To determine the relationship between the minimum wavelength of X-rays and the potential difference through which electrons are accelerated, we use the concept of X-ray production in a Coolidge tube. When electrons are accelerated through a potential difference \( V \), their kinetic energy becomes \( eV \), where \( e \) is the charge of the electron. Upon collision with a target, this energy can be converted into a photon of X-ray, obeying the energy conservation principle. The energy of a photon is given by \( E = \frac{hc}{\lambda} \), where \( h \) is Planck's constant, \( c \) is the speed of light, and \( \lambda \) is the wavelength. Thus, equating the energy, we have:
\(eV = \frac{hc}{\lambda_{\text{min}}}\)
Rearranging to find the minimum wavelength \(\lambda_{\text{min}}\), we obtain:
\(\lambda_{\text{min}} = \frac{hc}{eV}\)
This expression shows that the minimum wavelength is inversely proportional to the potential difference \( V \). Therefore, the correct proportionality for the minimum wavelength \(\lambda_{\text{min}}\) is:
\(\lambda_{\text{min}} \propto \frac{1}{V}\)
AB is a part of an electrical circuit (see figure). The potential difference \(V_A - V_B\), at the instant when current \(i = 2\) A and is increasing at a rate of 1 amp/second is: