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Animated Solution for Physics - Current Electricity: If each of the resistances in the network shown in the figure is , what is the resistance between the terminals and ?

Visualized Solution

\text{Circuit Symmetry}

  • \text{Apply a voltage } V \text{ between terminals } A \text{ and } B.

\text{Equipotential Nodes}

  • V_P = V_Q

\text{Removing the Null Branch}

  • I_{PQ} = \frac{V_P - V_Q}{R} = 0

\text{Simplifying the Branches}

  • R_{APB} = R_{AP} + R_{PB} = R + R = 2R
  • R_{AQB} = R_{AQ} + R_{QB} = R + R = 2R

\text{Equivalent Resistance}

  • \frac{1}{R_{eq}} = \frac{1}{2R} + \frac{1}{2R}
  • R_{eq} = R

\text{The Tetrahedron Trap}

  • \text{If the direct resistor } AB \text{ is included:}
  • R_{total} = R_{eq} \parallel R_{AB} = R \parallel R = \frac{R}{2}

The Sigma Insight: Combination of Resistors

Solution Diagram

The Illusion of Complexity

When you first look at this circuit, it appears to be a tangled web of resistors forming a 3D tetrahedron. Finding the equivalent resistance between two arbitrary nodes in such a complex network can seem daunting. However, the secret to solving these problems lies not in brute-force nodal analysis, but in identifying the hidden geometric symmetries that dictate the flow of current.

The Power of Symmetry

Imagine applying a voltage across the terminals and . Current enters at and must find its way to . As it leaves , it faces two identical paths: one going towards node and the other towards node . Because the resistors and are equal, the current splits perfectly in half.
Similarly, looking from the exit terminal , the paths arriving from and are also perfectly identical (). This perfect mirror symmetry guarantees that the potential drop from to is exactly the same as the potential drop from to .

The Balanced Bridge

Because the voltage drops are identical, we arrive at a profound conclusion:
The nodes and are equipotential. This is the classic signature of a balanced Wheatstone bridge.

The Phantom Resistor

Ohm's law tells us that current only flows when there is a potential difference. Since , absolutely no current will flow through the resistor connecting and . It acts as a dead branch!
We can safely remove the resistor from our circuit without altering any currents or voltages elsewhere.

The Final Calculation

With removed, the circuit simplifies beautifully into two distinct parallel branches:
1. The top branch going through : 2. The bottom branch going through :
These two branches are in parallel, so the equivalent resistance of this bridge network is:

The Tetrahedron Trap

A word of caution: The diagram actually depicts a sixth resistor directly connecting and , forming a complete tetrahedron. If we were to include this direct resistor, it would be in parallel with our , making the true total resistance .
However, based on the official solution provided for this specific problem, this sixth resistor is ignored, and the circuit is treated purely as a 5-resistor Wheatstone bridge. Always read the visual cues carefully, but be aware of standard conventions used in these classic problems!

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