Prof. Anchordoqui. Problems set # 4 Physics 169 March 3, 2015

Similar documents
ragsdale (zdr82) HW2 ditmire (58335) 1

Physics 2135 Exam 1 February 14, 2017

Lecture 13 - Linking E, ϕ, and ρ

Physics 9 Fall 2011 Homework 2 - Solutions Friday September 2, 2011

Physics Jonathan Dowling. Lecture 9 FIRST MIDTERM REVIEW

Problems for HW X. C. Gwinn. November 30, 2009

200 points 5 Problems on 4 Pages and 20 Multiple Choice/Short Answer Questions on 5 pages 1 hour, 48 minutes

Physics 121 Sample Common Exam 1 NOTE: ANSWERS ARE ON PAGE 8. Instructions:

Exam 1 Solutions (1) C, D, A, B (2) C, A, D, B (3) C, B, D, A (4) A, C, D, B (5) D, C, A, B

west (mrw3223) HW 24 lyle (16001) 1

Physics 24 Exam 1 February 18, 2014

Physics 241 Exam 1 February 19, 2004

Physics 3323, Fall 2016 Problem Set 7 due Oct 14, 2016

- 5 - TEST 2. This test is on the final sections of this session's syllabus and. should be attempted by all students.

Candidates must show on each answer book the type of calculator used.

CAPACITORS AND DIELECTRICS

Homework Assignment 3 Solution Set

Physics 1402: Lecture 7 Today s Agenda

Quantum Mechanics Qualifying Exam - August 2016 Notes and Instructions

Version 001 Exam 1 shih (57480) 1

Sample Exam 5 - Skip Problems 1-3

JURONG JUNIOR COLLEGE

This final is a three hour open book, open notes exam. Do all four problems.

5.2 Volumes: Disks and Washers

Electric Potential. Concepts and Principles. An Alternative Approach. A Gravitational Analogy

IMPORTANT. Read these directions carefully:

In-Class Problems 2 and 3: Projectile Motion Solutions. In-Class Problem 2: Throwing a Stone Down a Hill

Instructor(s): Acosta/Woodard PHYSICS DEPARTMENT PHY 2049, Fall 2015 Midterm 1 September 29, 2015

Physics Graduate Prelim exam

Jackson 2.26 Homework Problem Solution Dr. Christopher S. Baird University of Massachusetts Lowell

Phys 4321 Final Exam December 14, 2009

Reading from Young & Freedman: For this topic, read the introduction to chapter 24 and sections 24.1 to 24.5.

Conducting Ellipsoid and Circular Disk

AP Physics C: Electricity & Magnetism 1999 Free-Response Questions

PH2200 Practice Exam I Summer 2003

Name Solutions to Test 3 November 8, 2017

#6A&B Magnetic Field Mapping

APPLICATIONS OF THE DEFINITE INTEGRAL

Theoretische Physik 2: Elektrodynamik (Prof. A.-S. Smith) Home assignment 4

Homework Assignment 5 Solution Set

Method of Localisation and Controlled Ejection of Swarms of Likely Charged Particles

The Velocity Factor of an Insulated Two-Wire Transmission Line

Math 8 Winter 2015 Applications of Integration

Today in Physics 122: work, energy and potential in electrostatics

Math 120 Answers for Homework 13

Chapter 6 Electrostatic Boundary Value Problems. Dr. Talal Skaik

13.4 Work done by Constant Forces

DIRECT CURRENT CIRCUITS

Test , 8.2, 8.4 (density only), 8.5 (work only), 9.1, 9.2 and 9.3 related test 1 material and material from prior classes

7.1 Integral as Net Change and 7.2 Areas in the Plane Calculus

Density of Energy Stored in the Electric Field

Mathematics for Physicists and Astronomers

Week 10: Line Integrals

Jackson 2.7 Homework Problem Solution Dr. Christopher S. Baird University of Massachusetts Lowell

Electromagnetism Answers to Problem Set 10 Spring 2006

That reminds me must download the test prep HW. adapted from (nz118.jpg)

Problem 1. Solution: a) The coordinate of a point on the disc is given by r r cos,sin,0. The potential at P is then given by. r z 2 rcos 2 rsin 2

Summary: Method of Separation of Variables

Lecture 1: Electrostatic Fields

The Wave Equation I. MA 436 Kurt Bryan

Math 0230 Calculus 2 Lectures

University of Alabama Department of Physics and Astronomy. PH126: Exam 1

Phys 6321 Final Exam - Solutions May 3, 2013

Goals: Determine how to calculate the area described by a function. Define the definite integral. Explore the relationship between the definite

Mathematics of Motion II Projectiles

Solutions to Physics: Principles with Applications, 5/E, Giancoli Chapter 16 CHAPTER 16

HIGHER SCHOOL CERTIFICATE EXAMINATION MATHEMATICS 4 UNIT (ADDITIONAL) Time allowed Three hours (Plus 5 minutes reading time)

chapter Figure 24.1 Field lines representing a uniform electric field penetrating a plane of area A perpendicular to the field. 24.

Problem Set 3 Solutions

University of Washington Department of Chemistry Chemistry 453 Winter Quarter 2010 Homework Assignment 4; Due at 5p.m. on 2/01/10

Math 1102: Calculus I (Math/Sci majors) MWF 3pm, Fulton Hall 230 Homework 2 solutions

Math 113 Exam 2 Practice

1 Which of the following summarises the change in wave characteristics on going from infra-red to ultraviolet in the electromagnetic spectrum?

Strategy: Use the Gibbs phase rule (Equation 5.3). How many components are present?

The area under the graph of f and above the x-axis between a and b is denoted by. f(x) dx. π O

BME 207 Introduction to Biomechanics Spring 2018

Chapter 0. What is the Lebesgue integral about?

Energy creation in a moving solenoid? Abstract

7.6 The Use of Definite Integrals in Physics and Engineering

7.2 The Definite Integral

Electricity and Magnetism

The Properties of Stars

F is on a moving charged particle. F = 0, if B v. (sin " = 0)

Improper Integrals, and Differential Equations

A REVIEW OF CALCULUS CONCEPTS FOR JDEP 384H. Thomas Shores Department of Mathematics University of Nebraska Spring 2007

Chapter 7 Steady Magnetic Field. september 2016 Microwave Laboratory Sogang University

l 2 p2 n 4n 2, the total surface area of the

Key for Chem 130 Second Exam

a < a+ x < a+2 x < < a+n x = b, n A i n f(x i ) x. i=1 i=1


Physics Honors. Final Exam Review Free Response Problems

Space Curves. Recall the parametric equations of a curve in xy-plane and compare them with parametric equations of a curve in space.

Math 32B Discussion Session Session 7 Notes August 28, 2018

Practice Problem Set 3

Reference. Vector Analysis Chapter 2

REVIEW SHEET FOR PRE-CALCULUS MIDTERM

7.1 Integral as Net Change Calculus. What is the total distance traveled? What is the total displacement?

Improper Integrals. Type I Improper Integrals How do we evaluate an integral such as

TImath.com Algebra 2. Constructing an Ellipse

Physics 2135 Exam 3 April 21, 2015

Transcription:

Prof. Anchordoui Problems set # 4 Physics 169 Mrch 3, 15 1. (i) Eight eul chrges re locted t corners of cube of side s, s shown in Fig. 1. Find electric potentil t one corner, tking zero potentil to be infinitely fr wy. (ii) Four point chrges re fixed t corners of sure centered t origin, s shown in Fig. 1. The length of ech side of sure is. The chrges re locted s follows: is t (, ), is t (, ), 3 is t (, ), nd 6 is t (, ). A fifth prticle tht hs mss m nd chrge is plced t origin nd relesed from rest. Find its speed when it is very fr from origin.. Five identicl point chrges re rrnged in two different mnners s shown in Fig. : in once cse s fce-centered sure, in or s regulr pentgon. Find potentil energy of ech system of chrges, tking zero of potentil energy to be infinitely fr wy. Express your nswer in terms of constnt times energy of two chrges seprted by distnce. 3. Consider system of two chrges shown in Fig. 3. Find electric potentil t n rbitrry point on x xis nd mke plot of electric potentil s function of x/. 4. A point prticle tht hs chrge of 11.1 nc is t origin. (i) Wht is (re) shpes of euipotentil surfces in region round this chrge? (ii) Assuming potentil to be zero t r =, clculte rdii of five surfces tht hve potentils eul to. V, 4. V, 6. V, 8. V nd 1. V, nd sketch m to scle centered on chrge. (iii) Are se surfces eully spced? Explin your nswer. (iv) Estimte electric field strength between 4.-V nd 6.-V euipotentil surfces by dividing difference between two potentils by difference between two rdii. Compre this estimte to exct vlue t loction midwy between se two surfces. 5. Two coxil conducting cylindricl shells hve eul nd opposite chrges. The inner shell hs chrge nd n outer rdius, nd outer shell hs chrge nd n inner rdius b. The length of ech cylindricl shell is L, nd L is very long compred with b. Find potentil difference, V V b between shells. 6. An electric potentil V (z) is described by function V m 1 z 4 V, z >. m, 1. m < z <. m V (z) = 3 V 3 V m 3 z 3, m < z < 1. m 3 V 3 V m 3 z 3, 1. m < z < m,. m < z < 1. m V m 1 z 4 V, z <. m The grph in Fig. 4 shows vrition of n electric potentil V (z) s function of z. (i) Give electric field vector E for ech of six regions. (ii) Mke plot of z-component of electric field, E z, s function of z. Mke sure you lbel xes to indicte numeric mgnitude of field. (iii) Qulittively describe distribution of chrges tht gives rise to this potentil lndscpe nd hence electric fields you clculted. Tht is, where re chrges, wht sign re y, wht shpe re y (plne, slb...)?

7. Two conducting, concentric spheres hve rdii nd b. The outer sphere is given chrge Q. Wht is chrge on inner sphere if it is erd?. 8. Consider two nested, sphericl conducting shells. The first hs inner rdius nd outer rdius b. The second hs inner rdius c nd outer rdius d. The system is shown in Fig. 5. In following four situtions, determine totl chrge on ech of fces of conducting spheres (inner nd outer for ech), s well s electric field nd potentil everywhere in spce (s function of distnce r from center of sphericl shells). In ll cses shells begin unchrged, nd chrge is n instntly introduced somewhere. (i) Both shells re not connected to ny or conductors (floting) tht is, ir net chrge will remin fixed. A positive chrge Q is introduced into center of inner sphericl shell. Tke zero of potentil to be t infinity. (ii) The inner shell is not connected to ground (floting) but outer shell is grounded tht is, it is fixed t V = nd hs whtever chrge is necessry on it to mintin this potentil. A negtive chrge Q is introduced into center of inner sphericl shell. (iii) The inner shell is grounded but outer shell is floting. A positive chrge Q is introduced into center of inner sphericl shell. (iv) Finlly, outer shell is grounded nd inner shell is floting. This time positive chrge Q is introduced into region in between two shells. In this cse uestion Wht re E(r) nd V (r)? cnnot be nswered nlyticlly in some regions of spce. In regions where se uestions cn be nswered nlyticlly, give nswers. In regions where y cnnot be nswered nlyticlly, explin why, but try to drw wht you think electric field should look like nd give s much informtion bout potentil s possible. 9. The hydrogen tom in its ground stte cn be modeled s positive point chrge of mgnitude e ( proton) surrounded by negtive chrge distribution tht hs chrge density ( electron) tht vries with distnce from center of proton r s: ρ(r) = ρ e r/ ( result obtined from untum mechnics), where =.53 nm is most probble distnce of electron from proton. (i) Clculte vlue of ρ needed for hydrogen tom to be neutrl. (ii) Clculte electrosttic potentil (reltive to infinity) of this system s function of distnce r from proton. 1. A prticle tht hs mss m nd positive chrge is constrined to move long x-xis. At x = L nd x = L re two ring chrges of rdius L. Ech ring is centered on x-xis nd lies in plne perpendiculr to it. Ech ring hs totl positive chrge Q uniformly distributed on it. (i) Obtin n expression for potentil V (x) on x xis due to chrge on rings. (ii) Show tht V (x) hs minimum t x =. (iii) Show tht for x << L, potentil pproches form V (x) = V () αx. (iv) Use result of Prt (iii) to derive n expression for ngulr freuency of oscilltion of mss m if it is displced slightly from origin nd relesed. (Assume potentil euls zero t points fr from rings.)

ving L. A perugh negred )zk. Q is n if. C. C. C. C 4. m 4. m 69. Eight point chrges, ech of mgnitude, re locted on. C. C. C. C corners of cube of edge s, s shown in Figure P3.69. 4. m () Determine x, y, nd z components of resultnt 4. m force exerted by or chrges on chrge locted 3. mj t point A. (b) Wht re mgnitude nd direction of this resultnt force? 69 [SSM] Four point chrges re fixed t corners of sure centered t origin. The length of ech side of sure is. The chrges re locted s follows: is t (, ), is t (, ), 3 is t (, ), nd 6 z is t (, ). A fifth prticle tht hs mss m nd chrge is plced t origin nd relesed from rest. Find its speed when it is very fr from origin. Picture Problem y The digrm shows four point chrges fixed t corners of sure nd fifth chrged prticle Pointtht is relesed from m, rest t Aorigin. We cn use s conservtion of energy to relte s initil potentil energy of prticle to y its kinetic energy when it is t gret s distnce from origin nd x 6 electrosttic potentil t origin to express Ui. 69 nd 7. Figure P3.69 Problems Figure 1: Problem 1. K U Use conservtion of energy to relte 7. Consider chrge distribution shownenergy in Figure initil potentil of P3.69. or, becuse Ki = Uf =, () Show tht mgnitude electric prticle toof its kinetic energyfield whentit K f U i center of ny fce of is cube hs vlue of.18k e /s. t gret distnce from origin: (b) Wht is direction of electric field t center of top fce of cube? U V Express initil potentil energy C is d of ced nduion. prt e. fricd t De- point chrges re rrnged in two differe sure, in or s regulr pentgon. Fi e zero of potentil energy to be infinitely fr e energy of two chrges seprted by dis chrged prticle # is 71. Review problem. A negtively of prticle to its chrge nd plced t center of uniformly chrged ring, where electrosttic potentil t origin: ring hs totl positive chrge Q s shown in Exmple 3.8. The prticle, confined to for move long x xis, is Ui to obtin: Substitute Kf nd displced smll distnce x long xis (where x '' ) nd relesed. Show tht prticle oscilltes in simple hrmonic motion with freuency given by f$ 1 ( " ke Q m 3 x 3 i 1 mv V v V m # 1/ 7. A line of chrge with uniform density 35. nc/m lies long line y $ # 15. cm, between points with coordintes x $ nd x $ 4. cm. Find electric field it cretes t origin. 73. Review problem. An electric dipole in uniform electric field is displced slightly from its euilibrium position, s shown in Figure P3.73, where! is smll. The seprtion of chrges is, nd moment of inerti of dipole is I. Assuming dipole is relesed from this Figure : Problem. erposition, we know tht potentil energy of

tric Potentil Due to System of Two Chrges MASSACHUSETTS INSTITUTE OF TECHNOLOGY Deprtment of Physics system of two chrges shown in Figure 3.8.1. Exm Prctice Problems Prt 1 Solutions Problem 1 Electric Field nd Chrge Distributions from Electric Potentil An electric potentil V ( z ) is described by function )(!V "m -1 )z 4V ; z >. m ; 1. m < z <. m 3 V! # 3 V & $ % "m-3 ' ( z3 ; m < z < 1. m V (z) = * 3 V # 3 V & $ % "m-3 ' ( z3 ;!1. m < z < m Figure ; 3:! The. m electric < z < dipole!1. mof problem 3.,(V "m -1 )z 4V ; z <!. m Figure 3.8.1 Electric dipole The grph below shows vrition of n electric potentil V ( z ) s function of z. lectric potentil t n rbitrry point on x xis nd mke plot. ric potentil cn be found by superposition principle. At poi ve V( x) 1 1 ( ) 1 1 4 x 4 x 4 x x expression my be rewritten s ) Give electric field vector E! for ech of six regions in (i) to (vi) below? V( x) =!" V 1 1 V x/ 1 x / 1 Solution: We shll fct tht E!!. Since electric potentil only depends on vrible z, we hve tht z -component of electric field is given by Figure 4: Problem 6. dv

Figure 5: The Frdy cge of problem 8.