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handbook of modern sensors

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3.3 Magnetism 55<br />

3.3.3 Toroid<br />

Another useful device that can produce a magnetic field is a toroid (Fig. 3.14B), which<br />

we can describe as a solenoid bent into the shape <strong>of</strong> a doughnut. A calculation <strong>of</strong> the<br />

magnetic field inside the toroid gives the following relationship:<br />

B = µ 0 i 0 N<br />

2π r , (3.32)<br />

where N is the total number <strong>of</strong> turns and r is the radius <strong>of</strong> the inner circular line where<br />

the magnetic field is calculated. In contrast to a solenoid, B is not constant over the<br />

cross section <strong>of</strong> a toroid. Also, for an ideal case, the magnetic field is equal to zero<br />

outside a toroid.<br />

The density <strong>of</strong> a magnetic field, or the number <strong>of</strong> magnetic lines passing through<br />

a given surface, is defined as the magnetic flux B for that surface:<br />

∫<br />

B = B dS. (3.33)<br />

The integral is taken over the surface, and if the magnetic field is constant and is<br />

everywhere at a right angle to the surface, the solution <strong>of</strong> the integral is very simple:<br />

B = BA, where A is the surface area. Flux, or flow <strong>of</strong> the magnetic field, is analogous<br />

to the flux <strong>of</strong> electric field. The SI unit for magnetic flux, as follows from the above,<br />

is tesla meter 2 , to which is named weber. It is abbreviated as Wb:<br />

1Wb = 1T m 2 . (3.34)<br />

3.3.4 Permanent Magnets<br />

Permanent magnets are useful components for fabricating magnetic <strong>sensors</strong> for the<br />

detection <strong>of</strong> motion, displacement, position, and so forth. To select the magnet for<br />

any particular application, the following characteristics should be considered:<br />

• Residual inductance (B) in gauss—how strong the magnet is<br />

• Coercive force (H ) in oersteds—how well will the magnet resist external demagnetization<br />

forces<br />

• Maximum energy product, MEP, (BH ) is gauss oersteds times 10 6 . A strong<br />

magnet that is also very resistant to demagnetization forces has a high MEP.<br />

Magnets with a higher MEP are better, stronger, and more expensive.<br />

• The temperature coefficient in %/ ◦ C shows how much B changes with temperature.<br />

Magnets are produced from special alloys (see Table A.6). Examples are rare<br />

earth (e.g., samarium)–cobalt alloys. These are the best magnets; however, they are<br />

too hard for machining and must be ground if shaping is required. Their maximum<br />

MEP is about 16 × 10 6 . Another popular alloy is Alnico, which contains aluminum,<br />

nickel, cobalt, iron, and some additives. These magnets can be cast or sintered by

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