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Electronics - Analogue
10. Inductors
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Inductors
Coils
Chokes
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Basic Inductor
Coil
of
wire
3D field
Field of each
coil
adds to form a strong
magnetic
field
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Faraday's Law
Vind = N dF/dt
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Self inductance
(L)
Measure of a
coil's
ability to establish an
induced voltage
as a result of a change in its current
Unit is
Henry
(H)
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Current through inductor
Magnetic field
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Change in
current
Magnetic field changes
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Induced voltage via
self
inductance
Opposes
the change in
current
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Lenz's
Law
When the current through a coil changes, an
induced voltage
is created as a result of the changing magnetic field and the direction of the induced voltage is such that it always
opposes
the change in current
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Induced voltage
Depends on
L
and
di/dt
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Energy Storage
Stores
energy
in the
magnetic field
created by the current
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Physical characteristics of inductors
Cross
sectional area
A
Core material
(magnetic or non-magnetic)
Number of
turns
(N)
D.C. resistance
or
winding resistance
(Rw)
Winding Capacitance
(Cw)
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Inductors in Series
LT = L1 +
L2
+
L3
+ ... = LN
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Parallel
Inductors
Total
inductance
<
smallest
inductance
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Inductors in D.C. Circuits
No induced voltage when current is constant
Inductor appears as
short
to D.C.
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Time Constant
t = L/
R
Inductors action
opposes
a change in current
Current
cannot
change instantaneously
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Energising and De-energising Inductors
1.
Exponential increase
and
decrease
in current
2.
Time constant
t =
L/R
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Induced voltage in the Series RL Circuit
Prevents
current from changing instantaneously
L acts as
open
circuit to
non-changing
current
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Voltage in RL circuit as inductor de-energises
Induced voltage
opposes
change in
steady
state current
All energy stored in inductor in magnetic field is
dissipated
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Instantaneous VL when SW1 is closed =
25V
, after 5t VL =
0V
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Instantaneous VL when SW1 opens and SW2 closes =
208V
, after 5t VL =
0V
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Exponential Formulae
For
increasing
and
decreasing
current in inductors
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Current and voltage in inductor
Current
lags
inductor voltage by
90°
Faster
the rate of change of current the larger the
induced voltage
VL
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Inductive Reactance (XL)
Opposition to
sinusoidal
current
Increases
with frequency
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In AC circuits with inductors, current
lags
voltage by
90°
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Ohm's Law in AC circuits with inductors
R
replaced by
XL
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Power in an inductor
Instantaneous power p=
vi
True power ideally
0
, practically (
Irms
)^2 * Rw
Reactive power Pr=VrmsIrms=Vrms^
2/XL
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Quality Factor (Q) of a coil
Q = XL/Rw
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Inductor Applications
Power supply
filter
RF
choke
Tuned
circuits
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Testing Inductors
Ohmmeter - open reads infinity,
good
reads Rw,
shorted windings
reads lower Rw
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