To find the value of \( R \) given the scenario of a meter bridge, we will use the principle of the Wheatstone bridge. The balance point condition in the meter bridge can be expressed as:
\[\frac{R_1}{R_2} = \frac{l_1}{l_2}\]where:
Substituting the known values into the balance condition:
\[\frac{4.5}{R} = \frac{60}{40}\]Solving for \( R \):
\(R = \frac{4.5 \times 40}{60} = 3 \, \Omega\)
The resistance of the wire can also be expressed in terms of its physical dimensions:
\(R = \frac{\rho L}{A}\)
where:
Substituting the known resistance of the wire and solving for resistivity:
\[3 = \frac{\rho \times 0.1}{\pi (7 \times 10^{-8})}\]Simplifying gives:
\[\rho = 3 \times \pi \times 7 \times 10^{-8} \times 10\]\[\rho = 3 \times 7 \times \pi \times 10^{-7}\]Comparing with \( R \times 10^{-7} \, \Omega \, m \), we find:
\(R = 3 \times 7 \approx 66\)
Therefore, the value of \( R \) is 66.
For a balanced Wheatstone bridge in a meter bridge setup:
\[ \frac{4.5}{R} = \frac{60}{40} \]
Solving for \(R\):
\[ R = \frac{4.5 \times 40}{60} = 3 \, \Omega \]
Now, using the formula for resistance:
\[ R = \frac{\rho \ell}{A} = \frac{\rho \ell}{\pi r^2} \]
where \(\ell = 10 \, \text{cm} = 0.1 \, \text{m}\) and \(r = \sqrt{7} \times 10^{-4} \, \text{m}\).
Substitute values:
\[ 3 = \frac{\rho \times 0.1}{\pi (\sqrt{7} \times 10^{-4})^2} \]
\[ \rho = 66 \times 10^{-7} \, \Omega \, \text{m} \]
Thus, \(R = 66\).

Let \( C_{t-1} = 28, C_t = 56 \) and \( C_{t+1} = 70 \). Let \( A(4 \cos t, 4 \sin t), B(2 \sin t, -2 \cos t) \text{ and } C(3r - n_1, r^2 - n - 1) \) be the vertices of a triangle ABC, where \( t \) is a parameter. If \( (3x - 1)^2 + (3y)^2 = \alpha \) is the locus of the centroid of triangle ABC, then \( \alpha \) equals: