System variables. Basic Modeling Concepts. Basic elements single and. Power = effort x flow. Power = F x v. Power = V x i. Power = T x w.
|
|
- Oswald Gallagher
- 6 years ago
- Views:
Transcription
1 Basic Modling Concpts Basic lmnts singl and multiport t dvics Systm variabls v m F V i Powr F x v T w Powr T x w Powr V x i P Q Powr P x Q Powr ort x low
2 Eort & low ar powr variabls Eorts t... Flows... Forc (F) Nwtons Voltag (V) Volts V Torqu (T) N-mtrs Prssur (P) N /m Vlocity (V) Currnt (i) m/s Amps Ang. vlocity(w) rad/s Volum low (Q) m / s powr ort () x low () Systm variabls Gnralizd powr and nrgy variabls hav th ollowing rlations: dq / dt q is a gnralizd displacmnt dp / dt p is a gnralizd momntum. A stat ttrahdron xplains ths rlations dp/dt p q dq/dt
3 Physical Systms Variabl Typs VARIABLE MECHANICAL TRANSLATION Eort Forc (F) (Nwtons N) MECHANICAL ROTATION Torqu (T) (N-m) ELECTRICAL Voltag (Volts V) HYDRAULIC Prssur (P) (N/m ) Flow Vlocity (v) (m/s) Angular vlocity (w) (rad/s) Currnt (i) (Amprs A) Volum low (Q) (m /s) Displacmnt Momntum Displacmnt (x) (m) Momntum (N-s) Angl (rad) Angular momntum (N-m-s) Charg (q) (A-s) Flux linkag (V-s) Volum (m ) Prssur momntum (N-s/ m ) Word bond graphs. Word bond graph : Simpl rprsntation o physical systm; using words to imply a systm componnt. Exampl: Car Startr/Solnoid battry motor bndix Th word bond graph can b drawn as battry voltag currnt motor torqu angular vlocity bndix
4 Word bond graphs Car Modl: - Powr rom ngin is d to clutch - Transmittd to gar box. Slcts gar - Powr lows to whls via a dirntial gar box and driv shat. whl ngin T clutch T gar-box T driv shat w w w T4 w4 T5 dirntial gar box T6 w5 w6 throttl control gar slction whl Eorts: Torqus (T,T,T,T4,T5,T6) Flows: Vlocitis ( w,w,w,w4,w5,w6) Concpt o causality Causality : Indicats WHO causs WHAT to WHOM A B A B in bond graph notation, in bond graph notation, A B A low () ort () ort () B low () I lmnt A imposs an ort on lmnt B, thn lmnt B rsponds back with a low or vic-vrsa,
5 Basic lmnts To convrt a word bond graph to complt bond graph w nd som basic lmnts. Basic lmnts. Sourc o ort. (SE) Sourc o low (SF) Constant ort junction () Constant low junction () Inrtia lmnt (I) Mass,inductors,luid pips Capacitiv lmnt (C) Spring,capacitor,lywhl Rsistiv lmnt (R) Damprs, rsistors Transormr lmnt (TF) Lvrs,transormrs Gyrator lmnt (GY) Cntriugal pump, gnrators With ths lmnts, bond graph modls o dynamic systms can b cratd in any nrgy domain. BOND GRAPHS and PHYSICAL VARIABLES Powr Flow Concpt powr Powr A B A B Causality Concpt powr powr A low B ort A ort low B A imposs ort on B, B rsponds with a low B imposs ort on A, A rsponds with a low
6 FUNDAMENTALS OF BOND GRAPH MODELING low powr ort powr low ort k b C 4 R m I x(t) F SE b C R k 4 m I x(t) F SE To Sum Eorts To Sum Flows A rsistiv lmnt (R). Thr is a static rlation btwn ort & low. Rsistiv lmnts ar idalization o dvics lik, damprs, rsistors, luid carrying pips. R () Linar R Non linar R Units o R Mch. translation Mch rotation Elctrical Hydraulic N-s/m N-m-s V/A (Ohms) N-s/ m
7 Rsistiv lmnt (R) Causality considrations : A rsistiv lmnt taks ithr orm R R Rlation :g () Rlation :g - () R R R lmnt R R 5 R R 5
8 Capacitiv lmnt (C). In a capacitiv lmnt a static rlation xists btwn ort & displacmnt. Ths dvics stor or dissipat nrgy without loss. Capacitiv lmnts ar idalization o dvics lik, springs, capacitors, accumulators. Cq (q) q q Units o C Linar C Non linar C Mch. translation Mch rotation Elctrical Hydraulic N/m N-m/rad arads N/ m 5 Capacitiv lmnt (C) Causality considrations : Intgral causality C dt q C C dq dt Prrrd orm or computational purposs Drivativ causality C d dq C dt dt dq d C dt dt This is not prrrd orm or computational purposs
9 C 4 C lmnt 4 C S 4 Inrtia lmnt (I). Thr is a static rlation btwn low & momntum. Ths dvics stor kintic nrgy Inrtia lmnts ar to modl inductanc cts in lctrical circuits, mass & inrtia cts in mchanical & hydraulic systms. Ip p g(p) p Units o I Linar I Non linar I Mch. translation N-s /m Mch rotation N-m-s Elctrical Hydraulic V-s/A (Hnrys) N-s /m 5
10 Inrtia lmnt (I) Causality considrations : Intgral causality I dt p I I dp dt Impuls Momntum orm Prrrd orm or computational purposs. Drivativ causality I d dp I dt dt dp d I dt dt Nwton s law orm This is not prrrd orm o causality or I lmnt. I lmnt I 4 4 I S 4
11 Th sourc lmnts SE & SF) An ort sourc : Systm/lmnt which maintains an input ort. SE s ar voltag sourcs, orcs, prssur. A low sourc : Systm/dvic which maintains a an input low. SF s ar vlocity sourcs, currnt, low sourcs V m Vhicl suspnsion systm. Road Eort Sourc Flow sourc Sourc lmnts (SE & SF) Causality considrations : Eort Sourc Flow sourc SE SF Th ort sourc imposs an ort on th connctd junction or lmnt Flow sourc imposs a low onto th systm, connctd junction or lmnt.
12 Sourc SE lmnt SE5 5 5 SE 5 Sourc SF lmnt SF5 5 5 SF 5 Transormr lmnt (TF) Two port lmnts altring magnitud o ithr low or ort ar transormr lmnts. Transormrs hav static rlation btwn input low/ort & output low/ort by mans o a transormr modulus. v F a v b a v b F a b F F v F v A A A A F P v Q A A P,Q A lvr Hydraulic Ram Ratio (a/b) & (A/A) is transormr modulus. Othr xampls: gar st, lctrical transormr, pullys.
13 Transormr lmnt (TF) Causality considrations : m.. TF m m m.. TF m m TF Incorrct causal orm, not possibl TF lmnt 4 4 TF TF TF45 5
14 TF lmnt 4 4 TF /TF /TF45 5 Gyrator lmnt (GY) Gyrators : Two port lmnts which rlat input ort to output low or vicvrsa by mans o a modulus. Typical xampls: voic coil, lctric motor, gnrator. ω F v v v i Τ ω F r v r v F F r ω i r T Gyro-scop I th rotor spins rapidly, & a small F will yild a proportional vlocity v, & vic-vrsa Motor Angular vlocity output is proportional to applid voltag
15 Gyrator lmnt (GY) Causality considrations : r.. GY r r r.. GY r r GY GY Incorrct causal orm, not possibl GY lmnt GY 5 4 GY GY45 5
16 GY lmnt 4 4 GY /GY /GY45 5 Th () junction lmnt i i i c c i -i i PPP
17 Th () junction cont. ( junction) : Is a common ort junction. All orts ar qual Th sum o th lows qual zro Th sum o th lows qual zro. Summation signs will b dtrmind by Powr Flow. Powr low and th () Junction
18 Causality and th () Junction Powr low and Causality () Junction
19 () Junction proprtis It is a common ort junction or all bonds attachd All orts ar qual Th sum o th lows qual zro. Powr consrving, powr in quals powr out Only on causal mark dtrmins th input ort and thus all othr orts will b outputs Thr can only b on bond and only on bond that sts th ort input Powr low hal arrows dtrmin how th lows will sum Th () junction lmnt V C i R N v F w Currnt through C and R is th sam. Summation o voltags Vlocity is common but sumation o orcs must ollow Nwton s law
20 Th () junction cont. ( junction) : Is a common low junction. All lows ar qual Th sum o th orts qual zro Th sum o th orts qual zro. Summation dtrmind by Powr Flow. Powr low and th () Junction
21 Causality and th () Junction Powr low and Causality () Junction
22 junction - 4 junction () Junction proprtis It is a common low junction or all bonds attachd All lows ar qual Th sum o th orts qual zro. Powr consrving, powr in quals powr out Only on causal mark dtrmins th input low and thus all othr lows will b outputs Thr can only b on bond and only on bond that sts th low input Powr low hal arrows dtrmin how th orts will sum
23 Causal bond(4) junction-c lmnt - 4 C S 4 4 C - Causal bond junction-i lmnt 4 I S 4 4 I
24 Causal bond junction R lmnt R Causal bond junction R lmnt - 4 R 4 Causal bond junction TF lmnt 4 5 TF45 - Causal bond junction TF lmnt - 4 TF45 5
25 Causal bond junction GY lmnt 4 5 GY45 - Causal bond junction GY lmnt - 4 GY45 5 Causal orms. Symbol Implid maning & variabl rlation. C I C I Prrrd intgral causal orm... dq/dt Prrrd intgral causal orm... dp/dt Drivativ causal orm...q intg ( )... not prrrd Drivativ causal orm...p intg ( )... not prrrd TF Prrrd orm or transormr lmnt. (or opposit) /m & /m OR m & m GY Prrrd orm or gyrator lmnt. (or opposit)
INC 693, 481 Dynamics System and Modelling: The Language of Bound Graphs Dr.-Ing. Sudchai Boonto Assistant Professor
INC 693, 48 Dynamics Systm and Modlling: Th Languag o Bound Graphs Dr.-Ing. Sudchai Boonto Assistant Prossor Dpartmnt o Control Systm and Instrumntation Enginring King Mongkut s Unnivrsity o Tchnology
More informationME242 MECHANICAL ENGINEERING SYSTEMS LECTURE 27: Ideal Machines: Transformers and Gyrators 2.4 IDEAL MACHINES. Machine
E4 ECHANICAL ENGINEERING SYSES LECURE 7: Idal achins: ransformrs and Gyrators.4 E4 - Spring 005 - Eugnio Schustr 343 1 Idal IDEAL ACHINES achin An idal machin is a two port dvic that transmits work from
More informationMCE503: Modeling and Simulation of Mechatronic Systems Discussion on Bond Graph Sign Conventions for Electrical Systems
MCE503: Modling and Simulation o Mchatronic Systms Discussion on Bond Graph Sign Convntions or Elctrical Systms Hanz ichtr, PhD Clvland Stat Univrsity, Dpt o Mchanical Enginring 1 Basic Assumption In a
More informationMECE 3304 Exam Booklet
Univrity o Txa Rio Grand Vally MECE 3304 Exam Booklt Dpartmnt o Mchanical Enginring Rv /6/207 ELEMENT TYPES Figur : R-lmnt Figur 4: Tranormr Elmnt Figur 2: C-lmnt Figur 3: I-lmnt Figur 5: Gyrator Elmnt
More informationINC 693, 481 Dynamics System and Modelling: Linear Graph Modeling II Dr.-Ing. Sudchai Boonto Assistant Professor
INC 69, 48 Dynamics Systm and Modlling: Linar Graph Modling II Dr.-Ing. Sudchai Boonto Assistant Profssor Dpartmnt of Control Systm and Instrumntation Enginring King Mongkut s Unnivrsity of Tchnology Thonuri
More informationMechatronics 1: ME 392Q-6 & 348C 31-Aug-07 M.D. Bryant. Analogous Systems. e(t) Se: e. ef = p/i. q = p /I, p = " q C " R p I + e(t)
V + - K R + - - k b V R V L L J + V C M B Analogous Systems i = q. + ω = θ. C -. λ/l = q v = x F T. Se: e e(t) e = p/i R: R 1 I: I e C = q/c C = dq/dt e I = dp/dt Identical dierential equations & bond
More informationVoltage, Current, Power, Series Resistance, Parallel Resistance, and Diodes
Lctur 1. oltag, Currnt, Powr, Sris sistanc, Paralll sistanc, and Diods Whn you start to dal with lctronics thr ar thr main concpts to start with: Nam Symbol Unit oltag volt Currnt ampr Powr W watt oltag
More informationBrief Introduction to Statistical Mechanics
Brif Introduction to Statistical Mchanics. Purpos: Ths nots ar intndd to provid a vry quick introduction to Statistical Mchanics. Th fild is of cours far mor vast than could b containd in ths fw pags.
More informationThe Transmission Line Wave Equation
1//5 Th Transmission Lin Wav Equation.doc 1/6 Th Transmission Lin Wav Equation Q: So, what functions I (z) and V (z) do satisfy both tlgraphr s quations?? A: To mak this asir, w will combin th tlgraphr
More information7.4 Potential Difference and Electric Potential
7.4 Potntial Diffrnc and Elctric Potntial In th prvious sction, you larnd how two paralll chargd surfacs produc a uniform lctric fild. From th dfinition of an lctric fild as a forc acting on a charg, it
More informationDesign Guidelines for Quartz Crystal Oscillators. R 1 Motional Resistance L 1 Motional Inductance C 1 Motional Capacitance C 0 Shunt Capacitance
TECHNICAL NTE 30 Dsign Guidlins for Quartz Crystal scillators Introduction A CMS Pirc oscillator circuit is wll known and is widly usd for its xcllnt frquncy stability and th wid rang of frquncis ovr which
More informationPipe 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 informationDirect Approach for Discrete Systems One-Dimensional Elements
CONTINUUM & FINITE ELEMENT METHOD Dirct Approach or Discrt Systms On-Dimnsional Elmnts Pro. Song Jin Par Mchanical Enginring, POSTECH Dirct Approach or Discrt Systms Dirct approach has th ollowing aturs:
More informationThe pn junction: 2 Current vs Voltage (IV) characteristics
Th pn junction: Currnt vs Voltag (V) charactristics Considr a pn junction in quilibrium with no applid xtrnal voltag: o th V E F E F V p-typ Dpltion rgion n-typ Elctron movmnt across th junction: 1. n
More informationLast time. Resistors. Circuits. Question. Quick Quiz. Quick Quiz. ( V c. Which bulb is brighter? A. A B. B. C. Both the same
Last tim Bgin circuits Rsistors Circuits Today Rsistor circuits Start rsistor-capacitor circuits Physical layout Schmatic layout Tu. Oct. 13, 2009 Physics 208 Lctur 12 1 Tu. Oct. 13, 2009 Physics 208 Lctur
More informationExam 1. It is important that you clearly show your work and mark the final answer clearly, closed book, closed notes, no calculator.
Exam N a m : _ S O L U T I O N P U I D : I n s t r u c t i o n s : It is important that you clarly show your work and mark th final answr clarly, closd book, closd nots, no calculator. T i m : h o u r
More informationECE 344 Microwave Fundamentals
ECE 44 Microwav Fundamntals Lctur 08: Powr Dividrs and Couplrs Part Prpard By Dr. hrif Hkal 4/0/08 Microwav Dvics 4/0/08 Microwav Dvics 4/0/08 Powr Dividrs and Couplrs Powr dividrs, combinrs and dirctional
More informationSynchronous machines
Synchronous gnrator (altrnator): transorms mchanical nrgy into lctric nrgy; dsignd to gnrat sinusoidal oltags and currnts; usd in most powr plants, or car altrnators, tc. Synchronous motor: transorms lctric
More informationME 321 Kinematics and Dynamics of Machines S. Lambert Winter 2002
3.4 Forc Analysis of Linkas An undrstandin of forc analysis of linkas is rquird to: Dtrmin th raction forcs on pins, tc. as a consqunc of a spcifid motion (don t undrstimat th sinificanc of dynamic or
More informationModule 8 Non equilibrium Thermodynamics
Modul 8 Non quilibrium hrmodynamics ctur 8.1 Basic Postulats NON-EQUIIRIBIUM HERMODYNAMICS Stady Stat procsss. (Stationary) Concpt of ocal thrmodynamic qlbm Extnsiv proprty Hat conducting bar dfin proprtis
More informationENGI9496 Modeling and Simulation of Dynamic Systems Bond Graphs
ENGI9496 Modeling and Simulation of Dynamic Systems Bond Graphs Topics covered so far: Analogies between mechanical (translation and rotation), fluid, and electrical systems o Review of domain-specific
More informationDefinition1: The ratio of the radiation intensity in a given direction from the antenna to the radiation intensity averaged over all directions.
Dirctivity or Dirctiv Gain. 1 Dfinition1: Dirctivity Th ratio of th radiation intnsity in a givn dirction from th antnna to th radiation intnsity avragd ovr all dirctions. Dfinition2: Th avg U is obtaind
More informationIntroduction to the quantum theory of matter and Schrödinger s equation
Introduction to th quantum thory of mattr and Schrödingr s quation Th quantum thory of mattr assums that mattr has two naturs: a particl natur and a wa natur. Th particl natur is dscribd by classical physics
More informationCalculation of electromotive force induced by the slot harmonics and parameters of the linear generator
Calculation of lctromotiv forc inducd by th lot harmonic and paramtr of th linar gnrator (*)Hui-juan IU (**)Yi-huang ZHANG (*)School of Elctrical Enginring, Bijing Jiaotong Univrity, Bijing,China 8++58483,
More informationElectromagnetism Physics 15b
lctromagntism Physics 15b Lctur #8 lctric Currnts Purcll 4.1 4.3 Today s Goals Dfin lctric currnt I Rat of lctric charg flow Also dfin lctric currnt dnsity J Charg consrvation in a formula Ohm s Law vryon
More informationMath 34A. Final Review
Math A Final Rviw 1) Us th graph of y10 to find approimat valus: a) 50 0. b) y (0.65) solution for part a) first writ an quation: 50 0. now tak th logarithm of both sids: log() log(50 0. ) pand th right
More informationPHYS ,Fall 05, Term Exam #1, Oct., 12, 2005
PHYS1444-,Fall 5, Trm Exam #1, Oct., 1, 5 Nam: Kys 1. circular ring of charg of raius an a total charg Q lis in th x-y plan with its cntr at th origin. small positiv tst charg q is plac at th origin. What
More informationNEW APPLICATIONS OF THE ABEL-LIOUVILLE FORMULA
NE APPLICATIONS OF THE ABEL-LIOUVILLE FORMULA Mirca I CÎRNU Ph Dp o Mathmatics III Faculty o Applid Scincs Univrsity Polithnica o Bucharst Cirnumirca @yahoocom Abstract In a rcnt papr [] 5 th indinit intgrals
More informationELECTROMAGNETIC INDUCTION CHAPTER - 38
. (a) CTOMAGNTIC INDUCTION CHAPT - 38 3 3.dl MT I M I T 3 (b) BI T MI T M I T (c) d / MI T M I T. at + bt + c s / t Volt (a) a t t Sc b t Volt c [] Wbr (b) d [a., b.4, c.6, t s] at + b. +.4. volt 3. (a)
More informationAddition of angular momentum
Addition of angular momntum April, 0 Oftn w nd to combin diffrnt sourcs of angular momntum to charactriz th total angular momntum of a systm, or to divid th total angular momntum into parts to valuat th
More informationSAFE HANDS & IIT-ian's PACE EDT-15 (JEE) SOLUTIONS
It is not possibl to find flu through biggr loop dirctly So w will find cofficint of mutual inductanc btwn two loops and thn find th flu through biggr loop Also rmmbr M = M ( ) ( ) EDT- (JEE) SOLUTIONS
More informationElectric (Rocket) Propulsion. EP Overview
Elctric (Rockt) Propulsion EP Ovrviw Elctric Propulsion-1 Basics Rockt Propulsion Elmnts Propllant Enrgy Sourc Storag Fd Systm sam in chmical rockts Storag Convrsion Acclrator Elctric Propulsion- 1 Elctric
More informationIntroduction to Condensed Matter Physics
Introduction to Condnsd Mattr Physics pcific hat M.P. Vaughan Ovrviw Ovrviw of spcific hat Hat capacity Dulong-Ptit Law Einstin modl Dby modl h Hat Capacity Hat capacity h hat capacity of a systm hld at
More informationIVE(TY) Department of Engineering E&T2520 Electrical Machines 1 Miscellaneous Exercises
TRANSFORMER Q1 IE(TY) Dpartmnt of Enginring E&T50 Elctrical Machins 1 Miscllanous Exrciss Q Q3 A singl phas, 5 ka, 0/440, 60 Hz transformr gav th following tst rsults. Opn circuit tst (440 sid opn): 0
More informationECE602 Exam 1 April 5, You must show ALL of your work for full credit.
ECE62 Exam April 5, 27 Nam: Solution Scor: / This xam is closd-book. You must show ALL of your work for full crdit. Plas rad th qustions carfully. Plas chck your answrs carfully. Calculators may NOT b
More informationLecture 28 Title: Diatomic Molecule : Vibrational and Rotational spectra
Lctur 8 Titl: Diatomic Molcul : Vibrational and otational spctra Pag- In this lctur w will undrstand th molcular vibrational and rotational spctra of diatomic molcul W will start with th Hamiltonian for
More informationSlide 1. Slide 2. Slide 3 DIGITAL SIGNAL PROCESSING CLASSIFICATION OF SIGNALS
Slid DIGITAL SIGAL PROCESSIG UIT I DISCRETE TIME SIGALS AD SYSTEM Slid Rviw of discrt-tim signals & systms Signal:- A signal is dfind as any physical quantity that varis with tim, spac or any othr indpndnt
More informationHydrogen Atom and One Electron Ions
Hydrogn Atom and On Elctron Ions Th Schrödingr quation for this two-body problm starts out th sam as th gnral two-body Schrödingr quation. First w sparat out th motion of th cntr of mass. Th intrnal potntial
More informationThe POG Modeling Technique Applied to Electrical Systems
The POG Modeling Technique Applied to Electrical Systems Roberto ZANASI Computer Science Engineering Department (DII) University of Modena and Reggio Emilia Italy E-mail: roberto.zanasi@unimo.it Outline
More informationIYPT 2000 Problem No. 3 PLASMA
IYPT 000 Problm No. 3 PLASMA Tam Austria Invstigat th lctrical conducivity of th flam of a candl. Examin th influnc of rlvant paramtrs, in particular, th shap and polarity of th lctrods. Th xprimnts should
More informationGeneral 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 information6. The Interaction of Light and Matter
6. Th Intraction of Light and Mattr - Th intraction of light and mattr is what maks lif intrsting. - Light causs mattr to vibrat. Mattr in turn mits light, which intrfrs with th original light. - Excitd
More informationThe Relativistic Stern-Gerlach Force C. Tschalär 1. Introduction
Th Rlativistic Strn-Grlach Forc C. Tschalär. Introduction For ovr a dcad, various formulations of th Strn-Grlach (SG) forc acting on a particl with spin moving at a rlativistic vlocity in an lctromagntic
More information10. The Discrete-Time Fourier Transform (DTFT)
Th Discrt-Tim Fourir Transform (DTFT Dfinition of th discrt-tim Fourir transform Th Fourir rprsntation of signals plays an important rol in both continuous and discrt signal procssing In this sction w
More informationChapter 3: Capacitors, Inductors, and Complex Impedance
haptr 3: apacitors, Inductors, and omplx Impdanc In this chaptr w introduc th concpt of complx rsistanc, or impdanc, by studying two ractiv circuit lmnts, th capacitor and th inductor. W will study capacitors
More information2. Background Material
S. Blair Sptmbr 3, 003 4. Background Matrial Th rst of this cours dals with th gnration, modulation, propagation, and ction of optical radiation. As such, bic background in lctromagntics and optics nds
More informationPreliminary Fundamentals
1.0 Introduction Prliminary Fundamntals In all of our prvious work, w assumd a vry simpl modl of th lctromagntic torqu T (or powr) that is rquird in th swing quation to obtain th acclrating torqu. This
More informationa 1and x is any real number.
Calcls Nots Eponnts an Logarithms Eponntial Fnction: Has th form y a, whr a 0, a an is any ral nmbr. Graph y, Graph y ln y y Th Natral Bas (Elr s nmbr): An irrational nmbr, symboliz by th lttr, appars
More informationChapter 3: Capacitors, Inductors, and Complex Impedance
haptr 3: apacitors, Inductors, and omplx Impdanc In this chaptr w introduc th concpt of complx rsistanc, or impdanc, by studying two ractiv circuit lmnts, th capacitor and th inductor. W will study capacitors
More informationLecture 2: Discrete-Time Signals & Systems. Reza Mohammadkhani, Digital Signal Processing, 2015 University of Kurdistan eng.uok.ac.
Lctur 2: Discrt-Tim Signals & Systms Rza Mohammadkhani, Digital Signal Procssing, 2015 Univrsity of Kurdistan ng.uok.ac.ir/mohammadkhani 1 Signal Dfinition and Exampls 2 Signal: any physical quantity that
More informationPart 7: Capacitance And Capacitors
Part 7: apacitanc And apacitors 7. Elctric harg And Elctric Filds onsidr a pair of flat, conducting plats, arrangd paralll to ach othr (as in figur 7.) and sparatd by an insulator, which may simply b air.
More informationNARAYANA I I T / P M T A C A D E M Y. C o m m o n P r a c t i c e T e s t 1 6 XII STD BATCHES [CF] Date: PHYSIS HEMISTRY MTHEMTIS
. (D). (A). (D). (D) 5. (B) 6. (A) 7. (A) 8. (A) 9. (B). (A). (D). (B). (B). (C) 5. (D) NARAYANA I I T / P M T A C A D E M Y C o m m o n P r a c t i c T s t 6 XII STD BATCHES [CF] Dat: 8.8.6 ANSWER PHYSIS
More informationBasic Polyhedral theory
Basic Polyhdral thory Th st P = { A b} is calld a polyhdron. Lmma 1. Eithr th systm A = b, b 0, 0 has a solution or thr is a vctorπ such that π A 0, πb < 0 Thr cass, if solution in top row dos not ist
More informationFinite Element Models for Steady Flows of Viscous Incompressible Fluids
Finit Elmnt Modls for Stad Flows of Viscous Incomprssibl Fluids Rad: Chaptr 10 JN Rdd CONTENTS Govrning Equations of Flows of Incomprssibl Fluids Mid (Vlocit-Prssur) Finit Elmnt Modl Pnalt Function Mthod
More informationAS 5850 Finite Element Analysis
AS 5850 Finit Elmnt Analysis Two-Dimnsional Linar Elasticity Instructor Prof. IIT Madras Equations of Plan Elasticity - 1 displacmnt fild strain- displacmnt rlations (infinitsimal strain) in matrix form
More informationIntroduction to physical systems, their modeling and simulation: A Bond Graph Approach
Josph Anand Vaz, Dpartmnt o Mchanical Enginring, Dr B R Ambdkar NIT, Jalandhar 440, India Introduction to physical systms, thir modling and simulation: A Bond Graph Approach Anand Vaz Prossor Dpartmnt
More informationStatus of LAr TPC R&D (2) 2014/Dec./23 Neutrino frontier workshop 2014 Ryosuke Sasaki (Iwate U.)
Status of LAr TPC R&D (2) 214/Dc./23 Nutrino frontir workshop 214 Ryosuk Sasaki (Iwat U.) Tabl of Contnts Dvlopmnt of gnrating lctric fild in LAr TPC Introduction - Gnrating strong lctric fild is on of
More information1.2 Faraday s law A changing magnetic field induces an electric field. Their relation is given by:
Elctromagntic Induction. Lorntz forc on moving charg Point charg moving at vlocity v, F qv B () For a sction of lctric currnt I in a thin wir dl is Idl, th forc is df Idl B () Elctromotiv forc f s any
More informationExam 2 Thursday (7:30-9pm) It will cover material through HW 7, but no material that was on the 1 st exam.
Exam 2 Thursday (7:30-9pm) It will covr matrial through HW 7, but no matrial that was on th 1 st xam. What happns if w bash atoms with lctrons? In atomic discharg lamps, lots of lctrons ar givn kintic
More informationIntroduction to the Fourier transform. Computer Vision & Digital Image Processing. The Fourier transform (continued) The Fourier transform (continued)
Introduction to th Fourir transform Computr Vision & Digital Imag Procssing Fourir Transform Lt f(x) b a continuous function of a ral variabl x Th Fourir transform of f(x), dnotd by I {f(x)} is givn by:
More information2/12/2013. Overview. 12-Power Transmission Text: Conservation of Complex Power. Introduction. Power Transmission-Short Line
//03 Ovrviw -owr Transmission Txt: 4.6-4.0 ECEGR 45 owr ystms Consrvation of Complx owr hort in owr Transmission owr Transmission isualization Radial in Mdium and ong in owr Transmission oltag Collaps
More informationMaxwellian Collisions
Maxwllian Collisions Maxwll ralizd arly on that th particular typ of collision in which th cross-sction varis at Q rs 1/g offrs drastic siplifications. Intrstingly, this bhavior is physically corrct for
More informationAddition of angular momentum
Addition of angular momntum April, 07 Oftn w nd to combin diffrnt sourcs of angular momntum to charactriz th total angular momntum of a systm, or to divid th total angular momntum into parts to valuat
More information+ f. e f. Ch. 8 Inflation, Interest Rates & FX Rates. Purchasing Power Parity. Purchasing Power Parity
Ch. 8 Inlation, Intrst Rats & FX Rats Topics Purchasing Powr Parity Intrnational Fishr Ect Purchasing Powr Parity Purchasing Powr Parity (PPP: Th purchasing powr o a consumr will b similar whn purchasing
More informationCHAPTER 1. Introductory Concepts Elements of Vector Analysis Newton s Laws Units The basis of Newtonian Mechanics D Alembert s Principle
CHPTER 1 Introductory Concpts Elmnts of Vctor nalysis Nwton s Laws Units Th basis of Nwtonian Mchanics D lmbrt s Principl 1 Scinc of Mchanics: It is concrnd with th motion of matrial bodis. odis hav diffrnt
More informationSan José State University Aerospace Engineering AE 138 Vector-Based Dynamics for Aerospace Applications, Fall 2016
San José Stat Univrsity Arospac Enginring AE 138 Vctor-Basd Dynamics for Arospac Applications, Fall 2016 Instructor: Offic Location: Email: Offic Hours: Class Days/Tim: Classroom: Prof. J.M. Huntr E272F
More informationBasic Logic Review. Rules. Lecture Roadmap Combinational Logic. Textbook References. Basic Logic Gates (2-input versions)
Lctur Roadmap ombinational Logic EE 55 Digital Systm Dsign with VHDL Lctur Digital Logic Rrshr Part ombinational Logic Building Blocks Basic Logic Rviw Basic Gats D Morgan s Law ombinational Logic Building
More informationHigh Energy Physics. Lecture 5 The Passage of Particles through Matter
High Enrgy Physics Lctur 5 Th Passag of Particls through Mattr 1 Introduction In prvious lcturs w hav sn xampls of tracks lft by chargd particls in passing through mattr. Such tracks provid som of th most
More informationFinite element discretization of Laplace and Poisson equations
Finit lmnt discrtization of Laplac and Poisson quations Yashwanth Tummala Tutor: Prof S.Mittal 1 Outlin Finit Elmnt Mthod for 1D Introduction to Poisson s and Laplac s Equations Finit Elmnt Mthod for 2D-Discrtization
More informationFEM FOR HEAT TRANSFER PROBLEMS دانشگاه صنعتي اصفهان- دانشكده مكانيك
FEM FOR HE RNSFER PROBLEMS 1 Fild problms Gnral orm o systm quations o D linar stady stat ild problms: For 1D problms: D D g Q y y (Hlmholtz quation) d D g Q d Fild problms Hat transr in D in h h ( D D
More informationDeepak Rajput
Q Prov: (a than an infinit point lattic is only capabl of showing,, 4, or 6-fold typ rotational symmtry; (b th Wiss zon law, i.. if [uvw] is a zon axis and (hkl is a fac in th zon, thn hu + kv + lw ; (c
More informationPHYSICS 489/1489 LECTURE 7: QUANTUM ELECTRODYNAMICS
PHYSICS 489/489 LECTURE 7: QUANTUM ELECTRODYNAMICS REMINDER Problm st du today 700 in Box F TODAY: W invstigatd th Dirac quation it dscribs a rlativistic spin /2 particl implis th xistnc of antiparticl
More informationWhy is a E&M nature of light not sufficient to explain experiments?
1 Th wird world of photons Why is a E&M natur of light not sufficint to xplain xprimnts? Do photons xist? Som quantum proprtis of photons 2 Black body radiation Stfan s law: Enrgy/ ara/ tim = Win s displacmnt
More informationDerivation of Electron-Electron Interaction Terms in the Multi-Electron Hamiltonian
Drivation of Elctron-Elctron Intraction Trms in th Multi-Elctron Hamiltonian Erica Smith Octobr 1, 010 1 Introduction Th Hamiltonian for a multi-lctron atom with n lctrons is drivd by Itoh (1965) by accounting
More informationExtraction of Doping Density Distributions from C-V Curves
Extraction of Doping Dnsity Distributions from C-V Curvs Hartmut F.-W. Sadrozinski SCIPP, Univ. California Santa Cruz, Santa Cruz, CA 9564 USA 1. Connction btwn C, N, V Start with Poisson quation d V =
More informationClassical Magnetic Dipole
Lctur 18 1 Classical Magntic Dipol In gnral, a particl of mass m and charg q (not ncssarily a point charg), w hav q g L m whr g is calld th gyromagntic ratio, which accounts for th ffcts of non-point charg
More informationMiddle East Technical University Department of Mechanical Engineering ME 413 Introduction to Finite Element Analysis
Middl East Tchnical Univrsity Dpartmnt of Mchanical Enginring ME Introduction to Finit Elmnt Analysis Chaptr 5 Two-Dimnsional Formulation Ths nots ar prpard by Dr. Cünyt Srt http://www.m.mtu.du.tr/popl/cunyt
More informationWhere k is either given or determined from the data and c is an arbitrary constant.
Exponntial growth and dcay applications W wish to solv an quation that has a drivativ. dy ky k > dx This quation says that th rat of chang of th function is proportional to th function. Th solution is
More informationSection 11.6: Directional Derivatives and the Gradient Vector
Sction.6: Dirctional Drivativs and th Gradint Vctor Practic HW rom Stwart Ttbook not to hand in p. 778 # -4 p. 799 # 4-5 7 9 9 35 37 odd Th Dirctional Drivativ Rcall that a b Slop o th tangnt lin to th
More informationVII. Quantum Entanglement
VII. Quantum Entanglmnt Quantum ntanglmnt is a uniqu stat of quantum suprposition. It has bn studid mainly from a scintific intrst as an vidnc of quantum mchanics. Rcntly, it is also bing studid as a basic
More information1 Isoparametric Concept
UNIVERSITY OF CALIFORNIA BERKELEY Dpartmnt of Civil Enginring Spring 06 Structural Enginring, Mchanics and Matrials Profssor: S. Govindj Nots on D isoparamtric lmnts Isoparamtric Concpt Th isoparamtric
More informationCoupled Pendulums. Two normal modes.
Tim Dpndnt Two Stat Problm Coupld Pndulums Wak spring Two normal mods. No friction. No air rsistanc. Prfct Spring Start Swinging Som tim latr - swings with full amplitud. stationary M +n L M +m Elctron
More information2008 AP Calculus BC Multiple Choice Exam
008 AP Multipl Choic Eam Nam 008 AP Calculus BC Multipl Choic Eam Sction No Calculator Activ AP Calculus 008 BC Multipl Choic. At tim t 0, a particl moving in th -plan is th acclration vctor of th particl
More informationSCALING OF SYNCHROTRON RADIATION WITH MULTIPOLE ORDER. J. C. Sprott
SCALING OF SYNCHROTRON RADIATION WITH MULTIPOLE ORDER J. C. Sprott PLP 821 Novmbr 1979 Plasma Studis Univrsity of Wisconsin Ths PLP Rports ar informal and prliminary and as such may contain rrors not yt
More informationECE 2210 / 00 Phasor Examples
EE 0 / 00 Phasor Exampls. Add th sinusoidal voltags v ( t ) 4.5. cos( t 30. and v ( t ) 3.. cos( t 5. v ( t) using phasor notation, draw a phasor diagram of th thr phasors, thn convrt back to tim domain
More informationA crash-course in transistor circuits
A crash-cours in transistor circuits Patrick R. LClair July 19, 2011 Contnts 1 Transistors 1 1.1 Basic charactristics.................................... 1 1.2 Notation...........................................
More informationFourier Transforms and the Wave Equation. Key Mathematics: More Fourier transform theory, especially as applied to solving the wave equation.
Lur 7 Fourir Transforms and th Wav Euation Ovrviw and Motivation: W first discuss a fw faturs of th Fourir transform (FT), and thn w solv th initial-valu problm for th wav uation using th Fourir transform
More informationEE243 Advanced Electromagnetic Theory Lec # 23 Scattering and Diffraction. Reading: Jackson Chapter , lite
Applid M Fall 6, Nuruthr Lctur #3 Vr /5/6 43 Advancd lctromagntic Thory Lc # 3 cattring and Diffraction calar Diffraction Thory Vctor Diffraction Thory Babint and Othr Principls Optical Thorm ading: Jackson
More information5. Equation of state for high densities
5 1 5. Equation of stat for high dnsitis Equation of stat for high dnsitis 5 Vlocity distribution of lctrons Classical thrmodynamics: 6 dimnsional phas spac: (x,y,z,px,py,pz) momntum: p = p x+p y +p z
More informationFigure 1: Closed surface, surface with boundary, or not a surface?
QUESTION 1 (10 marks) Two o th topological spacs shown in Figur 1 ar closd suracs, two ar suracs with boundary, and two ar not suracs. Dtrmin which is which. You ar not rquird to justiy your answr, but,
More informationLecture 37 (Schrödinger Equation) Physics Spring 2018 Douglas Fields
Lctur 37 (Schrödingr Equation) Physics 6-01 Spring 018 Douglas Filds Rducd Mass OK, so th Bohr modl of th atom givs nrgy lvls: E n 1 k m n 4 But, this has on problm it was dvlopd assuming th acclration
More informationSupplementary Materials
6 Supplmntary Matrials APPENDIX A PHYSICAL INTERPRETATION OF FUEL-RATE-SPEED FUNCTION A truck running on a road with grad/slop θ positiv if moving up and ngativ if moving down facs thr rsistancs: arodynamic
More informationByeong-Joo Lee
OSECH - MSE calphad@postch.ac.kr Equipartition horm h avrag nrgy o a particl pr indpndnt componnt o motion is ε ε ' ε '' ε ''' U ln Z Z ε < ε > U ln Z β ( ε ' ε '' ε ''' / Z' Z translational kintic nrgy
More informationThe van der Waals interaction 1 D. E. Soper 2 University of Oregon 20 April 2012
Th van dr Waals intraction D. E. Sopr 2 Univrsity of Orgon 20 pril 202 Th van dr Waals intraction is discussd in Chaptr 5 of J. J. Sakurai, Modrn Quantum Mchanics. Hr I tak a look at it in a littl mor
More informationProbability and Stochastic Processes: A Friendly Introduction for Electrical and Computer Engineers Roy D. Yates and David J.
Probability and Stochastic Procsss: A Frindly Introduction for Elctrical and Computr Enginrs Roy D. Yats and David J. Goodman Problm Solutions : Yats and Goodman,4.3. 4.3.4 4.3. 4.4. 4.4.4 4.4.6 4.. 4..7
More informationChemical 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 informationSeptember 23, Honors Chem Atomic structure.notebook. Atomic Structure
Atomic Structur Topics covrd Atomic structur Subatomic particls Atomic numbr Mass numbr Charg Cations Anions Isotops Avrag atomic mass Practic qustions atomic structur Sp 27 8:16 PM 1 Powr Standards/ Larning
More informationPhys 402: Nonlinear Spectroscopy: SHG and Raman Scattering
Rquirmnts: Polariation of Elctromagntic Wavs Phys : Nonlinar Spctroscopy: SHG and Scattring Gnral considration of polariation How Polarirs work Rprsntation of Polariation: Jons Formalism Polariation of
More informationPrinciples of Humidity Dalton s law
Principls of Humidity Dalton s law Air is a mixtur of diffrnt gass. Th main gas componnts ar: Gas componnt volum [%] wight [%] Nitrogn N 2 78,03 75,47 Oxygn O 2 20,99 23,20 Argon Ar 0,93 1,28 Carbon dioxid
More informationChapter 8: Electron Configurations and Periodicity
Elctron Spin & th Pauli Exclusion Principl Chaptr 8: Elctron Configurations and Priodicity 3 quantum numbrs (n, l, ml) dfin th nrgy, siz, shap, and spatial orintation of ach atomic orbital. To xplain how
More information