To find the ratio of the de-Broglie wavelengths of a proton and an alpha particle accelerated through the same potential, we use the de-Broglie wavelength formula:
\(\lambda = \frac{h}{\sqrt{2mKE}}\),
where:
For a particle accelerated through a potential \(V\), the kinetic energy is \(KE = qV\), where \(q\) is the charge of the particle.
Thus, the de-Broglie wavelength is given by:
\(\lambda = \frac{h}{\sqrt{2mqV}}\)
Let's denote the de-Broglie wavelengths of the proton and alpha particle as \(\lambda_p\) and \(\lambda_\alpha\) respectively:
\(\lambda_p = \frac{h}{\sqrt{2m_pq_pV}}\)
\(\lambda_\alpha = \frac{h}{\sqrt{2m_\alpha q_\alpha V}}\)
To find the ratio \(\frac{\lambda_p}{\lambda_\alpha}\):
\(\frac{\lambda_p}{\lambda_\alpha} = \frac{\sqrt{2m_\alpha q_\alpha V}}{\sqrt{2m_p q_p V}}\)
The potential \(V\) is the same, so it cancels out:
\(\frac{\lambda_p}{\lambda_\alpha} = \sqrt{\frac{m_\alpha q_\alpha}{m_p q_p}}\)
For a proton:
For an alpha particle:
Substitute these into the ratio formula:
\(\frac{\lambda_p}{\lambda_\alpha} = \sqrt{\frac{6.68 \times 10^{-27} \times 2}{1.67 \times 10^{-27} \times 1}}\)
\(\frac{\lambda_p}{\lambda_\alpha} = \sqrt{8}\)
Thus, the ratio of the de-Broglie wavelengths of the proton and alpha particle is \(\sqrt{8} : 1\).
Therefore, the correct answer is: \(\sqrt{8} : 1\).