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: \(\sqrt{8} : 1\).

Two loudspeakers (\(L_1\) and \(L_2\)) are placed with a separation of \(10 \, \text{m}\), as shown in the figure. Both speakers are fed with an audio input signal of the same frequency with constant volume. A voice recorder, initially at point \(A\), at equidistance to both loudspeakers, is moved by \(25 \, \text{m}\) along the line \(AB\) while monitoring the audio signal. The measured signal was found to undergo \(10\) cycles of minima and maxima during the movement. The frequency of the input signal is _____________ Hz.
(Speed of sound in air is \(324 \, \text{m/s}\) and \( \sqrt{5} = 2.23 \)) 