\(λ_p ∝ λ^{2}_e\)
\(λ_p ∝ λ_e\)
\(λ_p ∝ \sqrtλ_e\)
\(λ_p ∝ \sqrt{\frac{1}{λ_e}}\)
To determine the relationship between the de Broglie wavelengths of an electron and a photon when they have the same kinetic energy, we start by considering the de Broglie wavelength formulae for both particles:
The de Broglie wavelength λ for a particle is given by:
λ = \frac{h}{p}
where h is Planck's constant and p is the momentum of the particle.
In the case of an electron, the kinetic energy (KE) is related to its momentum (p_e) by:
KE = \frac{p_e^2}{2m_e}
Solving for p_e gives:
p_e = \sqrt{2m_e \cdot KE}
Substituting in the de Broglie wavelength formula for the electron:
λ_e = \frac{h}{\sqrt{2m_e \cdot KE}}
For a photon, the kinetic energy (KE) is related directly to its momentum (p_p) and the speed of light (c) as:
KE = p_p \cdot c
So, the momentum of the photon is:
p_p = \frac{KE}{c}
Substituting in the de Broglie wavelength formula for the photon:
λ_p = \frac{h}{\frac{KE}{c}} = \frac{h \cdot c}{KE}
Since the kinetic energy of both the electron and the photon is the same, we equate the expressions for kinetic energy:
KE = \frac{h^2}{2m_e \cdot λ_e^2} = h \cdot c / λ_p
Solving for λ_p in terms of λ_e, we get:
λ_p = \frac{hc \cdot λ_e^2}{h^2} = \frac{c \cdot λ_e^2}{h}
This tells us that:
λ_p \propto λ^{2}_e
Thus, the correct relationship between the de Broglie wavelengths of the electron and the photon is λ_p \propto λ^{2}_e, which corresponds to the given correct answer.