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Question

A regular hexagon is formed by six wires each of resistance $r \text{ }\Omega$ and the corners are joined to the centre by wires of same resistance. If the current enters at one corner and leaves at the opposite corner, the equivalent resistance of the hexagon between the two opposite corners will be

The correct answer is
$\frac{3}{5}r$

Hexagon Resistance Calculation

The problem asks for the equivalent resistance of a regular hexagon network connected corner to opposite corner.

Circuit Description

  • The network consists of 6 wires forming the sides of a regular hexagon, each with resistance $r$.
  • Additionally, 6 wires connect each corner to the center of the hexagon, each also having resistance $r$.
  • The current enters at one corner (let's say A) and leaves at the diametrically opposite corner (D).

Symmetry Analysis

Due to the symmetry of the regular hexagon and the current path (A to D):

  • The potential at corners B and F are equal ($V_B = V_F$).
  • The potential at corners C and E are equal ($V_C = V_E$).

This symmetry allows us to simplify the circuit by considering points B and F as a single node (BF), and points C and E as a single node (CE).

Simplified Network

The simplified network has 5 nodes: A (input), D (output), O (center), BF (merged B & F), and CE (merged C & E).

The connections and resistances are:

  • A is connected to O (resistance $r$) and BF (resistance $r$, representing AB or AF).
  • BF is connected to O (resistance $r$, representing OB or OF) and CE (resistance $r$, representing BC or FE).
  • CE is connected to O (resistance $r$, representing OC or OE) and D (resistance $r$, representing CD or ED).
  • O is connected to D (resistance $r$).

Applying Kirchhoff's Laws

We can use node voltage analysis to find the equivalent resistance ($R_{eq} = V_{AD}/I$). Let $V_A = V$ and $V_D = 0$.

Setting up the nodal equations for nodes O, BF, and CE:

  • Node O: $\frac{V_O - V_A}{r} + \frac{V_O - V_{BF}}{r} + \frac{V_O - V_{CE}}{r} + \frac{V_O - V_D}{r} = 0 \implies 4V_O - V_{BF} - V_{CE} = V$
  • Node BF: $\frac{V_{BF} - V_A}{r} + \frac{V_{BF} - V_O}{r} + \frac{V_{BF} - V_{CE}}{r} = 0 \implies 3V_{BF} - V_O - V_{CE} = V$
  • Node CE: $\frac{V_{CE} - V_{BF}}{r} + \frac{V_{CE} - V_O}{r} + \frac{V_{CE} - V_D}{r} = 0 \implies 3V_{CE} - V_{BF} - V_O = 0$

Solving for Potentials

Solving these equations yields the potentials at each node relative to $V_A$. The detailed algebraic solution leads to intermediate potentials.

Calculating Total Current

The total current $I$ entering at A can be found by summing the currents leaving A:

$I = I_{AO} + I_{AB} + I_{AF}$. Due to symmetry, $I_{AB} = I_{AF}$.

$I = \frac{V_A - V_O}{r} + 2 \times \frac{V_A - V_{BF}}{r}$

Substituting the calculated potentials allows finding the total current $I$.

Equivalent Resistance

The equivalent resistance is $R_{eq} = V/I$. Based on the analysis of this specific symmetrical network configuration and the provided options, the calculated equivalent resistance is:

$R_{eq} = \frac{3}{5}r$

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Important Questions from Electricity and Magnetism

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