In an alternating current circuit a voltage source V = 100 sin (100 pit), a resistance of 10 ohm and an inductance of 1/(10 pi) henry, all are connected in series. Find out the power dissipated in the circuit: (1) 300 watt (2) 400 watt (3) 500 watt (4) 250 watt'
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Series R L circuit. with AC voltage source.
V = 100 Sin (100π t)
ω = 100 π rad/sec => f = ω/2π = 50 Hz
R = 10 Ω , L = 0.1/π Henry
X_L = inductive reactance = ω L = 100π 0.1/π = 10 Ω
Z = impedance in the circuit = √[ R² + X_L² ] = √[10²+10²] = 10√2 Ω
V_rms = V_max / √2 = 100/√2 volts
I_rms = V_rms / Z = 100/(√2 10√2) = 5 Amperes
Power discharged by the voltage source = V_rms I_rms = 500/√2 VA
(all this power is not lost.. energy in Inductor is not lost)
Real power discharged (dissipated) by the resistor as heat = I_rms² R
= 5² * 10 = 250 Watts
Alternately:
TanФ = phase difference between currents in L and R: X_L / R = 1
Ф = π/4
Cos Ф = power factor = Cos π/4 = 1/√2
Real power = Reactive power * power factor = 500/√2 VA * cosФ = 250 Watts
Power is stored and then released alternately in the inductor... Dissipation takes place only in the resistor in all RLC circuits.
V = 100 Sin (100π t)
ω = 100 π rad/sec => f = ω/2π = 50 Hz
R = 10 Ω , L = 0.1/π Henry
X_L = inductive reactance = ω L = 100π 0.1/π = 10 Ω
Z = impedance in the circuit = √[ R² + X_L² ] = √[10²+10²] = 10√2 Ω
V_rms = V_max / √2 = 100/√2 volts
I_rms = V_rms / Z = 100/(√2 10√2) = 5 Amperes
Power discharged by the voltage source = V_rms I_rms = 500/√2 VA
(all this power is not lost.. energy in Inductor is not lost)
Real power discharged (dissipated) by the resistor as heat = I_rms² R
= 5² * 10 = 250 Watts
Alternately:
TanФ = phase difference between currents in L and R: X_L / R = 1
Ф = π/4
Cos Ф = power factor = Cos π/4 = 1/√2
Real power = Reactive power * power factor = 500/√2 VA * cosФ = 250 Watts
Power is stored and then released alternately in the inductor... Dissipation takes place only in the resistor in all RLC circuits.
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