Chapter 13
Inductors
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Common form of an inductor is a coil of
wire |
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Used in radio tuning circuits |
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In fluorescent lights |
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Part of ballast circuit |
Inductors
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On power systems |
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Part of the protection circuitry used
to control short-circuit currents during faults |
Electromagnetic Induction
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Voltage is induced |
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When a magnet moves through a coil of
wire |
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When a conductor moves through a
magnetic field |
Electromagnetic Induction
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Change in current in one coil can
induce a voltage in a second coil |
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Change in current in a coil can induce
a voltage in that coil |
Electromagnetic Induction
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Faraday’s Law |
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Voltage is induced in a circuit
whenever the flux linking the circuit is changing |
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Magnitude of voltage is proportional to
rate of change of the flux linkages with respect to time |
Electromagnetic Induction
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Lenz’s Law |
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Polarity of the induced voltage opposes
the cause producing it |
Induced Voltage and
Induction
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If a constant current is applied |
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No voltage is induced |
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If current is increased |
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Inductor will develop a voltage with a
polarity to oppose increase |
Induced Voltage and
Induction
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If current is decreased |
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Voltage is formed with a polarity that
opposes decrease |
Iron-Core Inductors
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Have flux almost entirely confined to
their cores |
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Flux lines pass through the windings |
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Flux linkage as product |
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Flux times number of turns |
Iron-Core Inductors
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By Faraday’s law |
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Induced voltage is equal to rate of
change of NF |
Air-Core Inductors
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All flux lines do not pass through all
of the windings |
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Flux is directly proportional to
current |
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Induced voltage directly proportional
to rate of change of current |
Self-Inductance
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Voltage induced in a coil is
proportional to rate of change of the current |
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Proportionality constant is L |
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Self-inductance of the coil-units are
Henrys (H) |
Self-Inductance
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Inductance of a coil is one Henry |
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If the voltage created by its changing
current is one volt |
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When its current changes at rate of one
amp per second |
Inductance Formulas
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Inductance of a coil is given by |
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l is the length of coil in meters |
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A is cross-sectional area in square
meters |
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N is number of turns |
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µ is permeability of core |
Inductance Formulas
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If air gap is used, formula for
inductance is |
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Where µo is permeability of
air |
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Ag is area of air gap |
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lg is length of gap |
Computing Induced Voltage
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When using equation |
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If current is increasing, voltage is
positive |
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If current is decreasing, voltage is
negative |
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Di/Dt is slope for currents described with
straight lines |
Inductances in Series
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For inductors in series |
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Total inductance is sum of individual
inductors (similar to resistors in series) |
Inductances in Parallel
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Inductors in parallel add as resistors
do in parallel |
Core Types
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Type of core depends on intended use
and frequency range |
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For audio or power supply applications |
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Inductors with iron cores are generally
used |
Core Types
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Iron-core inductors |
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Large inductance values but have large
power losses at high frequencies |
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For high-frequency applications |
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Ferrite-core inductors are used |
Variable Inductors
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Used in tuning circuits |
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Inductance may be varied by changing
the coil spacing |
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Inductance may be changed by moving a
core in or out |
Circuit Symbols
Stray Capacitance
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Turns of inductors are separated by
insulation |
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May cause stray or parasitic
capacitance |
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At low frequencies, it can be ignored |
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At high frequencies, it must be taken
into account |
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Some coils are wound in multiple
sections to reduce stray capacitance |
Stray Inductance
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Current-carrying components have some
stray inductance |
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Due to magnetic effects of current |
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Leads of resistors, capacitors, etc.
have inductance |
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These leads are often cut short to
reduce stray inductance |
Inductance and Steady
State DC
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Voltage across an inductance with
constant dc current is zero |
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Since it has current but no voltage, it
looks like a short circuit at steady state |
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For non-ideal inductors |
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Resistance of windings must be
considered |
Energy Stored by an
Inductance
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When energy flows into an inductor |
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Energy is stored in its magnetic field |
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When the field collapses |
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Energy returns to the circuit |
Energy Stored by an
Inductance
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No power is dissipated, so there is no
power loss |
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Energy stored is given by |
Troubleshooting Hints
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Use ohmmeter |
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Open coil will have infinite resistance |
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Coil can develop shorts between its
windings causing excessive current |
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Checking with an ohmmeter may indicate
lower resistance |