To understand the behavior of the diffraction pattern in this scenario, we must consider the principles of wave-particle duality and the concept of electron diffraction. Particularly, the concept of de Broglie wavelength is crucial here. The de Broglie wavelength \(\lambda\) of a particle is given by:
\(\lambda = \frac{h}{p}\)
where:
As the speed \(v\) of the electrons increases, their momentum \(p\) also increases. Therefore, from the de Broglie equation, we see that an increase in momentum leads to a decrease in the de Broglie wavelength \(\lambda\).
The angular width (\Delta \theta) of the central maximum in a single-slit diffraction pattern for a wave of wavelength \(\lambda\) can be determined using the formula:
\(\Delta \theta = \frac{2\lambda}{a}\)
where \(a\) is the width of the slit.
From this relation, it is evident that the angular width \(\Delta \theta\) is directly proportional to the wavelength \(\lambda\). Thus, if the wavelength \(\lambda\) decreases due to an increase in the speed of the electrons, the angular width of the central maximum will decrease as well.
Therefore, the correct statement is: The angular width of the central maximum will decrease.
If the monochromatic source in Young's double slit experiment is replaced by white light,
1. There will be a central dark fringe surrounded by a few coloured fringes
2. There will be a central bright white fringe surrounded by a few coloured fringes
3. All bright fringes will be of equal width
4. Interference pattern will disappear