The Anatomy of a Voltmeter
Imagine you are holding a delicate moving coil galvanometer. It is a highly sensitive instrument designed to detect even the faintest trickle of electric current. However, if you were to connect it directly across a high-voltage source, the massive surge of current would instantly fry its delicate coil.
So, how do we transform this fragile current-detector into a robust voltage-measuring device? The secret lies in resistance.
By connecting a very high resistance in series with the galvanometer, we restrict the flow of current. This combination of a galvanometer and a high series resistance is exactly what constitutes a standard voltmeter. The high resistance ensures that when the voltmeter is connected in parallel across a circuit component, it draws a negligible amount of current, thereby not altering the actual voltage it is trying to measure.
The Master Equation
According to Ohm's Law, the potential difference V across this entire series combination is simply the product of the current flowing through it and its total resistance.
The maximum voltage this setup can safely measure corresponds to the maximum safe current the galvanometer can handle, known as the full-scale deflection current, denoted by Ig.
Here, Rg is the internal resistance of the galvanometer, and R is the external high resistance connected in series.
Executing the Calculation
Let's carefully extract the values given in our problem:
- Full-scale deflection current, Ig=4 mA=4×10−3 A
- Galvanometer resistance, Rg=50 Ω
- Series resistance, R=5 kΩ=5000 Ω
First, we determine the total resistance of our newly minted voltmeter:
Rtotal=Rg+R=50+5000=5050 Ω
Now, we substitute this back into our master equation to find the maximum measurable voltage:
The Final Verdict
The theoretical maximum voltage our voltmeter can measure is exactly 20.2 V. When we look at the given options, we must select the closest approximate value.
Therefore, the maximum voltage is close to 20 V, making option (d) the correct choice.