Step 1: Recall the laws of refraction.
When a ray of light travels from one optical medium to another, it bends at the interface between the two media. This phenomenon is called refraction. The extent of bending depends on the refractive indices of the two media and the angle of incidence. Snell's law governs this bending: \[ n_1 \sin \theta_1 = n_2 \sin \theta_2 \] where \( n_1 \) and \( n_2 \) are the refractive indices of the first and second media, respectively, and \( \theta_1 \) and \( \theta_2 \) are the angles of incidence and refraction, respectively, measured with respect to the normal to the surface.
Step 2: Identify the optical densities of air and water.
Air is a rarer medium (lower optical density, refractive index \( n_{air} \approx 1 \)), and water is a denser medium (higher optical density, refractive index \( n_{water} \approx 1.33 \)).
Step 3: Apply Snell's law for light travelling from a rarer to a denser medium.
When light travels from a rarer medium (air) to a denser medium (water), \( n_1<_2 \). According to Snell's law: \[ \sin \theta_2 = \frac{n_1}{n_2} \sin \theta_1 \] Since \( \frac{n_1}{n_2}<1 \), we have \( \sin \theta_2<\sin \theta_1 \). For angles between 0 and 90 degrees, a smaller sine value corresponds to a smaller angle. Therefore, \( \theta_2<\theta_1 \).
Step 4: Interpret the change in angle with respect to the normal.
The angle of refraction \( \theta_2 \) is smaller than the angle of incidence \( \theta_1 \). This means that the refracted ray bends towards the normal.
Step 5: Consider the case of light incident along the normal.
If the ray of light enters perpendicularly to the surface (along the normal), the angle of incidence \( \theta_1 = 0^\circ \). In this case, \( \sin \theta_1 = 0 \), and from Snell's law, \( \sin \theta_2 = 0 \), which means \( \theta_2 = 0^\circ \). So, there is no bending, and the light passes straight through. However, the question states that the light enters obliquely. Therefore, when a ray of light travels from air to water obliquely, it bends towards the normal.
Two light beams fall on a transparent material block at point 1 and 2 with angle \( \theta_1 \) and \( \theta_2 \), respectively, as shown in the figure. After refraction, the beams intersect at point 3 which is exactly on the interface at the other end of the block. Given: the distance between 1 and 2, \( d = 4/3 \) cm and \( \theta_1 = \theta_2 = \cos^{-1} \frac{n_2}{2n_1} \), where \( n_2 \) is the refractive index of the block and \( n_1 \) is the refractive index of the outside medium, then the thickness of the block is cm.