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:
\(\lambda_{\text{min}} \propto \frac{1}{V}\)
A sphere of radius R is cut from a larger solid sphere of radius 2R as shown in the figure. The ratio of the moment of inertia of the smaller sphere to that of the rest part of the sphere about the Y-axis is :
The current passing through the battery in the given circuit, is:
A bob of heavy mass \(m\) is suspended by a light string of length \(l\). The bob is given a horizontal velocity \(v_0\) as shown in figure. If the string gets slack at some point P making an angle \( \theta \) from the horizontal, the ratio of the speed \(v\) of the bob at point P to its initial speed \(v_0\) is :