\( 9^\circ \)
Step 1: Use the prism formula
For a small-angled prism, the refractive index (\( n \)) is related to the angle of the prism (\( A \)) and the angle of minimum deviation (\( D_m \)) by the formula: \[ n = \frac{\sin \left(\frac{A + D_m}{2} \right)}{\sin \left(\frac{A}{2} \right)} \] Given: \[ n = 1.6, \quad D_m = 4.2^\circ \] For small angles (in degrees), we approximate: \[ \sin x \approx x \text{ (in radians)} \] Step 2: Solve for \( A \)
Rewriting the equation: \[ 1.6 = \frac{\left(\frac{A + 4.2}{2} \right)}{\left(\frac{A}{2} \right)} \] \[ 1.6 \times \frac{A}{2} = \frac{A + 4.2}{2} \] Multiplying by 2: \[ 1.6 A = A + 4.2 \] \[ 1.6A - A = 4.2 \] \[ 0.6A = 4.2 \] \[ A = \frac{4.2}{0.6} = 7^\circ \] Thus, the angle of the prism is \( 7^\circ \).
A source and an observer move away from each other with same velocity of 10 m-1 with respect to the ground. If the observer finds the frequency of sound coming from the source as 1980 Hz, then the actual frequency of the source is (speed of sound in air = 340 ms-1)
Two convex lenses of focal lengths 20 cm and 30 cm are placed in contact with each other co-axially. The focal length of the combination is: