PHYS 1444 – Section 004 Lecture #21

Slides:



Advertisements
Similar presentations
We have been using voltage sources that send out a current in a single direction called direct current (dc). Current does not have to flow continuously.
Advertisements

Alternating Current Circuits
Alternating Current Circuits
Copyright © 2009 Pearson Education, Inc. Lecture 10 – AC Circuits.
3/31/2020USF Physics 1011 Physics 101 AC Circuits.
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.
Copyright © 2009 Pearson Education, Inc. Chapter 30 Inductance, Electromagnetic Oscillations, and AC Circuits.
Alternating Current Circuits
Thursday, Dec. 1, 2011PHYS , Fall 2011 Dr. Jaehoon Yu 1 PHYS 1444 – Section 003 Lecture #23 Thursday, Dec. 1, 2011 Dr. Jaehoon Yu LR circuit LC.
Monday, Apr. 9, 2012PHYS , Spring 2012 Dr. Jaehoon Yu 1 PHYS 1444 – Section 004 Lecture #18 Monday, April 9, 2012 Dr. Jaehoon Yu Induction of EMF.
Wendesday, Apr. 26, 2006PHYS , Spring 2006 Dr. Jaehoon Yu 1 PHYS 1444 – Section 003 Lecture #23 Wednesday, Apr. 26, 2006 Dr. Jaehoon Yu Phasor.
Monday, Apr. 24, 2006PHYS , Spring 2006 Dr. Jaehoon Yu 1 PHYS 1444 – Section 501 Lecture #22 Monday, Apr. 24, 2006 Dr. Jaehoon Yu AC Circuit w/
Wendesday, Nov. 23, 2005PHYS , Fall 2005 Dr. Jaehoon Yu 1 PHYS 1444 – Section 003 Lecture #22 Wednesday, Nov. 23, 2005 Dr. Jaehoon Yu Achievements.
Tuesday, Dec. 6, 2011PHYS , Fall 2011 Dr. Jaehoon Yu 1 PHYS 1444 – Section 003 Lecture #24 Tuesday, Dec. 6, 2011 Dr. Jaehoon Yu Achievements of.
Monday, Apr. 23, 2012PHYS , Spring 2012 Dr. Jaehoon Yu 1 PHYS 1444 – Section 004 Lecture #22 Monday, April 23, 2012 Dr. Jaehoon Yu Extension of.
Class 34 Today we will: learn about inductors and inductance
Wednesday, Apr. 18, 2012PHYS , Spring 2012 Dr. Jaehoon Yu 1 PHYS 1444 – Section 004 Lecture #21 Wednesday, April 18, 2012 Dr. Jaehoon Yu AC Circuit.
Tuesday, July 2, 2013PHYS , Summer 2013 Dr. Jaehoon Yu 1 PHYS 1442 – Section 001 Lecture #14 Tuesday, July 2, 2013 Dr. Jaehoon Yu Chapter 22 −Maxwell’s.
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 17 AC circuits RLC circuits Transformer Maxwell.
Copyright © 2009 Pearson Education, Inc. Chapter 33 Inductance, Electromagnetic Oscillations, and AC Circuits Part II.
Monday, July 1, 2013PHYS , Summer 2013 Dr. Jaehoon Yu 1 PHYS 1442 – Section 001 Lecture #13 Monday, July 1, 2013 Dr. Jaehoon Yu Chapter 21 -Mutual.
PHYS 1442 – Section 004 Lecture #16 Weednesday March 19, 2014 Dr. Andrew Brandt Chapter 22 Maxwell and the c.
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.
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.
Chapter 8 Alternating Current Circuits. AC Circuit An AC circuit consists of a combination of circuit elements and an AC generator or source An AC circuit.
Monday, Apr. 16, 2012PHYS , Spring 2012 Dr. Jaehoon Yu 1 PHYS 1444 – Section 004 Lecture #20 Monday, April 16, 2012 Dr. Jaehoon Yu Today’s homework.
Tuesday, April 26, PHYS Dr. Andrew Brandt PHYS 1444 – Section 02 Lecture #20 Tuesday April 26, 2011 Dr. Andrew Brandt AC Circuits Maxwell.
Monday, April 23, PHYS , Spring 2007 Dr. Andrew Brandt PHYS 1444 – Section 004 Lecture #19 Monday, April 23, 2007 Dr. Andrew Brandt Inductance.
Wednesday, Apr. 19, 2006PHYS , Spring 2006 Dr. Jaehoon Yu 1 PHYS 1444 – Section 501 Lecture #21 Wednesday, Apr. 19, 2006 Dr. Jaehoon Yu Energy.
Weds. November 30, PHYS , Dr. Andrew Brandt PHYS 1444 – Section 04 Lecture #23 Wednesday November 30, 2011 Dr. Andrew Brandt Last HW Dec.
Copyright R. Janow – Spring 2016 Physics Electricity and Magnetism Lecture 14 - AC Circuits, Resonance Y&F Chapter 31, Sec Phasor Diagrams.
Chapter 33 Alternating Current Circuits. Electrical appliances in the house use alternating current (AC) circuits. If an AC source applies an alternating.
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.
Chapter 13 The Basic Elements and Phasors. Objectives Be able to add and subtract sinusoidal voltages or currents Use phasor format to add and subtract.
PHYS 1441 – Section 001 Lecture #16
Levitation above a Superconductor
PHYS 1444 – Section 501 Lecture #15
PHYS 1444 – Section 004 Lecture #18
PHYS 1443 – Section 001 Lecture #19
Physics Electricity and Magnetism Lecture 14 - AC Circuits, Resonance Y&F Chapter 31, Sec Phasor Diagrams for Voltage and Current The Series.
PHYS 1444 – Section 501 Lecture #22
Inductance, Electromagnetic Oscillations, and AC Circuits
Alternating Current Electricity
PHYS 1444 – Section 003 Lecture #15
PHYS 1444 – Section 02 Lecture #19
Physics Electricity and Magnetism Lecture 14 - AC Circuits, Resonance Y&F Chapter 31, Sec Phasor Diagrams for Voltage and Current The Series.
Chapter 31 Electromagnetic Oscillations and 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.
CHAPTER 6 (BEE) AC Fundamentals
Make it simpler???.
PHYS 1444 – Section 003 Lecture #22
PHYS 1444 – Section 003 Lecture #21
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
PHYS 1441 – Section 001 Lecture #21
PHYS 1444 – Section 002 Lecture #15
PHYS 1444 – Section 501 Lecture #13
PHYS 1441 – Section 001 Lecture #23
PHYS 1441 – Section 001 Lecture #24
PHYS 1444 – Section 002 Lecture #15
PHYS 1444 – Section 003 Lecture #20
Physics Electricity and Magnetism Lecture 14 - AC Circuits, Resonance Y&F Chapter 31, Sec Phasor Diagrams for Voltage and Current The Series.
PHYS 1441 – Section 001 Lecture #22
Physics Electricity and Magnetism Lecture 14 - AC Circuits, Resonance Y&F Chapter 31, Sec Phasor Diagrams for Voltage and Current The Series.
Presentation transcript:

PHYS 1444 – Section 004 Lecture #21 Wednesday, April 18, 2012 Dr. Jaehoon Yu AC Circuit w/ Inductance only AC Circuit w/ Capacitance only LRC circuit Achievements of Maxwell’s Equations Wednesday, Apr. 18, 2012 PHYS 1444-004, Spring 2012 Dr. Jaehoon Yu

PHYS 1444-004, Spring 2012 Dr. Jaehoon Yu Announcements Your planetarium extra credit Please bring your planetarium extra credit sheet by the beginning of the class next Monday, Apr. 30 Be sure to tape one edge of the ticket stub with the title of the show on top Term exam #2 Non-comprehensive Date and time: 5:30 – 6:50pm, Wednesday, Apr. 25 Location: SH103 Coverage: CH. 27 – 1 to what we finish today (CH31.1?) Please do NOT miss the exam!! Evaluation Bring your electronic device with a web capability on Apr. 30. Reading Assignments CH30.9 – CH30.11 Wednesday, Apr. 18, 2012 PHYS 1444-004, Spring 2012 Dr. Jaehoon Yu

AC Circuit w/ Inductance only From Kirchhoff’s loop rule, we obtain Thus Using the identity where What does this mean? Current and voltage are “out of phase by π/2 or 90o”. In other words the current reaches its peak ¼ cycle after the voltage What happens to the energy? No energy is dissipated The average power is 0 at all times The energy is stored temporarily in the magnetic field Then released back to the source Wednesday, Apr. 18, 2012 PHYS 1444-004, Spring 2012 Dr. Jaehoon Yu

AC Circuit w/ Inductance only How are the resistor and inductor different in terms of energy? Inductor Resistor How are they the same? They both impede the flow of charge For a resistance R, the peak voltage and current are related to Similarly, for an inductor we may write Where XL is the inductive reactance of the inductor What do you think is the unit of the reactance? The relationship is not valid at a particular instance. Why not? Since V0 and I0 do not occur at the same time Stores the energy temporarily in the magnetic field and then releases it back to the emf source Does not store energy but transforms it to thermal energy, losing it to the environment 0 when ω=0. Ω Wednesday, Apr. 18, 2012 PHYS 1444-004, Spring 2012 Dr. Jaehoon Yu is valid!

PHYS 1444-004, Spring 2012 Dr. Jaehoon Yu Example 30 – 9 Reactance of a coil. A coil has a resistance R=1.00Ω and an inductance of 0.300H. Determine the current in the coil if (a) 120 V DC is applied to it; (b) 120 V AC (rms) at 60.0Hz is applied. Is there a reactance for DC? Nope. Why not? Since ω=0, So for DC power, the current is from Kirchhoff’s rule For an AC power with f =60Hz, the reactance is Since the resistance can be ignored compared to the reactance, the rms current is Wednesday, Apr. 18, 2012 PHYS 1444-004, Spring 2012 Dr. Jaehoon Yu

AC Circuit w/ Capacitance only What happens when a capacitor is connected to a DC power source? The capacitor quickly charges up. There is no steady current flow in the circuit Since the capacitor prevents the flow of the DC current What do you think will happen if it is connected to an AC power source? The current flows continuously. Why? When the AC power turns on, charge begins to flow one direction, charging up the plates When the direction of the power reverses, the charge flows in the opposite direction Wednesday, Apr. 18, 2012 PHYS 1444-004, Spring 2012 Dr. Jaehoon Yu

AC Circuit w/ Capacitance only From Kirchhoff’s loop rule, we obtain The current at any instance is The charge Q on the plate at any instance is Thus the voltage across the capacitor is Using the identity Where Wednesday, Apr. 18, 2012 PHYS 1444-004, Spring 2012 Dr. Jaehoon Yu

AC Circuit w/ Capacitance only So the voltage is What does this mean? Current and voltage are “out of phase by π/2 or 90o” but in this case, the voltage reaches its peak ¼ cycle after the current What happens to the energy? No energy is dissipated The average power is 0 at all times The energy is stored temporarily in the electric field Then released back to the source Applied voltage and the current in the capacitor can be written as Where the capacitive reactance XC is defined as Again, this relationship is only valid for rms quantities Infinite when ω=0. Wednesday, Apr. 18, 2012 PHYS 1444-004, Spring 2012 Dr. Jaehoon Yu

PHYS 1444-004, Spring 2012 Dr. Jaehoon Yu Example 30 – 10 Capacitor reactance. What are the peak and rms current in the circuit in the figure if C=1.0μF and Vrms=120V? Calculate for (a) f=60Hz, and then for (b) f=6.0x105Hz. The peak voltage is The capacitance reactance is Thus the peak current is The rms current is Wednesday, Apr. 18, 2012 PHYS 1444-004, Spring 2012 Dr. Jaehoon Yu

PHYS 1444-004, Spring 2012 Dr. Jaehoon Yu AC Circuit w/ LRC The voltage across each element is VR is in phase with the current VL leads the current by 90o VC lags the current by 90o From Kirchhoff’s loop rule V=VR+VL+VC However since they do not reach the peak voltage at the same time, the peak voltage of the source V0 will not equal VR0+VL0+VC0 The rms voltage also will not be the simple sum of the three Let’s try to find the total impedance, peak current I0 and the phase difference between I0 and V0. Wednesday, Apr. 18, 2012 PHYS 1444-004, Spring 2012 Dr. Jaehoon Yu

PHYS 1444-004, Spring 2012 Dr. Jaehoon Yu AC Circuit w/ LRC The current at any instance is the same at all point in the circuit The currents in each elements are in phase Why? Since the elements are in series How about the voltage? They are not in phase. The current at any given time is The analysis of LRC circuit is done using the “phasor” diagram in which arrows are drawn in an xy plane to represent the amplitude of each voltage, just like vectors The lengths of the arrows represent the magnitudes of the peak voltages across each element; VR0=I0R, VL0=I0XL and VC0=I0XC The angle of each arrow represents the phase of each voltage relative to the current, and the arrows rotate at the angular frequency ω to take into account the time dependence. The projection of each arrow on y axis represents voltage across each element at any given time Wednesday, Apr. 18, 2012 PHYS 1444-004, Spring 2012 Dr. Jaehoon Yu

PHYS 1444-004, Spring 2012 Dr. Jaehoon Yu Phasor Diagrams At t=0, I=0. Thus VR0=0, VL0=I0XL, VC0=I0XC At t=t, Thus, the voltages (y-projections) are +90o -90o Wednesday, Apr. 18, 2012 PHYS 1444-004, Spring 2012 Dr. Jaehoon Yu

PHYS 1444-004, Spring 2012 Dr. Jaehoon Yu AC Circuit w/ LRC Since the sum of the projections of the three vectors on the y axis is equal to the projection of their sum. The sum of the projections represents the instantaneous voltage across the whole circuit which is the source voltage So we can use the sum of all vectors as the representation of the peak source voltage V0. V0 forms an angle φ to VR0 and rotates together with the other vectors as a function of time, We determine the total impedance Z of the circuit defined by the relationship or From Pythagorean theorem, we obtain Thus the total impedance is Wednesday, Apr. 18, 2012 PHYS 1444-004, Spring 2012 Dr. Jaehoon Yu

PHYS 1444-004, Spring 2012 Dr. Jaehoon Yu AC Circuit w/ LRC The phase angle φ is or What is the power dissipated in the circuit? Which element dissipates the power? Only the resistor The average power is Since R=Zcosφ We obtain The factor cosφ is referred as the power factor of the circuit For a pure resistor, cosφ=1 and For a capacitor or inductor alone φ=-90o or +90o, so cosφ=0 and Wednesday, Apr. 18, 2012 PHYS 1444-004, Spring 2012 Dr. Jaehoon Yu

PHYS 1444-004, Spring 2012 Dr. Jaehoon Yu Maxwell’s Equations The development of EM theory by Oersted, Ampere and others was not done in terms of EM fields The idea of fields was introduced somewhat by Faraday Scottish physicist James C. Maxwell unified all the phenomena of electricity and magnetism in one theory with only four equations (Maxwell’s Equations) using the concept of fields This theory provided the prediction of EM waves As important as Newton’s law since it provides dynamics of electromagnetism This theory is also in agreement with Einstein’s special relativity The biggest achievement of 19th century electromagnetic theory is the prediction and experimental verifications that the electromagnetic waves can travel through the empty space What do you think this accomplishment did? Open a new world of communication It also yielded the prediction that the light is an EM wave Since all of Electromagnetism is contained in the four Maxwell’s equations, this is considered as one of the greatest achievements of human intellect Wednesday, Apr. 18, 2012 PHYS 1444-004, Spring 2012 Dr. Jaehoon Yu