1
|
|
2
|
- Common form of an inductor is a coil of wire
- Used in radio tuning circuits
- In fluorescent lights
|
3
|
- On power systems
- Part of the protection circuitry used to control short-circuit currents
during faults
|
4
|
- Voltage is induced
- When a magnet moves through a coil of wire
- When a conductor moves through a magnetic field
|
5
|
- Change in current in one coil can induce a voltage in a second coil
- Change in current in a coil can induce a voltage in that coil
|
6
|
- Faraday’s Law
- Voltage is induced in a circuit whenever the flux linking the circuit
is changing
- Magnitude of voltage is proportional to rate of change of the flux
linkages with respect to time
|
7
|
- Lenz’s Law
- Polarity of the induced voltage opposes the cause producing it
|
8
|
- If a constant current is applied
- If current is increased
- Inductor will develop a voltage with a polarity to oppose increase
|
9
|
- If current is decreased
- Voltage is formed with a polarity that opposes decrease
|
10
|
- Have flux almost entirely confined to their cores
- Flux lines pass through the windings
- Flux linkage as product
- Flux times number of turns
|
11
|
- By Faraday’s law
- Induced voltage is equal to rate of change of NF
|
12
|
- All flux lines do not pass through all of the windings
- Flux is directly proportional to current
- Induced voltage directly proportional to rate of change of current
|
13
|
- Voltage induced in a coil is proportional to rate of change of the
current
- Proportionality constant is L
- Self-inductance of the coil-units are Henrys (H)
|
14
|
- Inductance of a coil is one Henry
- If the voltage created by its changing current is one volt
- When its current changes at rate of one amp per second
|
15
|
- Inductance of a coil is given by
- l is the length of coil in meters
- A is cross-sectional area in square meters
- N is number of turns
- µ is permeability of core
|
16
|
- If air gap is used, formula for inductance is
- Where µo is permeability of air
- Ag is area of air gap
- lg is length of
gap
|
17
|
- When using equation
- If current is increasing, voltage is positive
- If current is decreasing, voltage is negative
- Di/Dt is slope for currents described with straight lines
|
18
|
- For inductors in series
- Total inductance is sum of individual inductors (similar to resistors
in series)
|
19
|
- Inductors in parallel add as resistors do in parallel
|
20
|
- Type of core depends on intended use and frequency range
- For audio or power supply applications
- Inductors with iron cores are generally used
|
21
|
- Iron-core inductors
- Large inductance values but have large power losses at high frequencies
- For high-frequency applications
- Ferrite-core inductors are used
|
22
|
- Used in tuning circuits
- Inductance may be varied by changing the coil spacing
- Inductance may be changed by moving a core in or out
|
23
|
|
24
|
- Turns of inductors are separated by insulation
- May cause stray or parasitic capacitance
- At low frequencies, it can be ignored
- At high frequencies, it must be taken into account
- Some coils are wound in multiple sections to reduce stray capacitance
|
25
|
- Current-carrying components have some stray inductance
- Due to magnetic effects of current
- Leads of resistors, capacitors, etc. have inductance
- These leads are often cut short to reduce stray inductance
|
26
|
- Voltage across an inductance with constant dc current is zero
- Since it has current but no voltage, it looks like a short circuit at
steady state
- For non-ideal inductors
- Resistance of windings must be considered
|
27
|
- When energy flows into an inductor
- Energy is stored in its magnetic field
- When the field collapses
- Energy returns to the circuit
|
28
|
- No power is dissipated, so there is no power loss
- Energy stored is given by
|
29
|
- Use ohmmeter
- Open coil will have infinite resistance
- Coil can develop shorts between its windings causing excessive current
- Checking with an ohmmeter may indicate lower resistance
|