To solve this problem, we need to find out the relationship between the accelerating voltage of electrons and the de-Broglie wavelength associated with them. The de-Broglie wavelength \( \lambda \) is given by the equation:
\lambda = \frac{h}{p}
where:
The momentum \( p \) of an electron accelerated by a voltage \( V \) can be found using:
p = \sqrt{2meV}
where:
Substituting for \( p \) in the de-Broglie wavelength formula:
\lambda = \frac{h}{\sqrt{2meV}}
This shows that the de-Broglie wavelength is inversely proportional to the square root of the voltage \( V \). Therefore, as the voltage increases, the wavelength decreases. Specifically, if the voltage is increased from 25 kV to 100 kV, we have:
\lambda \propto \frac{1}{\sqrt{V}}
If the initial voltage is \( V_1 = 25 \, \text{kV} \) and the final voltage is \( V_2 = 100 \, \text{kV} \), then the initial and final wavelengths \( \lambda_1 \) and \( \lambda_2 \) are related by:
\frac{\lambda_2}{\lambda_1} = \sqrt{\frac{V_1}{V_2}} = \sqrt{\frac{25}{100}} = \frac{1}{2}
Thus, the final wavelength \( \lambda_2 \) becomes half of the initial wavelength \( \lambda_1 \), meaning the de-Broglie wavelength decreases by 2 times.
Therefore, out of the given options, the correct answer is that the de-Broglie wavelength associated with the electrons would "decrease by 2 times".
