The Anatomy of a Real Circuit
Welcome! Let's visualize the circuit we are dealing with. We have a battery with an internal resistance of 0.9 Ω, and it is connected to a real inductor.
It is crucial to remember that a real inductor isn't perfect; it is made of a long wire, which means it has its own small resistance. In this case, the coil's resistance is 0.1 Ω. The moment we close the switch, the inductor opposes the sudden change, and the current will start to flow and grow gradually rather than instantly jumping to its maximum value.
The Mathematics of Growth
To find how the current grows over time, we use the standard L−R circuit growth equation. The current i at any time t is given by:
Here, i0 is the maximum saturation current that the circuit will eventually reach after a long time, and Req is the total equivalent resistance of the circuit.
Crunching the Numbers
First, let's find the total equivalent resistance. Since the internal resistance of the battery and the resistance of the coil are connected in series, we simply add them up:
The question asks for the time when the current reaches 80% of its maximum value. So, we substitute i as 0.8i0 into our growth equation:
The i0 on both sides cancels out beautifully. We are left with:
Rearranging this, we bring the exponential term to the left and subtract 0.8 from 1, which gives us 0.2:
Applying Natural Logarithms
Notice that 0.2 is exactly 51. If we take the reciprocal of both sides, the negative sign in the exponent disappears:
Taking the natural logarithm on both sides, the exponent comes down:
The Final Countdown
We are almost there! Let's substitute the values and get the answer. The inductance L is 10 mH, which is 10×10−3 H. The problem gives us ln5 as 1.6.
Multiplying these out, 10×1.6 is 16. So, the time t is:
This matches option (d) perfectly!
The Time Constant (τ)
Think about this: the quantity RL is called the time constant of the circuit, often denoted by τ. It tells us how sluggish the circuit is. A larger inductance or a smaller resistance means the current takes much longer to reach its maximum value. In our circuit, τ=10 ms. Understanding this helps you intuitively grasp how fast any L−R circuit will respond to changes.