Given that a photon and an electron have the same energy \( E \), we need to determine the ratio \( \frac{\lambda_p}{\lambda_e} \) of the photon wavelength \( \lambda_p \) to the de Broglie wavelength of the electron \( \lambda_e \).
The energy of a photon is given by:
\[ E = \frac{hc}{\lambda_p} \]
Solving for \( \lambda_p \),
\[ \lambda_p = \frac{hc}{E} \]
The de Broglie wavelength of an electron is given by:
\[ \lambda_e = \frac{h}{p} \]
The momentum \( p \) of the electron with kinetic energy \( E \) is:
\[ p = \sqrt{2mE} \]
Substituting this into the de Broglie wavelength formula:
\[ \lambda_e = \frac{h}{\sqrt{2mE}} \]
Now, we calculate the ratio \( \frac{\lambda_p}{\lambda_e} \):
\[ \frac{\lambda_p}{\lambda_e} = \frac{\frac{hc}{E}}{\frac{h}{\sqrt{2mE}}} \]
Simplifying this expression:
\[ \frac{\lambda_p}{\lambda_e} = \frac{hc}{E} \times \frac{\sqrt{2mE}}{h} = \frac{c\sqrt{2mE}}{E} \]
If \( E \) is indeed kinetic energy, simplifying gives:
\[ \frac{\lambda_p}{\lambda_e} = \frac{\sqrt{2mE}}{c} \]
Thus, the correct ratio is:
\(\frac{\sqrt{2mE}}{c}\).
If \( \lambda \) and \( K \) are de Broglie wavelength and kinetic energy, respectively, of a particle with constant mass. The correct graphical representation for the particle will be: