The problem involves finding the position where the minima (dark fringes) corresponding to two different wavelengths coincide in Young’s Double Slit Experiment (YDSE).
The condition for minimum intensity for a given wavelength \(\lambda\) is:
\(d \sin\theta = \left(m + \dfrac{1}{2}\right)\lambda\)
where \(d\) is the slit separation, \(\theta\) is the angular position of the minima, and \(m\) is the order of the minimum.
For small angles, \(\sin\theta \approx \tan\theta = \dfrac{x}{L}\), where \(x\) is the distance from the central maximum and \(L\) is the distance between the slits and the screen.
Hence, the condition for minima becomes:
\(d \dfrac{x}{L} = \left(m + \dfrac{1}{2}\right)\lambda\)
For the minima of both wavelengths to coincide, their positions must be equal:
\(\lambda_1\left(m_1 + \dfrac{1}{2}\right) = \lambda_2\left(m_2 + \dfrac{1}{2}\right)\)
Given:
\(450(m_1 + \tfrac{1}{2}) = 550(m_2 + \tfrac{1}{2})\)
Assuming \(m_1 = m_2 = m\):
\(450m + 225 = 550m + 275\)
\(m = 0.5\)
The position of the coincident minima is given by:
\(x = \dfrac{m + \tfrac{1}{2}}{L} \cdot \dfrac{\lambda_1 \lambda_2}{\lambda_2 - \lambda_1}\)
Substituting the values:
\(x = \dfrac{0.5 + 0.5}{1.5} \cdot \dfrac{450 \times 10^{-9} \times 550 \times 10^{-9}} {(550 - 450)\times 10^{-9}}\)
\(x \approx 1.65\,\text{mm}\)
Therefore, the distance from the central maximum where the minima of both wavelengths coincide is \(1.65\,\text{mm}\).