\(\textbf{Solution:} \text{ The intensity } I \text{ in a Young's double-slit experiment is related to the path difference } \Delta x \text{ between the waves by the formula:}\)
\[I = I_0 \cos^2 \left( \frac{\Delta x}{2 \lambda} \right)\]\(\text{When the intensity is } \frac{I_0}{2}, \text{ we have:}\)
\(\frac{I_0}{2} = I_0 \cos^2 \left( \frac{\Delta x}{2 \lambda} \right)\)
\(\text{This simplifies to:}\)
\(\cos^2 \left( \frac{\Delta x}{2 \lambda} \right) = \frac{1}{2}\)
\(\text{Thus, } \Delta x = \frac{\lambda}{2}.\)
List-I | List-II |
---|---|
(A) Mn2+ | (I) Pyrolusite ore |
(B) Spin only Magnetic Moment | (II) An alloy of 4f metal, iron and traces of S, C, Al and Ca |
(C) MnO2 | (III) μs = √n(n + 2) BM |
(D) Misch metal | (IV) Highest oxidation states |