357766 When a certain metal surface is illuminated with a light of wavelength \(\lambda\), the stopping potential is \(V\), when the same surface is illuminated by light of wavelength \(2 \lambda\), the stoping potential is \(\left(\dfrac{V}{3}\right)\). The threshold wavelength for the surface is
357767
The graph of stopping potential \(v_{s}\) against frequency \(v_{0}\) of incident radiation is plotted for two different metals \(P\) and \(Q\) as shown in the graph. \(\phi_{p}\) and \(\phi_{Q}\) are work - functions of \(P\) and \(Q\) respectively, then
357766 When a certain metal surface is illuminated with a light of wavelength \(\lambda\), the stopping potential is \(V\), when the same surface is illuminated by light of wavelength \(2 \lambda\), the stoping potential is \(\left(\dfrac{V}{3}\right)\). The threshold wavelength for the surface is
357767
The graph of stopping potential \(v_{s}\) against frequency \(v_{0}\) of incident radiation is plotted for two different metals \(P\) and \(Q\) as shown in the graph. \(\phi_{p}\) and \(\phi_{Q}\) are work - functions of \(P\) and \(Q\) respectively, then
357766 When a certain metal surface is illuminated with a light of wavelength \(\lambda\), the stopping potential is \(V\), when the same surface is illuminated by light of wavelength \(2 \lambda\), the stoping potential is \(\left(\dfrac{V}{3}\right)\). The threshold wavelength for the surface is
357767
The graph of stopping potential \(v_{s}\) against frequency \(v_{0}\) of incident radiation is plotted for two different metals \(P\) and \(Q\) as shown in the graph. \(\phi_{p}\) and \(\phi_{Q}\) are work - functions of \(P\) and \(Q\) respectively, then
357766 When a certain metal surface is illuminated with a light of wavelength \(\lambda\), the stopping potential is \(V\), when the same surface is illuminated by light of wavelength \(2 \lambda\), the stoping potential is \(\left(\dfrac{V}{3}\right)\). The threshold wavelength for the surface is
357767
The graph of stopping potential \(v_{s}\) against frequency \(v_{0}\) of incident radiation is plotted for two different metals \(P\) and \(Q\) as shown in the graph. \(\phi_{p}\) and \(\phi_{Q}\) are work - functions of \(P\) and \(Q\) respectively, then