The resistivity \(ρ\) of a material is an intrinsic property and does not change when the wire is deformed. Therefore, \(ρ' = ρ\).
The resistance \(R\) of a wire is given by \(R = \frac{ρL}{A}\), where \(L\) is the length and \(A\) is the cross-sectional area. When the radius of the wire is halved, the new area \(A'\) becomes \(\frac{\pi(r/2)^2}{πr^2} = \frac{1}{4}\). Since the volume remains constant \(AL = A'L'\), and using \(A' = \frac{1}{4}A\), we find \(L' = 4L\).
The new resistance \(R'\) is given by: \(R' = \frac{ρL'}{A'} = \frac{ρ(4L)}{\frac{1}{4}A} = 16R\).
Hence, \(R' = 16R\).
The power \(P\) is given by \(P = \frac{V^2}{R}\). After stretching, \(P'\) is given by \(P' = \frac{V^2}{R'} = \frac{V^2}{16R} = \frac{1}{16}P\). Thus, \(P' = \frac{1}{16}P\).
Value | Original | Stretched |
---|---|---|
Resistivity ρ | ρ | ρ |
Resistance R | R | 16R |
Power P | P | \(\frac{1}{16}P\) |
Hence, the correct relationship is: \(ρ' = ρ, R' = 16R, P' = \frac{1}{16} P\).
Two cells of emf 1V and 2V and internal resistance 2 \( \Omega \) and 1 \( \Omega \), respectively, are connected in series with an external resistance of 6 \( \Omega \). The total current in the circuit is \( I_1 \). Now the same two cells in parallel configuration are connected to the same external resistance. In this case, the total current drawn is \( I_2 \). The value of \( \left( \frac{I_1}{I_2} \right) \) is \( \frac{x}{3} \). The value of x is 1cm.