We are given the following two equations:
\(eV = \frac{hc}{\lambda} - \frac{hc}{\lambda_0}\) ....(i)
\(eV/4 = \frac{hc}{2 \lambda} - \frac{hc}{\lambda_0}\) .....(ii)
From equations (i) and (ii), we can proceed as follows:
\(\Rightarrow 4 = \frac{\frac{1}{\lambda} - \frac{1}{\lambda_0}}{\frac{1}{2 \lambda} - \frac{1}{\lambda_0}}\)
On solving the above equation, we find that:
\(\lambda_0 = 3 \lambda\)
The wavelength \(\lambda_0\) is three times the wavelength \(\lambda\).
An alpha particle moves along a circular path of radius 0.5 mm in a magnetic field of \( 2 \times 10^{-2} \, \text{T} \). The de Broglie wavelength associated with the alpha particle is nearly
(Planck’s constant \( h = 6.63 \times 10^{-34} \, \text{Js} \))
A full wave rectifier circuit with diodes (\(D_1\)) and (\(D_2\)) is shown in the figure. If input supply voltage \(V_{in} = 220 \sin(100 \pi t)\) volt, then at \(t = 15\) msec: 
The dual nature of matter and the dual nature of radiation were throughgoing concepts of physics. At the beginning of the 20th century, scientists untangled one of the best-kept secrets of nature – the wave-particle duplexity or the dual nature of matter and radiation.
Electronic Emission
The least energy that is needed to emit an electron from the surface of a metal can be supplied to the loose electrons.
Photoelectric Effect
The photoelectric effect is a phenomenon that involves electrons getting away from the surface of materials.
Heisenberg’s Uncertainty Principle states that both the momentum and position of a particle cannot be determined simultaneously.