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The Sigma Insight: Electrical Instruments
The Magic of the Meter Bridge
Imagine you are standing in a laboratory, looking at a simple yet incredibly elegant piece of apparatus: the meter bridge. It consists of a uniform wire exactly one meter (100 cm) long, stretched taut across a wooden board. This device is a practical application of the famous Wheatstone bridge principle, allowing us to determine unknown resistances with remarkable precision.
The core principle is beautifully simple. When the galvanometer shows zero deflection (the null point), the bridge is balanced. At this magical point, the ratio of the resistances in the left and right gaps is perfectly equal to the ratio of the lengths of the wire segments on either side of the jockey.
Mathematically, this is expressed as:
where is the balancing length from the left end, and is the remaining length of the wire.
Analyzing the Initial Setup
Let's dive into the first part of our problem. We are given that a resistance is placed in the left gap and a resistance is placed in the right gap. The null point is found at a distance of from the left end.
By plugging these values into our master equation, we get:
This tells us a crucial piece of information: the resistance is exactly four times the resistance . Keep this ratio safe; it is the key to unlocking the rest of the problem.
The Modified Setup
Now, the experiment takes a twist. We decide to replace the resistance in the left gap with a new resistance that is four times larger, i.e., . The resistance in the right gap remains untouched.
Because we have changed the resistance on one side, the balance of the bridge is disturbed. The null point must shift to a new position to restore equilibrium. Let's call this new balancing length .
Our new balancing equation becomes:
Final Calculation and Conclusion
This equation might look a bit intimidating, but remember that we already know the value of the ratio . Let's substitute the value we found earlier () into our new equation:
The and the cancel each other out perfectly, leaving us with a beautifully simple equation:
Now, we just cross-multiply to solve for :
The new null point is exactly at .
Think about the physical intuition here: by increasing the left resistance to , we made it exactly equal to the right resistance (since ). When the resistances in both gaps are identical, the bridge must balance exactly in the middle of the wire. The math perfectly aligns with the physical reality!
Similar Questions
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In the experimental set up of meter bridge shown in the figure, the null point is obtained at a distance of from . If a resistor is connected in series with , the null point shifts by . The resistance that should be connected in parallel with such that the null point shifts back to its initial position is
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A resistance of is connected across one gap of a meter-bridge (the length of the wire is 100 cm) and an unknown resistance, greater than , is connected across the other gap. When these resistances are interchanged, the balance point shifts by 20 cm. Neglecting any corrections, the unknown resistance is
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A meter bridge is set-up as shown in figure, to determine an unknown resistance using a standard resistor. The galvanometer shows null point when tapping-key is at mark. The end-corrections are and respectively for the ends and . The determined value of is
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During an experiment with a meter bridge, the galvanometer shows a null point when the jockey is pressed at using a standard resistance of , as shown in the scale used in the meter bridge is . The unknown resistance is
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are different values of . Further, and are the null points obtained corresponding to and respectively. For which resistor, the value of will be the most accurate and why?
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Assertion: In a meter bridge experiment, null point for an unknown resistance is measured. Now, the unknown resistance is put inside an enclosure maintained at a higher temperature. The null point can be obtained at the same point as before by decreasing the value of the standard resistance. Reason: Resistance of a metal increases with increase in temperature.
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In a meter bridge, the wire of length has a non-uniform cross-section such that the variation of its resistance with length is . Two equal resistance are connected as shown in the figure. The galvanometer has zero deflection when the jockey is at point . What is the length ?
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