To determine the effective resistance when the wires are connected in series, we need to first understand the difference in resistance calculation for parallel and series circuits.
Given: The effective resistance of a parallel connection of four wires is \(0.25\, \Omega\).
Let's denote the resistance of each wire as \(R\). In a parallel circuit, the total resistance \(R_{\text{parallel}}\) is given by:
\(\frac{1}{R_{\text{parallel}}} = \frac{1}{R_1} + \frac{1}{R_2} + \frac{1}{R_3} + \frac{1}{R_4}\)
Since all wires have the same resistance \(R\), the equation becomes:
\(\frac{1}{R_{\text{parallel}}} = \frac{1}{R} + \frac{1}{R} + \frac{1}{R} + \frac{1}{R} = \frac{4}{R}\)
Given that \(R_{\text{parallel}} = 0.25\, \Omega\), we can substitute:
\(\frac{1}{0.25} = \frac{4}{R}\)
Solving for \(R\):
\(4 = \frac{4}{R} \cdot 0.25\)
\(R = 1\, \Omega\)
This means each wire has a resistance of \(1\, \Omega\).
When these wires are connected in series, the total resistance \(R_{\text{series}}\) is simply the sum of individual resistances:
\(R_{\text{series}} = R_1 + R_2 + R_3 + R_4 = 4 \cdot R = 4 \cdot 1 \, \Omega = 4\, \Omega\)
Thus, the effective resistance when the wires are connected in series is \(4\, \Omega\).
Therefore, the correct answer is: \(4\, \Omega\).

A wire of resistance $ R $ is bent into a triangular pyramid as shown in the figure, with each segment having the same length. The resistance between points $ A $ and $ B $ is $ \frac{R}{n} $. The value of $ n $ is:

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Resistance is the measure of opposition applied by any object to the flow of electric current. A resistor is an electronic constituent that is used in the circuit with the purpose of offering that specific amount of resistance.
R=V/I
In this case,
v = Voltage across its ends
I = Current flowing through it
All materials resist current flow to some degree. They fall into one of two broad categories:
Resistance measurements are normally taken to indicate the condition of a component or a circuit.