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478 ⏐⏐⏐ INDUCTORS<br />

Type: Open Core Coil<br />

Typical Values: 3 mH to 40 mH<br />

Applications: Used in low-pass<br />

filter circuits. Found in speaker<br />

crossover networks.<br />

Type: Toroid Coil<br />

Typical Values: 1 mH to 30 mH<br />

Applications: Used as a choke in AC<br />

power lines circuits to filter transient<br />

and reduce EMI interference. This<br />

coil is found in many electronic<br />

appliances.<br />

Type: Hash Choke Coil<br />

Typical Values: 3 µ H to 1 mH<br />

Applications: Used in AC supply<br />

lines that deliver high currents.<br />

Type: Delay Line Coil<br />

Typical Values: 10 µ H to 50 µ H<br />

Applications: Used in color<br />

televisions to correct for timing<br />

differences between the color<br />

signal and black and white signal.<br />

Type: Common Mode Choke Coil<br />

Typical Values: 0.6 mH to 50 mH<br />

Applications: Used in AC line filters,<br />

switching power supplies, battery<br />

charges and other electronic equipment.<br />

Fiber<br />

insulator<br />

3"<br />

Coil<br />

Plastic tube<br />

Inner<br />

core<br />

Type: RF Chokes<br />

Typical Values: 10 µ H to 50 µ H<br />

Applications: Used in radio,<br />

television, and communication<br />

circuits. Found in AM, FM, and<br />

UHF circuits.<br />

Type: Moiled Coils<br />

Typical Values: 0.1 µ H to 100 µ H<br />

Applications: Used in a wide variety<br />

of circuit such as oscillators, filters,<br />

pass-band filters, and others.<br />

Type: Surface Mounted Inductors<br />

Typical Values: 0.01 µ H to 100 µ H<br />

Applications: Found in many<br />

electronic circuits that require<br />

miniature components on<br />

multilayered PCB.<br />

Type: Adjustable RF Coil<br />

Typical Values: 1 µ H to 100 µ H<br />

Applications: Variable inductor<br />

used in oscillators and various RF<br />

circuits such as CB transceivers,<br />

televisions, and radios.<br />

FIG. 12.11<br />

Typical areas of application for inductive elements.<br />

12.6 INDUCED VOLTAGE<br />

The inductance of a coil is also a measure of the change in flux linking<br />

a coil due to a change in current through the coil; that is,<br />

L � N � df<br />

�<br />

di<br />

(H) (12.4)<br />

where N is the number of turns, f is the flux in webers, and i is the current<br />

through the coil. If a change in current through the coil fails to<br />

result in a significant change in the flux linking the coil through its center,<br />

the resulting inductance level will be relatively small. For this reason<br />

the inductance of a coil is sensitive to the point of operation on the<br />

hysteresis curve (described in detail in Section 11.8). If the coil is operating<br />

on the steep slope, the change in flux will be relatively high for a<br />

change in current through the coil. If the coil is operating near or in saturation,<br />

the change in flux will be relatively small for the same change<br />

in current, resulting in a reduced level of inductance. This effect is particularly<br />

important when we examine ac circuits since a dc level asso-

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