\(K_p\) \(>\) \(K_e\)
\(K_p\) \(<\) \(K_e\)
The de Broglie wavelength for a particle is given by:
\[\lambda = \frac{h}{p},\]
where \(h\) is Planck's constant and \(p\) is the momentum.
For the proton and electron:
\[\lambda_{\text{proton}} = \lambda_{\text{electron}} \implies p_{\text{proton}} = p_{\text{electron}}.\]
The kinetic energy is related to momentum as:
\[K = \frac{p^2}{2m}.\]
Since \(p_{\text{proton}} = p_{\text{electron}}\):
\[K_{\text{proton}} = \frac{p^2}{2m_p}, \quad K_{\text{electron}} = \frac{p^2}{2m_e}.\]
Given \(m_p>m_e\), it follows that:
\[K_{\text{proton}}<K_{\text{electron}}.\]
Thus:
\[K_p<K_e.\]
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: