Here the width of principal maxima is $2.5\,mm$, therefore its half width is $\frac{\beta}{2}=\frac{2.5}{2}=1.25 \times 10^{-3}\,m$
Diffraction angle $\theta=\frac{\beta / 2}{ D }=\frac{1.25 \times 10^{-3}}{2}$
$\therefore a \theta=\lambda \therefore \theta=\lambda / a =\frac{1.25 \times 10^{-3}}{2}$
$\lambda=\frac{1.25 \times 10^{-3}}{2} \times a =\frac{1.25 \times 10^{-3} \times 10^{-3}}{2}$
$\lambda=6.25 \times 10^{-7} m =6250 \mathring A$
Generate a complete, print-ready paper with questions like this in minutes — across 16+ boards, with answer keys.
$y = A{e^{ - \frac{{bt}}{{2m}}}}\sin (\omega 't + \phi )$
where the symbols have their usual meanings. If a $2\ kg$ mass $(m)$ is attached to a spring of force constant $(K)$ $1250\ N/m$ , the period of the oscillation is $\left( {\pi /12} \right)s$ . The damping constant $‘b’$ has the value. ..... $kg/s$

