To determine the change in the resolving power of a scanning microscope when protons are used instead of electrons, we need to consider the de Broglie wavelength relation. The resolving power of a microscope is inversely proportional to the wavelength of the particles used.
The de Broglie wavelength \(\lambda\) is given by:
\(\lambda = \frac{h}{mv}\)
where:
For electrons and protons at the same speed, the formula becomes:
\(\lambda_e = \frac{h}{m_e v}\) and \(\lambda_p = \frac{h}{m_p v}\)
where:
The ratio of their wavelengths is:
\(\frac{\lambda_p}{\lambda_e} = \frac{m_e}{m_p}\)
Given that the mass of a proton is approximately 1837 times that of an electron \((m_p = 1837 \cdot m_e)\), the ratio simplifies to:
\(\frac{\lambda_p}{\lambda_e} = \frac{1}{1837}\)
As the resolving power \((RP)\) is inversely proportional to the wavelength:
\(\text{RP} \propto \frac{1}{\lambda}\)
The resolving power of the scanning proton microscope compared to the electron microscope is given by:
\(\frac{\text{RP}_p}{\text{RP}_e} = \frac{\lambda_e}{\lambda_p} = 1837\)
Thus, the resolving power changes by a factor of 1837. Therefore, the correct answer is:
1837