For a circular aperture, the radius of the first dark ring in the Fraunhofer diffraction pattern, often referred to as the Airy disk radius \( r_1 \), is given by: \[ r_1 = 1.22 \frac{\lambda f}{D}, \] where \( D \) is the diameter of the aperture. Given that the radius \( a = 0.05 \, \text{cm} \), the diameter \( D = 2a = 0.1 \, \text{cm} \). Substituting the given values: \[ r_1 = 1.22 \times \frac{5 \times 10^{-5} \, \text{cm} \times 20 \, \text{cm}}{0.1 \, \text{cm}} = 1.22 \times 10^{-2} \, \text{cm} = 12.20 \times 10^{-3} \, \text{cm}. \] This calculation confirms that the radius of the first dark ring matches option (b).
Light from a point source in air falls on a spherical glass surface (refractive index, \( \mu = 1.5 \) and radius of curvature \( R = 50 \) cm). The image is formed at a distance of 200 cm from the glass surface inside the glass. The magnitude of distance of the light source from the glass surface is 1cm.
Distance between object and its image (magnified by $-\frac{1}{3}$ ) is 30 cm. The focal length of the mirror used is $\left(\frac{\mathrm{x}}{4}\right) \mathrm{cm}$, where magnitude of value of x is _______ .
When an object is placed 40 cm away from a spherical mirror an image of magnification $\frac{1}{2}$ is produced. To obtain an image with magnification of $\frac{1}{3}$, the object is to be moved: