To solve this problem, we need to consider the properties of resistors, particularly how resistance changes with the length of the conductor.
- The initial resistance of the wire of length \( l \) is 10 Ω.
- When the wire is stretched to double its length, \( 2l \), the resistance changes due to the formula for resistance: \(R = \rho \frac{L}{A}\), where \( \rho \) is the resistivity, \( L \) is the length, and \( A \) is the cross-sectional area of the wire.
- Since the volume of the wire remains constant when stretched, \((l \cdot A_1) = (2l \cdot A_2)\), where \( A_1 \) and \( A_2 \) are the original and new cross-sectional areas, respectively. So, \(A_2 = \frac{A_1}{2}\).
- Therefore, the new resistance is given by \(R' = \rho \frac{2l}{A_2} = \rho \frac{2l}{A_1/2} = 4 \cdot \rho \frac{l}{A_1} = 4 \cdot 10 \, \Omega = 40\, \Omega\).
- Now, this wire is bent to form a circle. In a circle, the resistance across any diameter consists of two resistors, each of resistance equal to half of the total resistance of the circular wire: \(\frac{40}{2} = 20 \, \Omega\) per semicircle.
- These two semicircular resistors are in parallel when measured across a diameter. The formula for equivalent resistance \( R \) of two parallel resistors is: \(\frac{1}{R} = \frac{1}{R_1} + \frac{1}{R_2}\)
Here, both \( R_1 \) and \( R_2 \) are 20 Ω, so: \(\frac{1}{R} = \frac{1}{20} + \frac{1}{20} = \frac{2}{20} = \frac{1}{10}\). - Therefore, the equivalent resistance, \( R \), across a diameter is 10 Ω.
Hence, the correct answer is 10 Ω.