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When the frequency is high, the capacitive reactance is low. This is why a capacitor allows the flow of high frequency AC because its reactance decreases with increasing frequency.
Inductance (measured in henries, symbol H) is a measure of the generated emf for a unit change in current. For example, an inductor with an inductance of 1 H produces an emf of 1 V when the current through the inductor changes at the rate of 1 A s .
An inductor is a passive electrical device used in electrical circuits for its property of inductance. An inductor is usually made as a coil (or solenoid) of conducting material, typically copper wire, wrapped around a core either of air or of ferromagnetic material.
Electrical current through the conductor creates a magnetic flux proportional to the current. A change in this current creates a change in magnetic flux that, in turn, generates an emf that acts to oppose this change in current.
The inductance of an inductor is determined by several factors:
The inductance of a solenoid is defined by:
where is the permeability of the core material (in this case air), is the cross-sectional area of the solenoid, is the number of turns and is the length of the solenoid.
Permeability is the property of a material which describes the magnetisation developed in that material when excited by a source.
The permeability of free space is henry per metre.
Determine the inductance of a coil with a core material of air. A cross-sectional area of , with 1000 turns and a length of 0,1 m
We are calculating inductance, so we use the equation:
The permeability is that for free space: henry per metre.
The inductance of the coil is H/m.
Calculate the inductance of a 5 cm long solenoid with a diameter of 4 mm and 2000 turns.
Again this is an inductance problem, so we use the same formula as the worked example above.
An inductor in an AC circuit also has a reactance, . Reactance is the property of an inductor that opposes the flow of AC current. Reactance is defined by:
where is the inductance and is the frequency of the AC.
If we examine the equation for the reactance of an inductor, we see that inductive reactance increases with increasing frequency. Therefore, when the frequency is low, the inductive reactance is very low. This is why an inductor allows the flow of DC and low frequency AC because its reactance decreases with decreasing frequency.
When the frequency is high, the inductive reactance is high. This is why an inductor blocks the flow of high frequency AC because its reactance increases with increasing frequency.
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