BROCK UNIVERSITY. Physics 1P22/1P92. Mid-term Test 2: 19 March Solutions

Similar documents
BROCK UNIVERSITY. Name: Student #: Page 1 of 8

General Physics II (PHYS 104) Exam 2: March 21, 2002

104 Practice Exam 1-2/21/02

Physics 2135 Exam 2 October 18, 2016

Physics 2135 Exam 2 March 22, 2016

Physics 2401 Summer 2, 2008 Exam II

Physics 2135 Exam 2 October 20, 2015

Class 6. Capacitance and Capacitors. Physics 106. Winter Press CTRL-L to view as a slide show. Class 6. Physics 106.

Agenda for Today. Elements of Physics II. Capacitors Parallel-plate. Charging of capacitors

What does it mean for an object to be charged? What are charges? What is an atom?

Agenda for Today. Elements of Physics II. Capacitors Parallel-plate. Charging of capacitors

MasteringPhysics: Assignment Print View. Problem 30.50

Capacitance, Resistance, DC Circuits

Which one of the pipes emits sound with the lowest frequency? Which one of the pipes emits sound with the next lowest frequency?

1) Two lightbulbs, one rated 30 W at 120 V and another rated 40 W at 120 V, are arranged in two different circuits.

Phys102 Second Major-133 Zero Version Coordinator: A.A.Naqvi Tuesday, August 05, 2014 Page: 1

PHYS 2135 Exam II March 20, 2018

LAST Name (print) ALL WORK MUST BE SHOWN FOR THE FREE RESPONSE QUESTION IN ORDER TO RECEIVE FULL CREDIT.

Review. Multiple Choice Identify the letter of the choice that best completes the statement or answers the question.

Physics 24 Exam 2 March 18, 2014

Physics 2212 GJ Quiz #3 Solutions Fall I. (16 points) The electric potential in a certain region of space depends on position according to

Capacitors. HPP Activity 68v1. Charge Inside the Body A Close Look at Cell Membranes

P114 University of Rochester NAME S. Manly Spring 2010

Clicker Session Currents, DC Circuits

physics 4/7/2016 Chapter 31 Lecture Chapter 31 Fundamentals of Circuits Chapter 31 Preview a strategic approach THIRD EDITION

P202 Practice Exam 2 Spring 2004 Instructor: Prof. Sinova

Physics Circuits: Series

4 Electric circuits. Serial and parallel resistors V 3 V 2 V Serial connection of resistors:

Power lines. Why do birds sitting on a high-voltage power line survive?

ConcepTest PowerPoints

Chapter 21 Electric Current and Direct- Current Circuits

Chapter 19 Lecture Notes

Capacitance. A different kind of capacitor: Work must be done to charge a capacitor. Capacitors in circuits. Capacitor connected to a battery

Physics Investigation 10 Teacher Manual

Electric Charge and Electric field

The next two questions pertain to the situation described below. Consider a parallel plate capacitor with separation d:

EXPERIMENT 5A RC Circuits

AP Physics C. Electric Circuits III.C

Exam 1--PHYS 102--Spring 2013

General Physics (PHY 2140)

Version 001 CIRCUITS holland (1290) 1

PH 102 Exam I N N N N. 3. Which of the following is true for the electric force and not true for the gravitational force?

1. A1, B3 2. A1, B2 3. A3, B2 4. A2, B2 5. A3, B3 6. A1, B1 7. A2, B1 8. A2, B3 9. A3, B1

Series & Parallel Resistors 3/17/2015 1

Gurgaon TOPIC: ELECTROSTATIC Assignment 1 (2018)

Physics 212 Midterm 2 Form A

Ohm's Law and Resistance

shown in Fig. 4, is initially uncharged. How much energy is stored in the two capacitors after the switch S is closed for long time?

Insulators Non-metals are very good insulators; their electrons are very tightly bonded and cannot move.

Hollow Conductors. A point charge +Q is placed at the center of the conductors. The induced charges are: 1. Q(I1) = Q(I2) = -Q; Q(O1) = Q(O2)= +Q

De La Salle University Manila Physics Fundamentals for Engineering 2 Quiz No. 3 Reviewer

Lecture Outline Chapter 21. Physics, 4 th Edition James S. Walker. Copyright 2010 Pearson Education, Inc.

Physics 208, Spring 2016 Exam #2

Physics 6B. Practice Final Solutions

PHYSICS ASSIGNMENT ES/CE/MAG. Class XII

Series and Parallel. How we wire the world

WELCOME TO PERIOD 14. Homework Exercise #13 is due today. Watch video 3 Edison s Miracle of Light for class discussion next Tuesday or Wednesday.

ConcepTest PowerPoints

Physics Tutorial - Currents and Circuits

10/14/2018. Current. Current. QuickCheck 30.3

26 Capacitance and Dielectrics

Louisiana State University Physics 2102, Exam 2, March 5th, 2009.

Test Review Electricity

Physics 106 Sections 1 & 2 Midterm Exam #1 Fall 2011

Student ID Number. Part I. Lecture Multiple Choice (43 points total)

Physics 102 Spring 2007: Final Exam Multiple-Choice Questions

Capacitors GOAL. EQUIPMENT. CapacitorDecay.cmbl 1. Building a Capacitor

University of Maryland Department of Physics. Spring 2009 Final Exam 20. May (175 points) Post grades on web? (Initial, please) Yes No

General Physics (PHY 2140)

Tactics Box 23.1 Using Kirchhoff's Loop Law

Physics 22: Homework 4

LABORATORY 4 ELECTRIC CIRCUITS I. Objectives

ELECTRICITY. Electric Circuit. What do you already know about it? Do Smarty Demo 5/30/2010. Electric Current. Voltage? Resistance? Current?

CHAPTER 16,18,19 TEST REVIEW

Intermediate Physics PHYS102

Physics 126 Fall 2004 Practice Exam 1. Answer will be posted about Oct. 5.

= e = e 3 = = 4.98%

Circuits. PHY2054: Chapter 18 1

Physics 1502: Lecture 9 Today s Agenda

[1] (b) Fig. 1.1 shows a circuit consisting of a resistor and a capacitor of capacitance 4.5 μf. Fig. 1.1

Practice Exam 1. Necessary Constants and Equations: Electric force (Coulomb s Law): Electric field due to a point charge:

Basics of Network Theory (Part-I)

Direct-Current Circuits. Physics 231 Lecture 6-1

To receive full credit, you must show all your work (including steps taken, calculations, and formulas used).

Electric Charge. Electric Charge ( q ) unbalanced charges positive and negative charges. n Units Coulombs (C)

, where the sum is over all pairs of charges (q 1, q 2 ) that are

CHAPTER 20 ELECTRIC CIRCUITS

2/25/2014. Circuits. Properties of a Current. Conservation of Current. Definition of a Current A. I A > I B > I C B. I B > I A C. I C D. I A E.

Lecture #3. Review: Power

Review. Spring Semester /21/14. Physics for Scientists & Engineers 2 1

Physics 2220 Fall 2010 George Williams SECOND MIDTERM - REVIEW PROBLEMS

As we discussed in class, here are the key properties of the topographical map:

Lecture 7.1 : Current and Resistance

ENERGY AND TIME CONSTANTS IN RC CIRCUITS By: Iwana Loveu Student No Lab Section: 0003 Date: February 8, 2004

Phys222 W16 Exam 2: Chapters Key. Name:

PHYS 212 Final Exam (Old Material) Solutions - Practice Test

Capacitance: The ability to store separated charge C=Q/V. Capacitors! Capacitor. Capacitance Practice SPH4UW 24/08/2010 Q = CV

Physics 9 Monday, April 7, 2014

General Physics II Summer Session 2013 Review Ch - 16, 17, 18

Class 8. Resistivity and Resistance Circuits. Physics 106. Winter Press CTRL-L to view as a slide show. Class 8. Physics 106.

Transcription:

BROCK UNIVERSITY Physics 1P22/1P92 Mid-term Test 2: 19 March 2010 Solutions 1. [6 marks] (See Page 746, CP # 24, and pages 15 16 of the posted Ch. 22 lecture notes from 4 March.) A 3.0 V potential difference is applied between the ends of a nichrome wire of diameter 0.80 mm and length 50 cm. The resistivity of nichrome is 1.5 10 6 Ω m. Calculate the current in the wire. Solution: Strategy: First calculate the resistance of the wire, then use Ohm s law to determine the current. Step 1: R = ρl A = ρl πr 2 = 1.5 10 6 (0.5) π(4 10 3 ) 2 = 1.492078 Ω Using Ohm s law, the current through the wire is I = V R 3 = 1.492078 = 2.01 A Thus, the current through the wire is 2.0 A.

2. [6 marks] A parallel-plate capacitor is charged using a 10 V battery; then the battery is removed. A dielectric slab is then slid between the plates of the capacitor, filling all the space between the plates; this reduces the voltage difference between the plates to 4.0 V. Calculate the dielectric constant of the dielectric. S olution: This is very similar to Example 21.12 on Page 709 of the textbook. I ll solve it in a slightly different way than shown in the textbook (but check the textbook method to see which you prefer). The capacitance C 1 before the dielectric is inserted is increased to C 2 = κc 1 after the dielectric is inserted. Noting that Q = C V, and also noting that the charge on the plates is constant (because the battery is disconnected before the dielectric is inserted), we conclude that C 1 V 1 = C 2 V 2 Therefore, C 2 = V 1 C 1 V 2 But the ratio in the previous equation is the dielectric constant κ, so κ = C 2 C 1 = V 1 V 2 = 10 4.0 = 2.5 Thus, the dielectric constant of the dielectric is 2.5.

3. [6 marks] Calculate the equivalent resistance for the entire circuit. Solution: (This is part of CP # 60 on Page 785; see pages 17ff of the Ch 23 lecture notes.) The 8 Ω resistor is in parallel with the bottom 24 Ω resistor; their equivalent resistance is ( 1 R 1 = 8 + 1 ) 1 ( 3 = 24 24 + 1 ) 1 ( ) 1 4 = = 24 24 24 4 = 6 Ω This equivalent resistance R 1 is in series with the 6 Ω resistor, so their equivalent resistance is R 2 = R 1 + 6 = 6 + 6 = 12 Ω Equivalent resistance R 2 is in parallel with the 24 Ω resistance to the right, so the equivalent resistance of this combination is R 3 = ( 1 12 + 1 ) 1 ( 2 = 24 24 + 1 ) 1 ( ) 1 3 = = 24 24 24 3 = 8 Ω Equivalent resistance R 3 is in series with the 4 Ω resistance, so the final equivalent resistance of the entire circuit is R = R 3 + 4 = 8 + 4 = 12 Ω

4. [6 marks] Consider the figure, and suppose the battery s voltage is 10 V and each light bulb has resistance 10 Ω. (a) Calculate the current flowing through each light bulb. (b) Calculate the power dissipated by each light bulb. Solution: (This is somewhat like Page 780, CQ # 18.) First calculate the total equivalent resistance of the circuit, then calculate the total current flowing from the battery, then calculate the individual currents through each light bulb, and finally determine the power dissipated in each bulb. The equivalent resistance of the two light bulbs in parallel is ( 1 R 1 = 10 + 1 ) 1 = 5 Ω 10 Thus, the total equivalent resistance of the circuit is 10 + 5 = 15 Ω. This means that the total current from the battery is I = V R = 10 15 = 0.6667 A All of the current from the battery passes through light bulb A, so I A = 0.67 A. Therefore, the power dissipated by light bulb A is P A = I 2 AR = 0.6667 2 (10) = 4.4 W The voltage across light bulb A is V = I A R = 6.7 V. Therefore, the voltage across each of light bulbs B and C is 10 6.7 = 3.3 V. This means that the current through each of light bulbs B and C is I B = I C = V R = 3.3 10 = 0.33 A The power dissipated by each of the light bulbs B and C is P B = P C = I 2 BR = 1.1 W

5. [4 marks] Consider the same circuit as in Question 4 (the figure is reproduced here for your convenience). Suppose that an ideal wire is added to the circuit so that it connects points 1 and 2. Calculate the current flowing through each light bulb and through the new wire. Solution: All of the current from the battery flows through light bulb A and then through the additional wire that connects points 1 and 2. No current flows through light bulbs B and C, since they are both in parallel with the short-circuit wire that connects points 1 and 2. Thus, the equivalent resistance of the circuit is just the resistance of light bulb A, which is 10 Ω. Thus the current through light bulb A and the additional wire connecting points 1 and 2 is I = V R = 10 10 = 1 A The current through light bulbs B and C is 0 A.

6. [12 marks] Indicate whether each statement is TRUE or FALSE. Then provide a BRIEF explanation (i.e. one or two sentences). Your explanation may include formulas, if you wish. Remember, brevity and clarity are courtesy. (a) In a series circuit with one battery and several resistances, the electric potential energy of each electron decreases as it moves through the circuit outside the battery. TRUE FALSE EXPLANATION: There is only one pathway, so each electron passes through each resistance. As each electron passes through each resistance, its electric potential energy decreases, according to Ohm s law. (b) In a series circuit that contains a battery and two light-bulbs with equal resistance, the bulb closer to the negative side of the battery is brighter. This happens because some current is used up in the first light-bulb, so there is not as much left by the time it reaches the second light bulb. EXPLANATION: Current is not used up in a circuit; what is used up is electric potential energy (which is converted to thermal energy and perhaps light). The same current passes through each resistance in a series circuit; since each light bulb has the same resistance, each also has the same brightness. (c) When additional parallel branches are added to a parallel circuit, where each new branch has some resistance, the overall resistance of the circuit increases, and therefore the overall current flowing from the battery decreases. EXPLANATION: Adding more branches to a parallel circuit decreases the equivalent resistance of the circuit, therefore increasing the overall current flowing from the battery. (d) The light bulbs in the following circuit all have the same resistance, and therefore they all have the same brightness. EXPLANATION: This is a parallel circuit with two branches. The branch with bulbs B and C has greater resistance than the branch with bulb A, so more current flows through bulb A. Since P = I 2 R, bulb A is brighter than bulbs B and C. (e) A parallel-plate capacitor is fully charged by a 10 V battery, after which the battery is disconnected. The plates are then moved further apart using insulating handles. After the plates are moved, the capacitance of the capacitor decreases. TRUE FALSE

EXPLANATION: Since C = ɛ 0 A/d, when the plates are farther apart, the capacitance decreases. (f) A parallel-plate capacitor is fully charged by a 10 V battery, after which the battery is disconnected. The plates are then moved further apart using insulating handles. After the plates are moved, the voltage difference between the plates is still 10 V. EXPLANATION: The charge remains constant, but the capacitance decreases (as we learned in Part (e)). This means that the voltage must increase, because Q = C V. (Remember that voltage is a measure of electric potential energy per unit charge; the work done in moving the plates increases the potential energy, just as the gravitational potential energy would increase if you lifted a mass to a higher level in a gravitational field.)