Lesson: Thrown for a Loop

Contributed by: VU Bioengineering RET Program, School of Engineering, Vanderbilt University

A shortwave loop antenna.
A loop carrying current.
copyright
Copyright © 2008 Trixt, Wikimedia Commons http://commons.wikimedia.org/wiki/File:Loop_antenna.jpg

Summary

Students begin to focus on the torque associated with a current carrying loop in a magnetic field. They solve example problems as a class and use diagrams to visualize the vector product. In addition, students learn to calculate the energy of this loop in the magnetic field. Through the associated activity, "Get Your Motor Running," students explore a physical model to gain empirical data and compare it to their calculated data. A homework assignment is also provided as a means of student assessment.
This engineering curriculum meets Next Generation Science Standards (NGSS).

Engineering Connection

Biomedical engineers must consider not only the force resulting from a charged particle in a magnetic field but also, a current traveling through a magnetic field. During resonance and relaxation, engineers can determine the frequency of the oscillating magnetic field based on a small current in the receiver coil of the MRI machine. In the homework assessment section of this lesson, students will have to determine the magnitude and direction of the torque on a current loop due to the magnetic field.

Pre-Req Knowledge

Students need to have an understanding of rotation and torque, since an important concept of this lesson is the torque created by a magnetic field. Students need to make the connection that torque on the loop leads the loop to rotate in the magnetic field. It is also crucial for the student to draw and label all example and homework problems (just as shown in the figure sets).

Learning Objectives

After this lesson students should be able to:

  • Describe the actions of a current loop in a magnetic field.
  • Draw and fully label a diagram of current acting through a loop.
  • Calculate the torque on a current loop due to a magnetic field.

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Educational Standards

Each TeachEngineering lesson or activity is correlated to one or more K-12 science, technology, engineering or math (STEM) educational standards.

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In the ASN, standards are hierarchically structured: first by source; e.g., by state; within source by type; e.g., science or mathematics; within type by subtype, then by grade, etc.

  • Develop and use models to illustrate that energy at the macroscopic scale can be accounted for as either motions of particles or energy stored in fields. (Grades 9 - 12) Details... View more aligned curriculum... Do you agree with this alignment?
  • Energy can be grouped into major forms: thermal, radiant, electrical, mechanical, chemical, nuclear, and others. (Grades 9 - 12) Details... View more aligned curriculum... Do you agree with this alignment?
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  • Results of scientific inquiry--new knowledge and methods--emerge from different types of investigations and public communication among scientists. In communicating and defending the results of scientific inquiry, arguments must be logical and demonstrate connections between natural phenomena, investigations, and the historical body of scientific knowledge. In addition, the methods and procedures that scientists used to obtain evidence must be clearly reported to enhance opportunities for further investigation. (Grades 9 - 12) Details... View more aligned curriculum... Do you agree with this alignment?
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Introduction/Motivation

We are making progress to solve the MRI challenge problem and determine the risks and dangers of an MRI. To do this, we need to learn what happens near a large electromagnet. We need to learn about the properties of magnetic fields, including the effects of a magnetic field on loops of current. As MRI machines evolved over time and were built with stronger magnets, engineers needed to account for the change in current.

Lesson Background and Concepts for Teachers

Legacy Cycle Information

This lesson fits into the Research and Revise phase of the legacy cycle in which students are provided with additional information enabling them to revise their initial ideas for solving the challenge. The research aspect consists of formal lecture and several example problems on how magnetic fields create torque on a current loop.

Torque on a Current Loop

Note: It may be helpful to review rotation, torque and kinetic energy at this point.

A drawing of a rectangle with force arrows pointing up and down, a vector labeled B pointing to the right, and a vector labeled torque pointing into the page.
Figure A

Consider a rectangular loop of current in a magnetic field with width w and length l, and current I. Let the loop be laid out on a horizontal plane and let a magnetic field B point directly to the right. (see Figure A)

First, the field will exert no force on the two width segments of the wire as in this length the current is parallel to the magnetic field. However, there will be a force on each of the lengths of the rectangular loop as the current is perpendicular to the field on that segment. The magnitude of these forces is:

Formula

Notice that these two forces are equal and opposite in magnitude, so there is no translational movement, but there is a torque about the center of the loop. The two torques from the forces can be calculated as:

Formula
where A is the area of the loop. The two torques are both accelerating the loop clockwise, so the total torque is:

Formula

A rectangle of current loop is sitting vertical to the page with force arrows pointing out from all sides. There is  a magnetic field line pointing perpendicularly at it from behind, and the current is traveling counterclockwise.
Figure B
copyright
Copyright © Eric Appelt, 2006

Once the loop is fully rotated, the forces appear in the configuration shown to the right. Notice that there is no longer any torque, but outward force in every direction. The forces on the width elements never contribute to the torque, but rather attempt to stretch the loop. At any angle during the rotation, the torque could be written as:

Formula

Generalizing further, imagine if the current loop actually consisted of N turns. While this would have no effect on the purely electrical properties of the circuit (assuming no resistance in the wire) the amount of current contributing to the magnetic force on the wire would be effectively multiplied by N. Thus,

: A loop of counterclockwise current is diagonal on the page with a vector pointing perpendicularly up through the center.
Figure C
copyright
Copyright © 2006 Eric Appelt, Vanderbilt University

Formula

We will define the magnetic moment of the current loop as a vector normal to the plane of the loop directed according to the right hand rule with respect to the current (see diagram). The magnitude of this vector will be NAI , and the vector will be denoted μ. With this definition, we can write:

Formula

This can be shown to work if the loop is not rectangular, and is valid for any loop in a plane. Note that the torque will accelerate the loop so that the magnetic moment will become parallel to the field.

Example:

A circular wire loop of 5 turns with a radius of 10 cm weighing 54 g with a current of 1.3 A is lying flat on a table. A strong uniform magnetic field of 3 T is projected up 30 degrees from the horizontal, as shown in the diagram. Find the magnitude of the torque on the current loop.

: A loop of wire is horizontal to the page with a magnetic field pointing up and to the left.
Figure D
copyright
Copyright © 2006 Eric Appelt, Vanderbilt University

Solution: Start by drawing the picture and labeling accordingly!

Formula

Note that the gravitational torque on this loop is

Formula

So the magnetic torque will rotate part of the loop off the table!

Energy of a Current Loop in a Magnetic Field

When a current loop is rotated through an (infinitesimally) small angle

dΘ
, the work done is

Formula
(Negative as the magnetic torque works to decrease the angle)

Then the decrease in potential energy is

Formula

And so by integrating

Formula

Since it is only the change in potential energy that we are ever interested in, we can simply make a convention for when the potential energy is zero, and get rid of

Formula
. In this case, if we say that the potential energy is zero at 90 degrees, then
Formula
.

Then,

Formula

Note that the potential energy is lowest when μ and B are parallel and there is no torque. It is highest when μ and B are antiparallel. In the antiparallel case, a slight nudge in either direction will create a torque sending it back towards the parallel position.

Example:

A solid hoop of copper with radius 35 cm weighing 200 g is bolted to a stand so that it may rotate freely as shown in the diagram below. A current of 5.5 A is sent around the hoop, and a uniform magnetic field of 2000 Gauss is directed up. Describe the motion of the hoop. What is the maximum kinetic energy of the hoop? What is the maximum angular velocity?

A loop of wire is connected at the sides to a stand, with a magnetic field pointing directly up at the wire
Figure E
copyright
Copyright © 2006 Eric Appelt, Vanderbilt University

Solution: Start by drawing the picture and labeling accordingly!

The hoop will oscillate back and forth, with a maximum kinetic energy when the hoop is oriented horizontally and will momentarily halt whenever it is vertical.

The initial potential energy is zero, and the minimum potential energy when the magnetic moment lines up with the field is

Formula

So the maximum kinetic energy is

K = -U = 0.423J

The moment of inertia of the hoop is

Formula
and
Formula

Thus

Formula

This is very close to 1 full rotation per second!

As a final note, one may notice that permanent magnets such as a compass needle have a tendency to rotate into the plane of a field, suggesting that they are comprised of a current loop. In fact, a permanent magnet can be explained as a collection of many tiny current loops, and from this model we will be able to explain the phenomena of attraction and repulsion.

Associated Activities

Attachments

Assessment

Homework: Assign students to complete the Current Loops in Magnetic Fieilds Homework set, which serves as an assessment tool.

Contributors

Eric Appelt

Copyright

© 2013 by Regents of the University of Colorado; original © 2006 Vanderbilt University

Supporting Program

VU Bioengineering RET Program, School of Engineering, Vanderbilt University

Acknowledgements

The contents of this digital library curriculum were developed under National Science Foundation RET grant nos. 0338092 and 0742871. However, these contents do not necessarily represent the policies of the NSF, and you should not assume endorsement by the federal government.

Last modified: July 20, 2017

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