The resistivity \(ρ\) of a material is an intrinsic property and remains unchanged when a wire is deformed. Thus, \(ρ' = ρ\). The resistance \(R\) of a wire is defined as \(R = \frac{ρL}{A}\), where \(L\) is the length and \(A\) is the cross-sectional area. When the wire's radius is halved, its new area \(A'\) becomes \(\frac{1}{4}\) of the original area. Given that the volume remains constant (\(AL = A'L'\)) and using \(A' = \frac{1}{4}A\), we deduce that \(L' = 4L\).
The new resistance \(R'\) is calculated as: \(R' = \frac{ρL'}{A'} = \frac{ρ(4L)}{\frac{1}{4}A} = 16R\). Therefore, \(R' = 16R\).
The power \(P\) is given by \(P = \frac{V^2}{R}\). Post-stretching, the new power \(P'\) is \(P' = \frac{V^2}{R'} = \frac{V^2}{16R} = \frac{1}{16}P\). Consequently, \(P' = \frac{1}{16}P\).
| Parameter | Original Value | Stretched Value |
|---|---|---|
| Resistivity ρ | ρ | ρ |
| Resistance R | R | 16R |
| Power P | P | \(\frac{1}{16}P\) |
The resulting relationships are: \(ρ' = ρ, R' = 16R, P' = \frac{1}{16} P\).