Gantry-Tau A New Three Degrees of Freedom Parallel Kinematic Robot
|
|
- Gabriella Price
- 5 years ago
- Views:
Transcription
1 Gant-au A w h Dg of Fom Paa Kinmatic Robot La Johannon, Vikto Bbuk, ogn Bogåh. Dpatmnt of Machin an Vhic Stm Cham Univit of chnoog, 4 9 Götbog, Swn -mai: a.johannon@m.cham.. Dpatmnt of Machin an Vhic Stm Cham Univit of chnoog, 4 9 Götbog, Swn -mai: vikto.bbuk@m.cham.. ABB Automation chnoog Pouct/Robotic 7 8 Vätå -mai: togn.bogah@.abb.com Abtact In th at ca, an incaing attntion ha bn pai to th tu of iffnt paa tuctu mchanim an thi appication, main tigg b Stwat that pnt an aicaft imuato tm. Paa tuctu fatu povi big avantag in potntia appication. Fo amp, paa obot ma giv high p an accation, high tatic an namic accuac an high tiffn than what i poib with th inutia obot u toa. A tpica imitation with man of th paa tuctu i that thi wokpac i ma compa to th ia tuctu. hi pap pnt a nw paa tuctu, th Gant-au, which povi g of fom (DOF) tanationa motion with a ag wokpac. h tuctu of th obot i patnt b ABB. h Gant-au obot i a i ink paa kinmatic tuctu with th ink configu accoing to --. h -- notation f to how man ink fom ach uting kinmatic cut of th obot. Ointationa DOF of th obot cou b povi b a coup tm. Fo a convntiona DOF ia gant obot two of th actuato contibut to th moving ma. h Gant-au can b contuct with cptiona ow moving ma inc th actuato a tationa an th tuctu ha inhnt high tiffn. h tuctu i thu ia fo man appication with man on high accation, fo intanc fo th pick an pac opation. h nomina inv an ict kinmatic of th tuctu a vop an optimiation i u to fin a contuction of Gant-au with maimum wokpac voum. Intouction Mot of th obot u in th inut a ia manipuato. A ia manipuato ha an opn kinmatic chain tuctu. hi tp of obot off high gnait an can b u fo vaiou appication. Howv th ia manipuato uff fom a ow atio btwn oa capacit an obot ma. h main aon fo thi a that th obot actuato contibut to th moving ma an that ach ink i ubjct to th wight of th foowing ink. hu th ink hav to b imnion with pct to ag fu tou, which man that th tuctu ha to b tiffn, an thu bcom havi. Accuac i imit b th fact that th ink magnif o thoughout th chain. Fo intanc a ma angua o in a vout joint a in th chain wi inuc a ag o fo th too cnt point (CP).
2 A paa manipuato i a co kinmatic chain mchanim. h it a vait of achitctu ign fo iffnt appication. h paa manipuato can b chaacti with compaion to it ia countpat a a tm with [4]: high atio btwn oa capacit an obot ma, high tiffn, high about accuac, imp inv kinmatic, mo ifficut ict kinmatic, ma wokpac. h high atio btwn oa capacit an obot ma i u to that th actuato oftn a ocat on a fi patfom an fo man of th tuctu th ink a on ubjct to aia foc an that th oa i itibut ov th chain. High tiffn i u to that th tna foc i itibut ov th chain. High about accuac i u to non cumuativ joint o an th high tiffn. h inv kinmatic pobm i oftn ov ai inc th chain can b tui paat an that iffnt configuation a gna fi in th ign poc. h oution of th ict kinmatic pobm i oftn ifficut inc in th gna ca th i no uniu oution. h contant ointation wokpac i ao oftn imit fo mot DOF fu paa manipuato. On appoach to gt btt wokpac popti i to vop manipuato wh th tanationa g of fom a paat fom th otationa g of fom o to ign manipuato that a not fu paa. hi pap pnt a nw paa tuctu, th Gant-au, which povi DOF tanationa motion with a ag wokpac. h tuctu of th obot i patnt b ABB [] an a ut inicat that th tuctu cou outpfom th ia gant tuctu fo man appication. au bong to th PRRS fami of paa manipuato with th HaGi a on of it cot ativ [4]. h PRRS notation cib th joint in th kinmatic chain fom actuation to th CP. hu ach chain i fom b a pimatic joint with actuation (P), a univa joint (RR), an fina a phica joint which connct to th moving pat. h chain fom th kinmatic cut wh th chain a ogani a a oub paaogam, a ing paaogam an a ing ink which a connct to th moving pat. h pimatic joint a th paa ina tack. Figu how a chmatic fo th Gant-au tuctu. B moving A, B an C aong th tack fom S A,B,C, to S A,B,C, th tanationa motion i conto fo th CP whi th ointation of th moving pat i maintain. Z S A, Y X A S B, A B S C, Fig:. Schmatic Gant-au. Goba cooinat tm i fin with th X-ai aong th iction fom S A, to S A,. h back ot pnt phica joint. h vcto i i- fin th ocation fo th univa joint PU i i- fom point A, B an C (figu ). h vcto n i i- fin th ativ ocation fo th CP with pct to th phica joint PS i i- (figu ). C C PU PU PU S A, PS 4 B PS PU PU PU S B, CP S C, Kinmatic ciption PS PS 5 n 4 PS n h Gant-au i a i ink paa kinmatic tuctu with th ink configu accoing to --. h -- notation f to how man ink fom ach uting kinmatic am. Gant- PS n n 5 n n CP CP Z Y X Fig:. Schmatic moving pat. CP
3 h ngth of th ink i mut b th am fo ink bonging to th am cut. h vcto i i-5 an n i i-5 a puiit to fufi th conition that th vcto btwn PS an PS mut b paa to th vcto btwn PU an PU, an that th vcto btwn PS an PS 4 mut b paa to th vcto btwn PU an PU 4, an that th vcto btwn PS 4 an PS 5 mut b paa to th vcto btwn PU 4 an PU 5. Anoth phap obviou puiit i that PS 5 mut b ocat outi th pan PS PU PS 4. Sphica joint, aowing th ink to pin aoun thi pincipa ai, can of cou pac th univa joint. Fo om appication it might b favouab to u on univa joint. hi can b achiv b aing a vout joint on ach ink that pvnt th tuctu fom bing ov contain. A 4 DOF n too ointation aangmnt can b achiv b aing a oub caan ai a hown in figu. hi coup aangmnt i u in th Dta obot ign []. Anoth vaiant of th Gant-au i hown in figu 4. hi aangmnt off 5 DOF imit too tit an cou b u fo wat jt cutting, pama cutting an a cutting. Fig:4. 5 DOF oo tit.. Inv kinmatic Fo th coni paa obot th inv kinmatic pobm i fomuat a foow. Cacuat th ocation of point A, B an C aong th ina tack fo a givn CP ocation. Lt ( a ) S A, ( b ) SB, ( c ) SC, A +, B +, C +, ( ) CP. H th paamt a, b an c a to b tmin an can b foun a th intction btwn ph with mipoint at CP n, CP n an CP n an th pctiv ina tack. h phica uation can b wittn a foow: ( S + a +, + n, ) + ( S +, + n, ) + ( S + + n ),, ( S B,, + b +, + n, ) + ( S B,, +, + n, ) + ( S + + n ) C,,,, Fig:. 4 DOF En too otation. ( SC,, + c +, + n, ) + ( SC,, +, + n, ) + ( S + + n ) C,,,, hn w can tmin th paamt
4 ± ± ± a b c, ( S + + n ) ( S + + n ), n, S,,,, ( S + + n ) ( S + + n ) B,,, n, S B,,,, B,,,, ( S + + n ) ( S + + n ) C,, n, S C,,,, C,,, h ign bfo th oot pion ci th configuation of th obot., Mathmatica mboic oftwa can ov th phica uation, but pouc a ath tniv oution. Poficint u of impification u i n in o to impif th oution. hi pobm i avoi b oving th uation in two tp. Fit fin th intction btwn two of th ph. h intction i ith a cic o a point. Igno th point ca fo now. h intction btwn th thi ph an on of th oth fom of cou ao a cic. Div th pan wh thi cic i ocat. Scon th intction of thi pan an th fit cic cib th poib ocation fo th CP. In th oution bow th intction cic btwn ph with mipoint at A an C i cacuat. A cacuation a thn on in a cooinat tm with th -ai pointing fom A to C.. Dict kinmatic Fo th coni paa obot th ict kinmatic pobm can b fomuat a foow. Cacuat th ocation of th CP fo givn A, B an C. h ph with aiu, an cib a poib ocation fo th CP fo fi A, B an C. h intction point btwn th ph cib th ocation of th CP. h mipoint of th ph an th phica uation a: A B C [ a a a] S A, + a [ ] + + n [ b b b ] SB, + b[ ] + + n [ ] S, + [ ] + n c c c C c + ( ) + ( ) + ( ) a a a ( ) + ( ) + ( ) b b b ( ) + ( ) + ( ) c c c A Fig:5. Intction btwn two ph. + A C, A C Mipoint fo th cic: AC D A +, A C A point on th pan: E B + B C B C + B C B C h noma vcto fo th pan: B C Diving th otation mati: a c θ tan, c a β D A C in c AC a C 4
5 co( θ ) in( θ ) Rot in( θ ) co( θ ) Rot co( β π / ) in( β π / ) in( β π / ) co( β π / ) Rot Rot Rot P + P P P S,,, P, +, Q, R P + P h noma vcto fo th pan an point D an E a tanfom into a cooinat tm with th -ai pointing fom A to C. ( ) Rot ( ) Rot D ( ) Rot E h phica uation can now b wittn in th nw cooinat tm a th intction btwn a cic an a ph. ( ) + ( ) ( ) + ( ) + ( ), wh ( ) Rot CP + P P S S CP Rot ( + P )( P ) P R + Q R h configuation of th obot ci which oution i vai. Wokpac optimiation In o to chaacti th wokpac of th manipuato th foowing optimiation pobm i fomuat. Fin th itanc btwn th tack that giv th agt co-ction wokpac fo a manipuato with ink of ua ngth. On mmtica pacmnt of th tack a coni. h wokpac i futh tict in th iction with th uimnt that th wokpac mut b a pat of th opn ctangua aa fom b th ina tack. wo tp of joint a coni both hown in figu. h caan joint put no tiction on th co-ction wokpac whi th ba an ockt joint imit th wokpac aong on iction. Caan joint Ba an ockt joint + P P + S o imit + P P + S Fig:. Joint -β β 5
6 h pobm i ov inpnnt fom th vcto n i an i b impoing th paamtiation on th mipoint of th th ph that intct at th CP. h optimiation paamt a an a hown in figu 7. Whn th ba an ockt joint i u, th optima ointation of th joint mut ao b coni β.8 A C B h ation btwn optima aa an ink ngth i a foow: Aa.95545* 4 Concuion Fig:7. Optimiation paamt. h ah in fom th opn ctangua aa which tict th wokpac. h optimiation pobm i ov b uing a non ina pogamming outin. h obtain optima co ction aa i hown in figu 8. In th pap th oution of th inv kinmatic an ict kinmatic pobm fo th nov paa tuctu obot hav bn obtain. h initia tu of th Gant-au tuctu ha montat goo wokpac popti of th obot. Futh tui a n in o to amin how comptitiv th coni tuctu i. Rfnc Z C A B [] Bogåh,., PKM ach impotant iu, a n fom a pouct vopmnt ppctiv at ABB Robotic, in Poc. Of th Wokhop on Funamnta Iu an Futu Rach Diction fo Paa Mchanim an Manipuato, (E. Cémnt M., Goin an Imm Ebt-Uphoff), Octob -4,, Qubc Cit, Qubc, Canaa, 8-8. Y Fig:8. Optima co ction wokpac. h taight in how th imit fo ba an ockt joint with β.8 o. h cic how th maimum achabiit fo ach cut without imitation impo b th joint. A ong a β in( ) an th ba an ockt joint a ointat a in figu 8 th optima ation btwn ink ngth an th optimiation paamt a th am fo both joint tp, nam: [] Bogåh,., Inutia Robot, Intnationa Pubication umb WO /448 A. [] Cav, R. 988, DELA, a fat obot with paa gomt, in Poc. Of th 8 th Intnationa Smpoium on Inutia Robot, (Eito H. van Bu), 9-. [4] Mt, J.-P., Paa Robot, Kuw Acamic Pubih, Docht, h than. [5] Stwat, D. 95, A patfom with i g of fom, Pocing of th Intitut of Mchanica Engin, Lonon, 8, 7-8.
Differential Kinematics
Lctu Diffntia Kinmatic Acknowgmnt : Pof. Ouama Khatib, Robotic Laboato, tanfo Univit, UA Pof. Ha Aaa, AI Laboato, MIT, UA Guiing Qution In obotic appication, not on th poition an ointation, but th vocit
More informationFI 3103 Quantum Physics
7//7 FI 33 Quantum Physics Axan A. Iskana Physics of Magntism an Photonics sach oup Institut Tknoogi Banung Schoing Equation in 3D Th Cnta Potntia Hyognic Atom 7//7 Schöing quation in 3D Fo a 3D pobm,
More informationNeural Networks The ADALINE
Lat Lctu Summay Intouction to ua to Bioogica uon Atificia uon McCuoch an itt LU Ronbatt cton Aan Bnaino, a@i.it.ut.t Machin Laning, 9/ ua to h ADALI M A C H I L A R I G 9 / cton Limitation cton aning u
More informationThe angle between L and the z-axis is found from
Poblm 6 This is not a ifficult poblm but it is a al pain to tansf it fom pap into Mathca I won't giv it to you on th quiz, but know how to o it fo th xam Poblm 6 S Figu 6 Th magnitu of L is L an th z-componnt
More informationWho is this Great Team? Nickname. Strangest Gift/Friend. Hometown. Best Teacher. Hobby. Travel Destination. 8 G People, Places & Possibilities
Who i thi Gt Tm? Exi Sh th foowing i of infomtion bot of with o tb o tm mt. Yo o not hv to wit n of it own. Yo wi b givn on 5 mint to omih thi tk. Stngt Gift/Fin Niknm Homtown Bt Th Hobb Tv Dtintion Robt
More informationCDS 101: Lecture 7.1 Loop Analysis of Feedback Systems
CDS : Lct 7. Loop Analsis of Fback Sstms Richa M. Ma Goals: Show how to compt clos loop stabilit fom opn loop poptis Dscib th Nqist stabilit cition fo stabilit of fback sstms Dfin gain an phas magin an
More informationRectification and Depth Computation
Dpatmnt of Comput Engnng Unvst of Cafona at Santa Cuz Rctfcaton an Dpth Computaton CMPE 64: mag Anass an Comput Vson Spng 0 Ha ao 4/6/0 mag cosponncs Dpatmnt of Comput Engnng Unvst of Cafona at Santa Cuz
More informationAQUIFER DRAWDOWN AND VARIABLE-STAGE STREAM DEPLETION INDUCED BY A NEARBY PUMPING WELL
Pocing of h 1 h Innaional Confnc on Enionmnal cinc an chnolog Rho Gc 3-5 pmb 15 AUIFER DRAWDOWN AND VARIABE-AGE REAM DEPEION INDUCED BY A NEARBY PUMPING WE BAAOUHA H.M. aa Enionmn & Eng Rach Iniu EERI
More informationPartial Fraction Expansion
Paial Facion Expanion Whn ying o find h inv Laplac anfom o inv z anfom i i hlpfl o b abl o bak a complicad aio of wo polynomial ino fom ha a on h Laplac Tanfom o z anfom abl. W will illa h ing Laplac anfom.
More informationThe local orthonormal basis set (r,θ,φ) is related to the Cartesian system by:
TIS in Sica Cooinats As not in t ast ct, an of t otntias tat w wi a wit a cnta otntias, aning tat t a jst fnctions of t istanc btwn a atic an so oint of oigin. In tis cas tn, (,, z as a t Coob otntia an
More informationGeometric Predicates P r og r a m s need t o t es t r ela t ive p os it ions of p oint s b a s ed on t heir coor d ina t es. S im p le exa m p les ( i
Automatic Generation of SS tag ed Geometric PP red icates Aleksandar Nanevski, G u y B lello c h and R o b ert H arp er PSCICO project h ttp: / / w w w. cs. cm u. ed u / ~ ps ci co Geometric Predicates
More informationInstruction Execution
MIPS Piplining Cpt280 D Cuti Nlon Intuction Excution C intuction: x = a + b; Ambly intuction: a a,b,x Stp 1: Stp 2: Stp 3: Stp : Stp 5: Stp 6: Ftch th intuction Dtmin it i an a intuction Ftch th ata a
More informationESCI 341 Atmospheric Thermodynamics Lesson 16 Pseudoadiabatic Processes Dr. DeCaria
ESCI 34 Atmohi hmoynami on 6 Puoaiabati Po D DCaia fn: Man, A an FE obitaill, 97: A omaion of th uialnt otntial tmatu an th tati ngy, J Atmo Si, 7, 37-39 Btt, AK, 974: Futh ommnt on A omaion of th uialnt
More informationMethods for calculation of the coupling coefficients in the Coupling Cavity Model of arbitrary chain of resonators
Method for cacuation of the couping coefficient in the Couping Cavity Mode of arbitrary chain of reonator M.I. Ayzaty V.V.Mytrocheno Nationa Science Center Kharov Intitute of Phyic and echnoogy (NSC KIP)
More informationOn Self-Avoiding Walks across n-dimensional Dice and Combinatorial Optimization: An Introduction
On Sf-Avoiing Waks acoss n-dimnsiona Dic an ombinatoia Optimization: An Intoction Fanc Bgz ompt Scinc Raigh, N, USA Vsion: Sn Sp 5:5: EDT 3 ontnts Th fab -- Abot Gt an Hans saching fo ks (an abot Jok hiing
More informationPH672 WINTER Problem Set #1. Hint: The tight-binding band function for an fcc crystal is [ ] (a) The tight-binding Hamiltonian (8.
PH67 WINTER 5 Poblm St # Mad, hapt, poblm # 6 Hint: Th tight-binding band function fo an fcc cstal is ( U t cos( a / cos( a / cos( a / cos( a / cos( a / cos( a / ε [ ] (a Th tight-binding Hamiltonian (85
More informationPrevious knowlegde required. Spherical harmonics and some of their properties. Angular momentum. References. Angular momentum operators
// vious owg ui phica haoics a so o thi poptis Goup thoy Quatu chaics pctoscopy H. Haga 8 phica haoics Rcs Bia. iv «Iucib Tso thos A Itouctio o chists» Acaic ss D.A. c Quai.D. io «hii hysiu Appoch oécuai»
More informationChapter 7 Dynamic stability analysis I Equations of motion and estimation of stability derivatives - 4 Lecture 25 Topics
Chapt 7 Dynamic stability analysis I Equations of motion an stimation of stability ivativs - 4 ctu 5 opics 7.8 Expssions fo changs in aoynamic an populsiv focs an momnts 7.8.1 Simplifi xpssions fo changs
More informationSolutions to Supplementary Problems
Solution to Supplmntay Poblm Chapt Solution. Fomula (.4): g d G + g : E ping th void atio: G d 2.7 9.8 0.56 (56%) 7 mg Fomula (.6): S Fomula (.40): g d E ping at contnt: S m G 0.56 0.5 0. (%) 2.7 + m E
More informationGAUSS PLANETARY EQUATIONS IN A NON-SINGULAR GRAVITATIONAL POTENTIAL
GAUSS PLANETARY EQUATIONS IN A NON-SINGULAR GRAVITATIONAL POTENTIAL Ioannis Iaklis Haanas * and Michal Hany# * Dpatmnt of Physics and Astonomy, Yok Univsity 34 A Pti Scinc Building Noth Yok, Ontaio, M3J-P3,
More informationORBITAL TO GEOCENTRIC EQUATORIAL COORDINATE SYSTEM TRANSFORMATION. x y z. x y z GEOCENTRIC EQUTORIAL TO ROTATING COORDINATE SYSTEM TRANSFORMATION
ORITL TO GEOCENTRIC EQUTORIL COORDINTE SYSTEM TRNSFORMTION z i i i = (coωcoω in Ωcoiinω) (in Ωcoω + coωcoiinω) iniinω ( coωinω in Ωcoi coω) ( in Ωinω + coωcoicoω) in icoω in Ωini coωini coi z o o o GEOCENTRIC
More informationCOMPSCI 230 Discrete Math Trees March 21, / 22
COMPSCI 230 Dict Math Mach 21, 2017 COMPSCI 230 Dict Math Mach 21, 2017 1 / 22 Ovviw 1 A Simpl Splling Chck Nomnclatu 2 aval Od Dpth-it aval Od Badth-it aval Od COMPSCI 230 Dict Math Mach 21, 2017 2 /
More informationGRAVITATION. (d) If a spring balance having frequency f is taken on moon (having g = g / 6) it will have a frequency of (a) 6f (b) f / 6
GVITTION 1. Two satllits and o ound a plant P in cicula obits havin adii 4 and spctivly. If th spd of th satllit is V, th spd of th satllit will b 1 V 6 V 4V V. Th scap vlocity on th sufac of th ath is
More information(( ) ( ) ( ) ( ) ( 1 2 ( ) ( ) ( ) ( ) Two Stage Cluster Sampling and Random Effects Ed Stanek
Two ag ampling and andom ffct 8- Two Stag Clu Sampling and Random Effct Ed Stank FTE POPULATO Fam Labl Expctd Rpon Rpon otation and tminology Expctd Rpon: y = and fo ach ; t = Rpon: k = y + Wk k = indx
More informationKinetics. Central Force Motion & Space Mechanics
Kintics Cntal Foc Motion & Spac Mcanics Outlin Cntal Foc Motion Obital Mcanics Exampls Cntal-Foc Motion If a paticl tavls un t influnc of a foc tat as a lin of action ict towas a fix point, tn t motion
More informationP a g e 5 1 of R e p o r t P B 4 / 0 9
P a g e 5 1 of R e p o r t P B 4 / 0 9 J A R T a l s o c o n c l u d e d t h a t a l t h o u g h t h e i n t e n t o f N e l s o n s r e h a b i l i t a t i o n p l a n i s t o e n h a n c e c o n n e
More informationSTRIPLINES. A stripline is a planar type transmission line which is well suited for microwave integrated circuitry and photolithographic fabrication.
STIPLINES A tiplin i a plana typ tanmiion lin hih i ll uitd fo mioav intgatd iuity and photolithogaphi faiation. It i uually ontutd y thing th nt onduto of idth, on a utat of thikn and thn oving ith anoth
More informationPLS-CADD DRAWING N IC TR EC EL L RA IVE ) R U AT H R ER 0. IDT FO P 9-1 W T OO -1 0 D EN C 0 E M ER C 3 FIN SE W SE DE EA PO /4 O 1 AY D E ) (N W AN N
A IV ) H 0. IT FO P 9-1 W O -1 0 C 0 M C FI S W S A PO /4 O 1 AY ) ( W A 7 F 4 H T A GH 1 27 IGO OU (B. G TI IS 1/4 X V -S TO G S /2 Y O O 1 A A T H W T 2 09 UT IV O M C S S TH T ) A PATO C A AY S S T
More informationMidterm Exam. CS/ECE 181B Intro to Computer Vision. February 13, :30-4:45pm
Nam: Midtm am CS/C 8B Into to Comput Vision Fbua, 7 :-4:45pm las spa ouslvs to th dg possibl so that studnts a vnl distibutd thoughout th oom. his is a losd-boo tst. h a also a fw pags of quations, t.
More informationsin sin 1 d r d Ae r 2
Diffction k f c f Th Huygn-Fnl Pincil tt: Evy unobtuct oint of vfont, t givn intnt, v ouc of hicl cony vlt (ith th m funcy tht of th imy v. Th mlitu of th oticl fil t ny oint byon i th uoition of ll th
More informationStudying the Steady State Performance Characteristics of Induction Motor with Field Oriented Control Comparing to Scalar Control
EJERS, Euopan Jounal of Engining Rach and Scinc Studying th Stady Stat fomanc Chaactitic of nduction Moto with Fild Ointd Contol Compaing to Scala Contol Hamdy Mohamd Soliman Abtact Fild ointd contol i
More informationThree-Level Five-Phase Space Vector PWM Inverter for a Two Five-Phase Series Connected Induction Machine Drive
Engy an Pow Engining, 21, 1-17 oi:1.4236/p.21.213 Publih Onlin Fbuay 21 (http://www.cip.og/jounal/p) Th-Lvl Fiv-Pha Spac Vcto PWM Invt fo a Two Fiv-Pha Si Connct Inuction Machin Div N. R. ABJADI 1, J.
More informationGRAVITATION 4) R. max. 2 ..(1) ...(2)
GAVITATION PVIOUS AMCT QUSTIONS NGINING. A body is pojctd vtically upwads fom th sufac of th ath with a vlocity qual to half th scap vlocity. If is th adius of th ath, maximum hight attaind by th body
More informationSolutions to Problems : Chapter 19 Problems appeared on the end of chapter 19 of the Textbook
Solutions to Poblems Chapte 9 Poblems appeae on the en of chapte 9 of the Textbook 8. Pictue the Poblem Two point chages exet an electostatic foce on each othe. Stategy Solve Coulomb s law (equation 9-5)
More informationExtinction Ratio and Power Penalty
Application Not: HFAN-.. Rv.; 4/8 Extinction Ratio and ow nalty AVALABLE Backgound Extinction atio is an impotant paamt includd in th spcifications of most fib-optic tanscivs. h pupos of this application
More informationNoise in electronic components.
No lto opot5098, JDS No lto opot Th PN juto Th ut thouh a PN juto ha fou opot t: two ffuo ut (hol fo th paa to th aa a lto th oppot to) a thal at oty ha a (hol fo th aa to th paa a lto th oppot to, laka
More informationModule 6: Two Dimensional Problems in Polar Coordinate System
Modl6/Lon Modl 6: Two Dimnional Poblm in Pola Coodinat Stm 6 INTRODUCTION I n an laticit poblm th pop choic o th coodinat tm i tml impotant c thi choic tablih th complit o th mathmatical pion mplod to
More informationAnouncements. Conjugate Gradients. Steepest Descent. Outline. Steepest Descent. Steepest Descent
oucms Couga Gas Mchal Kazha (6.657) Ifomao abou h Sma (6.757) hav b pos ol: hp://www.cs.hu.u/~msha Tch Spcs: o M o Tusay afoo. o Two paps scuss ach w. o Vos fo w s caa paps u by Thusay vg. Oul Rvw of Sps
More informationEE243 Advanced Electromagnetic Theory Lec # 22 Scattering and Diffraction. Reading: Jackson Chapter 10.1, 10.3, lite on both 10.2 and 10.
Appid M Fa 6, Nuuth Lctu # V //6 43 Advancd ctomagntic Thoy Lc # Scatting and Diffaction Scatting Fom Sma Obcts Scatting by Sma Dictic and Mtaic Sphs Coction of Scatts Sphica Wav xpansions Scaa Vcto Rading:
More informationLecture 3.2: Cosets. Matthew Macauley. Department of Mathematical Sciences Clemson University
Lctu 3.2: Costs Matthw Macauly Dpatmnt o Mathmatical Scincs Clmson Univsity http://www.math.clmson.du/~macaul/ Math 4120, Modn Algba M. Macauly (Clmson) Lctu 3.2: Costs Math 4120, Modn Algba 1 / 11 Ovviw
More informationCoulomb s Law Worksheet Solutions
PHLYZIS ulb Law Wrkht Slutin. w charg phr 0 c apart attract ach thr with a frc f 3.0 0 6 N. What frc rult fr ach f th fllwing chang, cnir paratly? a Bth charg ar ubl an th itanc rain th a. b An uncharg,
More informationB l 4 P A 1 DYNAMICS OF RECIPROCATING ENGINES
DYNMIS OF REIROTING ENGINES This chapte studies the dnaics of a side cank echaniss in an anatica wa. This is an eape fo the anatica appoach of soution instead of the gaphica acceeations and foce anases.
More informationA Comparative Study and Analysis of an Optimized Control Strategy for the Toyota Hybrid System
Pag 563 Wol Elctic Vhicl Jounal Vol. 3 - ISSN 3-6653 - 9 AVERE EVS4 Stavang, Noway, May 13-16, 9 A Compaativ Stuy an Analysis of an Optimiz Contol Statgy fo th Toyota Hybi Systm Tho Hofman 1, Thijs Punot
More informationTwo- and Three-Dimensional Stress Analysis
Two- and Thee-Dimensiona Stess Anasis Stesses, w d, d d Components of Catesian stess acting at an infinitesima ome st inde = diection of pane noma nd inde = stess diection Fom otationa eqiibim abot the
More informationPeriod vs. Length of a Pendulum
Gaphcal Mtho n Phc Gaph Intptaton an Lnazaton Pat 1: Gaphng Tchnqu In Phc w u a vat of tool nclung wo, quaton, an gaph to mak mol of th moton of objct an th ntacton btwn objct n a tm. Gaph a on of th bt
More information2 tel
Us. Timeless, sophisticated wall decor that is classic yet modern. Our style has no limitations; from traditional to contemporar y, with global design inspiration. The attention to detail and hand- craf
More informationFourier transforms (Chapter 15) Fourier integrals are generalizations of Fourier series. The series representation
Pof. D. I. Nass Phys57 (T-3) Sptmb 8, 03 Foui_Tansf_phys57_T3 Foui tansfoms (Chapt 5) Foui intgals a gnalizations of Foui sis. Th sis psntation a0 nπx nπx f ( x) = + [ an cos + bn sin ] n = of a function
More informationPHY132 Lecture 6 02/05/2010. Lecture 6 1
Claical Phyic II PHY3 Lectue 6 The lectic Potential ti - II /5/ Lectue 6 Wok by a Vaying Foce Wok i a cala quantity, an we can thu a little piece of wok togethe, i.e. um a eie of ot-pouct of the foce F(
More informationPhysics 240: Worksheet 15 Name
Physics 40: Woksht 15 Nam Each of ths poblms inol physics in an acclatd fam of fnc Althouh you mind wants to ty to foc you to wok ths poblms insid th acclatd fnc fam (i.. th so-calld "won way" by som popl),
More information* Meysam Mohammadnia Department of Nuclear Engineering, East Tehran Branch, Islamic Azad University, Tehran, Iran *Author for Correspondence
Indian Jouna o Fundanta and ppid Li Scincs ISSN: 65 Onin n Opn ccss, Onin Intnationa Jouna vaiab at www.cibtch.og/sp.d/js///js.ht Vo. S, pp. 7-/Mysa Rsach tic CQUISITION N NLYSIS OF FLUX N CURRENT COEFFICIENTS
More informationCHAPTER 5 CIRCULAR MOTION
CHAPTER 5 CIRCULAR MOTION and GRAVITATION 5.1 CENTRIPETAL FORCE It is known that if a paticl mos with constant spd in a cicula path of adius, it acquis a cntiptal acclation du to th chang in th diction
More informationCBSE-XII-2013 EXAMINATION (MATHEMATICS) The value of determinant of skew symmetric matrix of odd order is always equal to zero.
CBSE-XII- EXAMINATION (MATHEMATICS) Cod : 6/ Gnal Instuctions : (i) All qustions a compulso. (ii) Th qustion pap consists of 9 qustions dividd into th sctions A, B and C. Sction A compiss of qustions of
More informationSolid state physics. Lecture 3: chemical bonding. Prof. Dr. U. Pietsch
Solid stat physics Lctu 3: chmical bonding Pof. D. U. Pitsch Elcton chag dnsity distibution fom -ay diffaction data F kp ik dk h k l i Fi H p H; H hkl V a h k l Elctonic chag dnsity of silicon Valnc chag
More informationHomework Set 4 Physics 319 Classical Mechanics. m m k. x, x, x, x T U x x x x l 2. x x x x. x x x x
Poble 78 a) The agangian i Hoewok Set 4 Phyic 319 Claical Mechanic k b) In te of the cente of a cooinate an x x1 x x1 x xc x x x x x1 xc x xc x x x x x1 xc x xc x, x, x, x T U x x x x l 1 1 1 1 1 1 1 1
More information( )( )( ) ( ) + ( ) ( ) ( )
3.7. Moel: The magnetic fiel is that of a moving chage paticle. Please efe to Figue Ex3.7. Solve: Using the iot-savat law, 7 19 7 ( ) + ( ) qvsinθ 1 T m/a 1.6 1 C. 1 m/s sin135 1. 1 m 1. 1 m 15 = = = 1.13
More informationThis lecture. Transformations in 2D. Where are we at? Why do we need transformations?
Thi lectue Tanfomation in 2D Thoma Sheme Richa (Hao) Zhang Geomet baic Affine pace an affine tanfomation Ue of homogeneou cooinate Concatenation of tanfomation Intouction to Compute Gaphic CMT 36 Lectue
More informationSME 3033 FINITE ELEMENT METHOD. Bending of Prismatic Beams (Initial notes designed by Dr. Nazri Kamsah)
Bnding of Prismatic Bams (Initia nots dsignd by Dr. Nazri Kamsah) St I-bams usd in a roof construction. 5- Gnra Loading Conditions For our anaysis, w wi considr thr typs of oading, as iustratd bow. Not:
More informationLecture 7 Diffusion. Our fluid equations that we developed before are: v t v mn t
Cla ot fo EE6318/Phy 6383 Spg 001 Th doumt fo tutoal u oly ad may ot b opd o dtbutd outd of EE6318/Phy 6383 tu 7 Dffuo Ou flud quato that w dvlopd bfo a: f ( )+ v v m + v v M m v f P+ q E+ v B 13 1 4 34
More informationCoordinate Geometry. = k2 e 2. 1 e + x. 1 e. ke ) 2. We now write = a, and shift the origin to the point (a, 0). Referred to
Coodinate Geomet Conic sections These ae pane cuves which can be descibed as the intesection of a cone with panes oiented in vaious diections. It can be demonstated that the ocus of a point which moves
More informationAltitude measurement using laser beam reflected from water surface
Altitu maumnt uing la bam flct fom wat ufac Sh. Mohamma Nja an M. H. Haji Miaii Downloa fom ij.iut.ac.i at 3:35 IRDT on Monay Sptmb 7th 08 Abtact: In thi pap altitu maumnt fom wat ufac uing la bam i pnt.
More informationOH BOY! Story. N a r r a t iv e a n d o bj e c t s th ea t e r Fo r a l l a g e s, fr o m th e a ge of 9
OH BOY! O h Boy!, was or igin a lly cr eat ed in F r en ch an d was a m a jor s u cc ess on t h e Fr en ch st a ge f or young au di enc es. It h a s b een s een by ap pr ox i ma t ely 175,000 sp ect at
More informationPhysics Courseware Physics II Electric Field and Force
Physics Cousewae Physics II lectic iel an oce Coulomb s law, whee k Nm /C test Definition of electic fiel. This is a vecto. test Q lectic fiel fo a point chage. This is a vecto. Poblem.- chage of µc is
More informationEquilibria of a cylindrical plasma
// Miscellaneous Execises Cylinical equilibia Equilibia of a cylinical plasma Consie a infinitely long cyline of plasma with a stong axial magnetic fiel (a geat fusion evice) Plasma pessue will cause the
More informationAakash. For Class XII Studying / Passed Students. Physics, Chemistry & Mathematics
Aakash A UNIQUE PPRTUNITY T HELP YU FULFIL YUR DREAMS Fo Class XII Studying / Passd Studnts Physics, Chmisty & Mathmatics Rgistd ffic: Aakash Tow, 8, Pusa Road, Nw Dlhi-0005. Ph.: (0) 4763456 Fax: (0)
More informationReferences. Basic structure. Power Generator Technologies for Wind Turbine. Synchronous Machines (SM)
Gnato chnologi fo Wind ubin Mhdad Ghandhai mhdad@kth. Rfnc 1. Wind Plant, ABB, chnical Alication Pa No.13.. WECC Wind Plant Dynamic Modling Guid, WECC Rnwabl Engy Modling ak Foc. 3. Wind ubin Plant Caabiliti
More informationLoad Equations. So let s look at a single machine connected to an infinite bus, as illustrated in Fig. 1 below.
oa Euatons Thoughout all of chapt 4, ou focus s on th machn tslf, thfo w wll only pfom a y smpl tatmnt of th ntwok n o to s a complt mol. W o that h, but alz that w wll tun to ths ssu n Chapt 9. So lt
More informationFall 2004/05 Solutions to Assignment 5: The Stationary Phase Method Provided by Mustafa Sabri Kilic. I(x) = e ixt e it5 /5 dt (1) Z J(λ) =
8.35 Fall 24/5 Solution to Aignment 5: The Stationay Phae Method Povided by Mutafa Sabi Kilic. Find the leading tem fo each of the integal below fo λ >>. (a) R eiλt3 dt (b) R e iλt2 dt (c) R eiλ co t dt
More informationPH126 Exam I Solutions
PH6 Exam I Solutions q Q Q q. Fou positively chage boies, two with chage Q an two with chage q, ae connecte by fou unstetchable stings of equal length. In the absence of extenal foces they assume the equilibium
More informationT h e C S E T I P r o j e c t
T h e P r o j e c t T H E P R O J E C T T A B L E O F C O N T E N T S A r t i c l e P a g e C o m p r e h e n s i v e A s s es s m e n t o f t h e U F O / E T I P h e n o m e n o n M a y 1 9 9 1 1 E T
More informationADA COMPLIANT BARRIER FREE SELECTED ITEMS
1900 I PW ADJUTAB D 1 1/8" ADA MPIANT BAI F TD ITM D 11 1/8" UNIVA MUNTING MT UI, UB-7-2 AND ADA QUIMNT FATU U ITD 10 YA GUAANT PW ADJUTAB TANDAD AND MDIUM DUTY MMIA APPIATIN ADJUTAB BAK HK TANDAD UNIVA
More informationON A GENERALIZED PROBABILITY DISTRIBUTION IN ASSOCIATION WITH ALEPH ( ) - FUNCTION
Intnational Jounal of Engining, Scinc and athmatic Vol. 8, Iu, Januay 8, ISSN: 3-94 Impact Facto: 6.765 Jounal Hompag: http://www.ijm.co.in, Email: ijmj@gmail.com Doubl-Blind P Riwd Rfd Opn Acc Intnational
More informationLecture 2: Frequency domain analysis, Phasors. Announcements
EECS 5 SPRING 24, ctu ctu 2: Fquncy domain analyi, Phao EECS 5 Fall 24, ctu 2 Announcmnt Th cou wb it i http://int.c.bkly.du/~5 Today dicuion ction will mt Th Wdnday dicuion ction will mo to Tuday, 5:-6:,
More informationA L A BA M A L A W R E V IE W
A L A BA M A L A W R E V IE W Volume 52 Fall 2000 Number 1 B E F O R E D I S A B I L I T Y C I V I L R I G HT S : C I V I L W A R P E N S I O N S A N D TH E P O L I T I C S O F D I S A B I L I T Y I N
More informationOverview. 1 Recall: continuous-time Markov chains. 2 Transient distribution. 3 Uniformization. 4 Strong and weak bisimulation
Rcall: continuous-tim Makov chains Modling and Vification of Pobabilistic Systms Joost-Pit Katon Lhstuhl fü Infomatik 2 Softwa Modling and Vification Goup http://movs.wth-aachn.d/taching/ws-89/movp8/ Dcmb
More information8 - GRAVITATION Page 1
8 GAVITATION Pag 1 Intoduction Ptolmy, in scond cntuy, gav gocntic thoy of plantay motion in which th Eath is considd stationay at th cnt of th univs and all th stas and th plants including th Sun volving
More informationChapter 7. A Quantum Mechanical Model for the Vibration and Rotation of Molecules
Chaptr 7. A Quantu Mchanica Mo for th Vibration an Rotation of Mocus Haronic osciator: Hook s aw: F k is ispacnt Haronic potntia: V F k k is forc constant: V k curvatur of V at quiibriu Nwton s quation:
More informationO -x 0. 4 kg. 12 cm. 3 kg
Anwer, Key { Homework 9 { Rubin H andau 1 Thi print-out houd have 18 quetion. Check that it i compete before eaving the printer. Ao, mutipe-choice quetion may continue on the net coumn or page: nd a choice
More informationCS 491 G Combinatorial Optimization
CS 49 G Cobinatorial Optiization Lctur Nots Junhui Jia. Maiu Flow Probls Now lt us iscuss or tails on aiu low probls. Thor. A asibl low is aiu i an only i thr is no -augnting path. Proo: Lt P = A asibl
More informationESCI 341 Atmospheric Thermodynamics Lesson 14 Curved Droplets and Solutions Dr. DeCaria
ESCI 41 Atmophric hrmodynamic Lon 14 Curd Dropt and Soution Dr. DCaria Rfrnc: hrmodynamic and an Introduction to hrmotatitic, Can Phyica Chmitry, Lin A hort Cour in Coud Phyic, Rogr and Yau hrmodynamic
More informationFI 2201 Electromagnetism
F Eectomagnetism exane. skana, Ph.D. Physics of Magnetism an Photonics Reseach Goup Magnetostatics MGNET VETOR POTENTL, MULTPOLE EXPNSON Vecto Potentia Just as E pemitte us to intouce a scaa potentia V
More informationGUIDE FOR SUPERVISORS 1. This event runs most efficiently with two to four extra volunteers to help proctor students and grade the student
GUIDE FOR SUPERVISORS 1. This vn uns mos fficinly wih wo o fou xa voluns o hlp poco sudns and gad h sudn scoshs. 2. EVENT PARAMETERS: Th vn supviso will povid scoshs. You will nd o bing a im, pns and pncils
More informationn gativ b ias to phap s 5 Q mou ntd ac oss a 50 Q co-a xial l, i t whn bias no t back-bia s d, so t hat p ow fl ow wi ll not b p ositiv. Th u s, if si
DIOD E AND ITS APPLI AT C I O N: T h diod is a p-t p, y intin s ic, n-typ diod consis ting of a naow lay of p- typ smiconducto and a naow lay of n-typ smiconducto, wi th a thick gion of intins ic o b twn
More informationCase Study Vancomycin Answers Provided by Jeffrey Stark, Graduate Student
Cas Stuy Vancomycin Answrs Provi by Jffry Stark, Grauat Stunt h antibiotic Vancomycin is liminat almost ntirly by glomrular filtration. For a patint with normal rnal function, th half-lif is about 6 hours.
More informationResearch Article Kineto-Elastodynamic Characteristics of the Six-Degree-of-Freedom Parallel Structure Seismic Simulator
Jouna of Robotics Voume 11, Atice ID 489695, 17 pages doi:1.1155/11/489695 Reseach Atice Kineto-Eastodynamic Chaacteistics of the Six-Degee-of-Feedom Paae Stuctue Seismic Simuato Yongjie Zhao Depatment
More informationBasic oces an Keple s Laws 1. Two ientical sphees of gol ae in contact with each othe. The gavitational foce of attaction between them is Diectly popotional to the squae of thei aius ) Diectly popotional
More information2011 HSC Mathematics Extension 1 Solutions
0 HSC Mathmatics Etsio Solutios Qustio, (a) A B 9, (b) : 9, P 5 0, 5 5 7, si cos si d d by th quotit ul si (c) 0 si cos si si cos si 0 0 () I u du d u cos d u.du cos (f) f l Now 0 fo all l l fo all Rag
More informationTrade Patterns, Production networks, and Trade and employment in the Asia-US region
Trade Patterns, Production networks, and Trade and employment in the Asia-U region atoshi Inomata Institute of Developing Economies ETRO Development of cross-national production linkages, 1985-2005 1985
More informationChapter 6. NEWTON S 2nd LAW AND UNIFORM CIRCULAR MOTION
Chapte 6 NEWTON S nd LAW AND UNIFORM CIRCULAR MOTION Phyic 1 1 3 4 ting Quetion: A ball attached to the end of a ting i whiled in a hoizontal plane. At the point indicated, the ting beak. Looking down
More informationHydrogen atom. Energy levels and wave functions Orbital momentum, electron spin and nuclear spin Fine and hyperfine interaction Hydrogen orbitals
Hydogn atom Engy lvls and wav functions Obital momntum, lcton spin and nucla spin Fin and hypfin intaction Hydogn obitals Hydogn atom A finmnt of th Rydbg constant: R ~ 109 737.3156841 cm -1 A hydogn mas
More informationthe output is Thus, the output lags in phase by θ( ωo) radians Rewriting the above equation we get
Th output y[ of a frquncy-sctiv LTI iscrt-tim systm with a frquncy rspons H ( xhibits som ay rativ to th input caus by th nonro phas rspons θ( ω arg{ H ( } of th systm For an input A cos( ωo n + φ, < n
More informationMassachusetts Institute of Technology Department of Mechanical Engineering
Massachustts Institut of Tchnolog Dpartmnt of Mchanical Enginring. Introduction to Robotics Mid-Trm Eamination Novmbr, 005 :0 pm 4:0 pm Clos-Book. Two shts of nots ar allowd. Show how ou arrivd at our
More informationHow!do!humans!combine!sounds!into!an! infinite!number!of!utterances? How!do!they!use!these!utterances!!to! communicate!and!express!meaning?
Linguistics How!o!humans!combin!s!into!an! H h bi i infinit!numb!of!uttancs? Supcomputing an Linguistics Kis Hyln Univsity of Luvn RU Quantitativ Lxicology an Vaiational Linguistics Linguistics Linguistics
More information(, ) which is a positively sloping curve showing (Y,r) for which the money market is in equilibrium. The P = (1.4)
ots lctu Th IS/LM modl fo an opn conomy is basd on a fixd pic lvl (vy sticky pics) and consists of a goods makt and a mony makt. Th goods makt is Y C+ I + G+ X εq (.) E SEK wh ε = is th al xchang at, E
More informationfor the magnetic induction at the point P with coordinate x produced by an increment of current
5. tatng wth th ffnta psson B fo th magntc nucton at th pont P wth coonat pouc by an ncmnt of cunt at, show pcty that fo a oop cayng a cunt th magntc nucton at P s B Ω wh Ω s th so ang subtn by th oop
More informationChapter 28: Magnetic Field and Magnetic Force. Chapter 28: Magnetic Field and Magnetic Force. Chapter 28: Magnetic fields. Chapter 28: Magnetic fields
Chapte 8: Magnetic fiels Histoically, people iscoe a stone (e 3 O 4 ) that attact pieces of ion these stone was calle magnets. two ba magnets can attact o epel epening on thei oientation this is ue to
More informationE F. and H v. or A r and F r are dual of each other.
A Duality Thom: Consid th following quations as an xampl = A = F μ ε H A E A = jωa j ωμε A + β A = μ J μ A x y, z = J, y, z 4π E F ( A = jω F j ( F j β H F ωμε F + β F = ε M jβ ε F x, y, z = M, y, z 4π
More informationSTATISTICAL MECHANICS OF DIATOMIC GASES
Pof. D. I. ass Phys54 7 -Ma-8 Diatomic_Gas (Ashly H. Cat chapt 5) SAISICAL MECHAICS OF DIAOMIC GASES - Fo monatomic gas whos molculs hav th dgs of fdom of tanslatoy motion th intnal u 3 ngy and th spcific
More informationTHIS PAGE DECLASSIFIED IAW E
THS PAGE DECLASSFED AW E0 2958 BL K THS PAGE DECLASSFED AW E0 2958 THS PAGE DECLASSFED AW E0 2958 B L K THS PAGE DECLASSFED AW E0 2958 THS PAGE DECLASSFED AW EO 2958 THS PAGE DECLASSFED AW EO 2958 THS
More informationDoublets and Other Allied Well Patterns
oults an Oth Alli Wll Pattns SUPRI TR- B William E. Bigham cm 000 Pfom un ontact Nums E-F6-00B5 an E-FG-96B99 Stanfo Univsit Stanfo, alifonia AKNOWLEGEMENTS Lt m stat ths acknowlgmnts with a isclaim.
More information1. (25pts) Answer the following questions. Justify your answers. (Use the space provided below and the next page)
Phyi 6 xam#3 1. (pt) Anwr th foowing qution. Jutify your anwr. (U th pa providd bow and th nxt pag) a). Two inrtia obrvr ar in rativ motion. Whih of th foowing quantiti wi thy agr or diagr on? i) thir
More information