The Ratio of Charge to Mass (e/m) for an Electron

Size: px
Start display at page:

Download "The Ratio of Charge to Mass (e/m) for an Electron"

Transcription

1 The Ratio of Charge to Mass (e/m) for an Electron OBJECT: The object of this experiment is to determine the ratio of charge to mass (e/m) for an electron and compare it with its theoretical value. THEORY: When an electron moves with speed v perpendicular to a magnetic field of intensity B, a magnetic force F acts on the electron. The magnitude of this force is given by Where; e is the charge of an electron and v is the speed of electron F = B e v (1) The direction of this force is perpendicular to the direction of magnetic field and to the direction of motion of the electron. Since the magnetic force acting on the electron is always perpendicular the electron s direction of the motion, the electron will travel in a circular path of radius r. The centripetal force required to keep the electron moving in a circular path is supplied by the magnetic force acting on it. The expression for the required centripetal force is m v F = r () where; m is the mass of electron and r is the radius of electron s path. Equating equations (1) and () yields m v r = B e v (3) If we solve the Eq. (3) for the ratio of electronic charge to mass (e/m) we obtain e = m v B r (4) The velocity of the electron is yet known, but it can be found as follows. When an electron is accelerated through a potential difference V a (anode potential), the gain in its kinetic energy is equal to work done on the electron by the electric field. This work W is equal to V a e. Thus 1 W = V a e = mv (5) 1

2 Solving Eq. (5) for v yields v = V e/m a (6) Substituting Eq.(6) into Eq.(4) and solving for (e/m) one obtains e V = a m B r (7) Final equation will be used to find the experimental value for the ratio (e/m) for an electron in terms of the accelerating anode potential V a, the magnetic intensity B, and radius r of the circular path of the electron. EXPERIMENTAL DETERMINATION OF THE RATIO e/m FOR AN ELECTRON a) Calculation of B : The Helmholtz arrangement for the production of homogeonus magnetic field is characterized in that two indiviual circular conductors of equal radius the centers of which are in the common axis and have a distances equal to the radius of the conductors carry same current. The magnetic induction of B in the central region of such a Helmholtz- coil system may be calculated from the mean radius of the coils R (0,068 m), the number of turns n (30) of one coil and the current I B (A), µ n 0 B = IB R Volt sec m ( Tesla = ) (8) where µ 0=1.56*10-6 (Volt sec/a.m.). To calculate the magnetic field intensity,the current I B (flowing through both coils) must be introduced; it is assumed that the current in both coils equal. It is noted that the start of each coil is connected to the four 4 mm socket (A) on the side of the bobbin, and the finish to the 4 mm socket (Z). For a normal connected series Helmholtz arrangement, the power supply should be connected to sockets (A), with sockets Z interconnected.

3 Experimental set-up: Connect the deflection tube in to the circuit shown below, with both deflecting plates at anode potential; Switch on and observe the path of undeflected beam. Figure 1 Specification: Maximum filament voltage is 7.5 V Anode voltage V Typical operation V Anode current 1 ma Procedure: 1. Energise the Helmholtz coil and observe, with reference to the screen that a. the radius (r) decreases with the increase coil current I B at fixed V a values, b. the radius (r) increase with increase in anode potential V a, indicating a higher electron beam velocity, with fixed I B Explain the reasons of above observations.. At different fixed values of V a,calculate the value of B as a function of the coil current I B using Eq.(8) and measure each corresponding radius (r). Determine the value of (e/m) by plotting the graph of 1/r versus B /V a (see Eq.7). The slope of the graph gives (e/m) wheree V a is fixed. 3. Repeat the previous calculations by, this time, plotting V a against the B r for various anode potentials at fixed B value. The slope of the graph gives (e/m). Compare the previous and present obtained (e/m) values. 4. Calculate the theoretical value of ratio (e/m) for an electron by dividing the theoretical value of its mass. 5. Determine the percentagee error in your experimental result by comparing the obtained experimental value of (e/m) with its theoretical value, and list the possible errorr sources. 3

4 Questions: 1. What is the reason behind the experimental determination of (e/m) value?. If the earth s magnetic field were used to deflect an electron beam, calculate the smallest possible diameter of the required tube. Assume that the accelarating potential difference is the same as that used here. 3. Could the coil power be an AC source? Explain your answer in detail. 4. What experimental differences, if any, would result if the tube produced a beam of protons rather than electrons? Prelab Questions 1. Who discovered the electron and when?. What is the electron? (charge, mass. etc) 3. What is the proton and neutron? (charge, mass etc) 4. What is the magnetic field? How can electron move in magnetic field? Is electron energy change with applied magnetic field? 5. What is the world s magnetic field? 6. What is the electric field? How can electron move in electric field? Is electron energy change with applied electric field? 7. How can you produce homogeneous magnetic field? 4

5 ATTENTION!!! You have to solve pre-lab questions before the experiment. You should visit web sites belows for other resources; (Turkish) For calculations, you need to use least square fitting method to obtain the (e/m) slope. You may find useful informations on following webpages or you can use Exprimental Physics(EP 371) lecture notes. Res.Assist Ebru BAKIR Res.Assist Haydar MUTAF 5

Experiment 1 1. Charge- to- Mass Ratio of the Electron Physics 2150 Experiment No. 1 University of Colorado

Experiment 1 1. Charge- to- Mass Ratio of the Electron Physics 2150 Experiment No. 1 University of Colorado Experiment 1 1 Introduction Charge- to- Mass Ratio of the Electron Physics 2150 Experiment No. 1 University of Colorado Both the charge and the mass of the electron are fundamental constants of considerable

More information

Ratio of Charge to Mass for the Electron

Ratio of Charge to Mass for the Electron Ratio of Charge to Mass for the Electron For a positive charge moving in a uniform magnetic field B with velocity v, the force F on the charge is always perpendicular to the magnetic field and the velocity.

More information

Laboratory 14: Ratio of Charge to Mass for the Electron

Laboratory 14: Ratio of Charge to Mass for the Electron Laboratory 14: Ratio of Charge to Mass for the Electron Introduction The discovery of the electron as a discrete particle of electricity is generally credited to the British physicist Sir J. J. Thomson

More information

EXPERIMENT 2-6. e/m OF THE ELECTRON GENERAL DISCUSSION

EXPERIMENT 2-6. e/m OF THE ELECTRON GENERAL DISCUSSION Columbia Physics: Lab -6 (ver. 10) 1 EXPERMENT -6 e/m OF THE ELECTRON GENERAL DSCUSSON The "discovery" of the electron by J. J. Thomson in 1897 refers to the experiment in which it was shown that "cathode

More information

Pre Lab for Ratio of Mass to. Charge of an Electron

Pre Lab for Ratio of Mass to. Charge of an Electron Pre Lab for Ratio of Mass to Charge of an Electron The direction of the magnetic force on a charged particle moving in the magnetic field is given by the right hand rule. Students need practice using the

More information

CHARGE TO MASS RATIO FOR THE ELECTRON

CHARGE TO MASS RATIO FOR THE ELECTRON CHARGE TO MASS RATIO FOR THE ELECTRON OBJECTIVE: To measure the ratio of the charge of an electron to its mass. METHOD: A stream of electrons is accelerated by having them "fall" through a measured potential

More information

This lab was adapted from Kwantlen University College s Determination of e/m lab.

This lab was adapted from Kwantlen University College s Determination of e/m lab. e /m: Charge to Mass Ratio of the Electron This lab was adapted from Kwantlen University College s Determination of e/m lab. Purpose To determine the charge to mass ratio of the electron, e /m, using Helmholtz

More information

Determining the Charge to Mass Ratio (e/m) for an Electron

Determining the Charge to Mass Ratio (e/m) for an Electron Determining the Charge to Mass Ratio (e/m) for an Electron Introduction In order to determine the charge to mass ratio (e/m) for an electron we create a beam of electrons by heating a metal filament in

More information

v = E B FXA 2008 UNIT G485 Module Magnetic Fields BQv = EQ THE MASS SPECTROMETER

v = E B FXA 2008 UNIT G485 Module Magnetic Fields BQv = EQ THE MASS SPECTROMETER UNIT G485 Module 1 5.1.2 Magnetic Fields 11 Thus, in order for the particle to suffer NO DEFLECTION and so exit the device at Y : From which : MAGNETIC FORCE UP = ELECTRIC FORCE DOWN BQv = EQ THE MASS

More information

Charge-to-mass ratio for the electron

Charge-to-mass ratio for the electron Charge-to-mass ratio for the electron Introduction This is a variation of the original experiment carried out by J.J.Thomson in 1895. The deflection of a charge moving in a magnetic field is clearly demonstrated.

More information

THE CHARGE-TO-MASS RATIO OF THE ELECTRON

THE CHARGE-TO-MASS RATIO OF THE ELECTRON THE CHARGE-TO-MASS RATIO OF THE ELECTRON Is the beam that produces images on a cathode ray tube (CRT) television or computer monitor a beam of particles or of waves? This was a lively source of debate

More information

Lab 1: Determination of e/m for the electron

Lab 1: Determination of e/m for the electron Lab 1: Determination of e/m for the electron Background Reading: Tipler, Llewellyn pp. 125 130; this covers the original method of Thomson which is somewhat different from that used in this experiment

More information

Ratio of Charge to Mass (e/m) for the Electron

Ratio of Charge to Mass (e/m) for the Electron Objective: In this experiment you will determine the ratio of charge to mass (e/m) of the electron, by measuring the deflecting of electrons as they move through a magnetic field. Apparatus: e/m apparatus

More information

Homework 2: Forces on Charged Particles

Homework 2: Forces on Charged Particles Homework 2: Forces on Charged Particles 1. In the arrangement shown below, 2 C of positive charge is moved from plate S, which is at a potential of 250 V, to plate T, which is at a potential of 750 V.

More information

PhysicsAndMathsTutor.com 1

PhysicsAndMathsTutor.com 1 PhysicsAndMathsTutor.com 1 1. Millikan determined the charge on individual oil droplets using an arrangement as represented in the diagram. The plate voltage necessary to hold a charged droplet stationary

More information

MAGNETIC DEFLECTION. OBJECTIVE: To observe the effect of a magnetic field on an electron beam. To measure the Earth s magnetic field.

MAGNETIC DEFLECTION. OBJECTIVE: To observe the effect of a magnetic field on an electron beam. To measure the Earth s magnetic field. MAGNETIC DEFLECTION OBJECTIVE: To observe the effect of a magnetic field on an electron beam. To measure the Earth s magnetic field. THEORY: Moving charges exert forces on one another that are not observed

More information

MAGNETIC DEFLECTION. OBJECTIVE: To observe the effect of a magnetic field on an electron beam. To measure the Earth s magnetic field.

MAGNETIC DEFLECTION. OBJECTIVE: To observe the effect of a magnetic field on an electron beam. To measure the Earth s magnetic field. MAGNETIC DEFLECTION OBJECTIVE: To observe the effect of a magnetic field on an electron beam. To measure the Earth s magnetic field. THEORY: Moving charges exert forces on one another that are not observed

More information

Finding e/m. Purpose. The purpose of this lab is to determine the charge to mass ratio of the electron. Equipment

Finding e/m. Purpose. The purpose of this lab is to determine the charge to mass ratio of the electron. Equipment Finding e/m Purpose The purpose of this lab is to determine the charge to mass ratio of the electron. Equipment Pasco Model SE-9638 E/M Apparatus Digital Multi-Meter, DMM Power Supply, Elenco Lead, Banana/Banana

More information

Charge to Mass Ratio of The Electron

Charge to Mass Ratio of The Electron Introduction Charge to Mass Ratio of The Electron The electron was first discovered by Sir J.J. Thomson in 1897 at the Cavendish Laboratory in Cambridge, England. His experimental apparatus is not very

More information

MEASUREMENT OF THE CHARGE TO MASS RATIO (e/m e ) OF AN ELECTRON

MEASUREMENT OF THE CHARGE TO MASS RATIO (e/m e ) OF AN ELECTRON MEASUREMENT OF THE CHARGE TO MASS RATIO (e/m e ) OF AN ELECTRON Object This experiment will allow you to observe and understand the motion of a charged particle in a magnetic field and to measure the ratio

More information

Magnetic Deflection of Electrons

Magnetic Deflection of Electrons Magnetic Deflection of Electrons Objective Materials 1. Banana leads 2. Cathode ray tube 3. Fisher 1V/30V power supply (set to 30V) 4. Fluke digital multimeter 5. High voltage power supply 6. Solenoid

More information

Lab 5 - ELECTRON CHARGE-TO-MASS RATIO

Lab 5 - ELECTRON CHARGE-TO-MASS RATIO 79 Name Date Partners OBJECTIVES OVERVIEW Lab 5 - ELECTRON CHARGE-TO-MASS RATIO To understand how electric and magnetic fields impact an electron beam To experimentally determine the electron charge-to-mass

More information

MAGNETIC DEFLECTION. OBJECTIVE: To observe the effect of a magnetic field on an electron beam. To measure the Earth s magnetic field.

MAGNETIC DEFLECTION. OBJECTIVE: To observe the effect of a magnetic field on an electron beam. To measure the Earth s magnetic field. MAGNETIC DEFLECTION OBJECTIVE: To observe the effect of a magnetic field on an electron beam. To measure the Earth s magnetic field. THEORY: Moving charges exert forces on one another that are not observed

More information

Deflection of Electrons

Deflection of Electrons Deflection of Electrons Every statement in physics has to state relations between observable quantities. E. Mach (1838-1916) OBJECTIVES To determine the effect of electric and magnetic fields on a beam

More information

Brown University PHYS 0060 Physics Department LAB B -190

Brown University PHYS 0060 Physics Department LAB B -190 Physics Department LAB B -190 THE FORCE OF A MAGNETIC FIELD ON A MOVING ELECTRIC CHARGE DETERMINATION OF THE RATIO OF CHARGE TO MASS, e/m, FOR ELECTRONS References: H.D. Young, University Physics, Eleventh

More information

Chapter 1 The discovery of the electron 1.1 Thermionic emission of electrons

Chapter 1 The discovery of the electron 1.1 Thermionic emission of electrons Chapter 1 The discovery of the electron 1.1 Thermionic emission of electrons Learning objectives: What are cathode rays and how were they discovered? Why does the gas in a discharge tube emit light of

More information

Measurement of Charge-to-Mass (e/m) Ratio for the Electron

Measurement of Charge-to-Mass (e/m) Ratio for the Electron Measurement of Charge-to-Mass (e/m) Ratio for the Electron Experiment objectives: measure the ratio of the electron charge-to-mass ratio e/m by studying the electron trajectories in a uniform magnetic

More information

Charge to Mass Ratio of The Electron

Charge to Mass Ratio of The Electron Physics Topics Charge to Mass Ratio of The Electron If necessary, review the following topics and relevant textbook sections from Serway / Jewett Physics for Scientists and Engineers, 9th Ed. Electric

More information

Lab 6 - ELECTRON CHARGE-TO-MASS RATIO

Lab 6 - ELECTRON CHARGE-TO-MASS RATIO 101 Name Date Partners OBJECTIVES OVERVIEW Lab 6 - ELECTRON CHARGE-TO-MASS RATIO To understand how electric and magnetic fields impact an electron beam To experimentally determine the electron charge-to-mass

More information

KE = 1 2 mv2 = ev. (1)

KE = 1 2 mv2 = ev. (1) The e/m ratio Objective To measure the electronic charge-to-mass ratio e/m, by injecting electrons into a magnetic field and examining their trajectories. We also estimate the magnitude of the earth s

More information

PHYSICS 12 NAME: Magnetic Field and Force

PHYSICS 12 NAME: Magnetic Field and Force NAME: Magnetic Field and Force 1. An aircraft whose wingspan is 15 m carries a static charge of 0.60 C. It travels at 240 m/s perpendicular to a 1.5x10-4 T magnetic field. What magnetic force does the

More information

The e/m Ratio of the Electron

The e/m Ratio of the Electron OBJECTIVE The e/m Ratio of the Electron To study the behavior of a charged particle in the presence of a potential difference. To study the behavior of a charged particle moving in a magnetic field. To

More information

MEASUREMENT OF THE CHARGE TO MASS RATIO (e/m e ) OF AN ELECTRON

MEASUREMENT OF THE CHARGE TO MASS RATIO (e/m e ) OF AN ELECTRON MEASUREMENT OF THE CHARGE TO MASS RATIO (e/m e ) OF AN ELECTRON Object This experiment will allow you to observe and understand the motion of a charged particle in a magnetic field and to measure the ratio

More information

Lab in a Box Measuring the e/m ratio

Lab in a Box Measuring the e/m ratio Safety Precautions All the signal voltages are small and harmless. The mains voltages in the mains powered equipment is dangerous but is screened in normal use. The fine beam tube requires dangerous contact

More information

B = 8 0 NI/[r (5) 3/2 ],

B = 8 0 NI/[r (5) 3/2 ], ELECTRON BEAM IN A MAGNETIC FIELD Introduction: A charged body moving relative to a magnetic field experiences a force which is perpendicular to both the velocity of the particle and to the magnetic field.

More information

Experiment 5 Deflection of Electrons

Experiment 5 Deflection of Electrons Experiment 5 Deflection of Electrons Every statement in physics has to state relations between observable quantities. E. Mach OBJECTIVES To determine the effect of electric and magnetic fields on a beam

More information

Lab 7 - ELECTRON CHARGE-TO-MASS RATIO

Lab 7 - ELECTRON CHARGE-TO-MASS RATIO 107 Name Date Partners Lab 7 - ELECTRON CHARGE-TO-MASS RATIO OBJECTIVES To understand how electric and magnetic fields impact an electron beam To experimentally determine the electron charge-to-mass ratio

More information

Lab 6 - Electron Charge-To-Mass Ratio

Lab 6 - Electron Charge-To-Mass Ratio Lab 6 Electron Charge-To-Mass Ratio L6-1 Name Date Partners Lab 6 - Electron Charge-To-Mass Ratio OBJECTIVES To understand how electric and magnetic fields impact an electron beam To experimentally determine

More information

Mass of the Electron

Mass of the Electron PHY 192 Charge and Mass of the Electron Spring 2013 1 Mass of the Electron Motivation for the Experiment The aim of this experiment is to measure the mass of the electron. The mass will be deduced from

More information

Lab 5 - ELECTRON CHARGE-TO-MASS RATIO

Lab 5 - ELECTRON CHARGE-TO-MASS RATIO 81 Name Date Partners Lab 5 - ELECTRON CHARGE-TO-MASS RATIO OBJECTIVES To understand how electric and magnetic fields impact an electron beam To experimentally determine the electron charge-to-mass ratio

More information

Other Formulae for Electromagnetism. Biot's Law Force on moving charges

Other Formulae for Electromagnetism. Biot's Law Force on moving charges Other Formulae for Electromagnetism Biot's Law Force on moving charges 1 Biot's Law. Biot's Law states that the magnetic field strength (B) is directly proportional to the current in a straight conductor,

More information

CHARGED PARTICLES IN FIELDS

CHARGED PARTICLES IN FIELDS The electron beam used to study motion of charged particles in electric and/or magnetic fields. CHARGED PARTICLES IN FIELDS Physics 41/61 Fall 01 1 Introduction The precise control of charged particles

More information

Charge to Mass Ratio of the Electron

Charge to Mass Ratio of the Electron Charge to Mass Ratio of the Electron 1. Purpose: To determine the charge to mass ratio of the electron, e/m, by subjecting a beam of electrons to a magnetic field and examining their trajectories. It can

More information

MAGNETISM LAB: The Charge-to-Mass Ratio of the Electron

MAGNETISM LAB: The Charge-to-Mass Ratio of the Electron Physics 7B Charge-to-mass: e/m p. 1 NAME: DL SECTION NUMBER: GSI: LAB PARTNERS: MAGNETISM LAB: The Charge-to-Mass Ratio of the Electron Introduction In this lab you will explore the motion of a charged

More information

Electron charge-to-mass ratio

Electron charge-to-mass ratio (ta initials) first name (print) last name (print) brock id (ab17cd) (lab date) Experiment 4 Electron charge-to-mass ratio In this Experiment you will learn the relationship between electric and magnetic

More information

Magnetic Fields & Forces

Magnetic Fields & Forces Magnetic Fields & Forces Oersted discovered that an electric current will produce a magnetic field around conductor only a moving charge creates a magnetic field the magnetic field is circular around the

More information

PHYSICS 30 ELECTROMAGNETISM ASSIGNMENT 3 VERSION:0

PHYSICS 30 ELECTROMAGNETISM ASSIGNMENT 3 VERSION:0 Communication includes statement of the physics concept used and how it is applied in the situation along with diagrams, word explanations and calculations in a well laid out formula, substitution, answer

More information

Chapter 23 Electric Potential. Copyright 2009 Pearson Education, Inc.

Chapter 23 Electric Potential. Copyright 2009 Pearson Education, Inc. Chapter 23 Electric Potential Units of Chapter 23 Electric Potential Energy and Potential Difference Relation between Electric Potential and Electric Field Electric Potential Due to Point Charges Potential

More information

Magnets and Electromagnetism

Magnets and Electromagnetism Review 9 Magnets and Electromagnetism 1. A 1.2 cm wire carrying a current of 0.8 A is perpendicular to a 2.4 T magnetic field. What is the magnitude of the force on the wire? 2. A 24 cm length of wire

More information

THE CHARGE-TO-MASS RATIO OF THE ELECTRON (e/m)

THE CHARGE-TO-MASS RATIO OF THE ELECTRON (e/m) THE CHARGE-TO-MASS RATIO OF THE ELECTRON (e/m) INTRODUCTION In this experiment you will be measuring the charge to mass ratio, e/m, of the electron. The h/e apparatus consists of an electron gun, a helium

More information

PhysicsAndMathsTutor.com 1

PhysicsAndMathsTutor.com 1 PhysicsAndMathsTutor.com 1 Q1. (a) The diagram below shows a narrow beam of electrons produced by attracting electrons emitted from a filament wire to a metal plate which has a small hole in it. (i) Why

More information

Magnetic Fields & Forces

Magnetic Fields & Forces Magnetic Fields & Forces Oersted discovered that an electric current will produce a magnetic field around conductor only a moving charge creates a magnetic field the magnetic field is circular around the

More information

Charge to mass Ratio. Nature of the Atom: Dalton's Contributions to Science. 6) qm ratio notes.notebook. December 13, 2018

Charge to mass Ratio. Nature of the Atom: Dalton's Contributions to Science. 6) qm ratio notes.notebook. December 13, 2018 Nature of the Atom: Charge to mass Ratio Studies of atoms from John Dalton's atmospheric studies indicated that properties were cyclic moving from group to group. This suggested some unit of atomic structure

More information

Chapter 12. Magnetism and Electromagnetism

Chapter 12. Magnetism and Electromagnetism Chapter 12 Magnetism and Electromagnetism 167 168 AP Physics Multiple Choice Practice Magnetism and Electromagnetism SECTION A Magnetostatics 1. Four infinitely long wires are arranged as shown in the

More information

Force Due to Magnetic Field You will use

Force Due to Magnetic Field You will use Force Due to Magnetic Field You will use Units: 1 N = 1C(m/s) (T) A magnetic field of one tesla is very powerful magnetic field. Sometimes it may be convenient to use the gauss, which is equal to 1/10,000

More information

21 MAGNETIC FORCES AND MAGNETIC FIELDS

21 MAGNETIC FORCES AND MAGNETIC FIELDS CHAPTER 1 MAGNETIC FORCES AND MAGNETIC FIELDS ANSWERS TO FOCUS ON CONCEPTS QUESTIONS 1 (d) Right-Hand Rule No 1 gives the direction of the magnetic force as x for both drawings A and B In drawing C, the

More information

Chapter 27 Magnetic Field and Magnetic Forces

Chapter 27 Magnetic Field and Magnetic Forces Chapter 27 Magnetic Field and Magnetic Forces Lecture by Dr. Hebin Li Goals for Chapter 27 To study magnets and the forces they exert on each other To calculate the force that a magnetic field exerts on

More information

3B SCIENTIFIC PHYSICS

3B SCIENTIFIC PHYSICS B SCIENTIFIC PHYSICS ElectronBeam Deflection Tube D 6 Instruction sheet / LF 9 8 7 6 7 6 Fluorescent screen Lower deflection plate Boss with mm plug for connecting deflection plates Electron gun mm sockets

More information

Physics 106, Section 1

Physics 106, Section 1 Physics 106, Section 1 Magleby Exam 2, Summer 2012 Exam Cid You are allowed a pencil and a testing center calculator. No scratch paper is allowed. Testing center calculators only. 1. A circular coil lays

More information

θ θ θ θ current I Fig. 6.1 The conductor and the magnetic field are both in the plane of the paper. State

θ θ θ θ current I Fig. 6.1 The conductor and the magnetic field are both in the plane of the paper. State 3 1 (a) A straight conductor carrying a current I is at an angle θ to a uniform magnetic field of flux density B, as shown in Fig. 6.1. magnetic field, flux density B θ θ θ θ current I Fig. 6.1 The conductor

More information

PhysicsAndMathsTutor.com

PhysicsAndMathsTutor.com PhysicsAndMathsTutor.com 1 1. Define electric field strength at a point in space....... [Total 1 marks] 2. Fig. 1 shows a square flat coil of insulated wire placed in a region of a uniform magnetic field

More information

Electric Deflection of Electrons

Electric Deflection of Electrons Electric Deflection of Electrons Objective The purpose of this experiment is to observe that the spacial deflection of an electron in a cathode ray tube is directly proportional to the deflection potential.

More information

Advanced Higher Physics. Electromagnetism

Advanced Higher Physics. Electromagnetism Wallace Hall Academy Physics Department Advanced Higher Physics Electromagnetism Problems AH Physics: Electromagnetism 1 2013 Data Common Physical Quantities QUANTITY SYMBOL VALUE Gravitational acceleration

More information

Discussion Question 7A P212, Week 7 RC Circuits

Discussion Question 7A P212, Week 7 RC Circuits Discussion Question 7A P1, Week 7 RC Circuits The circuit shown initially has the acitor uncharged, and the switch connected to neither terminal. At time t = 0, the switch is thrown to position a. C a

More information

Lab 7: Magnetic fields and forces Lab Worksheet

Lab 7: Magnetic fields and forces Lab Worksheet Lab 7: Magnetic fields and forces Lab Worksheet Name This sheet is the lab document your TA will use to score your lab. It is to be turned in at the end of lab. To receive full credit you must use complete

More information

Experiment V Motion of electrons in magnetic field and measurement of e/m

Experiment V Motion of electrons in magnetic field and measurement of e/m Experiment V Motion of electrons in magnetic field and measurement of e/m In Experiment IV you observed the quantization of charge on a microscopic bead and measured the charge on a single electron. In

More information

Fig. 2.1 I =... A [2] Suggest why it would be impossible for overhead cables carrying an alternating current to float in the Earth s magnetic field.

Fig. 2.1 I =... A [2] Suggest why it would be impossible for overhead cables carrying an alternating current to float in the Earth s magnetic field. 1 (a) Fig. 2.1 shows a horizontal current-carrying wire placed in a uniform magnetic field. I region of uniform magnetic field wire Fig. 2.1 The magnetic field of flux density 0.070 T is at right angles

More information

AP Physics Electromagnetic Wrap Up

AP Physics Electromagnetic Wrap Up AP Physics Electromagnetic Wrap Up Here are the glorious equations for this wonderful section. This is the equation for the magnetic force acting on a moving charged particle in a magnetic field. The angle

More information

Instruction Manual for EP-20 e/m of the Electron Apparatus

Instruction Manual for EP-20 e/m of the Electron Apparatus Instruction Manual for EP-20 e/m of the Electron Apparatus Introduction This self-contained apparatus is designed for the measurement of e/m of the electron by observing the radius of the circular path

More information

PHYS 241 EXAM #2 November 9, 2006

PHYS 241 EXAM #2 November 9, 2006 1. ( 5 points) A resistance R and a 3.9 H inductance are in series across a 60 Hz AC voltage. The voltage across the resistor is 23 V and the voltage across the inductor is 35 V. Assume that all voltages

More information

1. An isolated stationary point charge produces around it. a) An electric field only. b) A magnetic field only. c) Electric as well magnetic fields.

1. An isolated stationary point charge produces around it. a) An electric field only. b) A magnetic field only. c) Electric as well magnetic fields. 1. An isolated stationary point charge produces around it. a) An electric field only. b) A magnetic field only. c) Electric as well magnetic fields. 2. An isolated moving point charge produces around it.

More information

Physics Tutorial MF1 Magnetic Forces

Physics Tutorial MF1 Magnetic Forces Physics Tutorial MF1 Magnetic Forces 1 Magnetic Forces The force F on a charge q moving with velocity v in a magnetic field is: F = qv The force F on a straight conductor of length L carrying a current

More information

Test Review FQ3eso_U5_4_Electric field_test_review

Test Review FQ3eso_U5_4_Electric field_test_review Test Review FQ3eso_U5_4_Electric field_test_review Identify the letter of the choice that best completes the statement or answers the question. 1.- In which diagram do the field lines best represent the

More information

In a particular investigation the atomic spacing of the crystal is m and the electrons are accelerated through 3000 V.

In a particular investigation the atomic spacing of the crystal is m and the electrons are accelerated through 3000 V. 1 Crystal structure can be investigated using the diffraction of an electron beam. A typical diffraction pattern is shown. In a particular investigation the atomic spacing of the crystal is 2.3 10 11 m

More information

1 Written and composed by: Prof. Muhammad Ali Malik (M. Phil. Physics), Govt. Degree College, Naushera

1 Written and composed by: Prof. Muhammad Ali Malik (M. Phil. Physics), Govt. Degree College, Naushera ELECTROMAGNETISM Q # 1. Describe the properties of magnetic field due to current in a long straight conductor. Ans. When the heavy current is passed through a straight conductor: i. A magnetic field is

More information

Today s lecture: Motion in a Uniform Magnetic Field continued Force on a Current Carrying Conductor Introduction to the Biot-Savart Law

Today s lecture: Motion in a Uniform Magnetic Field continued Force on a Current Carrying Conductor Introduction to the Biot-Savart Law PHYSICS 1B Today s lecture: Motion in a Uniform Magnetic Field continued Force on a Current Carrying Conductor Introduction to the Biot-Savart Law Electricity & Magnetism A Charged Particle in a Magnetic

More information

You should be able to demonstrate and show your understanding of:

You should be able to demonstrate and show your understanding of: OCR B Physics H557 Module 6: Field and Particle Physics You should be able to demonstrate and show your understanding of: 6.1: Fields (Charge and Field) Field: A potential gradient Field Strength: Indicates

More information

PHYSICS 12 NAME: Electrostatics Review

PHYSICS 12 NAME: Electrostatics Review NAME: Electrostatics Review 1. An electron orbits a nucleus which carries a charge of +9.6 x10-19 C. If the electron s orbital radius is 2.0 x10-10 m, what is its electric potential energy? A. -6.9 x10-18

More information

Ch 17 Problem Set 31. A toaster is rated at 600 W when connected to a 120-V source. What current does the toaster carry, and what is its resistance?

Ch 17 Problem Set 31. A toaster is rated at 600 W when connected to a 120-V source. What current does the toaster carry, and what is its resistance? Ch 17 Problem Set 31. A toaster is rated at 600 W when connected to a 120-V source. What current does the toaster carry, and what is its resistance? 33. How many 100-W lightbulbs can you use in a 120-V

More information

Magnetic Fields; Sources of Magnetic Field

Magnetic Fields; Sources of Magnetic Field This test covers magnetic fields, magnetic forces on charged particles and current-carrying wires, the Hall effect, the Biot-Savart Law, Ampère s Law, and the magnetic fields of current-carrying loops

More information

1 P a g e h t t p s : / / w w w. c i e n o t e s. c o m / Physics (A-level)

1 P a g e h t t p s : / / w w w. c i e n o t e s. c o m / Physics (A-level) 1 P a g e h t t p s : / / w w w. c i e n o t e s. c o m / Capacitance (Chapter 18): Physics (A-level) Every capacitor has two leads, each connected to a metal plate, where in between there is an insulating

More information

Charge to Mass Ratio of Electron Lab 11 SAFETY

Charge to Mass Ratio of Electron Lab 11 SAFETY HB 10-20-08 Charge to Mass Ratio of Electron Lab 11 1 Charge to Mass Ratio of Electron Lab 11 Equipment ELWE e/m tube, ELWE Helmholtz coils, ELWE 4 voltage power supply, Safety Glasses, Fluke multimeter,

More information

General Physics (PHY 2140)

General Physics (PHY 2140) General Physics (PHY 2140) Lecture 8 Electricity and Magnetism 1. Magnetism Application of magnetic forces Ampere s law 2. Induced voltages and induction Magnetic flux http://www.physics.wayne.edu/~alan/2140website/main.htm

More information

P Q 2 = -3.0 x 10-6 C

P Q 2 = -3.0 x 10-6 C 1. Which one of the following represents correct units for electric field strength? A. T B. N/C C. J / C D. N m 2 /C 2 2. The diagram below shows two positive charges of magnitude Q and 2Q. P Q 2Q Which

More information

Physics for Scientists & Engineers 2

Physics for Scientists & Engineers 2 Review Physics for Scientists & Engineers 2 Spring Semester 2005 Lecture 21 The force that a magnetic field exerts on a charge moving with velocity v is given by! F B = q v!! B! The magnitude of the force

More information

The Cyclotron I. 1. Motion of the charges occurs in two semicircular containers, D 1. and D 2

The Cyclotron I. 1. Motion of the charges occurs in two semicircular containers, D 1. and D 2 1. Motion of the charges occurs in two semicircular containers, D 1 and D 2 referred to as the Dees 2. The Dees are evacuated in order to minimize energy loss from collisions 3. A high frrequency alternating

More information

1. The diagram shows the electric field lines produced by an electrostatic focussing device.

1. The diagram shows the electric field lines produced by an electrostatic focussing device. 1. The diagram shows the electric field lines produced by an electrostatic focussing device. Which one of the following diagrams best shows the corresponding equipotential lines? The electric field lines

More information

Chapter 27 Magnetism 1/20/ Magnets and Magnetic Fields Magnets and Magnetic Fields Magnets and Magnetic Fields

Chapter 27 Magnetism 1/20/ Magnets and Magnetic Fields Magnets and Magnetic Fields Magnets and Magnetic Fields Chapter 27 Magnetism Magnets have two ends poles called north and south. Like poles repel; unlike poles attract. However, if you cut a magnet in half, you don t get a north pole and a south pole you get

More information

2. A proton is traveling with velocity v, to the right, through a magnetic field pointing into the page as indicated in the figure below.

2. A proton is traveling with velocity v, to the right, through a magnetic field pointing into the page as indicated in the figure below. 1. An electron has a mass of 9.11 x 10-31 kg and its charge is -1.6 x 10-19 C. The electron is released from rest in a vacuum between two flat, parallel metal plates that are 10 cm apart. The potential

More information

Chapter 29. Magnetic Fields

Chapter 29. Magnetic Fields Chapter 29 Magnetic Fields Outline 29.1 Magnetic Fields and Forces 29.2 Magnetic Force Acting on a Current-Carrying Conductor 29.4 Motion of a Charged Particle in a Uniform Magnetic Field 29.5 Applications

More information

Chapter 12. Project 4 Classical Physics. Experiment A: The Charge to Mass Ratio of the Electron

Chapter 12. Project 4 Classical Physics. Experiment A: The Charge to Mass Ratio of the Electron Chapter 12 Project 4 Classical Physics Experiment A: The Charge to Mass Ratio of the Electron 12A.1 Objectives (a) To perform Lenard's classic experiment to determine e/m. (b) To evaluate the ratio e/m

More information

DO PHYSICS ONLINE MOTORS AND GENERATORS FARADAY S LAW ELECTROMAGNETIC INDUCTION

DO PHYSICS ONLINE MOTORS AND GENERATORS FARADAY S LAW ELECTROMAGNETIC INDUCTION DO PHYSICS ONLINE MOTORS AND GENERATORS FARADAY S LAW ELECTROMAGNETIC INDUCTION English Michael Faraday (1791 1867) who experimented with electric and magnetic phenomena discovered that a changing magnetic

More information

Physics Week 5(Sem. 2) Name. Magnetism. Chapter Summary. Magnetic Fields

Physics Week 5(Sem. 2) Name. Magnetism. Chapter Summary. Magnetic Fields Physics Week 5(Sem. 2) Name Chapter Summary Magnetism Magnetic Fields Permanent magnets have long been used in navigational compasses. The needle in a compass is supported to allow it to freely rotate

More information

e/m APPARATUS Instruction Manual and Experiment Guide for the PASCO scientific Model SE D 5/ PASCO scientific $5.

e/m APPARATUS Instruction Manual and Experiment Guide for the PASCO scientific Model SE D 5/ PASCO scientific $5. Includes Teacher's Notes and Typical Experiment Results Instruction Manual and Experiment Guide for the PASCO scientific Model SE9638 020347D 5/94 e/m APPARATUS 987 PASCO scientific $5.00 020347D e/m

More information

Unit 4 Magnetism Essential Fundamentals of Magnetism 1. Magnetism is a fundamental force.

Unit 4 Magnetism Essential Fundamentals of Magnetism 1. Magnetism is a fundamental force. Unit 4 Magnetism Essential Fundamentals of Magnetism 1. Magnetism is a fundamental force. Early Booklet E.C.: + 1 Unit 4 Hwk. Pts.: / 34 Unit 4 Lab Pts.: / 36 Late, Incomplete, No Work, No Units Fees?

More information

a. Clockwise. b. Counterclockwise. c. Out of the board. d. Into the board. e. There will be no current induced in the wire

a. Clockwise. b. Counterclockwise. c. Out of the board. d. Into the board. e. There will be no current induced in the wire Physics 1B Winter 2012: Final Exam For Practice Version A 1 Closed book. No work needs to be shown for multiple-choice questions. The first 10 questions are the makeup Quiz. The remaining questions are

More information

Experiment 4: Charge to mass ratio (e/m) of the electron

Experiment 4: Charge to mass ratio (e/m) of the electron Experiment 4: Charge to mass ratio (e/m) of the electron Nate Saffold nas2173@columbia.edu Office Hour: Monday, 5:30PM-6:30PM @ Pupin 1216 INTRO TO EXPERIMENTAL PHYS-LAB 1494/2699 Introduction Our first

More information

(a) zero. B 2 l 2. (c) (b)

(a) zero. B 2 l 2. (c) (b) 1. Two identical co-axial circular loops carry equal currents circulating in the same direction: (a) The current in each coil decrease as the coils approach each other. (b) The current in each coil increase

More information

Unit 8: Electromagnetism

Unit 8: Electromagnetism Multiple Choice Portion Unit 8: Electromagnetism 1. Four compasses are placed around a conductor carrying a current into the page, as shown below. Which compass correctly shows the direction of the magnetic

More information

Physics 6B Summer 2007 Final

Physics 6B Summer 2007 Final Physics 6B Summer 2007 Final Question 1 An electron passes through two rectangular regions that contain uniform magnetic fields, B 1 and B 2. The field B 1 is stronger than the field B 2. Each field fills

More information