The resistance (\(R\)) of a wire depends on its material 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. Substituting this, the resistance becomes:
\( R = \rho \frac{L}{\pi r^2} \)
Let the initial resistance be \(R_1\). Given:
So, the initial resistance is:
\( R = \rho \frac{L}{\pi r^1}^2 \)
Let the new resistance be \(R_2\). The problem states the new wire has:
First, calculate the new cross-sectional area (\(A_2\)):
\( A_2 = \pi r_2^2 = \pi \left(\frac{r}{2}\right)^2 = \pi \frac{r^2}{4} \)
Now, calculate the new resistance (\(R_2\)) using the resistance formula:
\( R_2 = \rho \frac{L_2}{A_2} \)
Substitute the values for \(L_2\) and \(A_2\):
\( R_2 = \rho \frac{L/2}{\pi r^2/4} \)
Simplify the expression:
\( R_2 = \rho \frac{L}{2} \times \frac{4}{\pi r^2} = \rho \frac{4L}{2\pi r^2} = \rho \frac{2L}{\pi r^2} \)
We can rewrite \(R_2\) by factoring out the expression for the initial resistance (\(R\)):
\( R_2 = 2 \left( \rho \frac{L}{\pi r^2} \right) \)
Since \(R = \rho \frac{L}{\pi r^2}\), we have:
\( R_2 = 2R \)
Therefore, the resistance of the new wire is \(2R\).
If the length of a resistor is doubled, what happens to its resistance, assuming all other factors remain constant?
A cylindrical wire of length L and radius r has resistance R. The resistance of another wire of the same material but of twice its length and one-fourth its radius is:
Which of the following metals has the lowest electrical resistivity?
When electric current is passed through a wire, the amount of heat produced in a wire depends upon _______.
I. Length
II. Thickness
A uniform wire of resistance 9Ω is bent in the form of an equilateral triangle. Find the effective resistance across a side of the triangle.
The value of carbon resistance is 54 × 103 Ω. The percentage tolerance is 5%. What is the colour code sequence of carbon resistance?
Which of the following relations are wrong?
I. The specific conductance is given by the relation \(k = \frac{1}{R}\left( {l/A} \right)\)
II. The equivalent conducting is given by the relation \(\lambda = \frac{{100\;K}}{C}\)
III. The specific resistance is given by the relation \(\rho = \frac{{Rl}}{A}\)