The resistance (\(R\)) of a wire depends on its material's resistivity (\(\rho\)), length (\(L\)), and cross-sectional area (\(A\)). The formula is:
\( R = \rho \frac{L}{A} \)
For a cylindrical wire, the cross-sectional area is \(A = \pi r^2\), where \(r\) is the radius. Thus, the resistance is:
\( R = \rho \frac{L}{\pi r^2} \)
Let the original wire have length \(L_1 = L\), radius \(r_1 = r\), and resistance \(R_1 = R\). The resistivity is \(\rho\).
From the formula:
\( R = \rho \frac{L}{\pi r^2} \quad (1) \)
The new wire has:
The new cross-sectional area (\(A_2\)) is:
\( A_2 = \pi r_2^2 = \pi \left(\frac{r}{2}\right)^2 = \pi \frac{r^2}{4} \)
The new resistance (\(R_2\)) is:
\( R_2 = \rho \frac{L_2}{A_2} \)
Substitute the values for \(L_2\) and \(A_2\):
\( R_2 = \rho \frac{L/2}{\pi r^2 / 4} \)
Simplify the expression:
\( R_2 = \rho \frac{L}{2} \times \frac{4}{\pi r^2} \)
\( R_2 = \rho \frac{4L}{2 \pi r^2} \)
\( R_2 = 2 \left( \rho \frac{L}{\pi r^2} \right) \)
Comparing this with the original resistance formula (Equation 1), we see that \(\rho \frac{L}{\pi r^2} = R\).
Therefore, the new resistance \(R_2\) is:
\( R_2 = 2R \)
The resistance of the new wire is 2R.
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