Electric Circuits Assessment Problems

Slides:



Advertisements
Similar presentations
-Mutual Inductance -LC Circuit
Advertisements

Instrumentation (AMME2700) 1 Instrumentation Dr. Xiaofeng Wu.
1 Chapter 24--Examples. 2 Problem In the figure to the left, a potential difference of 20 V is applied across points a and b. a) What is charge on each.
DC CIRCUITS: CHAPTER 4.
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.
Ch 32 Inductance 32.1 Self Inductance L = N B /I  L = -L(dI/dt) Units: Tm 2 /A = Henry Solenoid P32.4 (p.916) P32.3 (p.916)
ECE 201 Circuit Theory I1 Inductance Inductor –A coil of wire wrapped around a supporting core (magnetic or non-magnetic) –The time-varying current in.
Circuit Elements Electric circuit is the interconnection of circuit elements ActivePassive Not capable of generating energy e.g. resistor, inductor, capacitor.
ECE 201 Circuit Theory I1 Capacitance Capacitance occurs whenever electrical conductors are separated by a dielectric, or insulating material. Applying.
Series-Parallel Combinations of Inductance and Capacitance
RL Circuits PH 203 Professor Lee Carkner Lecture 21.
CAPACITOR AND INDUCTOR
© 2012 Pearson Education, Inc. { Chapter 30 Inductance.
Lecture - 4 Inductance and capacitance equivalent circuits
Physics for Scientists and Engineers, 6e Chapter – 32 Inductance.
Fall 2008 Physics 121 Practice Problem Solutions 13 Electromagnetic Oscillations AC Circuits Contents: 121P13 - 2P, 3P, 9P, 33P, 34P, 36P, 49P, 51P, 60P,
© 2012 Pearson Education, Inc. { Chapter 31 Alternating Current Circuits (cont.)
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.
30. Inductance Self & Mutual Inductance Inductance: unit : H (henry)
Fluid flow analogy. Power and energy in an inductor.
Chapter 6. Capacitance and inductance
Inductance and Magnetic Energy Chapter 32 Mutual Inductance Self-Inductance Inductors in Circuits Magnetic Energy.
1 Chapter 6 Capacitors and Inductors 電路學 ( 一 ). 2 Capacitors and Inductors Chapter 6 6.1Capacitors 6.2Series and Parallel Capacitors 6.3Inductors 6.4Series.
Chapter 32 Inductance.
Chapter 14 Inductive Transients. 2 Transients Voltages and currents during a transitional interval –Referred to as transient behavior of the circuit Capacitive.
Fundamentals of Electric Circuit Analysis, by Clayton Paul Copyright 2000 © John Wiley & Sons. Inc. All rights reserved. Figure 5.1 A parallel-plate capacitor.
© 2012 Pearson Education, Inc. A current i flows through an inductor L in the direction from point b toward point a. There is zero resistance in the wires.
Chapter 32 Inductance. Self-inductance Some terminology first: Use emf and current when they are caused by batteries or other sources Use induced emf.
Chapter-23 Alternating Current Circuits. AC Circuits All the equipment in this operating room use alternating current circuits.
ECA1212 Introduction to Electrical & Electronics Engineering Chapter 3: Capacitors and Inductors by Muhazam Mustapha, October 2011.
Copyright © 2009 Pearson Education, Inc. Chapter 33 Inductance, Electromagnetic Oscillations, and AC Circuits Part II.
6.1 The Inductor Is a passive element ( can not generate energy) Represented graphically as a coiled wire Symbolized by the letter L Measured in henrys.
Unit 5: Day 9 – Energy Stored in a Magnetic Field of an Inductor Power delivered by an inductor Work done to increase the current in an inductor The energy.
Alexander-Sadiku Fundamentals of Electric Circuits
Chapter 30 Lecture 31: Faraday’s Law and Induction: II HW 10 (problems): 29.15, 29.36, 29.48, 29.54, 30.14, 30.34, 30.42, Due Friday, Dec. 4.
EKT 101 Electric Circuit Theory
7. Direct Current circuits. 11 Find the currents, which flow in all the wires of the circuit in this figure 12  9 V 6 V b a cd 18 
Alternating Current Circuits. AC Sources  : angular frequency of AC voltage  V max : the maximum output voltage of AC source.
PHYS 222 SI Exam Review 11/3/14. Answer: D Answer: D,D.
Response of First Order RL and RC
Announcements Midterm Exam next Wednesday Exam starts at 6 PM, ~1 hr. Closed book, one page of notes Bring a calculator (not phone, computer, iPad, etc.)
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.
Inductance Inductor A coil of wire wrapped around a supporting core (magnetic or non-magnetic) The time-varying current in the wire produces a time-varying.
Electric Circuits (EELE 2312)
Chapter 6. Capacitance and inductance
Capacitance Capacitance occurs whenever electrical conductors are separated by a dielectric, or insulating material. Applying a voltage to the conductors.
Inductance and Capacitance Response of First Order RL and RC
EKT 101 Electric Circuit Theory
Inductance, Electromagnetic Oscillations, and AC Circuits
EKT 101 Electric Circuit Theory
The Energy Storage Elements
site.iugaza.edu.ps/ajasser
EKT101 Electric Circuit Theory
ECE 3301 General Electrical Engineering
Capacitors and Inductors
Chapter 3 Inductance and Capacitance
Chapter 7 – Response of First Order RL and RC Circuits
Inductors in Series. Inductors in Series Therefore inductor combine like resistor.
6.1 The Inductor Is a passive element ( can not generate energy)
Capacitors 2 conducting plates separated by an insulator (or dielectric) Connect to a voltage source, stores +q and –q on plates: q = Cv C = capacitance.
Inductance Inductor A coil of wire wrapped around a supporting core (magnetic or non-magnetic) The time-varying current in the wire produces a time-varying.
Capacitors Devices used to store charge.
Capacitance Capacitance occurs whenever electrical conductors are separated by a dielectric, or insulating material. Applying a voltage to the conductors.
Electric Circuits Assessment Problems
6.1 The Inductor Is a passive element ( can not generate energy)
Electric Circuits I (EELE 2310)
Chapter 33 Problems 3,10,17,21,22,26,32,33,37.
Capacitance Capacitance occurs whenever electrical conductors are separated by a dielectric, or insulating material. Applying a voltage to the conductors.
DC CIRCUITS: CHAPTER 4.
Presentation transcript:

Electric Circuits Assessment Problems Chapter 6 Inductance, Capacitance, and Mutual Inductance

Ppt下載 140.125.35.23

6.1 The current source in the circuit shown generates the current pulse 𝑖 𝑔 𝑡 =0, 𝑡<0 𝑖 𝑔 𝑡 =8 𝑒 −300𝑡 −8 𝑒 −1200𝑡 𝐴, 𝑡≥0 Find (a) 𝑣(0); (b) the instant of time, greater than zero, when the voltage v passes through zero; (c) the expression for the power delivered to the inductor; (p.204)

(d). the instant when the power delivered to the (d) the instant when the power delivered to the inductor is maximum; (e) the maximum power; (f) the instant of time when the stored energy is maximum; (g) the maximum energy stored in the inductor.

6.1 Ans 𝑖 𝑔 𝑡 =8 𝑒 −300𝑡 −8 𝑒 −1200𝑡 𝐴 , 𝑡≥0 𝑣=𝐿 𝑑 𝑖 𝑔 𝑑𝑡 𝑖 𝑔 𝑡 =8 𝑒 −300𝑡 −8 𝑒 −1200𝑡 𝐴 , 𝑡≥0 𝑣=𝐿 𝑑 𝑖 𝑔 𝑑𝑡 =4𝑚 [ −300∙8 𝑒 −300𝑡 −(−1200∙8 𝑒 −1200𝑡 )] = −9.6 𝑒 −300𝑡 + 38.4 𝑒 −1200𝑡 𝑉 𝑣 0 + =−9.6+38.4 =28.8𝑉

6.1 Ans (b) −9.6 𝑒 −300𝑡 + 38.4 𝑒 −1200𝑡 =0 38.4 𝑒 −1200𝑡 =9.6 𝑒 −300𝑡 38.4 9.6 = 𝑒 −300𝑡 𝑒 −1200𝑡 𝑒 900𝑡 =4 ln 𝑒 900𝑡 = ln 4 𝑡= ln 4 900 =1.54𝑚𝑠

6.1 Ans (c) 𝑣 𝑡 =−9.6 𝑒 −300𝑡 + 38.4 𝑒 −1200𝑡 𝑖 𝑔 𝑡 =8 𝑒 −300𝑡 −8 𝑒 −1200𝑡 𝑝=𝑣𝑖 = −9.6 𝑒 −300𝑡 ∙38.4 𝑒 −1200𝑡 ∙ 8 𝑒 −300𝑡 −8 𝑒 −1200𝑡 = −76.8 𝑒 −600𝑡 +76.8 𝑒 −1500𝑡 +307.2 𝑒 −1500𝑡 −307.2 𝑒 −2400𝑡 =384 𝑒 −1500𝑡 −76.8 𝑒 −600𝑡 −307.2 𝑒 −2400𝑡

6.1 Ans (d) 𝑑 𝑑𝑡 384 𝑒 −1500𝑡 −76.8 𝑒 −600𝑡 −307.2 𝑒 −2400𝑡 =0 2𝑒 1800𝑡 −25 𝑒 900𝑡 +32=0 令𝑥= 𝑒 900𝑡 , 2 𝑥 2 −25𝑥+32=0 𝑥1=1.44766, 𝑥2=11.05234 𝑡1= ln⁡(1.44766) 900 =411.054𝑢𝑠 →𝑝 𝑡1 =32.719W 𝑡2= ln⁡(11.05234) 900 =2.6696𝑚𝑠 →𝑝 𝑡2 =−8.983W

6.1 Ans (e) 𝑡 𝑝𝑚𝑎𝑥 =2.6696𝑚𝑠 𝑝 𝑚𝑎𝑥 =𝑝 𝑡 𝑝𝑚𝑎𝑥 𝑝 𝑚𝑎𝑥 =𝑝 𝑡 𝑝𝑚𝑎𝑥 =384 𝑒 −1500∙411.054𝑢 −76.8 𝑒 −600∙411.054𝑢 −307.2 𝑒 −2400∙411.054𝑢 =32.72𝑊

6.1 Ans (f) 𝑊 is max when 𝑖 is max, 𝑖 is max when 𝑑𝑖 𝑑𝑡 is zero. When 𝑑𝑖 𝑑𝑡 =0,v=0,therefore t=1.54ms (g) 𝑖 𝑚𝑎𝑥 =8 𝑒 −300∙1.54𝑚 −8 𝑒 −1200∙1.54𝑚 =3.78𝐴 𝑊 𝑚𝑎𝑥 = 1 2 𝐿 𝑖 𝑚𝑎𝑥 2 = 1 2 ∙4𝑚∙ 3.78 2 =28.6𝑚𝐽

6. 2 The voltage at the terminals of the 0 6.2 The voltage at the terminals of the 0.6𝑢F capacitor shown in the figure is 0 for t<0 and 40 𝑒 −15000𝑡 sin30000t V for t>0. Find (a) 𝑖 0 ; (b) the power delivered to the capacitor at 𝑡= 𝜋 80 ms (c) the energy stored in the capacitor at 𝑡= 𝜋 80 ms 0.6𝑢𝐹 𝑣 𝑖 − + (p.208)

6.2 Ans 𝑖=C 𝑑𝑣 𝑑𝑡 =24𝑢 𝑑 𝑑𝑡 𝑒 −15000𝑡 𝑠𝑖𝑛30000𝑡 =24𝑢 −15000 𝑒 −15000𝑡 𝑠𝑖𝑛30000𝑡+30000 𝑒 −15000𝑡 𝑐𝑜𝑠30000𝑡 =[0.72𝑐𝑜𝑠30000𝑡−0.36𝑠𝑖𝑛30000𝑡] 𝑒 −15000𝑡 𝑖 0 =0.72 𝐴

6.2 Ans (b) 𝑖 𝜋 80 = [0.72𝑐𝑜𝑠30000 𝜋 80 −0.36𝑠𝑖𝑛30000 𝜋 80 ] 𝑒 −15000 𝜋 80 =−31.66𝑚𝐴 𝑣 𝜋 80 = 40 𝑒 −15000 𝜋 80 sin30000 𝜋 80 =20.505 𝑉 𝑝=𝑖𝑣=−649.23𝑚𝑊

6.2 Ans (c) 𝑊 𝜋 80 = 1 2 𝐶 𝑣 𝜋 80 2 = 1 2 ∙0.6𝑢∙ 20.505 2 =126.137𝑢𝐽

6. 3 The current in the capacitor of assessment problem 6 6.3 The current in the capacitor of assessment problem 6.2 is 0 for t<0 and 3 cos 50000𝑡 𝐴 for t≥0. Find (a) 𝑣(𝑡) (b) the maximum power delivered to the capacitor at any one instant of time (c) the maximum energy stored in the capacitor at any one instant of time. (p.208)

6.3 Ans 𝑣= 1 𝐶 0 𝑡 𝑖 𝑑𝑥 = 1 0.6𝑢 0 𝑡 3 cos 50000𝑥 𝑑𝑥 =100𝑠𝑖𝑛50000𝑡 𝑉, 𝑡≥0

6.3 Ans (b) 𝑝 𝑡 =𝑣𝑖= 100𝑠𝑖𝑛50000𝑡 ∙3 cos 50000𝑡 =150𝑠𝑖𝑛100000t W 𝑝 𝑚𝑎𝑥 =150𝑊 (c) 𝑤 𝑚𝑎𝑥 = 1 2 𝐶 𝑣 𝑚𝑎𝑥 2 = 1 2 ∙6𝑢∙ 100 2 =3𝑚𝐽

6.3 Ans (c) 𝑊 𝜋 80 = 1 2 𝐶 𝑣 𝜋 80 2 = 1 2 ∙0.6𝑢∙ 20.505 2 =126.137𝑢𝐽