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:
\(\frac{\lambda_e}{\lambda_{Ph}} = \left( \frac{E}{2m} \right)^{1/2} \frac{1}{c}\).
If the momentum of an electron is changed by P, then the de Broglie wavelength associated with it changes by \(1\%\). The initial momentum of the electron will be:
In a Vernier caliper, \(N+1\) divisions of vernier scale coincide with \(N\) divisions of main scale. If 1 MSD represents 0.1 mm, the vernier constant (in cm) is:
Identify the major product C formed in the following reaction sequence:
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.