\(K_p\) \(>\) \(K_e\)
\(K_p\) \(<\) \(K_e\)
To address this problem, understanding the de Broglie wavelength and its relationship with the kinetic energy of particles such as protons and electrons is essential.
The de Broglie wavelength (\(\lambda\)) for a particle is determined by the equation:
\(\lambda = \frac{h}{p}\)
Here, \(h\) represents Planck's constant, and \(p\) denotes the particle's momentum.
Momentum (\(p\)) can also be expressed in terms of kinetic energy (\(K\)) as:
\(p = \sqrt{2mK}\)
In this formula, \(m\) is the mass of the particle.
Given that a proton and an electron possess identical de Broglie wavelengths, we can establish the following equality:
\(\frac{h}{\sqrt{2m_p K_p}} = \frac{h}{\sqrt{2m_e K_e}}\)
By canceling Planck's constant (\(h\)) and rearranging, we obtain:
\(\sqrt{\frac{K_p}{m_p}} = \sqrt{\frac{K_e}{m_e}}\)
Squaring both sides of the equation yields:
\(\frac{K_p}{m_p} = \frac{K_e}{m_e}\)
Solving for \(K_p\), we find:
\(K_p = K_e \cdot \frac{m_p}{m_e}\)
Considering that the mass of a proton (\(m_p\)) significantly exceeds that of an electron (\(m_e\)), it follows that:
\(K_p \lt K_e\)
This demonstrates that when a proton and an electron share the same de Broglie wavelength, the proton's kinetic energy is lower than the electron's.
Therefore, the correct conclusion is:
\(K_p \lt K_e\)