11/13/2018.

Slides:



Advertisements
Similar presentations
Magnetism Alternating-Current Circuits
Advertisements

Electromagnetic Oscillations and Alternating Current
AC power. Resonance. Transformers.
Alternating Current Circuits
Lecture 20-1 Alternating Current (AC) = Electric current that changes direction periodically ac generator is a device which creates an ac emf/current.
Physics 121: Electricity & Magnetism – Lecture 13 Carsten Denker NJIT Physics Department Center for Solar–Terrestrial Research.
Copyright © 2009 Pearson Education, Inc. Lecture 10 – AC Circuits.
Exam 1Quiz 1Quiz 2. A series RLC circuit has a resistance of 25.0 , a capacitance of 50.0  F, and an inductance of H. If driven by a 120v, 60Hz.
chapter 33 Alternating Current Circuits
1 My Chapter 21 Lecture Outline. 2 Chapter 21: Alternating Currents Sinusoidal Voltages and Currents Capacitors, Resistors, and Inductors in AC Circuits.
Fall 2008 Physics 121 Practice Problem Solutions 13 Electromagnetic Oscillations AC Circuits Contents: 121P13 - 2P, 3P, 9P, 33P, 34P, 36P, 49P, 51P, 60P,
Chapter 22 Alternating-Current Circuits and Machines.
Ch – 35 AC Circuits.
ARRDEKTA INSTITUTE OF TECHNOLOGY GUIDED BY GUIDED BY Prof. R.H.Chaudhary Prof. R.H.Chaudhary Asst.prof in electrical Asst.prof in electrical Department.
Chapter 35.
Chapter 31 Electromagnetic Oscillations and Alternating Current Key contents LC oscillations, RLC circuits AC circuits (reactance, impedance, the power.
Copyright © 2010 Pearson Education, Inc. Lecture Outline Chapter 24 Physics, 4 th Edition James S. Walker.
Electromagnetic Oscillations and Alternating Current
Alternating Current Circuits
Chapter 24 Alternating-Current Circuits. Units of Chapter 24 Alternating Voltages and Currents Capacitors in AC Circuits RC Circuits Inductors in AC Circuits.
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.
Lecture 13 final part. Series RLC in alternating current The voltage in a capacitor lags behind the current by a phase angle of 90 degrees The voltage.
Lecture 17 AC circuits RLC circuits Transformer Maxwell.
Enrollment no.: Abhi P. Choksi Anuj Watal Esha N. Patel Guidied by: M. K. Joshi, P.R.Modha A.D.PATEL.INSTITUTE.
Electromagnetic Oscillations and Alternating Current Chapter 33.
L C LC Circuits 0 0 t V V C L t t U B U E Today... Oscillating voltage and current Transformers Qualitative descriptions: LC circuits (ideal inductor)
1 © Unitec New Zealand DE4401 AC R L C COMPONENTS.
Copyright © 2009 Pearson Education, Inc. Chapter 33 Inductance, Electromagnetic Oscillations, and AC Circuits Part II.
ELECTRICAL CIRCUIT CONCEPTS
Fig 33-CO These large transformers are used to increase the voltage at a power plant for distribution of energy by electrical transmission to the power.
Lecture 11 Electromagnetic Oscillations and Alternating Current Ch. 31 Topics –Generators –Transformers –LC Circuit Qualitatively –Electrical and Magnetic.
Slide 1Fig 33-CO, p Slide 2Fig 33-1, p the basic principle of the ac generator is a direct consequence of Faraday’s law of induction. When.
Lecture 19-1 Potential Difference Across Inductor VV ++ - I internal resistance Analogous to a battery An ideal inductor has r=0 All dissipative effects.
Halliday/Resnick/Walker Fundamentals of Physics 8th edition
Alternating Current Capacitors and Inductors are used in a variety of AC circuits.
Lecture 19-1 RL Circuits – Starting Current 2. Loop Rule: 3. Solve this differential equation τ=L/R is the inductive time constant 1.Switch to e at t=0.
PHYS219 Fall semester 2014 Lecture 16: AC Circuits with Inductors and Capacitors Dimitrios Giannios Purdue University.
Physics 213 General Physics Lecture Last Meeting: Self Inductance, RL Circuits, Energy Stored Today: Finish RL Circuits and Energy Stored. Electric.
Copyright © 2009 Pearson Education, Inc. Chapter 29 Electromagnetic Induction and Faraday’s Law.
Alternating Current Circuits
Levitation above a Superconductor
Alternating Current Kirchoff’s rules for loops and junctions may be used to analyze complicated circuits such as the one below, powered by an alternating.
Chapter 17 Resonance Circuits.
Physics Electricity and Magnetism Lecture 14 - AC Circuits, Resonance Y&F Chapter 31, Sec Phasor Diagrams for Voltage and Current The Series.
Inductance, Electromagnetic Oscillations, and AC Circuits
Lesson 11 Lesson 11 AC Circuits AC Ciruits Power
Alternating Current Electricity
5. Alternating Current Circuits
Lecture 6 (III): AC RESPONSE
Chapter 22: AC Circuits Figure (a) Direct current. (b) Alternating current.
An {image} series circuit has {image} , {image} , and {image}
The series of alternating current
Physics Electricity and Magnetism Lecture 14 - AC Circuits, Resonance Y&F Chapter 31, Sec Phasor Diagrams for Voltage and Current The Series.
LC Oscillations L C I Kirchoff’s loop rule 11/12/2018.
Chapter 31 Electromagnetic Oscillations and Alternating Current
Ch. 31.4–7: Electrical Oscillations, LC Circuits, Alternating Current
PHYS 1444 – Section 04 Lecture #22
General Physics (PHY 2140) Lecture 19 Electricity and Magnetism
Alternating Current Circuits and Electromagnetic Waves
AC circuits Physics /23/2018 Lecture XIX.
Physics Electricity and Magnetism Lecture 14 - AC Circuits, Resonance Y&F Chapter 31, Sec Phasor Diagrams for Voltage and Current The Series.
Alternating Current Circuits
ELL100: INTRODUCTION TO ELECTRICAL ENGG.
Lecture 11 Electromagnetic Oscillations and Alternating Current Ch. 31
Lecture Outline Chapter 24 Physics, 4th Edition James S. Walker
ECE131 BASIC ELECTRICAL & ELECTRONICS ENGG
Physics Electricity and Magnetism Lecture 14 - AC Circuits, Resonance Y&F Chapter 31, Sec Phasor Diagrams for Voltage and Current The Series.
Chapter 33 Problems 3,10,17,21,22,26,32,33,37.
Physics 312: Electronics (1) Lecture 7 AC Current I Fundamentals of Electronics Circuits (with CD-ROH) By: Charles Alexander, Hathew Sadika, McGraw Hill.
Physics Electricity and Magnetism Lecture 14 - AC Circuits, Resonance Y&F Chapter 31, Sec Phasor Diagrams for Voltage and Current The Series.
Presentation transcript:

11/13/2018

LECTURE 19 AC Generators AC Circuits Start by considering simple circuits with one element (R, C, or L) in addition to the driving emf. It will lead to Oscillations and Driven RLC circuits

Alternating Current Generators (DEMO) (N = 2 for this coil) DEMO: New AC Motor – coil, magnetic & light bulb – faster I crank the brighter the bulb 11/13/2018

Phasors for R V in phase with I 11/13/2018

Power Dissipated in a Resistor Peak value Average value 11/13/2018

Standard Alternating Voltage in the US +peak -peak 11/13/2018

Using rms values: summary Using rms values of current and voltage allows you to use the familiar dc formulas, such as V = IR and P = I 2 R. One ac ampere is said to flow in a circuit if it produces the same joule heating as one ampere of dc current under the same conditions. At your house the peak voltage will be 170 V 11/13/2018

What is the rms value of an AC voltage whose maximum value is 141 V? QUIZ lecture 19 What is the rms value of an AC voltage whose maximum value is 141 V? zero 70.7 V 100 V 141 V 240 V 11/13/2018

Inductors in AC Circuits 900 Potential drop, VL(t), leads the current, I(t) by 900 11/13/2018

Relationship between Irms & Vrms 11/13/2018

Phasors for L V leads I by 90 90 degrees out of phase…..if I and V 90 out of phase no power loss 11/13/2018

Quiz Questions If we increase the driving frequency in a circuit with a purely inductive load does IL Decrease Increase Remain the Same VL remains the same IL decreases If we increase the driving frequency in a circuit with a purely inductive load does VL Decrease Increase Remain the Same 11/13/2018

Capacitors in AC Circuits 900 Potential drop, VC(t), lags the current, I(t), by 900 11/13/2018

Relationship between Irms & VC,rms 11/13/2018

Phasors for C V lags I by 90 Conventions….most important 90 degrees out of phase But capacitors and inductors are 180 out of phase with each other 11/13/2018

Summary Symbol Reactance X C L L R IC current leads VC IL current lags VL 11/13/2018

Impedances for L, C, R R is resistance is capacitive reactance For high , XC goes to zero, C acts like a wire. For low , XC grows larger and at DC, C acts like an open switch XL = L is inductive Reactance For high , XL grows large and L acts like an open switch. For low , XL grows small and at DC, L acts like a conducting wire. 11/13/2018

Phasors for R V in phase with I 11/13/2018

Phasors for C V lags I by 90 11/13/2018

Phasors for L V leads I by 90 11/13/2018

AC Power Distribution AC power can travel at high voltages and low amps, therefore smaller power loss Tesla liked 60 Hz and 240 V Standard in Europe was defined by a German company AEG ( monopoly) who chose 50Hz (20% less efficient in generation, 10-15% less efficient in transmission) Originally Europe was also 110V, but they changed to reduce power loss and voltage drop for the same copper diameter Nikola Tesla http://www.teslasociety.com/ 11/13/2018

The Power Grid 11/13/2018

Example If 735 kV line is used to transmit electric energy 1000 km. I = 500 A and R = 0.220 W/km Energy is supplied at a rate of Energy dissipated from resistance of wires If you doubled the current and halved the voltage, energy dissipated 11/13/2018

LC Circuits ++++ - - - - R C L C ++++ - - - - Consider the LC and RC series circuits shown: Suppose that at t=0 the capacitor is charged to a value of Q. Is there is a qualitative difference in the time development of the currents produced in these two cases. Why?? 11/13/2018

LC Oscillations L C I ++++ - - - - Kirchoff’s loop rule 11/13/2018

LC Oscillations Q V C I V t L dI dt t 11/13/2018

Example 1 (a) Vab < 0 (b) Vab = 0 (c) Vab > 0 L C t=0 L C t=t1 + - Q Qo = L C t=t1 Q = At t=0, the capacitor in the LC circuit shown has a total charge Q0. At t = t1, the capacitor is uncharged. What is the value of Vab, the voltage across the inductor at time t1? (a) Vab < 0 (b) Vab = 0 (c) Vab > 0 11/13/2018

Example 2 (a) I2 = I0 (b) I2 = 2I0 (c) I2 = 4I0 t=0 + - Q Qo = At t=0 the capacitor has charge Q0; the resulting oscillations have frequency 0. The maximum current in the circuit during these oscillations has value I0. What is the relation between I0 and I2 , the maximum current in the circuit when the initial charge = 2Q0? (a) I2 = I0 (b) I2 = 2I0 (c) I2 = 4I0 11/13/2018

Example 3 (a) 2 = 1/2 0 (b) 2 = 0 (c) 2 = 20 t=0 + - Q Qo = At t=0 the capacitor has charge Q0; the resulting oscillations have frequency 0. The maximum current in the circuit during these oscillations has value I0. What is the relation between 0 and 2, the frequency of oscillations when the initial charge = 2Q0? (a) 2 = 1/2 0 (b) 2 = 0 (c) 2 = 20 11/13/2018