Animated Solution for Physics - Electromagnetic Induction: An arc lamp requires a direct current of 10 A at 80 V to function. If it is connected to a 220 V (rms), 50 Hz AC supply, the series inductor needed for it to work is close to
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Visualized Solution
Modeling the Arc Lamp
VDC=80 V
IDC=10 A
R=IDCVDC=1080=8Ω
AC Circuit Setup
Vrms=220 V
f=50 Hz
Irms=10 A
Z=IrmsVrms
Calculating Impedance
Z=10220=22Ω
Z=R2+XL2
22=82+XL2
Finding Inductive Reactance
222=82+XL2
484=64+XL2
XL2=484−64=420
XL=420Ω
Calculating Inductance
XL=2πfL
420=2π(50)L
L=100π420
L≈314.1620.49≈0.065 H
Why an Inductor?
Why not use a resistor to drop voltage?
Power loss in resistor: P=I2R
Power loss in ideal inductor: P=0
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The Sigma Insight: Alternating Current (AC) and Voltage
Solution Diagram
The Physics of the Arc Lamp
Why We Use Choke Coils
Imagine you have a powerful arc lamp that shines brilliantly, but it's a bit of a diva. It strictly demands a direct current (DC) of 10 A at 80 V. If you give it more, it burns out. If you give it less, it won't light up. Now, you only have a standard household AC supply of 220 V at 50 Hz. How do you safely connect this lamp without destroying it? This is a classic engineering problem that tests our understanding of AC circuits and impedance.
Modeling the Lamp
First, we need to understand the electrical characteristics of the arc lamp. Since it operates on DC, we can model it as a simple resistor. Using Ohm's Law (V=IR), we can find its resistance.
R=IDCVDC=1080=8Ω
So, our arc lamp is essentially an 8Ω resistor that needs exactly 10 A of current to function properly.
The Role of the Inductor
If we connect this 8Ω lamp directly to the 220 V AC supply, the current would be I=8220=27.5 A. This massive current would instantly destroy the lamp! We need to drop the excess voltage.
We could use a series resistor, but resistors dissipate energy as heat (P=I2R). Dropping that much voltage across a resistor would waste a huge amount of power. Instead, we use an inductor (often called a choke coil). An ideal inductor provides opposition to alternating current (called inductive reactance) but consumes zero average power. It's the perfect, energy-efficient solution!
The Master Equation
When we connect the inductor in series with the lamp, we create an L-R series circuit. The total opposition to current in this circuit is the impedance (Z). We know the circuit must allow exactly 10 A of current to flow from the 220 V supply.
Z=IrmsVrms=10220=22Ω
The impedance of an L-R series circuit is given by the phasor addition of resistance and inductive reactance:
Z=R2+XL2
Substituting our known values:
22=82+XL2
Final Calculation
Now, it's just a matter of algebra. Let's square both sides to remove the square root:
222=82+XL2
484=64+XL2
XL2=484−64=420
XL=420Ω
We know that inductive reactance is related to inductance (L) and frequency (f) by the formula XL=2πfL. Plugging in the frequency of 50 Hz:
420=2π(50)L
100πL=420
L=100π420
Since 420 is approximately 20.49, we get:
L≈314.1620.49≈0.065 H
Thus, an inductor of approximately 0.065 H is required to safely operate the arc lamp on the AC supply.