INDUCTIVE AC CIRCUITS
Inductors, like capacitors,
oppose current flow in AC circuits. They may also introduce a phase shift
between the voltage and the current in AC circuits. A large number of
electronic circuits are composed of inductors and resistors.
INDUCTORS IN AC CIRCUITS
Inductors in AC circuits
offer opposition to current flow. When an AC voltage is placed across an
inductor, it creates a magnetic field. As the AC voltage changes polarity, it
causes the magnetic field to expand and collapse. It also induces a voltage in
the inductor coil. This induced voltage is called a counter electromotive force (cemf); the greater the inductance, the
greater the cemf. The cemf is out of phase with the applied voltage by 180° and opposes the applied voltage. This opposition is as effective
in reducing current flow as a resistor.
The applied voltage and the induced voltage are 180° out of phase with each other in an inductive circuit.
The amount of voltage
induced in the inductor depends on the rate of change of the magnetic field.
The faster the magnetic field expands and collapses, the greater the induced
voltage. The total effective voltage across the inductor is the difference
between the applied voltage and the induced voltage. The induced voltage is
always less than the applied voltage.
Figure below shows the relationship of the current to the applied voltage. In a purely inductive circuit, the current lags behind the applied voltage by 90°.
The current lags the applied voltage in an AC inductive circuit.
Another way of stating this is that the
applied voltage leads the current by 90° in a pure inductive current. This can
be represented by the acronym ELI. Voltage (E) leads current (I) in an
inductive (L) circuit.
The opposition offered to
current flow by an inductor in an AC circuit is called inductive reactance and
is measured in ohms. The amount of inductive reactance offered by an inductor
depends on its inductance and the frequency of the applied voltage. The larger
the inductance, the larger the magnetic field generated and the greater the
opposition to current flow. Also, the higher the frequency, the greater the
opposition the inductor has to current flow.
The impedance of a circuit
containing both inductance and resistance is the total opposition to current
flow by both the inductor and the resistor. Because of the phase shift caused
by the inductor, the inductive reactance and the resistance cannot be added
directly.
The impedance (Z) is the vector sum of the inductive reactance and the resistance in the circuit. The impedance is expressed in ohms and is designated by the letter Z. Impedance can be defined in terms of Ohm’s law as:
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