The de-Broglie wavelength is given by:
\[ \lambda_{DB} = \frac{h}{p} = \frac{h}{\sqrt{2mK}}, \]
where \(m\) is the mass, \(K\) is the kinetic energy, and \(p\) is the momentum. Since the particles have the same energy \(K\), the de-Broglie wavelength becomes:
\[ \lambda_{DB} \propto \frac{1}{\sqrt{m}}. \]
Since \(\lambda_{DB} \propto \frac{1}{\sqrt{m}}\), the lighter the mass, the longer the wavelength:
\[ \lambda_e > \lambda_p > \lambda_\alpha. \]
The de Broglie wavelengths of a proton and an \(\alpha\) particle are \(λ_p\) and \(λ_\alpha\) respectively. The ratio of the velocities of proton and \(\alpha\) particle will be :
A body of mass 1000 kg is moving horizontally with a velocity of 6 m/s. If 200 kg extra mass is added, the final velocity (in m/s) is: