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Inspiring experiments exploit strong attraction of magnets

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F RONTLINE<br />

M AGNETISM<br />

<<strong>strong</strong>>Inspiring</<strong>strong</strong>> <<strong>strong</strong>>experiments</<strong>strong</strong>> <<strong>strong</strong>>exploit</<strong>strong</strong>><br />

<strong>strong</strong> <strong>attraction</strong> <strong>of</strong> <strong>magnets</strong><br />

The extra strength <strong>of</strong> neodymium iron boron <strong>magnets</strong><br />

provides opportunities for several <<strong>strong</strong>>experiments</<strong>strong</strong>><br />

(Featonby 2005). Here is a further selection that<br />

should encourage you to think <strong>of</strong> even more.<br />

Single-wire motor<br />

A<strong>strong</strong> neodymium disc magnet with a small cylindrical<br />

magnet is placed below a 1.5 V cell (figure 1).<br />

A copper wire frame is then bent into the shape<br />

shown, with a loop at the bottom, which makes contact<br />

with the cylindrical magnet. The size <strong>of</strong> this<br />

loop needs to be slightly bigger than the smaller<br />

magnet so that it is able to move freely, but still make<br />

good electrical contact. The top <strong>of</strong> the wire frame<br />

rests on top <strong>of</strong> the cell to complete the circuit.<br />

The magnet holds the cell balanced in the vertical<br />

position as well as being part <strong>of</strong> the circuit. The<br />

current will, in this case, flow outwards from the<br />

cylindrical magnet along and up both sides <strong>of</strong> the<br />

wire. It is the forces on the horizontal lower wire<br />

that provide the couple to rotate the whole frame.<br />

The copper frame used was obtained by stripping<br />

some 13 A mains cable containing 1 mm diameter<br />

copper wire, and this frame is approximately<br />

0.09 × 0.11 m. It is worth trying different-sized<br />

frames to achieve a good effect. The key is to keep<br />

the moment <strong>of</strong> inertia <strong>of</strong> the frame small.<br />

Simple motor with single magnet<br />

Asimilar arrangement has been described in a recent<br />

issue <strong>of</strong> Physics Education, but details are repeated<br />

here with some additional information. The <strong>strong</strong><br />

neodymium disc magnet holds the nail onto the bottom<br />

<strong>of</strong> the cell, but it is still free to rotate (figure 2).<br />

In this case it is the current flowing through the<br />

magnet that generates the force that rotates the<br />

magnet/nail arrangement. Avariety <strong>of</strong> magnet sizes<br />

can be used to demonstrate this. I have used discs<br />

from about 10 mm in diameter.<br />

I have also successfully used both flexible and<br />

rigid copper wire, and also a strip <strong>of</strong> aluminium foil<br />

to make the connection between the top <strong>of</strong> the<br />

Figure 1. Single copper wire rotating motor.<br />

1.5 V<br />

dry cell<br />

steel nail<br />

(2 inch)<br />

neodymium<br />

button<br />

magnet<br />

connecting wire<br />

magnetic field<br />

(within magnet)<br />

current<br />

steel nail<br />

neodymium magnet<br />

Figure 2. A simple motor made from a<br />

neodymium button magnet holding a 2 inch steel<br />

nail onto the bottom <strong>of</strong> a 1.5 V cell.<br />

battery and the magnet. The nail must be attached<br />

to the exact centre <strong>of</strong> the rotating magnet to produce<br />

steady motion.<br />

Rolling wire and kicking wire<br />

During many years <strong>of</strong> teaching I used to demonstrate<br />

the force on a conductor by rolling a thick<br />

piece <strong>of</strong> brass rod down two brass curtain rails<br />

(figure 3). This was possible using an Alnico magnet<br />

held above the wire, producing a vertical field.<br />

The disadvantage <strong>of</strong> this arrangement is that the magnet<br />

has to be moved to keep the wire moving.<br />

Asimilar experiment was carried out using a large<br />

Alnico U magnet (figure 4). The vertical field <strong>of</strong> the<br />

magnet is at right-angles to the current and the subsequent<br />

motion. The problem with this experiment is<br />

292 P HYSICS E DUCATION July 2006


Figures 3 and 4. The rolling wire (top image): a<br />

demonstration <strong>of</strong> the force on a conductor<br />

achieved by rolling a thick piece <strong>of</strong> brass rod along<br />

a pair <strong>of</strong> brass curtain rails using an Alnico<br />

magnet held above the wire to produce a vertical<br />

field. The kicking wire (bottom): a large Alnico U<br />

magnet is used to produce a vertical field at rightangles<br />

to the current and to the subsequent motion.<br />

the expense <strong>of</strong> the large Alnico magnet, but a similar<br />

effect can be obtained with magnadur <strong>magnets</strong>.<br />

With neodymium iron boron <strong>magnets</strong> a kicking<br />

wire can be set up for less than £5 by mounting<br />

a single round neodymium magnet in a hole in a<br />

block <strong>of</strong> wood and using a trapeze-style copper<br />

frame (figure 5).<br />

Double magnet roller<br />

We can use neodymium disc <strong>magnets</strong> as both the<br />

wheels <strong>of</strong> a roller and the source <strong>of</strong> the magnetic<br />

field. In this set-up (figure 6) two discs are placed<br />

carefully on the smoothed, flat end <strong>of</strong> a nail with its<br />

head cut <strong>of</strong>f. It is important that the nail axle is<br />

aligned exactly with the centres <strong>of</strong> the <strong>magnets</strong> to<br />

produce a good run. The strength <strong>of</strong> the neodymi-<br />

July 2006<br />

F RONTLINE<br />

Figure 5. Kicking wire set-up using a neodymium<br />

magnet and a copper wire trapeze frame. The<br />

wire carries the current across the top <strong>of</strong> the<br />

magnet and the force causes the frame to move.<br />

nail shaft<br />

aluminium foil<br />

neodymium magnet<br />

magnetic field<br />

inside magnet<br />

current<br />

Figure 6. Rolling motor (shaft <strong>of</strong> nail) with two<br />

neodymium disc <strong>magnets</strong>, with explanation.<br />

ums enables them to be fixed with like poles facing<br />

each other. This is essential to produce a turning<br />

force on both wheels in the same sense. The tracks<br />

are two strips <strong>of</strong> aluminium foil, stuck to the bench<br />

with overhanging ends for electrical contacts. The<br />

current flows down the aluminium and up through<br />

one magnet, along the nail and down through the<br />

P HYSICS E DUCATION 293


F RONTLINE<br />

Figure 7. Another simple motor that uses a<br />

neodymium magnet with a bolt through its centre.<br />

Figure 9. ‘Loudspeaker’with cardboard box.<br />

other. The forces arise within the magnetic wheels<br />

and the arrangement accelerates down the track.<br />

Other motors<br />

In figure 7 a ring magnet has a bolt through its centre<br />

and lies on a copper circuit board. The magnet makes<br />

contact outside a circle etched in the board and a pin<br />

though the centre enables contact to be made there.<br />

In figure 8 a strip <strong>of</strong> aluminium foil rotates rapidly<br />

on top <strong>of</strong> the <strong>magnets</strong>. Contact is made to the<br />

central part <strong>of</strong> the rotating foil with some pencil lead,<br />

while the foil touches the outside <strong>of</strong> the <strong>magnets</strong>.<br />

Loudspeaker<br />

The strength <strong>of</strong> the neodymium magnet can be<br />

shown with a simple ‘loudspeaker’(figure 9). Acoil<br />

<strong>of</strong> thin copper wire is taped to the surface <strong>of</strong> a shoe<br />

box with the leads connected to the earphone output<br />

<strong>of</strong> a portable hi-fi. Simply bring up a neodymium<br />

magnet and the forces on the coil move it to produce<br />

sound from the box. Varying the position <strong>of</strong><br />

the magnet and hence the strength <strong>of</strong> the field at the<br />

coil greatly affects the volume <strong>of</strong> the sound.<br />

Figure 8. A motor arrangement using a piece <strong>of</strong><br />

aluminium foil rotating rapidly on top <strong>of</strong> <strong>magnets</strong>.<br />

Figure 10. A simple<br />

but effective loudspeaker<br />

unit that uses<br />

a piece <strong>of</strong> aluminium<br />

foil over a large<br />

neodymium magnet<br />

and passes the<br />

output from a radio<br />

through the<br />

aluminium foil layer.<br />

Even simpler is to lay a small piece <strong>of</strong> aluminium<br />

foil over a large neodymium magnet and pass the<br />

output from a radio through the foil (figure 10). The<br />

sound from the radio is clearly heard. This set-up<br />

can also be used as a simple microphone.<br />

You may by now be thinking that neodymium <strong>magnets</strong><br />

are the best thing since sliced bread, but with<br />

their strength come disadvantages. Neodymium iron<br />

boron is susceptible to corrosion if unprotected,<br />

though this will not be <strong>of</strong> great concern to us because<br />

commercially available <strong>magnets</strong> are coated.<br />

Curie temperature<br />

Of more concern is the Curie temperature. At only<br />

120 ºC neodymium <strong>magnets</strong> cease to be magnetic,<br />

although this loss can be recovered by remagnetization.<br />

The comparable temperature for ferrite<br />

<strong>magnets</strong> is 250 ºC and for Alnico it is 550 ºC. The<br />

loss in magnetism in neodymium is irreversible at<br />

320 ºC compared with 860 ºC for Alnico.<br />

This low Curie temperature for neodymium can<br />

be demonstrated simply by using a tealight candle<br />

as a heat source (figure 11). A small neodymium<br />

294 P HYSICS E DUCATION July 2006


Figure 11. Demonstration <strong>of</strong> the Curie temperature.<br />

ring magnet is suspended on a swing cradle made<br />

<strong>of</strong> thick copper wire, which is in turn suspended on<br />

a frame <strong>of</strong> the same copper wire. This small magnet<br />

is attracted to a larger, fixed neodymium magnet<br />

(25 × 5 mm). When the candle is lit, it heats up<br />

the small magnet, which then loses its magnetism<br />

and falls back with the swing in the vertical position.<br />

This, however, takes it out <strong>of</strong> the flame and<br />

enables it to cool, be remagnetized and attracted<br />

once more to the larger magnet. Here it is again in<br />

the flame, so it heats and loses its magnetism again,<br />

F RONTLINE<br />

and the cycle repeats. The overall size <strong>of</strong> my demonstration<br />

can be seen from the size <strong>of</strong> the tealight<br />

used. Considerable testing is required to produce a<br />

reliable demonstration.<br />

Safety warning<br />

Neodymium <strong>magnets</strong> are dangerous because <strong>of</strong> their<br />

strength and the fact that they shatter easily. They<br />

should not be given to children to use unsupervised.They<br />

should be kept away from electronic<br />

apparatus and the magnetic strips on bank cards.<br />

References<br />

Featonby D 2005 Phys. Educ. 40 505–8<br />

Neodymium <strong>magnets</strong> are available from<br />

www.power<strong>magnets</strong>tore.co.uk<br />

www.sci-toys.com/scitoys/electro has<br />

instructions about how to construct a number <strong>of</strong><br />

<<strong>strong</strong>>experiments</<strong>strong</strong>> using neodymium <strong>magnets</strong><br />

www.wondermagnet.com also has some<br />

interesting <<strong>strong</strong>>experiments</<strong>strong</strong>><br />

www.amasci.com/neodemo.html includes some<br />

neodymium demonstrations<br />

David Featonby, North East Teacher Network<br />

coordinator.

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