A proton accelerated through a potential difference of V volts has a de-Broglie wavelength λ associated with it. In order to get the same wavelength associated with an $α$-particle, the required accelerating potential is |
V/16 V/8 4V 8V |
V/8 |
The correct answer is Option (2) → V/8 ** For a particle accelerated through potential $V$, $\lambda = \frac{h}{\sqrt{2m q V}}$ For proton: $\lambda = \frac{h}{\sqrt{2 m_p e V}}$ For $\alpha$-particle: $\lambda = \frac{h}{\sqrt{2 m_\alpha (2e) V'}}$ For same $\lambda$, $\sqrt{2 m_p e V} = \sqrt{2 m_\alpha (2e) V'}$ ⟹ $m_p V = 2 m_\alpha V'$ Since $m_\alpha = 4 m_p$ $V' = \frac{V}{8}$ ∴ Required accelerating potential for $\alpha$-particle is $\frac{V}{8}$ |