The momentum imparted to a surface by a light beam can be calculated using the relation: \[ p = \frac{I \cdot A}{c} \] Where:
\(I\) is the intensity of the light,
\(A\) is the area of the surface,
\(c\) is the speed of light in vacuum (\(3 \times 10^8 \, \text{m/s}\)).
Given:
\(I = 20 \, \text{W/cm}^2 = 20 \times 10^4 \, \text{W/m}^2\),
\(A = 25 \, \text{cm} \times 15 \, \text{cm} = 0.25 \, \text{m} \times 0.15 \, \text{m} = 0.0375 \, \text{m}^2\),
\(c = 3 \times 10^8 \, \text{m/s}\). Substitute the values into the formula: \[ p = \frac{(20 \times 10^4) \times 0.0375}{3 \times 10^8} = \frac{7500}{3 \times 10^8} = 2.5 \times 10^{-5} \, \text{kg ms}^{-1} \]
Since the light is perfectly reflected, the momentum doubles, so the total momentum imparted is: \[ 2 \times 2.5 \times 10^{-5} = 5 \times 10^{-5} \, \text{kg ms}^{-1} \] Thus, the momentum imparted to the surface by the light per second is \(1 \times 10^{-5} \, \text{kg ms}^{-1}\).
The waves that are produced when an electric field comes into contact with a magnetic field are known as Electromagnetic Waves or EM waves. The constitution of an oscillating magnetic field and electric fields gives rise to electromagnetic waves.
Electromagnetic waves can be grouped according to the direction of disturbance in them and according to the range of their frequency. Recall that a wave transfers energy from one point to another point in space. That means there are two things going on: the disturbance that defines a wave, and the propagation of wave. In this context the waves are grouped into the following two categories: