See 7 RCL series a.c. circuit applet

Slides:



Advertisements
Similar presentations
Alternating-Current Circuits
Advertisements

NEWMAR 115 – 12 – 20AU Full-Wave Rectifier with Choke-Input Filter.
Capacitor: Let us consider the following circuit consisting of an ac voltage source and a capacitor. The current has a phase shift of +  /2 relative to.
Lesson 25 AC Thèvenin Max Power Transfer. Learning Objectives Explain under what conditions a source transfers maximum power to a load. Determine the.
Q31.1 A resistor is connected across an ac source as shown. Which graph correctly shows the instantaneous current through the resistor and the instantaneous.
AC Circuits Physics 102 Professor Lee Carkner Lecture 24.
Alternating Current Circuits
Copyright © 2008 Pearson Education, Inc., publishing as Pearson Addison-Wesley Chapter 36. AC Circuits Today, a “grid” of AC electrical distribution systems.
ECE 442 Power Electronics1 NEWMAR 115 – 12 – 20AU Full-Wave Rectifier with Choke-Input Filter.
Physics for Scientists and Engineers II, Summer Semester Lecture 18: July 6 th 2009 Physics for Scientists and Engineers II.
Capacitor Load The capacitive reactance of a capacitor
Lesson 19 Impedance. Learning Objectives For purely resistive, inductive and capacitive elements define the voltage and current phase differences. Define.
Alternating Current Circuits
RLC Circuits Physics 102 Professor Lee Carkner Lecture 25.
RLC Circuits Physics 102 Professor Lee Carkner Lecture 25.
Copyright © 2009 Pearson Education, Inc. Lecture 10 – AC Circuits.
3/31/2020USF Physics 1011 Physics 101 AC Circuits.
Physics 2112 Unit 20 Outline: Driven AC Circuits Phase of V and I
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,
Lab 8: AC RLC Resonant Circuits Only 4 more labs to go!! DC – Direct Current time current AC – Alternating Current time current When using AC circuits,
Resonant Circuit.
Chapter 35.
Chapter 33 Alternating Current Circuits CHAPTER OUTLINE 33.1 AC Sources 33.2 Resistors in an AC Circuit 33.3 Inductors in an AC Circuit 33.4 Capacitors.
Copyright © 2009 Pearson Education, Inc. Chapter 30 Inductance, Electromagnetic Oscillations, and AC Circuits.
Rotating Generators and Faraday’s Law 0 For N loops of wire.
Chapter 31 Alternating Current.
In a series R-L-C circuit, the voltage across an inductor _____ the current. A.leads B.lags C.is in phase with.
Alternating Current Circuits
RLC Circuits. Ohm for AC  An AC circuit is made up with components. Power source Resistors Capacitor Inductors  Kirchhoff’s laws apply just like DC.
Alternating Current Electricity NCEA A.S 3.6 Text Chapters
1 Alternating Current Circuits Chapter Inductance CapacitorResistor.
P Class 26: Outline Hour 1: Driven Harmonic Motion (RLC) Hour 2: Experiment 11: Driven RLC Circuit.
Basic Electronics Ninth Edition Basic Electronics Ninth Edition ©2002 The McGraw-Hill Companies Grob Schultz.
Chapter 23 Alternating Current Circuits Capacitors and Capacitive Reactance The resistance in a purely resistive circuit has the same value at all.
Inductive Reactance Electronics. Inductors in AC Circuits.
Capacitors in AC Circuits. In a capacitor in a dc circuit, charge flows until the capacitor is charged. In an ac circuit with a capacitor, charge flows.
Alternating Current Circuits. Resistance Capacitive Reactance, X C.
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.
Alternating Current (AC) R, L, C in AC circuits
Chapter-23 Alternating Current Circuits. AC Circuits All the equipment in this operating room use alternating current circuits.
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.
AC Circuits.
Roll No.Name 41.RATIYA RAJU 42.SATANI DARSHANA 43.SAVALIYA MILAN 44.SISARA GOVIND 45.VALGAMA HARDIK 46.VADHER DARSHAK 47.VADOLIYA MILAN 48.VALA GOPAL.
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.
Physics 212 Lecture 21, Slide 1 Physics 212 Lecture 21.
Alternating-Current Circuits Physics Alternating current is commonly used everyday in homes and businesses throughout the word to power various.
VSVS L C R At every instant, the generator / supply voltage: (V S = V m sinωt) is given by: V S = V L + V C + V R IZ = IX L + IX C + IR These relationships.
Lecture 03: AC RESPONSE ( REACTANCE N IMPEDANCE ).
Alternating Current Circuits. AC Sources  : angular frequency of AC voltage  V max : the maximum output voltage of AC source.
1© Manhattan Press (H.K.) Ltd Series combination of resistors, capacitors and inductors Resistor and capacitor in series (RC circuit) Resistor and.
Alternating Current Capacitors and Inductors are used in a variety of AC circuits.
Physics 212 Lecture 20, Slide 1 Physics 212 Lecture 20 AC Circuits Phasors.
Inductor Arising from Faraday's law, the inductance L may be defined in terms of the emf generated to oppose a given change in current: Faraday's lawemf.
PHYS219 Fall semester 2014 Lecture 16: AC Circuits with Inductors and Capacitors Dimitrios Giannios Purdue University.
Chapter 22: Alternating Current
Electromagnetic Oscillations and Alternating Current
Electromagnetic Oscillations and Alternating Current
Alternating Current Electricity
5. Alternating Current Circuits
Electromagnetic Oscillations and Alternating Current
An AC voltage source drives a sinusoidal current through two resistors. The amplitude of the sinusoidal voltage across the top resistor is 4 V. The amplitude.
Time Domain to Phasor Domain (Linear Transformation)
Electromagnetic Oscillations and Alternating Current
AC CIRCUIT ANALYSIS Introduction SEE 1003 Section 08 Nik Din Muhamad.
Unless stated otherwise all AC voltage & current values are rms values
Chapter 33 Problems 3,10,17,21,22,26,32,33,37.
Presentation transcript:

See 7 RCL series a.c. circuit applet

Reactance is dependant on frequency ie By altering the frequency it is possible to reach the point at which V L = V C. At this stage, Z has its smallest value (so Z = R) and the current in the circuit will be a Maximum. The frequency when this occurs is called the resonant frequency f o. At resonance:

The 12V peak voltage supply has a variable frequency. Current readings are taken every 5 Hz giving a graph of I (A) vs f (Hz) The current peaks sharply at the resonant frequency of ~ 50 Hz. V S =12V (variable f) 2H 5μF5μF 500Ω A I (A) f (Hz) I max when X L - X C =0

1.Determine the resonant frequency for this circuit 2.Determine the reactance of the capacitor at this frequency 3.State the reactance of the inductor at this frequency 4.Explain, using phasors, why the circuit is at resonance 1.Determine the resonant frequency for this circuit 2.Determine the reactance of the capacitor at this frequency 3.State the reactance of the inductor at this frequency 4.Explain, using phasors, why the circuit is at resonance This LCR circuit has a 5.0 Ω resistor in series with a 250 µF capacitor and a 15 mH inductor. The AC supply is variable frequency and has a peak voltage of 6.0 V. 15 mH 250 µF 6 V variable frequency generator

1.Determine the resonant frequency for this circuit This LCR circuit has a 5.0 Ω resistor in series with a 250 µF capacitor and a 15 mH inductor. The AC supply is variable frequency and has a peak voltage of 6.0 V. LCR Circuits 15 mH 250 µF 6 V variable frequency generator At resonance X C = X L At resonance X C = X L

This LCR circuit has a 5.0 Ω resistor in series with a 250 µF capacitor and a 15 mH inductor. The AC supply is variable frequency and has a peak voltage of 6.0 V. LCR Circuits 15 mH 250 µF 6 V variable frequency generator 2.Determine the reactance of the capacitor at this frequency 3.State the reactance of the inductor at this frequency. X L = 7.7 Ω 4.Explain, using phasors, why the circuit is at resonance X L = 7.7 Ω X C = 7.7 Ω R = 5 Ω = At resonance |X C | = |X L | and the two vectors cancel