Question:

Equivalent resistance between the adjacent corners of a regular \(n\)-sided polygon of uniform wire of resistance \(R\) would be :

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When calculating equivalent resistance in networks, break down the network into series and parallel combinations. Remember the formulas for equivalent resistance in series and parallel.

Updated On: Mar 19, 2025
  • \(\frac{(n-1) R}{(2 n-1)}\)

  • \(\frac{(n-1) R}{n}\)

  • \(\frac{n^2 R}{n-1}\)

  • \(\frac{(n-1) R}{n^2}\)

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The Correct Option is D

Approach Solution - 1

Step 1: Analyze the Resistance of Each Side

Let \(r\) be the resistance of each side of the \(n\)-sided polygon. Since the total resistance of the wire is \(R\), and there are \(n\) sides, the resistance of each side is:

\[ r = \frac{R}{n} \]

Step 2: Consider Adjacent Corners A and B

When we consider the equivalent resistance between adjacent corners A and B, the polygon can be viewed as two resistors in parallel:

  • One resistor with resistance \(r\) (between A and B).
  • The other resistor with resistance \((n-1)r\) (the remaining part of the polygon).

Step 3: Calculate the Equivalent Resistance

The equivalent resistance (\(R_{eq(AB)}\)) between A and B is given by the formula for parallel resistors:

\[ \frac{1}{R_{eq(AB)}} = \frac{1}{r} + \frac{1}{(n-1)r} \] \[ R_{eq(AB)} = \frac{r \times (n-1)r}{r + (n-1)r} = \frac{(n-1)r^2}{nr} = \frac{(n-1)r}{n} \]

Step 4: Substitute the Value of \(r\)

Substitute \(r = \frac{R}{n}\) back into the equation:

\[ R_{eq(AB)} = \frac{(n-1)\left(\frac{R}{n}\right)}{n} = \frac{(n-1)R}{n^2} \]

Conclusion:

The equivalent resistance between the adjacent corners of the polygon is:

\[ \frac{(n-1)R}{n^2} \quad \text{(Option 4)}. \]

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Approach Solution -2

Suppose resistance of each arm is r, then r=R/n 
Req(AB)​=R1​+R2​R1​R2​​ 
r+(n−1)rr(n−1)r​ 
=nrr(n−1)r​ 
=nn−1​r 
=n2(n−1)R​

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Concepts Used:

Current Electricity

Current electricity is defined as the flow of electrons from one section of the circuit to another.

Types of Current Electricity

There are two types of current electricity as follows:

Direct Current

The current electricity whose direction remains the same is known as direct current. Direct current is defined by the constant flow of electrons from a region of high electron density to a region of low electron density. DC is used in many household appliances and applications that involve a battery.

Alternating Current

The current electricity that is bidirectional and keeps changing the direction of the charge flow is known as alternating current. The bi-directionality is caused by a sinusoidally varying current and voltage that reverses directions, creating a periodic back-and-forth motion for the current. The electrical outlets at our homes and industries are supplied with alternating current.