The ratio of the accelerating potentials required to accelerate (i) an \(α\)-particle and (ii) a proton to have the same de Broglie wavelength associated with them is (mass of \(α\) - particle = \(6.4\times 10^{-27}\) kg, mass of proton = \(1.6\times 10^{-27}\) kg)
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Use Einstein photoelectric equation for the two wavelengths and eliminate the work function.
Step 1: Use stopping potential in energy form:
Let $K_1 = eV$ and $K_2 = \frac{eV}{12}$. The energies of photons are in the ratio $\frac{1}{\lambda} : \frac{1}{6\lambda} = 6 : 1$.
Step 2: Solve:
Photon energies are $6x$ and $x$. Then $6x - \phi = K_1$ and $x - \phi = \frac{K_1}{12}$. Multiply the second by 12: $12x - 12\phi = K_1$. Equate: $6x - \phi = 12x - 12\phi$, so $11\phi = 6x$, $\phi = \frac{6x}{11}$.
The photon energy for $\lambda$ is $6x$, so $\phi = \frac{6x}{11}$ corresponds to a wavelength 11 times longer: $\lambda_0 = 11\lambda$ (C).
Final Answer:
$11\lambda$.
\[ \boxed{11\lambda} \]