The de Broglie wavelength (\(\lambda\)) of a particle is given by the equation:
\[
\lambda = \frac{h}{p}
\]
where \(h\) is Planck's constant and \(p\) is the momentum of the particle. The kinetic energy (\(K\)) of a particle is related to its momentum by:
\[
K = \frac{p^2}{2m} \implies p = \sqrt{2mK}
\]
where \(m\) is the mass of the particle.
For the electron (\(e\)), the kinetic energy is \(K_e = E\) and its mass is \(m_e\). The de Broglie wavelength of the electron is:
\[
\lambda_e = \frac{h}{p_e} = \frac{h}{\sqrt{2m_e K_e}} = \frac{h}{\sqrt{2m_e E}}
\]
For the proton (\(p\)), the kinetic energy is \(K_p = 3E\) and its mass is \(m_p = 1836 m_e\). The de Broglie wavelength of the proton is:
\[
\lambda_p = \frac{h}{p_p} = \frac{h}{\sqrt{2m_p K_p}} = \frac{h}{\sqrt{2(1836 m_e) (3E)}} = \frac{h}{\sqrt{11016 m_e E}}
\]
Now, we need to find the ratio of their de Broglie wavelengths (\(\lambda_e / \lambda_p\)):
\[
\frac{\lambda_e}{\lambda_p} = \frac{\frac{h}{\sqrt{2m_e E}}}{\frac{h}{\sqrt{11016 m_e E}}} = \frac{\sqrt{11016 m_e E}}{\sqrt{2m_e E}} = \sqrt{\frac{11016 m_e E}{2m_e E}}
\]
\[
\frac{\lambda_e}{\lambda_p} = \sqrt{\frac{11016}{2}} = \sqrt{5508}
\]
\[
\sqrt{5508} \approx 74.2159
\]
Rounding off to two decimal places, the ratio \(\lambda_e / \lambda_p\) is 74.22. This falls within the given range of 74.10 to 74.30.