to vrfy our control mthods. A block dagram of a control systm smulaton s shown n Fgur 4. s possbl to obtan rsults by th nvrs Jacoban or by th transposd Jacoban mthod but w prsnt, n ths papr, only th transportd mthod. Th rsults obtand by ths mthod ar shown n Fgur 5. Objctv poston and orntaton ˆ + - ε Transposd Jacoban: J t ntgral: s Knmatc modl Arm moton Fgur 4. Block dagram of smulaton systm Fgur 5. Rsults obtand by transposd Jacoban control (uppr lft: hand s kpt n uppr drcton, uppr rght: ts drcton s changd to rght, bottom lft: trackng a round trajctory, bottom rght: mov and swng SSN: SBN:

5 st WSEAS ntrnatonal Confrnc on BOMEDCAL ELECTRONCS and BOMEDCAL NFORMATCS (BEB '8 Rhods, Grc, August -, 8 All rsults show that ach sgmnt of an MC mmbran s proprly bnt to ralz th gvn trajctors of postons and orntatons of th nd ponts. By th nvrs Jacoban mthod, trajctors n Cartsan coordnats ar straghtforward and xponntally convrgd to th objctv, whr thy ar not by th transposd Jacoban. Howvr, an nvrs Jacoban s not stabl nar a sngular poston, n ths cas, at th uprght poston, whras a transposd Jacoban s dfnd and stabl at any pont. From ths rsults, t s confrmd that s possbl to control all thr DOF of a -D manpulator by ths mthods. 5 Conclusons n ths study, w dscrbd a nw typ of mult-dof manpulator usng a structur wth thr artfcal muscl (MC sgmnts, and proposd th knmatc modlng of multlnk motons for th control of th manpulator usng a transposd Jacoban or an nvrs Jacoban. Th snsors lmnts of motons was ralzd by MC flm too, bcaus was usd th spcal actuator-snsor sgmnts prsntd n Fgur a. Smulatons and xprmnts vrfy our approach. By usng th nvrs Jacoban and transposd Jacoban mthods, trajctors n Cartsan coordnats ar convrgd, but th nvrs Jacoban s not stabl nar a sngular poston whl th transposd Jacoban s dfnd and stabl at any pont. From th smulatd rsults, t s confrmd that s possbl to control all thr DOF of a -D manpulator by ths mthods. W consdr that s vry mportant to addrss th problm of th low conductvty of sgmnt ntrconnctons. t s possbl to ncras th wdth of th ntrconnctons and/or ncras th amount of gold platng, so that thr conductv layrs bcom thckr. Although bndng vlocty gnrally follows a gvn voltag sgnal, nonlnar charactrstcs, such as swng back moton, also contrbut to a dynamc rspons. Rfrncs [] K. Asaka and K. Oguro ( Bndng of polylctrolyt mmbran platnum composts by lctrc stmul art. Rspons kntcs. J. of Elctroanalytcal Chmstry, 48: [] K. Oguro, Y. Kawam, and H. Taknaka (99 Bndng of an on-conductng polymr flm-lctrod compost by an lctrc stmulus at low voltag. J. of Mcromachn Socty, 5:7 3. (n Japans [3] Y. Bar-Cohn (, Elctro-actv polymrs: currnt capablts and challngs. roc. of SE nt. Symp. on Smart Structurs and Matrals, EAAD [4]. opa, olymrs as Artfcal Muscl n Robotcs, Elctroncs, Computrs and Artfcal ntllgnc ECA 7 ntrnatonal Confrnc, Unvrsty of tst, Jun 9, 3, Romana. [5].opa, Usng of Elctroactv olymrs as Artfcal Muscl Smart Matrals, 3rd ARA Congrs, Brasov, Romana, 3 July 5 August, pp [6] Y. Nakabo, T. Muka, and K. Asaka (4, A mult- DOF robot manpulator wth a pattrnd artfcal muscl. Th nd Conf. on Artfcal Muscls. Osaka [7] Y. Nakabo, T. Muka, and K. Asaka (5 Knmatc modlng and vsual snsng of mult-dof robot manpulator wth pattrnd artfcal muscl. roc. EEE nt. Conf. Robotcs and Automaton, [8] A. unnng, Elctromcancal charactrzaton of onc olymr-mtal ompost snsng actuator, Tartu Unvrsty rss, 7. [9] Konyo M., Y. Konsh, S. Tadokoro, and T. Kshma, Dvlopmnt of Vlocty Snsor Usng onc olymr- Mtal Composts, roc. SE ntrnatonal Symposum on Smart Structurs, Confrnc on Elctro-Actv olymr Actuators and Dvcs, 3. SSN: SBN:

COMPLEX NUMBER PAIRWISE COMPARISON AND COMPLEX NUMBER AHP

COMPLEX NUMBER PAIRWISE COMPARISON AND COMPLEX NUMBER AHP ISAHP 00, Bal, Indonsa, August -9, 00 COMPLEX NUMBER PAIRWISE COMPARISON AND COMPLEX NUMBER AHP Chkako MIYAKE, Kkch OHSAWA, Masahro KITO, and Masaak SHINOHARA Dpartmnt of Mathmatcal Informaton Engnrng

More information

8-node quadrilateral element. Numerical integration

8-node quadrilateral element. Numerical integration Fnt Elmnt Mthod lctur nots _nod quadrlatral lmnt Pag of 0 -nod quadrlatral lmnt. Numrcal ntgraton h tchnqu usd for th formulaton of th lnar trangl can b formall tndd to construct quadrlatral lmnts as wll

More information

Electrochemical Equilibrium Electromotive Force. Relation between chemical and electric driving forces

Electrochemical Equilibrium Electromotive Force. Relation between chemical and electric driving forces C465/865, 26-3, Lctur 7, 2 th Sp., 26 lctrochmcal qulbrum lctromotv Forc Rlaton btwn chmcal and lctrc drvng forcs lctrochmcal systm at constant T and p: consdr G Consdr lctrochmcal racton (nvolvng transfr

More information

The Hyperelastic material is examined in this section.

The Hyperelastic material is examined in this section. 4. Hyprlastcty h Hyprlastc matral s xad n ths scton. 4..1 Consttutv Equatons h rat of chang of ntrnal nrgy W pr unt rfrnc volum s gvn by th strss powr, whch can b xprssd n a numbr of dffrnt ways (s 3.7.6):

More information

A Note on Estimability in Linear Models

A Note on Estimability in Linear Models Intrnatonal Journal of Statstcs and Applcatons 2014, 4(4): 212-216 DOI: 10.5923/j.statstcs.20140404.06 A Not on Estmablty n Lnar Modls S. O. Adymo 1,*, F. N. Nwob 2 1 Dpartmnt of Mathmatcs and Statstcs,

More information

Physics of Very High Frequency (VHF) Capacitively Coupled Plasma Discharges

Physics of Very High Frequency (VHF) Capacitively Coupled Plasma Discharges Physcs of Vry Hgh Frquncy (VHF) Capactvly Coupld Plasma Dschargs Shahd Rauf, Kallol Bra, Stv Shannon, and Kn Collns Appld Matrals, Inc., Sunnyval, CA AVS 54 th Intrnatonal Symposum Sattl, WA Octobr 15-19,

More information

External Equivalent. EE 521 Analysis of Power Systems. Chen-Ching Liu, Boeing Distinguished Professor Washington State University

External Equivalent. EE 521 Analysis of Power Systems. Chen-Ching Liu, Boeing Distinguished Professor Washington State University xtrnal quvalnt 5 Analyss of Powr Systms Chn-Chng Lu, ong Dstngushd Profssor Washngton Stat Unvrsty XTRNAL UALNT ach powr systm (ara) s part of an ntrconnctd systm. Montorng dvcs ar nstalld and data ar

More information

Polytropic Process. A polytropic process is a quasiequilibrium process described by

Polytropic Process. A polytropic process is a quasiequilibrium process described by Polytropc Procss A polytropc procss s a quasqulbrum procss dscrbd by pv n = constant (Eq. 3.5 Th xponnt, n, may tak on any valu from to dpndng on th partcular procss. For any gas (or lqud, whn n = 0, th

More information

Naresuan University Journal: Science and Technology 2018; (26)1

Naresuan University Journal: Science and Technology 2018; (26)1 Narsuan Unvrsty Journal: Scnc and Tchnology 018; (6)1 Th Dvlopmnt o a Corrcton Mthod or Ensurng a Contnuty Valu o Th Ch-squar Tst wth a Small Expctd Cll Frquncy Kajta Matchma 1 *, Jumlong Vongprasrt and

More information

Heisenberg Model. Sayed Mohammad Mahdi Sadrnezhaad. Supervisor: Prof. Abdollah Langari

Heisenberg Model. Sayed Mohammad Mahdi Sadrnezhaad. Supervisor: Prof. Abdollah Langari snbrg Modl Sad Mohammad Mahd Sadrnhaad Survsor: Prof. bdollah Langar bstract: n ths rsarch w tr to calculat analtcall gnvalus and gnvctors of fnt chan wth ½-sn artcls snbrg modl. W drov gnfuctons for closd

More information

COMPLIANCE ANALYSIS, OPTIMISATION AND COMPARISON OF A NEW 3PUS-PU MECHANISM. B. Wei

COMPLIANCE ANALYSIS, OPTIMISATION AND COMPARISON OF A NEW 3PUS-PU MECHANISM. B. Wei Intrnatonal Journal of Automotv and Mchancal Engnrng (IJAME) ISSN: 9-869 (Prnt); ISSN: 8-66 (Onln); Volum 7, pp. 9-99, Januar-Jun Unvrst Malasa Pahang DOI: http://d.do.org/.58/jam.7...9-99 COMPLIANCE ANALYSIS,

More information

Discrete Shells Simulation

Discrete Shells Simulation Dscrt Shlls Smulaton Xaofng M hs proct s an mplmntaton of Grnspun s dscrt shlls, th modl of whch s govrnd by nonlnar mmbran and flxural nrgs. hs nrgs masur dffrncs btwns th undformd confguraton and th

More information

Stress-Based Finite Element Methods for Dynamics Analysis of Euler-Bernoulli Beams with Various Boundary Conditions

Stress-Based Finite Element Methods for Dynamics Analysis of Euler-Bernoulli Beams with Various Boundary Conditions 9 Strss-Basd Fnt Elmnt Mthods for Dynamcs Analyss of Eulr-Brnoull Bams wth Varous Boundary Condtons Abstract In ths rsarch, two strss-basd fnt lmnt mthods ncludng th curvatur-basd fnt lmnt mthod (CFE)

More information

10/7/14. Mixture Models. Comp 135 Introduction to Machine Learning and Data Mining. Maximum likelihood estimation. Mixture of Normals in 1D

10/7/14. Mixture Models. Comp 135 Introduction to Machine Learning and Data Mining. Maximum likelihood estimation. Mixture of Normals in 1D Comp 35 Introducton to Machn Larnng and Data Mnng Fall 204 rofssor: Ron Khardon Mxtur Modls Motvatd by soft k-mans w dvlopd a gnratv modl for clustrng. Assum thr ar k clustrs Clustrs ar not rqurd to hav

More information

Lecture 23 APPLICATIONS OF FINITE ELEMENT METHOD TO SCALAR TRANSPORT PROBLEMS

Lecture 23 APPLICATIONS OF FINITE ELEMENT METHOD TO SCALAR TRANSPORT PROBLEMS COMPUTTION FUID DYNMICS: FVM: pplcatons to Scalar Transport Prolms ctur 3 PPICTIONS OF FINITE EEMENT METHOD TO SCR TRNSPORT PROBEMS 3. PPICTION OF FEM TO -D DIFFUSION PROBEM Consdr th stady stat dffuson

More information

ST 524 NCSU - Fall 2008 One way Analysis of variance Variances not homogeneous

ST 524 NCSU - Fall 2008 One way Analysis of variance Variances not homogeneous ST 54 NCSU - Fall 008 On way Analyss of varanc Varancs not homognous On way Analyss of varanc Exampl (Yandll, 997) A plant scntst masurd th concntraton of a partcular vrus n plant sap usng ELISA (nzym-lnkd

More information

Economics 600: August, 2007 Dynamic Part: Problem Set 5. Problems on Differential Equations and Continuous Time Optimization

Economics 600: August, 2007 Dynamic Part: Problem Set 5. Problems on Differential Equations and Continuous Time Optimization THE UNIVERSITY OF MARYLAND COLLEGE PARK, MARYLAND Economcs 600: August, 007 Dynamc Part: Problm St 5 Problms on Dffrntal Equatons and Contnuous Tm Optmzaton Quston Solv th followng two dffrntal quatons.

More information

Lecture 3: Phasor notation, Transfer Functions. Context

Lecture 3: Phasor notation, Transfer Functions. Context EECS 5 Fall 4, ctur 3 ctur 3: Phasor notaton, Transfr Functons EECS 5 Fall 3, ctur 3 Contxt In th last lctur, w dscussd: how to convrt a lnar crcut nto a st of dffrntal quatons, How to convrt th st of

More information

Decentralized Adaptive Control and the Possibility of Utilization of Networked Control System

Decentralized Adaptive Control and the Possibility of Utilization of Networked Control System Dcntralzd Adaptv Control and th Possblty of Utlzaton of Ntworkd Control Systm MARIÁN ÁRNÍK, JÁN MURGAŠ Slovak Unvrsty of chnology n Bratslava Faculty of Elctrcal Engnrng and Informaton chnology Insttut

More information

ACOUSTIC WAVE EQUATION. Contents INTRODUCTION BULK MODULUS AND LAMÉ S PARAMETERS

ACOUSTIC WAVE EQUATION. Contents INTRODUCTION BULK MODULUS AND LAMÉ S PARAMETERS ACOUSTIC WAE EQUATION Contnts INTRODUCTION BULK MODULUS AND LAMÉ S PARAMETERS INTRODUCTION As w try to vsualz th arth ssmcally w mak crtan physcal smplfcatons that mak t asr to mak and xplan our obsrvatons.

More information

VISUALIZATION OF DIFFERENTIAL GEOMETRY UDC 514.7(045) : : Eberhard Malkowsky 1, Vesna Veličković 2

VISUALIZATION OF DIFFERENTIAL GEOMETRY UDC 514.7(045) : : Eberhard Malkowsky 1, Vesna Veličković 2 FACTA UNIVERSITATIS Srs: Mchancs, Automatc Control Robotcs Vol.3, N o, 00, pp. 7-33 VISUALIZATION OF DIFFERENTIAL GEOMETRY UDC 54.7(045)54.75.6:59.688:59.673 Ebrhard Malkowsky, Vsna Vlčkovć Dpartmnt of

More information

Jones vector & matrices

Jones vector & matrices Jons vctor & matrcs PY3 Colást na hollscol Corcagh, Ér Unvrst Collg Cork, Irland Dpartmnt of Phscs Matr tratmnt of polarzaton Consdr a lght ra wth an nstantanous -vctor as shown k, t ˆ k, t ˆ k t, o o

More information

Outlier-tolerant parameter estimation

Outlier-tolerant parameter estimation Outlr-tolrant paramtr stmaton Baysan thods n physcs statstcs machn larnng and sgnal procssng (SS 003 Frdrch Fraundorfr fraunfr@cg.tu-graz.ac.at Computr Graphcs and Vson Graz Unvrsty of Tchnology Outln

More information

From Structural Analysis to FEM. Dhiman Basu

From Structural Analysis to FEM. Dhiman Basu From Structural Analyss to FEM Dhman Basu Acknowldgmnt Followng txt books wr consultd whl prparng ths lctur nots: Znkwcz, OC O.C. andtaylor Taylor, R.L. (000). Th FntElmnt Mthod, Vol. : Th Bass, Ffth dton,

More information

Analyzing Frequencies

Analyzing Frequencies Frquncy (# ndvduals) Frquncy (# ndvduals) /3/16 H o : No dffrnc n obsrvd sz frquncs and that prdctd by growth modl How would you analyz ths data? 15 Obsrvd Numbr 15 Expctd Numbr from growth modl 1 1 5

More information

September 27, Introduction to Ordinary Differential Equations. ME 501A Seminar in Engineering Analysis Page 1. Outline

September 27, Introduction to Ordinary Differential Equations. ME 501A Seminar in Engineering Analysis Page 1. Outline Introucton to Ornar Dffrntal Equatons Sptmbr 7, 7 Introucton to Ornar Dffrntal Equatons Larr artto Mchancal Engnrng AB Smnar n Engnrng Analss Sptmbr 7, 7 Outln Rvw numrcal solutons Bascs of ffrntal quatons

More information

MECH321 Dynamics of Engineering System Week 4 (Chapter 6)

MECH321 Dynamics of Engineering System Week 4 (Chapter 6) MH3 Dynamc of ngnrng Sytm Wk 4 (haptr 6). Bac lctrc crcut thor. Mathmatcal Modlng of Pav rcut 3. ompl mpdanc Approach 4. Mchancal lctrcal analogy 5. Modllng of Actv rcut: Opratonal Amplfr rcut Bac lctrc

More information

Dynamic Modeling and Vibration Control for Spacecraft s Solar Array Jian-Ping JIANG 1,a, *, Rui XU 2,b

Dynamic Modeling and Vibration Control for Spacecraft s Solar Array Jian-Ping JIANG 1,a, *, Rui XU 2,b Intrnatonal Confrnc on Mchancs and Cvl Engnrng (ICMCE 2014) Dynamc Modlng and Vbraton Control for Spaccraft s Solar Array Jan-Png JIANG 1,a, *, Ru XU 2,b 1,2 Collg of Arospac Scnc and Engnrng, Natonal

More information

Physics 256: Lecture 2. Physics

Physics 256: Lecture 2. Physics Physcs 56: Lctur Intro to Quantum Physcs Agnda for Today Complx Numbrs Intrfrnc of lght Intrfrnc Two slt ntrfrnc Dffracton Sngl slt dffracton Physcs 01: Lctur 1, Pg 1 Constructv Intrfrnc Ths wll occur

More information

Grand Canonical Ensemble

Grand Canonical Ensemble Th nsmbl of systms mmrsd n a partcl-hat rsrvor at constant tmpratur T, prssur P, and chmcal potntal. Consdr an nsmbl of M dntcal systms (M =,, 3,...M).. Thy ar mutually sharng th total numbr of partcls

More information

Lucas Test is based on Euler s theorem which states that if n is any integer and a is coprime to n, then a φ(n) 1modn.

Lucas Test is based on Euler s theorem which states that if n is any integer and a is coprime to n, then a φ(n) 1modn. Modul 10 Addtonal Topcs 10.1 Lctur 1 Prambl: Dtrmnng whthr a gvn ntgr s prm or compost s known as prmalty tstng. Thr ar prmalty tsts whch mrly tll us whthr a gvn ntgr s prm or not, wthout gvng us th factors

More information

A NEW GENERALISATION OF SAM-SOLAI S MULTIVARIATE ADDITIVE GAMMA DISTRIBUTION*

A NEW GENERALISATION OF SAM-SOLAI S MULTIVARIATE ADDITIVE GAMMA DISTRIBUTION* A NEW GENERALISATION OF SAM-SOLAI S MULTIVARIATE ADDITIVE GAMMA DISTRIBUTION* Dr. G.S. Davd Sam Jayakumar, Assstant Profssor, Jamal Insttut of Managmnt, Jamal Mohamd Collg, Truchraall 620 020, South Inda,

More information

CHAPTER 7d. DIFFERENTIATION AND INTEGRATION

CHAPTER 7d. DIFFERENTIATION AND INTEGRATION CHAPTER 7d. DIFFERENTIATION AND INTEGRATION A. J. Clark School o Engnrng Dpartmnt o Cvl and Envronmntal Engnrng by Dr. Ibrahm A. Assakka Sprng ENCE - Computaton Mthods n Cvl Engnrng II Dpartmnt o Cvl and

More information

Add sodium hydroxide solution

Add sodium hydroxide solution , :::.l9 &30 ~!fjrkh:+l. ~ S/::T..:=4... A studnt has four solutons lablld A, B, C and D. Each soluton contans on compound from th followng lst: FCh Th studnt dos som smpl tsts to dntfy th compounds prsnt.

More information

Α complete processing methodology for 3D monitoring using GNSS receivers

Α complete processing methodology for 3D monitoring using GNSS receivers 7-5-5 NATIONA TECHNICA UNIVERSITY OF ATHENS SCHOO OF RURA AND SURVEYING ENGINEERING DEPARTMENT OF TOPOGRAPHY AORATORY OF GENERA GEODESY Α complt procssng mthodology for D montorng usng GNSS rcvrs Gorg

More information

Radial Cataphoresis in Hg-Ar Fluorescent Lamp Discharges at High Power Density

Radial Cataphoresis in Hg-Ar Fluorescent Lamp Discharges at High Power Density [NWP.19] Radal Cataphorss n Hg-Ar Fluorscnt Lamp schargs at Hgh Powr nsty Y. Aura, G. A. Bonvallt, J. E. Lawlr Unv. of Wsconsn-Madson, Physcs pt. ABSTRACT Radal cataphorss s a procss n whch th lowr onzaton

More information

Review - Probabilistic Classification

Review - Probabilistic Classification Mmoral Unvrsty of wfoundland Pattrn Rcognton Lctur 8 May 5, 6 http://www.ngr.mun.ca/~charlsr Offc Hours: Tusdays Thursdays 8:3-9:3 PM E- (untl furthr notc) Gvn lablld sampls { ɛc,,,..., } {. Estmat Rvw

More information

Spectral stochastic finite element analysis of structures with random field parameters under bounded-but-uncertain forces

Spectral stochastic finite element analysis of structures with random field parameters under bounded-but-uncertain forces Southrn Cross Unvrsty Publcatons@SCU 23rd Australasan Confrnc on th Mchancs of Structurs and Matrals 24 Spctral stochastc fnt lmnt analyss of structurs wth random fld paramtrs undr boundd-but-uncrtan forcs

More information

Linear Algebra Provides a Basis for Elasticity without Stress or Strain

Linear Algebra Provides a Basis for Elasticity without Stress or Strain Soft, 05, 4, 5-4 Publshd Onln Sptmbr 05 n ScRs. http://www.scrp.org/ournal/soft http://dx.do.org/0.46/soft.05.400 Lnar Algbra Provds a Bass for Elastcty wthout Strss or Stran H. H. Hardy Math/Physcs Dpartmnt,

More information

CHAPTER 33: PARTICLE PHYSICS

CHAPTER 33: PARTICLE PHYSICS Collg Physcs Studnt s Manual Chaptr 33 CHAPTER 33: PARTICLE PHYSICS 33. THE FOUR BASIC FORCES 4. (a) Fnd th rato of th strngths of th wak and lctromagntc forcs undr ordnary crcumstancs. (b) What dos that

More information

Three-Node Euler-Bernoulli Beam Element Based on Positional FEM

Three-Node Euler-Bernoulli Beam Element Based on Positional FEM Avalabl onln at www.scncdrct.com Procda Engnrng 9 () 373 377 Intrnatonal Workshop on Informaton and Elctroncs Engnrng (IWIEE) Thr-Nod Eulr-Brnoull Bam Elmnt Basd on Postonal FEM Lu Jan a *,b, Zhou Shnj

More information

CHAPTER 6 DESIGN OF THE PV-UPQC SYSTEM FOR LONG VOLTAGE INTERRUPTION COMPENSATION

CHAPTER 6 DESIGN OF THE PV-UPQC SYSTEM FOR LONG VOLTAGE INTERRUPTION COMPENSATION 125 CHAPTER 6 DESIGN OF THE PV-UPQC SYSTEM FOR LONG VOLTAGE INTERRUPTION COMPENSATION INTRODUCTION Cntralzd powr gnraton systms ar facng th dual constrants of shortag of fossl ful and th nd to rduc hazardous

More information

Ch. 9 Common Emitter Amplifier

Ch. 9 Common Emitter Amplifier Ch. 9 Common mttr mplfr Common mttr mplfr nput and put oltags ar 180 o -of-phas, whl th nput and put currnts ar n-phas wth th nput oltag. Output oltag ( V ) V V V C CC C C C C and V C ar -of-phas 10 μ

More information

Chapter 6 Student Lecture Notes 6-1

Chapter 6 Student Lecture Notes 6-1 Chaptr 6 Studnt Lctur Nots 6-1 Chaptr Goals QM353: Busnss Statstcs Chaptr 6 Goodnss-of-Ft Tsts and Contngncy Analyss Aftr compltng ths chaptr, you should b abl to: Us th ch-squar goodnss-of-ft tst to dtrmn

More information

JEE-2017 : Advanced Paper 2 Answers and Explanations

JEE-2017 : Advanced Paper 2 Answers and Explanations DE 9 JEE-07 : Advancd Papr Answrs and Explanatons Physcs hmstry Mathmatcs 0 A, B, 9 A 8 B, 7 B 6 B, D B 0 D 9, D 8 D 7 A, B, D A 0 A,, D 9 8 * A A, B A B, D 0 B 9 A, D 5 D A, B A,B,,D A 50 A, 6 5 A D B

More information

Relate p and T at equilibrium between two phases. An open system where a new phase may form or a new component can be added

Relate p and T at equilibrium between two phases. An open system where a new phase may form or a new component can be added 4.3, 4.4 Phas Equlbrum Dtrmn th slops of th f lns Rlat p and at qulbrum btwn two phass ts consdr th Gbbs functon dg η + V Appls to a homognous systm An opn systm whr a nw phas may form or a nw componnt

More information

Dynamic Modeling and Inverse Dynamic Analysis of Flexible Parallel Robots

Dynamic Modeling and Inverse Dynamic Analysis of Flexible Parallel Robots nthwb.com Dnamc Modlng and Invrs Dnamc nalss of Flbl Paralll Robots Du Zhaoca and Yu Yuqng Collg of Mchancal Engnrng & ppld Elctroncs chnolog,ng Unvrst of chnolog,ng, Chna Corrspondng author E-mal: duzhaoca@mals.but.du.cn

More information

Phys 774: Nonlinear Spectroscopy: SHG and Raman Scattering

Phys 774: Nonlinear Spectroscopy: SHG and Raman Scattering Last Lcturs: Polaraton of Elctromagntc Wavs Phys 774: Nonlnar Spctroscopy: SHG and Scattrng Gnral consdraton of polaraton Jons Formalsm How Polarrs work Mullr matrcs Stoks paramtrs Poncar sphr Fall 7 Polaraton

More information

Formulation of the extended Finite Element and the matched asymptotic development methods applied to the transient heat transfer in brazed assembly

Formulation of the extended Finite Element and the matched asymptotic development methods applied to the transient heat transfer in brazed assembly 6th IASME/WSEAS Intrnatonal Confrnc on HEA RASFER, HERMAL EGIEERIG and EVIROME (HE'8) Rhods, Grc, August -, 8 Formulaton of th Xtndd Fnt Elmnt and th matchd asymptotc dvlopmnt mthods appld to th transnt

More information

FEFF and Related Codes

FEFF and Related Codes FEFF and Rlatd Cods Anatoly Frnl Profssor Physcs Dpartmnt, Yshva Unvrsty, w Yor, USA Synchrotron Catalyss Consortum, Broohavn atonal Laboratory, USA www.yu.du/faculty/afrnl Anatoly.Frnl@yu.du FEFF: John

More information

Folding of Regular CW-Complexes

Folding of Regular CW-Complexes Ald Mathmatcal Scncs, Vol. 6,, no. 83, 437-446 Foldng of Rgular CW-Comlxs E. M. El-Kholy and S N. Daoud,3. Dartmnt of Mathmatcs, Faculty of Scnc Tanta Unvrsty,Tanta,Egyt. Dartmnt of Mathmatcs, Faculty

More information

u x v x dx u x v x v x u x dx d u x v x u x v x dx u x v x dx Integration by Parts Formula

u x v x dx u x v x v x u x dx d u x v x u x v x dx u x v x dx Integration by Parts Formula 7. Intgration by Parts Each drivativ formula givs ris to a corrsponding intgral formula, as w v sn many tims. Th drivativ product rul yilds a vry usful intgration tchniqu calld intgration by parts. Starting

More information

Observer Bias and Reliability By Xunchi Pu

Observer Bias and Reliability By Xunchi Pu Obsrvr Bias and Rliability By Xunchi Pu Introduction Clarly all masurmnts or obsrvations nd to b mad as accuratly as possibl and invstigators nd to pay carful attntion to chcking th rliability of thir

More information

A CLOSED-FORM SOLUTION TO ANALYZE RCS OF CAVITY WITH RECTANGULAR CROSS SECTION

A CLOSED-FORM SOLUTION TO ANALYZE RCS OF CAVITY WITH RECTANGULAR CROSS SECTION Progrss In Elctromagntcs Rsarch, PIER 79, 195 208, 2008 A CLOSED-FORM SOLUTION TO ANALYZE RCS OF CAVITY WITH RECTANGULAR CROSS SECTION L. Xu, J. Tan, and X. W. Sh Natonal Ky Laboratory of Antnna and Mcrowav

More information

Basic Electrical Engineering for Welding [ ] --- Introduction ---

Basic Electrical Engineering for Welding [ ] --- Introduction --- Basc Elctrcal Engnrng for Wldng [] --- Introducton --- akayosh OHJI Profssor Ertus, Osaka Unrsty Dr. of Engnrng VIUAL WELD CO.,LD t-ohj@alc.co.jp OK 15 Ex. Basc A.C. crcut h fgurs n A-group show thr typcal

More information

Study interaction between intensive circularly polarized laser and hydrogen atom using a matrix method

Study interaction between intensive circularly polarized laser and hydrogen atom using a matrix method ISBN 978-1-84626-020-9 Procdngs of 3 rd Intrnatonal Workshop on Matrx Analyss angzhou,p.r.chna.july 9-13, 2009, pp. 199-202 ( Wll st y th pulshr ) Study ntracton twn ntnsv crcularly polarzd lasr and hydrogn

More information

Einstein Equations for Tetrad Fields

Einstein Equations for Tetrad Fields Apiron, Vol 13, No, Octobr 006 6 Einstin Equations for Ttrad Filds Ali Rıza ŞAHİN, R T L Istanbul (Turky) Evry mtric tnsor can b xprssd by th innr product of ttrad filds W prov that Einstin quations for

More information

Fakultät III Univ.-Prof. Dr. Jan Franke-Viebach

Fakultät III Univ.-Prof. Dr. Jan Franke-Viebach Unv.Prof. r. J. FrankVbach WS 067: Intrnatonal Economcs ( st xam prod) Unvrstät Sgn Fakultät III Unv.Prof. r. Jan FrankVbach Exam Intrnatonal Economcs Wntr Smstr 067 ( st Exam Prod) Avalabl tm: 60 mnuts

More information

Minimally Actuated Serial Robot

Minimally Actuated Serial Robot Mnmally Actuatd Sral Robot Mosh P. Mann, Lor Damt, Davd Zarrouk Abstract In ths papr, w propos a novl typ of sral robot wth mnmal actuaton. Th robot s a sral rgd structur consstng of multpl lnks connctd

More information

A NON-LINEAR MODEL FOR STUDYING THE MOTION OF A HUMAN BODY. Piteşti, , Romania 2 Department of Automotive, University of Piteşti

A NON-LINEAR MODEL FOR STUDYING THE MOTION OF A HUMAN BODY. Piteşti, , Romania 2 Department of Automotive, University of Piteşti ICSV Carns ustrala 9- July 7 NON-LINER MOEL FOR STUYING THE MOTION OF HUMN OY Ncola-oru Stănscu Marna Pandra nl Popa Sorn Il Ştfan-Lucan Tabacu partnt of ppld Mchancs Unvrsty of Ptşt Ptşt 7 Roana partnt

More information

Soft k-means Clustering. Comp 135 Machine Learning Computer Science Tufts University. Mixture Models. Mixture of Normals in 1D

Soft k-means Clustering. Comp 135 Machine Learning Computer Science Tufts University. Mixture Models. Mixture of Normals in 1D Comp 35 Machn Larnng Computr Scnc Tufts Unvrsty Fall 207 Ron Khardon Th EM Algorthm Mxtur Modls Sm-Suprvsd Larnng Soft k-mans Clustrng ck k clustr cntrs : Assocat xampls wth cntrs p,j ~~ smlarty b/w cntr

More information

Representation and Reasoning with Uncertain Temporal Relations

Representation and Reasoning with Uncertain Temporal Relations Rprsntaton and Rasonng wth Uncrtan Tmporal Rlatons Vladmr Ryaov (*) Sppo Puuronn (*) Vagan Trzyan (**) (*) Dpartmnt of Computr Scnc and Informaton Systms Unvrsty of Jyvaskyla P.O.Box 5 SF-4051 Jyvaskyla

More information

Pipe flow friction, small vs. big pipes

Pipe flow friction, small vs. big pipes Friction actor (t/0 t o pip) Friction small vs larg pips J. Chaurtt May 016 It is an intrsting act that riction is highr in small pips than largr pips or th sam vlocity o low and th sam lngth. Friction

More information

EE 570: Location and Navigation: Theory & Practice

EE 570: Location and Navigation: Theory & Practice EE 570: Locaton and Navgaton: Thor & Practc Navgaton Snsors and INS Mchanaton Thursda 8 F 013 NMT EE 570: Locaton and Navgaton: Thor & Practc Sld 1 of 10 Navgaton Snsors and INS Mchanaton Navgaton Equatons

More information

HORIZONTAL IMPEDANCE FUNCTION OF SINGLE PILE IN SOIL LAYER WITH VARIABLE PROPERTIES

HORIZONTAL IMPEDANCE FUNCTION OF SINGLE PILE IN SOIL LAYER WITH VARIABLE PROPERTIES 13 th World Confrnc on Earthquak Engnrng Vancouvr, B.C., Canada August 1-6, 4 Papr No. 485 ORIZONTAL IMPEDANCE FUNCTION OF SINGLE PILE IN SOIL LAYER WIT VARIABLE PROPERTIES Mngln Lou 1 and Wnan Wang Abstract:

More information

Phy213: General Physics III 4/10/2008 Chapter 22 Worksheet 1. d = 0.1 m

Phy213: General Physics III 4/10/2008 Chapter 22 Worksheet 1. d = 0.1 m hy3: Gnral hyscs III 4/0/008 haptr Worksht lctrc Flds: onsdr a fxd pont charg of 0 µ (q ) q = 0 µ d = 0 a What s th agntud and drcton of th lctrc fld at a pont, a dstanc of 0? q = = 8x0 ˆ o d ˆ 6 N ( )

More information

Ερωτήσεις και ασκησεις Κεφ. 10 (για μόρια) ΠΑΡΑΔΟΣΗ 29/11/2016. (d)

Ερωτήσεις και ασκησεις Κεφ. 10 (για μόρια) ΠΑΡΑΔΟΣΗ 29/11/2016. (d) Ερωτήσεις και ασκησεις Κεφ 0 (για μόρια ΠΑΡΑΔΟΣΗ 9//06 Th coffcnt A of th van r Waals ntracton s: (a A r r / ( r r ( (c a a a a A r r / ( r r ( a a a a A r r / ( r r a a a a A r r / ( r r 4 a a a a 0 Th

More information

ON THE INTEGRAL INVARIANTS OF KINEMATICALLY GENERATED RULED SURFACES *

ON THE INTEGRAL INVARIANTS OF KINEMATICALLY GENERATED RULED SURFACES * Iranan Journal of Scnc & Tchnology Transacton A ol 9 No A Prntd n Th Islamc Rpublc of Iran 5 Shraz Unvrsty ON TH INTGRAL INARIANTS OF KINMATICALLY GNRATD RULD SURFACS H B KARADAG AND S KLS Dpartmnt of

More information

FREE VIBRATION ANALYSIS OF FUNCTIONALLY GRADED BEAMS

FREE VIBRATION ANALYSIS OF FUNCTIONALLY GRADED BEAMS Journal of Appl Mathatcs an Coputatonal Mchancs, (), 9- FREE VIBRATION ANAYSIS OF FNCTIONAY GRADED BEAMS Stansław Kukla, Jowta Rychlwska Insttut of Mathatcs, Czstochowa nvrsty of Tchnology Czstochowa,

More information

Homotopy perturbation technique

Homotopy perturbation technique Comput. Mthods Appl. Mch. Engrg. 178 (1999) 257±262 www.lsvir.com/locat/cma Homotopy prturbation tchniqu Ji-Huan H 1 Shanghai Univrsity, Shanghai Institut of Applid Mathmatics and Mchanics, Shanghai 272,

More information

te Finance (4th Edition), July 2017.

te Finance (4th Edition), July 2017. Appndx Chaptr. Tchncal Background Gnral Mathmatcal and Statstcal Background Fndng a bas: 3 2 = 9 3 = 9 1 /2 x a = b x = b 1/a A powr of 1 / 2 s also quvalnt to th squar root opraton. Fndng an xponnt: 3

More information

Shape sensing of aerospace structures by coupling of isogeometric analysis and inverse finite element method

Shape sensing of aerospace structures by coupling of isogeometric analysis and inverse finite element method Shap snsng of arospac structurs by couplng of sogomtrc analyss and nvrs fnt lmnt mthod dnan Kfal and Erkan Otrkus Unvrsty of Strathclyd, 00 Montros Strt, Glasgow G4 0LZ, UK Ths papr prsnts a novl sogomtrc

More information

An Overview of Markov Random Field and Application to Texture Segmentation

An Overview of Markov Random Field and Application to Texture Segmentation An Ovrvw o Markov Random Fld and Applcaton to Txtur Sgmntaton Song-Wook Joo Octobr 003. What s MRF? MRF s an xtnson o Markov Procss MP (D squnc o r.v. s unlatral (causal: p(x t x,

More information

Full Waveform Inversion Using an Energy-Based Objective Function with Efficient Calculation of the Gradient

Full Waveform Inversion Using an Energy-Based Objective Function with Efficient Calculation of the Gradient Full Wavform Invrsion Using an Enrgy-Basd Objctiv Function with Efficint Calculation of th Gradint Itm yp Confrnc Papr Authors Choi, Yun Sok; Alkhalifah, ariq Ali Citation Choi Y, Alkhalifah (217) Full

More information

THREE DIMENSIONAL GEOMETRY MAINTENANCE FOR FORMATION FLYING ON ELLIPTIC ORBITS

THREE DIMENSIONAL GEOMETRY MAINTENANCE FOR FORMATION FLYING ON ELLIPTIC ORBITS HREE DIMENSIONAL GEOMERY MAINENANCE FOR FORMAION FLYING ON ELLIPIC ORBIS akanao SAIKI ), Koch NASUME ) and Jun chro KAWAGUCHI ) ABSRAC ) Mtsubsh Havy Industrs, Ltd. ) Mtsubsh Elctrc Co. ) Japan Arospac

More information

Chemical Physics II. More Stat. Thermo Kinetics Protein Folding...

Chemical Physics II. More Stat. Thermo Kinetics Protein Folding... Chmical Physics II Mor Stat. Thrmo Kintics Protin Folding... http://www.nmc.ctc.com/imags/projct/proj15thumb.jpg http://nuclarwaponarchiv.org/usa/tsts/ukgrabl2.jpg http://www.photolib.noaa.gov/corps/imags/big/corp1417.jpg

More information

EEC 686/785 Modeling & Performance Evaluation of Computer Systems. Lecture 12

EEC 686/785 Modeling & Performance Evaluation of Computer Systems. Lecture 12 EEC 686/785 Modlng & Prformanc Evaluaton of Computr Systms Lctur Dpartmnt of Elctrcal and Computr Engnrng Clvland Stat Unvrsty wnbng@.org (basd on Dr. Ra Jan s lctur nots) Outln Rvw of lctur k r Factoral

More information

NMT EE 589 & UNM ME 482/582 ROBOT ENGINEERING. Dr. Stephen Bruder NMT EE 589 & UNM ME 482/582

NMT EE 589 & UNM ME 482/582 ROBOT ENGINEERING. Dr. Stephen Bruder NMT EE 589 & UNM ME 482/582 NMT EE 589 & UNM ME 482/582 ROBOT ENGINEERING Dr. Stephen Bruder NMT EE 589 & UNM ME 482/582 4. Moton Knematcs 4.2 Angular Velocty Knematcs Summary From the last lecture we concluded that: If the jonts

More information

14. MODELING OF THIN-WALLED SHELLS AND PLATES. INTRODUCTION TO THE THEORY OF SHELL FINITE ELEMENT MODELS

14. MODELING OF THIN-WALLED SHELLS AND PLATES. INTRODUCTION TO THE THEORY OF SHELL FINITE ELEMENT MODELS 4. ODELING OF IN-WALLED SELLS AND PLAES. INRODUCION O E EORY OF SELL FINIE ELEEN ODELS Srő: Dr. András Skréns Dr. András Skréns BE odlng of thn-walld shlls and plats. Introducton to th thor of shll fnt

More information

:2;$-$(01*%<*=,-./-*=0;"%/;"-*

:2;$-$(01*%<*=,-./-*=0;%/;-* !"#$%'()%"*#%*+,-./-*+01.2(.*3+456789*!"#$%"'()'*+,-."/0.%+1'23"45'46'7.89:89'/' ;8-,"$4351415,8:+#9' Dr. Ptr T. Gallaghr Astrphyscs Rsarch Grup Trnty Cllg Dubln :2;$-$(01*%

More information

Journal of Theoretical and Applied Information Technology 10 th January Vol. 47 No JATIT & LLS. All rights reserved.

Journal of Theoretical and Applied Information Technology 10 th January Vol. 47 No JATIT & LLS. All rights reserved. Journal o Thortcal and Appld Inormaton Tchnology th January 3. Vol. 47 No. 5-3 JATIT & LLS. All rghts rsrvd. ISSN: 99-8645 www.att.org E-ISSN: 87-395 RESEARCH ON PROPERTIES OF E-PARTIAL DERIVATIVE OF LOGIC

More information

NON-SYMMETRY POWER IN THREE-PHASE SYSTEMS

NON-SYMMETRY POWER IN THREE-PHASE SYSTEMS O-YMMETRY OWER THREE-HAE YTEM Llana Marlna MATCA nvrsty of Orada, nvrstat str., no., 487, Orada; lmatca@uorada.ro Abstract. For thr-phas lctrcal systms, n non-symmtrcal stuaton, an analyz mthod costs on

More information

Search sequence databases 3 10/25/2016

Search sequence databases 3 10/25/2016 Sarch squnc databass 3 10/25/2016 Etrm valu distribution Ø Suppos X is a random variabl with probability dnsity function p(, w sampl a larg numbr S of indpndnt valus of X from this distribution for an

More information

Two-Temperature Plasma Modeling of Argon Gas Tungsten Arcs.

Two-Temperature Plasma Modeling of Argon Gas Tungsten Arcs. Ttl Autor(s) Two-Tmpratur Plasma Modlng of Argon Gas Tungstn Arcs Tasro, Snc; Tanaa, Manabu Ctaton Transactons of JWRI. 37(1) P.7-P.11 Issu Dat 2008-07 Txt Vrson publsr URL ttp://dl.andl.nt/11094/8887

More information

Sliding Mode Flow Rate Observer Design

Sliding Mode Flow Rate Observer Design Sliding Mod Flow Rat Obsrvr Dsign Song Liu and Bin Yao School of Mchanical Enginring, Purdu Univrsity, Wst Lafaytt, IN797, USA liu(byao)@purdudu Abstract Dynamic flow rat information is ndd in a lot of

More information

ON THE COMPLEXITY OF K-STEP AND K-HOP DOMINATING SETS IN GRAPHS

ON THE COMPLEXITY OF K-STEP AND K-HOP DOMINATING SETS IN GRAPHS MATEMATICA MONTISNIRI Vol XL (2017) MATEMATICS ON TE COMPLEXITY OF K-STEP AN K-OP OMINATIN SETS IN RAPS M FARAI JALALVAN AN N JAFARI RA partmnt of Mathmatcs Shahrood Unrsty of Tchnology Shahrood Iran Emals:

More information

General Notes About 2007 AP Physics Scoring Guidelines

General Notes About 2007 AP Physics Scoring Guidelines AP PHYSICS C: ELECTRICITY AND MAGNETISM 2007 SCORING GUIDELINES Gnral Nots About 2007 AP Physics Scoring Guidlins 1. Th solutions contain th most common mthod of solving th fr-rspons qustions and th allocation

More information

Group Consensus of Multi-agent Networks With Multiple Time Delays

Group Consensus of Multi-agent Networks With Multiple Time Delays Intrnatonal Confrnc on Artfcal Intllgnc: Tchnologs and Applcatons (ICAITA 06 Group Consnsus of Mult-agnt Ntworks Wth Multpl Tm Dlays Langhao J* Xnyu Zhao Qun Lu and Yong Wang Chongqng Ky Laboratory of

More information

Modeling and Simulation Analysis of Power Frequency Electric Field of UHV AC Transmission Line

Modeling and Simulation Analysis of Power Frequency Electric Field of UHV AC Transmission Line (IJACSA) Intrnatonal Journal of Advancd Computr Scnc and Applcatons, Vol., o., Modlng and Smulaton Analyss of Powr Frquncy Elctrc Fld of UHV AC Transmsson Ln Chn Han Collg of Elctronc and Elctrcal Engnrng

More information

INTERFACE CORNERS IN ANISOTROPIC/PIEZOELECTRIC/ VISCOELASTIC MATERIALS

INTERFACE CORNERS IN ANISOTROPIC/PIEZOELECTRIC/ VISCOELASTIC MATERIALS INERFAE ORNERS IN ANISOROPI/PIEZOELERI/ VISOELASI MAERIALS hyanbn Hwu a-lang uo Insttut of Aronautcs and Astronautcs Natonal hng ung Unvrsty anan AIWAN R.O.. Ansotropc matrals bhav dffrntly n dffrnt drctons.

More information

Section 7 - Controllers for Electric Drive Systems

Section 7 - Controllers for Electric Drive Systems ELEC463 Scton 7 - Controllrs for 7. Introducton An lctrcal drv normally has a numbr of control loops rgulatng a numbr of varabls of th drv. Of cours som drvs, such as V-f drvs, may b opratd n opn loop.

More information

Mathematical Model of Arterial Hemodynamics, Description, Computer Implementation, Results Comparison

Mathematical Model of Arterial Hemodynamics, Description, Computer Implementation, Results Comparison Appld Physcs Rsarch; Vol. 5, No. 3; 3 ISSN 96-9639 E-ISSN 96-9647 Publshd by Canadan Cntr of Scnc and Educaton Mathmatcal Modl of Artral Hmodynamcs, Dscrpton, Computr Implmntaton, Rsults Comparson Elshn

More information

Lecture 14. Relic neutrinos Temperature at neutrino decoupling and today Effective degeneracy factor Neutrino mass limits Saha equation

Lecture 14. Relic neutrinos Temperature at neutrino decoupling and today Effective degeneracy factor Neutrino mass limits Saha equation Lctur Rlc nutrnos mpratur at nutrno dcoupln and today Effctv dnracy factor Nutrno mass lmts Saha quaton Physcal Cosmoloy Lnt 005 Rlc Nutrnos Nutrnos ar wakly ntractn partcls (lptons),,,,,,, typcal ractons

More information

The Fourier Transform

The Fourier Transform /9/ Th ourr Transform Jan Baptst Josph ourr 768-83 Effcnt Data Rprsntaton Data can b rprsntd n many ways. Advantag usng an approprat rprsntaton. Eampls: osy ponts along a ln Color spac rd/grn/blu v.s.

More information

A Sub-Optimal Log-Domain Decoding Algorithm for Non-Binary LDPC Codes

A Sub-Optimal Log-Domain Decoding Algorithm for Non-Binary LDPC Codes Procdings of th 9th WSEAS Intrnational Confrnc on APPLICATIONS of COMPUTER ENGINEERING A Sub-Optimal Log-Domain Dcoding Algorithm for Non-Binary LDPC Cods CHIRAG DADLANI and RANJAN BOSE Dpartmnt of Elctrical

More information

Learning Spherical Convolution for Fast Features from 360 Imagery

Learning Spherical Convolution for Fast Features from 360 Imagery Larning Sphrical Convolution for Fast Faturs from 36 Imagry Anonymous Author(s) 3 4 5 6 7 8 9 3 4 5 6 7 8 9 3 4 5 6 7 8 9 3 3 3 33 34 35 In this fil w provid additional dtails to supplmnt th main papr

More information

Modelling of new generation plasma optical devices

Modelling of new generation plasma optical devices NUKLEONIKA 216;61(2):27212 do: 1.1515/nuka-216-35 ORIGINAL PAPER Modllng of nw gnraton plasma optcal dvcs Irna V. Ltovko, Aly A. Goncharov, Andrw N. Dobrovolsky, Lly V. Nako, Irna V. Nako Abstract. Th

More information

ANALYSIS: The mass rate balance for the one-inlet, one-exit control volume at steady state is

ANALYSIS: The mass rate balance for the one-inlet, one-exit control volume at steady state is Problm 4.47 Fgur P4.47 provds stady stat opratng data for a pump drawng watr from a rsrvor and dlvrng t at a prssur of 3 bar to a storag tank prchd 5 m abov th rsrvor. Th powr nput to th pump s 0.5 kw.

More information

Plasma Simulation Algorithm for the Two-Fluid Plasma Model

Plasma Simulation Algorithm for the Two-Fluid Plasma Model ELIGIBLE Plasma Smulaton Algorthm for th Two-Flud Plasma Modl U. Shumlak, C. Abrl, A. Hakm, and J. Lovrch Arospac & Enrgtcs Rsarch Program Unvrsty of Washngton, Sattl, USA Confrnc on Computatonal Physcs

More information

Difference -Analytical Method of The One-Dimensional Convection-Diffusion Equation

Difference -Analytical Method of The One-Dimensional Convection-Diffusion Equation Diffrnc -Analytical Mthod of Th On-Dimnsional Convction-Diffusion Equation Dalabav Umurdin Dpartmnt mathmatic modlling, Univrsity of orld Economy and Diplomacy, Uzbistan Abstract. An analytical diffrncing

More information