To solve the problem, we need to understand the relationship between the wavelength and the accelerating potential for both a proton and a deuteron. The de Broglie wavelength (\lambda) for a particle is given by:
\lambda = \frac{h}{\sqrt{2mE_k}}
where:
Both proton and deuteron have the same charge (q = e), but different masses. The mass of a proton (m_p) and the mass of a deuteron (m_d = 2m_p) are related by the factor of 2.
The ratio of wavelengths for proton and deuteron is given as:
\frac{\lambda_p}{\lambda_d} = 1:\sqrt{2}
Substituting the expressions for the wavelengths, we have:
\frac{\frac{h}{\sqrt{2m_p e V_p}}}{\frac{h}{\sqrt{2m_d e V_d}}} = \frac{\sqrt{2m_d e V_d}}{\sqrt{2m_p e V_p}} = 1:\sqrt{2}
Simplifying, we get:
\frac{\sqrt{m_d V_d}}{\sqrt{m_p V_p}} = 1:\sqrt{2}
Squaring both sides gives:
\frac{m_d V_d}{m_p V_p} = \frac{1}{2}
Substitute m_d = 2m_p:
\frac{2m_p V_d}{m_p V_p} = \frac{1}{2}
After simplifying:
\frac{V_d}{V_p} = \frac{1}{4}
This implies:
\frac{V_p}{V_d} = 4:1
Thus, the ratio V_p to V_d is 4:1, making the correct option: