Step 1: Understanding the Question:
The question asks what physical property a voltmeter must possess to minimize the "loading effect" on the circuit where the voltage is being measured.
Loading effect is a major source of systematic error in electrical measurements.
Step 2: Key Formula or Approach:
A voltmeter is always connected in parallel across the two points in a circuit whose potential difference is to be determined.
Let the circuit have an equivalent resistance of \( R_{\text{th}} \). When the voltmeter with internal resistance \( R_v \) is connected, the parallel combination becomes:
\[ R_{\text{eq}} = \frac{R_{\text{th}} \cdot R_v}{R_{\text{th}} + R_v} \]
To ensure that the circuit's original state is not disturbed, we require \( R_{\text{eq}} \approx R_{\text{th}} \). This is only possible if \( R_v \gg R_{\text{th}} \).
Step 3: Detailed Explanation:
Let us explore the impact of voltmeter resistance on the measurement error:
• Ideal Case: An ideal voltmeter must draw zero current from the test circuit. According to Ohm's Law:
\[ I_v = \frac{V}{R_v} \]
For \( I_v \) to be exactly zero, \( R_v \) must be infinite (\( \infty \)).
• Practical Loading Error: If a voltmeter with low resistance is connected across a high-resistance component, it creates a parallel bypass path.
This causes a significant drop in the equivalent resistance of that branch, drawing a large shunt current away from the circuit.
As a result, the voltage measured across the parallel branch drops significantly below the true open-circuit voltage. This drop is the loading error.
• Prevention: To minimize this loading error, voltmeters are engineered to have as high an internal resistance (\( R_v \)) as possible.
Step 4: Final Answer:
To minimize loading, practical voltmeters must possess a very high resistance.