INTRODUCTION TO CIRCUIT THEORY

Slides:



Advertisements
Similar presentations
Electricity & Magnetism
Advertisements

1 Dr. Un-ki Yang Particle Physics Group or Shuster 5.15 Amplifiers and Feedback 1.
Slide 1EE100 Summer 2008Bharathwaj Muthuswamy EE100 Su08 Lecture #2 (June 25 th 2008) For today: –Bart: slight change in office hours: Check website –Student.
Lect1EEE 2021 Introduction; Circuit Elements; Ohm's Law; KCL Dr. Holbert January 14, 2008.
1 Exam 1 Review Chapters 1, 2, 9. 2 Charge, q Recall Coulomb’s Law Unit: Newton meter 2 / coulomb 2 volt meter / coulomb Charge on an electron (proton)
1.1 Introduction * Objectives * Requirements & Grading Policy * Other information 1.2 Basic Circuit Concepts * Electrical quantities  current, voltage.
Circuit Theory What you will use this for –Power management –Signals between subsystems –Possible analog data types How the knowledge will help you –Understanding.
Chapter 20: Circuits Current and EMF Ohm’s Law and Resistance
Lecture 2 Basic Circuit Laws
Engineering H192 - Computer Programming Gateway Engineering Education Coalition Lab 4P. 1Winter Quarter Analog Electronics Lab 4.
ELECTRONICS PRIMER. Assignment: WEB-based Electronics Tutorial Basic definitions Components Ohm's Law LEDs and Transistors Additional electronics tutorials.
Basic Electric Circuits & Components
Electrical Engineering for Civil Engineer Dr. Basim Zafar Spring 2013 EE for CE Course Outlines MID TERM I Dr. Basim Zafar.
Electrical Circuits Dr. Sarika Khushalani Solanki
Overview of ENGR 220 Circuits 1 Fall 2005 Harding University Jonathan White.
1 Dr. Un-ki Yang Particle Physics Group or Shuster 5.15 Amplifiers and Feedback 1.
ELECTRONICS PRIMER I. Basic Electronics Current (I): Amount of charge passing a given point per unit time Voltage (V): Electrical pressure or force. If.
Engineering H192 - Computer Programming The Ohio State University Gateway Engineering Education Coalition Lab 3P. 1Winter Quarter Analog Electronics Lab.
ARRDEKTA INSTITUTE OF TECHNOLOGY GUIDED BY. GUIDED BY. Prof.Y.B.Vaghela. Prof.Y.B.Vaghela. Asst.prof in electrical Asst.prof in electrical Department Department.
110/16/2015 Applied Physics Lecture 19  Electricity and Magnetism Induced voltages and induction Energy AC circuits and EM waves Resistors in an AC circuits.
ECE 102 Engineering Computation Chapter 6 Circuit Elements Dr. Herbert G. Mayer, PSU Status 10/11/2015 For use at CCUT Fall 2015.
Physics 1202: Lecture 8 Today’s Agenda Announcements: –Lectures posted on: –HW assignments, solutions.
ELECTRICAL CIRCUIT CONCEPTS
Electric Current and Circuits. What is Current? Electric current is a flow of electric charge Electric current is a flow of electric charge I = Q/t I.
Determine the mathematical models that capture the behavior of an electrical system 1.Elements making up an electrical system 2.First-principles modeling.
NETWORK ANALYSIS. UNIT – I INTRODUCTION TO ELECTRICAL CIRCUITS: Circuit concept – R-L-C parameters Voltage and current sources Independent and dependent.
Analog Circuits Seth Price Department of Chemical Engineering New Mexico Tech Rev. 1/13/16.
Halliday/Resnick/Walker Fundamentals of Physics 8th edition
Chapters 17 through 23 Midterm Review. Midterm Exam ~ 1 hr, in class 15 questions 6 calculation questions One from each chapter with Ch. 17 and 18 combine.
Chapter 9 Sinusoids and Phasors
Chapter 25 : Electric circuits
Dr inż. Agnieszka Wardzińska Room: 105 Polanka cygnus.et.put.poznan.pl/~award Advisor hours: Monday: Wednesday:
Physics 213 General Physics Lecture Last Meeting: Self Inductance, RL Circuits, Energy Stored Today: Finish RL Circuits and Energy Stored. Electric.
Lecture 2, Slide 1EECS40, Spring 2004Prof. Sanders Introduction to circuit analysis OUTLINE Electrical quantities and sign conventions (review) Ideal basic.
1 Introduction; Circuit Elements; Ohm's Law; KCL Prepared by: PANDYA SHIVANSHI( ) CHHIKNIWALA PRANAVI( )
Chapter 12 RL Circuits.
Chapter 9 Sinusoids and Phasors
ELECTRONICS PRIMER.
Electrical Circuits.
Electrical circuits, power supplies and passive circuit elements
Unit 2 | Using tools, equipment and other devices
Inductance and Capacitance Response of First Order RL and RC
Electrical Circuits.
Electrical circuits, power supplies and passive circuit elements
EKT101 Electric Circuit Theory
5. Modeling of Electrical Systems
SERIES AND PARALLEL AC CIRCUITS
ME375 Handouts - Spring 2002ME375-Fall 2002
Introduction to Electronics
Exam 1 Review Chapters 1, 2, 9.
Power Circuit By: AAA.
Fundamentals of Electric Circuits
Electrical Circuits – DC Circuits Lecturer: Russ Tatro
General Physics (PHY 2140) Lecture 19 Electricity and Magnetism
Analogue Electronics 电子 2+2 Prof. Li Chen
Amateur Extra Q & A Study Pool
Electric Current And Related Parameters
Fundamental Electrical Engineering
Note: Current has polarity.
ELL100: INTRODUCTION TO ELECTRICAL ENG.
Kirchoff’s Laws.
ECE131 BASIC ELECTRICAL & ELECTRONICS ENGG
Electric Current And Related Parameters
Fundamentals of D.C. circuits
Kirchoff’s Laws.
Electronic Circuits-1(CNET-112) Level 4th Department of CNET
Sri Eshwar College of Engineering,
Basics of Electronic Circuits
Delivered by Mr. Rajitha de Silva Courtesy Ms. Shashika Lokuliyana.
Lecture 2 Electrical and Electronics Circuits. After you study, and apply ideas in this Lecture, you will: Understand differences among resistance, capacitance,
Presentation transcript:

INTRODUCTION TO CIRCUIT THEORY Oana Mihaela DROSU Dr. Eng., Lecturer Politehnica University of Bucharest Department of Electrical Engineering LPP ERASMUS+

Circuit Theory What you will use this for Power management Signals between subsystems Possible analog data types How the knowledge will help you Understanding power and energy requirements Behavior of digital electric signals Analog signal conditioning and limitations Understanding associated technologies

Circuit theory Topics Circuit Topology Voltage, Current and Power Kirchoff’s Laws Circuit components DC circuits AC circuits We will consistently use Systeme International d’Unites, or SI units here. Basic units are Meters[m], Kilograms[kg], Seconds[s], and Amperes[A].

Circuit Topology A circuit consists of a mesh of loops Represented as branches and nodes in an undirected graph. Circuit components reside in the branches Connectivity resides in the nodes Nodes represent wires Wires represent equipotentials

Voltage, Current and Power (1) The concept of charge The Coulomb [C] – the SI unit of charge An electron carries -1.6e-19 [C] Conservation of charge The concept of potential Attraction/repulsion of charges The electric field The energy of moving a charge in a field

Voltage, Current and Power (2) Voltage is a difference in electric potential always taken between two points. Absolute voltage is a nonsensical fiction. The concept of ground is also a (useful) fiction. It is a line integral of the force exerted by an electric field on a unit charge. Customarily represented by v or V. The SI unit is the Volt [V].

Voltage, Current and Power (3) Current is a movement of charge. It is the time derivative of charge passing through a circuit branch. Customarily represented by i or I. The SI unit is the Ampere [A].

Voltage, Current and Power (4) Power is the product of voltage by current. It is the time derivative of energy delivered to or extracted from a circuit branch. Customarily represented by P or W. The SI unit is the Watt [W].

Kirchoff’s Laws These laws add up to nothing! Yet they completely characterize circuit behavior. Kirchoff’s Voltage Law (KVL) - The sum of voltages taken around any loop is zero. The start and end points are identical; consequently there is no potential difference between them. Kirchoff’s Current Law (KCL) – The sum of currents entering any node is zero. A consequence of the law of conservation of charge.

Circuit components Active vs. Passive components Active ones may generate electrical power. Passive ones may store but not generate power. Lumped vs. Distributed Constants Distributed constant components account for propagation times through the circuit branches. Lumped constant components ignore these propagation times. Appropriate for circuits small relative to signal wavelengths. Linear, time invariant (LTI) components are those with constant component values.

Active circuit components Conservation of energy: active components must get their power from somewhere! From non-electrical sources Batteries (chemical) Dynamos (mechanical) Transducers in general (light, sound, etc.) From other electrical sources Power supplies Power transformers Amplifiers

Passive lumped constants Classical LTI Resistors are AC/DC components. Inductors are AC components (DC short circuit). Capacitors are AC components (DC open circuit). Other components Rectifier diodes. Three or more terminal devices, e.g. transistors. Transformers.

DC circuits The basic LTI component is the Resistor Ohm’s Law: V = I R Customarily represented by R. The SI unit is the Ohm []. Ohm’s Law: V = I R Ohm’s and Kirchoff’s laws completely prescribe the behavior of any DC circuit comprising LTI components.

Example: voltage divider Assume no current is drawn at the output terminals in measuring Vout. Ohm’s Law requires that VR1 = IR1 R1 and VR2 = IR2 R2, which is also Vout. KCL says the current leaving resistor R1 must equal the current entering R2, or IR1 = IR2, so we can write Vout = IR1 R2. KVL says the voltage around the loop including the battery and both resistors is 0, therefore Vin = VR1 + Vout, or Vin = IR1 R1 + IR1 R2. Thus, IR1 = Vin / (R1 + R2), and Vout = Vin R2 / (R1 + R2).

AC circuits -- Components Basic LTI components Resistor, R, [] (Ohms) Inductor, L, [H] (Henrys) Capacitor, C, [F] (Farads) Frequency Repetition rate, f, [Hz] (Hertz) Angular,  = 2f, [1/s] (radians/sec)

AC Components: Inductors Current in an inductor generates a magnetic field, B = K1 I Changes in the field induce an inductive voltage. V = K2 (dB/dt) The instantaneous voltage is V = L(dI/dt), where L = K1K2. This is the time domain behavior of an inductor.

AC Components: Capacitors Charge in a capacitor produces an electric field E, and thus a proportional voltage, Q = C V, Where C is the capacitance. The charge on the capacitor changes according to I = (dQ/dt). The instantaneous current is therefore I = C(dV/dt). This is the time domain behavior of a capacitor.

AC Circuits – Laplace Transform Transforms differential equations in time to algebraic equations in frequency (s domain). where the frequency variable s =  + j. For sinusoidal waves,  = 0, and s = j. Resistor behavior in s domain: v= iR. Inductor behavior in s domain: v= i (jL). Capacitor behavior in s domain: i= v (jC).

AC circuits -- Impedance Impedance and Ohm’s Law for AC: Impedance is Z = R + jX, where j = -1, and X is the reactance in []. Ohm’s AC Law in s domain: v = i Z Resistance R dissipates power as heat. Reactance X stores and returns power. Inductors have positive reactance Xl=L Capacitors have negative reactance Xc=-1/C

Impedance shortcuts The impedance of components connected in series is the complex sum of their impedances. The impedance of components connected in parallel is the reciprocal of the complex sum of their reciprocal impedances.

Example: low pass filter Magnitude and phase plots of A, where RC=1. The magnitude plot is log/log, while the phase plot is linear radians vs. log freq.

Homework problem Derive the filter gain of the pictured circuit. Plot the magnitude and phase of the filter for L = 6.3e-6 [H], R = 16 [], and C = 1.0e-7 [F]. For extra credit, also plot for R = 7 [] and 50 [].