Electromagnetic Induction Experiment



Similar documents
Magnetic Fields and Their Effects

The purposes of this experiment are to test Faraday's Law qualitatively and to test Lenz's Law.

Lab 3 - DC Circuits and Ohm s Law

Experiment 3: Magnetic Fields of a Bar Magnet and Helmholtz Coil

AC generator theory. Resources and methods for learning about these subjects (list a few here, in preparation for your research):

Experiment 3: Magnetic Fields of a Bar Magnet and Helmholtz Coil

Lesson 3 DIRECT AND ALTERNATING CURRENTS. Task. The skills and knowledge taught in this lesson are common to all missile repairer tasks.

Chapter 7. Magnetism and Electromagnetism ISU EE. C.Y. Lee

Mapping the Magnetic Field

Physics 221 Experiment 5: Magnetic Fields

ElectroMagnetic Induction. AP Physics B

1. The diagram below represents magnetic lines of force within a region of space.

The DC Motor. Physics 1051 Laboratory #5 The DC Motor

Exploring Magnetism. DataQuest

Physics 30 Worksheet #10 : Magnetism From Electricity

Magnetic Field of a Circular Coil Lab 12

Using an Oscilloscope

ELECTRODYNAMICS 05 AUGUST 2014

Experiment 5: Magnetic Fields of a Bar Magnet and of the Earth

Magnetism Basics. Magnetic Domains: atomic regions of aligned magnetic poles Random Alignment Ferromagnetic Alignment. Net Effect = Zero!

STUDY GUIDE: ELECTRICITY AND MAGNETISM

Lab E1: Introduction to Circuits

Electromagnetic Induction: Faraday's Law

Sources of electricity

Sources of electricity

Reading assignment: All students should read the Appendix about using oscilloscopes.

Magnetism. Magnetism. Magnetic Fields and Magnetic Domains. Magnetic Fields and Magnetic Domains. Creating and Destroying a Magnet

OVERCURRENT & EARTH FAULT RELAYS. To study the protection of equipment and system by relays in conjunction with switchgear.

Electronic WorkBench tutorial

E. K. A. ADVANCED PHYSICS LABORATORY PHYSICS 3081, 4051 NUCLEAR MAGNETIC RESONANCE

MEASURING INSTRUMENTS. By: Nafees Ahmed, Asstt, Prof, EE Deptt, DIT, Dehradun

General Physics (PHY 2140)

PS-6.2 Explain the factors that determine potential and kinetic energy and the transformation of one to the other.

Digital Energy ITI. Instrument Transformer Basic Technical Information and Application

Equipment: Power Supply, DAI, Transformer (8341), Variable resistance (8311), Variable inductance (8321), Variable capacitance (8331)

Ampere's Law. Introduction. times the current enclosed in that loop: Ampere's Law states that the line integral of B and dl over a closed path is 0

Experiment: Series and Parallel Circuits

Chapter 13: Electric Circuits

How strong are magnets?

Candidate Number. General Certificate of Education Advanced Level Examination June 2010

F B = ilbsin(f), L x B because we take current i to be a positive quantity. The force FB. L and. B as shown in the Figure below.

Coupled Inductors. Introducing Coupled Inductors

5. Measurement of a magnetic field

DC GENERATOR THEORY. LIST the three conditions necessary to induce a voltage into a conductor.

Physics 41, Winter 1998 Lab 1 - The Current Balance. Theory

DC generator theory. Resources and methods for learning about these subjects (list a few here, in preparation for your research):

Direction of Induced Current

NUCLEAR MAGNETIC RESONANCE. Advanced Laboratory, Physics 407, University of Wisconsin Madison, Wisconsin 53706

Candidate Number. General Certificate of Education Advanced Level Examination June 2014

Equipment: Power Supply, DAI, Synchronous motor (8241), Electrodynamometer (8960), Tachometer, Timing belt.

E/M Experiment: Electrons in a Magnetic Field.

Inductors & Inductance. Electronic Components

Name Partners Date. Energy Diagrams I

Simple Analysis for Brushless DC Motors Case Study: Razor Scooter Wheel Motor

Chapter 27 Magnetic Field and Magnetic Forces

Magnetic susceptibility. Basic principles and features on the PPMS.

FORCE ON A CURRENT IN A MAGNETIC FIELD

Components. Transformers

Introduction to Electricity & Magnetism. Dr Lisa Jardine-Wright Cavendish Laboratory

GETTING CURRENT: Generating Electricity Using a Magnet

DIRECT CURRENT GENERATORS

INTRODUCTION TO DESKTOP PUBLISHING

GROUND DETECTION CIRCUITS FOR STATIONARY APPLICATIONS (IN PLAIN DOWN TO EARTH LANGUAGE)

Measuring Impedance and Frequency Response of Guitar Pickups

Chapter 22: Electric motors and electromagnetic induction

Radio Control System

Chapter 22 Magnetism

Odyssey of the Mind Technology Fair. Simple Electronics

TEACHER S CLUB EXAMS GRADE 11. PHYSICAL SCIENCES: PHYSICS Paper 1

Ohm's Law and Circuits

H ello, I ll be demonstrating

FREQUENCY RESPONSE OF AN AUDIO AMPLIFIER

Experiment 8: Undriven & Driven RLC Circuits

Prelab Exercises: Hooke's Law and the Behavior of Springs

Motor Fundamentals. DC Motor

Lesson Plan for Electric Circuits

This topic explores the key concepts of magnetism as they relate to: the phenomenon of magnetism magnetic forces and fields a theory of magnetism.

physics 112N magnetic fields and forces

ACCELERATION DUE TO GRAVITY

Student Exploration: Circuits

Georgia Performance Standards Framework for Physical Science 8 th Grade. Powering Satellites

Magnetic Dipoles. Recall that an electric dipole consists of two equal but opposite charges separated by some distance, such as in

Maximum value. resistance. 1. Connect the Current Probe to Channel 1 and the Differential Voltage Probe to Channel 2 of the interface.

12. Transformers, Impedance Matching and Maximum Power Transfer

Eðlisfræði 2, vor 2007

Preview of Period 16: Motors and Generators

Light Bulbs in Parallel Circuits

Episode 126: Capacitance and the equation C =Q/V

Magnetic Field and Magnetic Forces

Physics 42 Lab 4 Fall 2012 Cathode Ray Tube (CRT)

AP Physics Electricity and Magnetism #4 Electrical Circuits, Kirchoff s Rules

Measuring Electric Phenomena: the Ammeter and Voltmeter

Experiment 2: Conservation of Momentum

Transformer Calculations

Motion of Charges in Combined Electric and Magnetic Fields; Measurement of the Ratio of the Electron Charge to the Electron Mass

Chapter 11. Inductors ISU EE. C.Y. Lee

Candidate Number. General Certificate of Education Advanced Level Examination June 2012

Chapter 21. Magnetic Forces and Magnetic Fields

Electrical Fundamentals Module 3: Parallel Circuits

45. The peak value of an alternating current in a 1500-W device is 5.4 A. What is the rms voltage across?

Transcription:

In this experiment, the activity will be based on a Phet simulation called Faraday s Electromagnetic Lab, created by a group at the University of Colorado at Boulder. This group has a number of good simulations of various topics. You can get to the main Phet site at http://phet.colorado.edu The link to take you directly to the simulation you ll be interacting with today is http://phet.colorado.edu/simulations/sims.php?sim=faradays_electromagnetic_lab When you run the simulation, note that it is actually five different simulations in one. You can switch from one to the other by using the tabs at the top of the simulation window. Part 1 Bar Magnet Start with the bar magnet simulation. In the menu at the right, check all of the checkboxes. You can click-and-drag to move the magnet, the compass, or the field meter around the screen. Move all three of these around to see what happens. A compass can be used, both in the simulation and in real life, to determine the direction of the magnetic field at a particular point. How does the compass indicate the field direction? The direction of the field is in the direction that the pole of the compass needle points. The field meter will give you the numerical value of the magnetic field at a particular point. Note that the field meter gives field in units of G, which stands for gauss. What is the conversion factor from tesla to gauss? Approximately what is the strength of the Earth s magnetic field in gauss? (Feel free to make use of the internet through the computer right in front of you!) At which point on the field meter is the meter measuring the magnetic field? Move the field meter around, and see where you can place it to find the highest possible magnetic field. Note that there is a slider in the menu. What is the magnitude of the largest field possible in this simulation, and where do you find that maximum field? 1

Part 2 Pickup coil Now, use the second tab at the top of the simulation window to switch to the Pickup coil simulation. This shows a bar magnet near a coil of wire. The coil of wire can be connected to a light bulb or a voltmeter. For now, leave the coil connected to the light bulb. Note that you can click-and-drag to move the magnet, or you can click-and-drag to move the light bulb (the coil will come with it, of course). In this simulation, there are at least five ways to get the light bulb to light up briefly. List the methods you come up with to light the bulb. 1. 2. 3. 4. 5. Describe what you should do so that the bulb brightness is maximized. What should the sliders be set to? What should you do when you move something on the screen? Feel free to switch to the voltmeter to try to maximize the voltmeter reading instead. In this simulation, adjusting the coil area doesn t seem to make much difference. This may, at first, surprise you, because you have been taught that induced voltage is related to the rate of change of magnetic flux, and magnetic flux has a factor of area in it. Why do you think that, in this simulation, increasing the coil area, even by a factor of 5, has a relatively minor impact on the induced voltage when you move the magnet or coil? What do the blue dots in the coil represent? [ ] positive charges [ ] negative charges When you move the coil toward the magnet, the dots should move in a direction consistent with the right-hand rule associated with F qvbsin. Do they? Explain. Think carefully about the component of the magnetic field that matters here. 2

Part 3 Electromagnet Now, use the third tab at the top of the simulation window to switch to the Electromagnet simulation. In the menu at the right, check all the checkboxes, which gives both a compass and a field meter on the screen. Here, instead of a bar magnet, we have an electromagnet a magnetic field is created by setting up a current in a coil. Start with the DC case, in which a battery is connected to the coil. DC, by the way, stands for. In this situation, what is the magnitude of the maximum magnetic field that can be achieved? Where is that maximum field located? Compare the magnetic field created by the electromagnet (in the DC case) to the magnetic field created by a bar magnet. Think about the case of a short stubby bar magnet, the same size as the coil. Do the electromagnet and the same-size bar magnet create similar fields? Identical fields? Completely different fields? Explain. In the DC case, can we change the magnitude of the magnetic field at a particular point without moving the coil? Explain. Now, switch to AC, which stands for. For the AC situation, you see a graph. What is this a graph of? On the vertical axis of the graph is On the horizontal axis of the graph is What does the magnetic field do, with the coil connected to the AC source? 3

Part 4 Transformer Use the fourth tab at the top of the window to switch to the Transformer simulation. This shows an electromagnet magnet near a pickup coil. The pickup coil can be connected to a light bulb or a voltmeter. For now, leave the coil connected to the light bulb. Note that you can click-and-drag to move the electromagnet, or you can click-anddrag to move the light bulb (the pickup coil will come with it, of course). In this simulation, there are at least six ways to get the light bulb to light up briefly, in the DC situation. List the methods you come up with to light the bulb. It might help to place the pickup coil so the coil for the electromagnet is inside the pickup coil. 1. 2. 3. 4. 5. 6. Now, switch to the AC electromagnet. Do you have to do anything special to make the light bulb light now? Staying with the AC source, use the meter on the pickup coil instead of the light bulb. You should be able to make the meter go from its maximum positive reading to its maximum negative reading and back. Describe everything you have to do to cause this to happen. Place the coils so that the coil for the electromagnet is inside the pickup coil. One thing you should observe is that using a larger-area pickup coil is less effective than using a smaller-area pickup coil. Explain why this is. Are the charges (blue dots) in the pickup coil in phase with those in the electromagnet? In other words, when the charges in the electromagnet are moving fastest, are the charges in the pickup coil moving fastest? Why or why not? 4

Part 5 Generator Now, use the last tab to switch to the generator situation. This shows a model of the process used by a hydroelectric power plant (such as at the Hoover Dam, near Las Vegas, or at Niagara Falls) to generate electricity. In this simulation, you have a pickup coil attached to a light bulb, a magnet attached to a wheel, and a faucet with a slider on it, that you can adjust to control the flow of water that will turn the wheel. Turn on the water. What happens to the light bulb? Assuming that the water starts with a lot of gravitational potential energy, as it does at a place like Niagara Falls, explain all the steps involved in transforming the water s gravitational potential energy into the electrical energy we see that lights up the bulb. You have a number of variables under your control in this simulation. Switch to the voltmeter instead of the light bulb. To make the voltmeter oscillate with its largest possible amplitude, describe the settings you should use on the simulation. Unlike what you have observed previously, increasing the area of the pickup coil in this situation produces more voltage. Explain why more area corresponds to a larger voltage in this situation. 5