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ELEC130 Electrical Engineering 1 Week 2 Module 1 Introductory Circuit Techniques 1 Software Electronic Workbench: Simulation Software Faculty PC’s Rm. ES210 - Go to Diomedes Login: cstudentnumber Password: access keys on students card + daymonth (ddmm) of birth TopClass: Class Discussion & Notices http://www.newcastle.edu.au:86/topclass/ Username: first name.last name Password: date of birth ddmmyy Email: first name.last name@studentmail 23-Feb-99 Lecture 2 2 Administration Items Laboratory & Tutorials start THIS WEEK A couple of corrections have been given to the Tutors and Laboratory demonstrators Quiz 1 - Week 3 - Lecture NEXT MONDAY Will cover to the end of Module 1 which will be completed next lecture before the quiz. Survey Subject Home Page: - through Dept. Pages http://www.ee.newcastle.edu.au/ http://www.ee.newcastle.edu.au/undergradcourse.html 23-Feb-99 Lecture 2 3 Last week Charge Symbol: Q q(t) Units: Coulombs or C Current Symbol: I i(t) Units: Amperes or A Voltage Symbol: V v(t) Units: Volts or V Power Symbol: P p(t) Units: Watts or W Resistance Symbol: R (I = Q / t Amps Units: Ohms or & V = P.t / Q volts) P = V . I Watts V = R . I Ohms 23-Feb-99 Lecture 2 4 Conventions Current - positive charge flow - through element = -3A 3A Voltage - measured across an element Power I + v(t) _ + Circuit v(t) or _ + - Delivering power 23-Feb-99 I element I Lecture 2 Absorbing power 5 Resistance Material - resistivity R = .l / A Poor conductor is large e.g. plastics, wood Good conductors is small e.g. copper, gold, aluminium Resistance - the most common materials used are: carbon composition nickel chromium wire wound (for high power applications) Can be physically small (10mm long) or large (>1m), can be fixed or variable 23-Feb-99 Lecture 2 6 Resistance Common - are small fixed with colour coded values: Black Brown Red Orange Yellow 23-Feb-99 0 1 2 3 4 Green Blue violet Grey White Lecture 2 5 6 7 8 9 Brown Red Gold Silver Nil 1% 2% 5% 10% 20% 7 Resistance Charge tends to flow from a higher voltage (potential) to a lower voltage I + Determine direction of the current. If not labelled - GUESS the direction. 4V 10 _ Potential of resistor where the current enters is positive and leaves is negative. (If guess is wrong - just get negative voltage for an answer) 23-Feb-99 Lecture 2 8 Conductance Sometimes easier to use inverse of resistance called conductance Symbol: Units: G Siemens S (mhos) G = R-1 e.g. 2 = 0.5 S NB: Useful when resistors are connected in parallel 23-Feb-99 Lecture 2 9 Some Analogies Charge Volume (of gas) Voltage Pressure Current Flow Rate Resistance Constriction 23-Feb-99 Lecture 2 10 Series and Parallel Elements Series elements have the same current Share voltage Parallel elements have the same voltage Share current ia(t) i(t) i(t) + va(t) + 23-Feb-99 - + vb(t) v(t) - + vc(t) - ib(t) ic(t) - + Lecture 2 v(t) 11 Kirchoff’s Voltage Law The sum of the voltages around a closed path is zero: (closed path) V=0 Convention is to move around a closed loop in a clockwise direction Analogy - Walk around campus How do you specify the polarity of voltages in the circuit? 23-Feb-99 Lecture 2 12 Kirchoffs Voltage Law example + I V1 V1 V2 Vs 0 _ + Vs R1 - + R2 Example: If Vs = 12 V and R1= R2 , then V1 = V2 = 6 V V2 _ 23-Feb-99 Lecture 2 13 Series Resistance R1 I + V1 R2 - + V2 Rn - + Vn - Vs + Vs = V1 + V2 + …….+ Vn Vs = R1 I + R2 I + …….+ Rn I Vs = (R1 + R2 + …….+ Rn)I where e.g. V1 = R1 I by Ohm’s Law Thus Req = R1 + R2 + …….+ Rn 23-Feb-99 Lecture 2 14 Lecture Exercise I + VX - 23-Feb-99 Lecture 2 15 Kirchoff’s Current Law Total charge (current) accumulating at a node is zero: (entering) I- (leaving) I=0 Convention is current entering a node is positive and leaving a node is negative Analogy - road intersection How do you specify the direction of current if it is not given? 23-Feb-99 Lecture 2 16 Kirchoff’s Current Law - example I1 node I2 I 1 + I3 - I 2 = 0 I3 23-Feb-99 Lecture 2 17 Parallel resistance + Is R1 R2 I1 I2 Is = I1 + I2 + …..+ In [ I = V. 1/R = V G ] V R n _ In Is = VG1 + VG2 +... + VGn Is = V (G1 + G2 +... + Gn) Is = V Geq Geq = G1 + G2 +... + Gn 1/Req = 1/R1+ 1/R2+...+ 1/Rn 23-Feb-99 Lecture 2 18 Two Parallel Resistors 1/Req = 1/R1 + 1/R2 + = (R1 + R2)/ R1.R2 - Req = R1.R2 / (R1 + R2) 23-Feb-99 Lecture 2 Vs R1 R2 I1 I2 19 Current Division Is Vs G1 G2 + + - Vs _ R1 R2 I1 I2 Is I1 Vs G1 G1 G1 G2 G1 R2 I1 Is Is G1 G2 R1 R2 NB: more current flows through path of lesser resistance 23-Feb-99 Lecture 2 20 Voltage Division I R1 V1 R1 V1 IR1 Vs R! R2 _ + Vs Vs I R! R2 + - + R2 R2 V2 Vs R! R2 V2 _ 23-Feb-99 Lecture 2 21 Series Sources Ideal independent voltage sources in series add algebraically +- +- +- +- I V1 V2 V3 Vn I R - VR + NB cases of parallel voltage sources are not resolvable. WHY? 23-Feb-99 Lecture 2 22 Parallel Sources Ideal independent current sources in parallel add algebraically IT + V _ In R I1 I2 I3 NB cases of series current sources are not resolvable. WHY? 23-Feb-99 Lecture 2 23 Example R2 and R3 are effectively open circuited and therefore can be omitted R7 and R8 are short circuited, and can be omitted 23-Feb-99 Lecture 2 24 Example continues 23-Feb-99 Lecture 2 25 Wye Delta Transformations Need to find equivalent resistance to determine current. HOW? (They are not in series, not in parallel) Use Y to transformation 23-Feb-99 Lecture 2 26 Equating Resistance's Resistance between X - Y In Ra // (Rb + Rc) X Ra Y Rb Rc In Y R1 + R3 RXY 23-Feb-99 X Z R1 R2 Z R3 Y Ra ( Rb Rc ) R1 R3 Ra ( Rb Rc ) Lecture 2 27 Solving simultaneously …. To obtain R1, R2, R3 in terms of Ra, Rb, Rc and vice versa 23-Feb-99 Lecture 2 28 Example cont. X X Y Z Z Y 23-Feb-99 Lecture 2 29 Linearity A linear circuit is one that contains only linear elements. Resistors, Voltage & Current sources, Inductors and Capacitors are linear elements. An example of a nonlinear element is a lamp or a diode. A diode allows current to flow freely in one direction, but blocks the flow of current in the other. Power is not linear due to V2 or I2 ! 23-Feb-99 Lecture 2 30 Superposition What to do when there is more than one source in a circuit? SUPERPOSITION - If a linear circuit is excited by more than one independent source, then the total response is simply the sum of the responses of the individual sources. How do you temporarily remove sources? Voltage source by a short circuit Current sources by an open circuit 23-Feb-99 Lecture 2 31 Superposition example R1 Vs + - R2 R3 Is I R2 23-Feb-99 Lecture 2 32