Obtain the answers (a) to (b) in Exercise 7.13 if the circuit is connected to a high frequency supply (240 V, 10 kHz). Hence, explain the statement that at very high frequency, an inductor in a circuit nearly amounts to an open circuit. How does an inductor behave in a dc circuit after the steady state?
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Given :
Inductance of Inductor =L= 0.5Hz
Resistance of resistor= R=100 ohms
Potential supply of voltage =v= 240V
Frequency of supply= 10kHz=10^ 4 Hz
Angular frequency= ω = 2πv = 2 x π x 10⁴ rad/s
a) Peak voltage,
Maximum current I0 = V0/(√ R2 + ω²L²)
= 240√2/√ (100)² x (2 π x 10⁴)² X (0.50)2²
= 1.1 X 10⁻² A
(b) For phase difference ɸ
tan ɸ = ωL/R = 2 x π x 10⁴ X 0.5/100 = 100 π
ɸ = 89.82° = 89.82 x π/180 rad
so, ωt = 89.82 x π/180
t = 89.82 x π/180 x 2 π x 10⁴ = 25 μs
I0 is very small. Hence at high frequencies, the inductor amounts to an open circuit.
after a steady state is achieved ω = 0.
[ Applicable to Dc circuit]
Hence inductor L behaves like a pure conducting object
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