To determine the product \(R_1R_2\), we need to use the principles of a meter bridge. By applying the formula for the meter bridge in both scenarios, we can create equations to solve for \(R_1\) and \(R_2\).
For the first scenario, where \(R_1\) and \(R_2\) are in series, the total resistance \(R_s=R_1+R_2\), and we have a null point at 60 cm from the left side. Using the meter bridge principle:
\(\frac{R_s}{10}=\frac{60}{40}\)
\(\Rightarrow R_s = \frac{60}{40} \times 10 = 15 \, \Omega\)
For the second scenario, where \(R_1\) and \(R_2\) are in parallel, the equivalent resistance \(R_p=\frac{R_1R_2}{R_1+R_2}\), and the null point is at 40 cm from the left. Thus:
\(\frac{R_p}{3}=\frac{40}{60}\)
\(\Rightarrow R_p = \frac{40}{60} \times 3 = 2 \, \Omega\)
Now, \(R_p=\frac{R_1R_2}{R_1+R_2}=2\) and \(R_1+R_2=15\). Substituting \(R_1+R_2=15\) into the equation for \(R_p\):
\(\frac{R_1R_2}{15} = 2\)
\(\Rightarrow R_1R_2 = 2 \times 15 = 30 \, \Omega^2\)
Thus, the product \(R_1R_2\) is \(30 \, \Omega^2\), which falls within the given range [30,30].