\(\frac{E_e}{E_{\text{ph}}} = \frac{2c}{v}\)
\(\frac{E_e}{E_{\text{ph}}} = \frac{v}{2c}\)
\(\frac{p_e}{p_{\text{ph}}} = \frac{2c}{v}\)
\(\frac{p_e}{p_{\text{ph}}} = \frac{v}{2c}\)
To solve the problem, we need to understand the concept of de Broglie wavelength, kinetic energy, and momentum for both electrons and photons.
\(\lambda = \frac{h}{p}\), where \(h\) is Planck's constant and \(p\) is the momentum of the particle.
\(\frac{h}{p_e} = \frac{h}{p_{\text{ph}}}\)
This implies:
\(p_e = p_{\text{ph}}\)
\(E_e = \frac{1}{2}mv^2\)
For non-relativistic speeds, the momentum \(p_e\) is \(mv\), so:
\(p_e = mv\)
\(E_{\text{ph}} = p_{\text{ph}}c\)
\(\frac{E_e}{E_{\text{ph}}} = \frac{\frac{1}{2}mv^2}{p_{\text{ph}}c}\)
Since \(p_{\text{ph}} = mv\), replace it to get:
\(\frac{E_e}{E_{\text{ph}}} = \frac{\frac{1}{2}mv^2}{mvc}\)
Canceling same terms, we obtain:
\(\frac{E_e}{E_{\text{ph}}} = \frac{v}{2c}\)
\(\frac{E_e}{E_{\text{ph}}} = \frac{v}{2c}\)