For an electron, the de Broglie wavelength is given by:
\(\lambda_e = \frac{h}{\sqrt{2mE}}\),
where:
For a photon, the energy is related to its momentum:
\(E = pc \, \Rightarrow \, \lambda_{Ph} = \frac{hc}{E}\),
where:
Now, comparing the wavelengths of the electron and the photon:
\(\Rightarrow \frac{\lambda_e}{\lambda_{Ph}} = \frac{h}{\sqrt{2mE}} \times \frac{E}{hc} = \left( \frac{E}{2m} \right)^{1/2} \frac{1}{c}\)
The ratio of the electron's de Broglie wavelength to the photon's wavelength is given by:
\(\frac{\lambda_e}{\lambda_{Ph}} = \left( \frac{E}{2m} \right)^{1/2} \frac{1}{c}\).
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 \( h = 6.63 \times 10^{-34} \, \text{Js} \))
AB is a part of an electrical circuit (see figure). The potential difference \(V_A - V_B\), at the instant when current \(i = 2\) A and is increasing at a rate of 1 amp/second is:
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.