The Setup
A Circuit in Waiting
Imagine a circuit where a resistor R and a capacitor C are connected in series with a direct current battery E. In parallel with the capacitor, we have a neon bulb. This bulb is a fascinating component; it acts like an open switch until the voltage across it reaches a specific threshold. In our case, this threshold is 120 V.
Because the neon bulb is filled with gas, its initial resistance is practically infinite. This means that before it lights up, no current flows through the bulb's branch. The circuit behaves exactly like a simple, standard RC charging circuit.
The Charging Phase
Building Up the Voltage
As soon as the switch is closed, the battery starts pushing charge onto the capacitor plates through the resistor. The voltage across the capacitor doesn't jump instantly; it builds up over time according to the classic charging equation:
We are given that the battery voltage E is 200 V. The bulb lights up when the capacitor voltage Vc reaches 120 V exactly at time t=5 s. Let's substitute these known values into our equation to see what we get:
The Math
Solving for Resistance
Now, the goal is to isolate our unknown variable, the resistance R. First, let's simplify the equation by dividing both sides by 200:
This simplifies neatly to 53.
Rearranging the terms to isolate the exponential part, we move the exponential to the left and 53 to the right:
To bring the variables down from the exponent, we need to take the natural logarithm (ln) of both sides.
−RC5=ln(2)−ln(5)=−ln(25)=−ln(2.5)
The negative signs on both sides cancel out beautifully, leaving us with:
Rearranging this to solve for R, we get:
The Grand Finale
Calculating the Value
We are given the value of the base-10 logarithm, log10(2.5)=0.4. To use this, we must convert our natural logarithm to a base-10 logarithm using the conversion factor 2.303:
Now, let's substitute all our values, including the capacitance C=2μF=2×10−6 F:
Let's crunch the numbers in the denominator: 2×0.4=0.8, and 0.8×2.303≈1.8424.
Dividing 5 by 1.8424 gives approximately 2.71. The 10−6 in the denominator moves to the numerator as 106.
And there we have it! The required resistance is 2.7×106Ω, which matches option (b). This setup is a classic example of a relaxation oscillator, where the RC time constant dictates the rhythm of the flashing bulb.