Lens Formula and Derivative for Error Analysis:
The lens formula is given by:
\[ \frac{1}{f} = \frac{1}{v} - \frac{1}{u} \]
Taking the derivative of both sides with respect to \(u\) and \(v\), we get:
\[ -\frac{df}{f^2} = -\frac{dv}{v^2} + \frac{du}{u^2} \]
Rearranging for \(df\):
\[ df = f^2 \left( \frac{dv}{v^2} + \frac{du}{u^2} \right) \]
Error in Measurement of Focal Length:
Since \(dv\) and \(du\) represent the measurement errors in \(v\) and \(u\),
respectively, we can substitute \(dv = \Delta v\) and \(du = \Delta u\):
\[ \Delta f = f^2 \left[ \frac{\Delta v}{v^2} + \frac{\Delta u}{u^2} \right] \]
Conclusion:
The error in the measurement of the focal length \(f\) is:
\[ \Delta f = f^2 \left[ \frac{\Delta u}{u^2} + \frac{\Delta v}{v^2} \right] \]
Consider the following sequence of reactions : 
Molar mass of the product formed (A) is ______ g mol\(^{-1}\).
In a Young's double slit experiment, three polarizers are kept as shown in the figure. The transmission axes of \( P_1 \) and \( P_2 \) are orthogonal to each other. The polarizer \( P_3 \) covers both the slits with its transmission axis at \( 45^\circ \) to those of \( P_1 \) and \( P_2 \). An unpolarized light of wavelength \( \lambda \) and intensity \( I_0 \) is incident on \( P_1 \) and \( P_2 \). The intensity at a point after \( P_3 \), where the path difference between the light waves from \( S_1 \) and \( S_2 \) is \( \frac{\lambda}{3} \), is:
