Sigma Percentile
JEE Advanced 2022
LEVELJEE Advanced

Animated Solution for Physics - Current Electricity: The figure shows a circuit having eight resistances of each, labelled to , and two ideal batteries with voltages and . Which of the following statement(s) is(are) correct?

Select Answer:

* Multiple Correct

Visualized Solution

  • The given circuit consists of identical resistors of each and ideal batteries.
  • Direct application of Kirchhoff's Loop Laws would result in multiple complex equations.
  • We must look for structural symmetries to simplify the network.

  • Observe the connections to the top node and bottom node .
  • Both and are connected to nodes , , and via identical resistors.
  • Due to this perfect mirror symmetry, .

  • Since , we can merge nodes and into a single equivalent node .
  • The corresponding resistors form parallel pairs:

  • Let's set the potential of the center node to ().
  • Right branch ( to ): The battery drops the potential to before .
  • Left branch ( to ): The battery raises the potential to before .

  • The entire circuit reduces to node connected to three branches:
  • 1. To via ( from to + of )
  • 2. To via ( from to + of )
  • 3. To via (from to )

  • Let the potential at node be .
  • Applying Kirchhoff's Current Law at node (sum of outgoing currents = 0):

  • Multiply the entire equation by to clear denominators:

  • Current through (Right branch):
  • Current through (Left branch):

  • Current from to : .
  • This splits equally to and , so .
  • Current from to is . It splits equally at to and .
  • So, . All options are correct!

The Sigma Insight: Kirchhoff's Laws

Solution Diagram

The Intimidating Web

When you first lay eyes on this circuit, it looks like a classic trap designed to drain your time during an exam. With eight resistors, two batteries, and multiple interconnected loops, setting up standard Kirchhoff's Loop equations would result in a massive, error-prone system of linear equations.
However, in advanced physics problems, brute force is rarely the intended path. The key to unlocking this problem lies in taking a step back and observing the geometry of the connections. Physics is deeply intertwined with symmetry, and recognizing it can turn a nightmare into a walk in the park.

The Power of Symmetry

Let's carefully trace the connections to the top node () and the bottom node (). Notice that node is connected to the left node (), the right node (), and the center node () through identical resistors (, , and ).
Now, look at node . It is also connected to the exact same three nodes (, , and ) through identical resistors (, , and ). Because the upper half and the lower half of the circuit are perfect mirror images of each other, the electrical potential at the top node must be exactly equal to the electrical potential at the bottom node.
Since there is no potential difference between them, we can virtually "fold" the circuit in half, merging nodes and into a single equivalent node, which we will call . When we do this, the corresponding resistors from the top and bottom halves end up in parallel. For example, the resistor from to is now in parallel with the resistor from to .
Applying this to all three pairs, our complex web collapses into a beautifully simple star network centered at , with legs reaching out to nodes , , and .

The Masterstroke

Smart Reference Node
Now we have a central node connected to the active branches containing the batteries. To make our Nodal Analysis (KCL) as clean as possible, we can choose any node as our reference potential. Instead of choosing ground () arbitrarily, let's make a strategic choice: let's set the potential of the center node to .
Why ? Look at the right branch connecting to . It contains a battery. If we start at () and cross the battery, the potential drops by exactly , landing us at a perfect just before the resistor . This means the entire right branch is simply a connection from node to through a total resistance of (the leg plus the of ).
Similarly, the left branch connects to with a battery. Starting at () and moving left, the potential increases by , putting the node before at . Thus, the left branch connects node to through .

The Final Calculation

Our entire circuit is now reduced to a single unknown node (let's call its voltage ) connected to three known potentials: , , and . We apply Kirchhoff's Current Law at node :
To solve this elegantly, multiply the entire equation by :
With the central voltage known, calculating the currents is trivial. The current through is the current in the right branch:
The current through is the current in the left branch:
To find the currents in the folded resistors, we calculate the total branch current and split it. The current flowing from to is . Because of symmetry, this splits equally between and , giving .
Similarly, the flowing from the left splits equally at node , giving . Evaluating all the options, we find that every single statement provided is perfectly correct!

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