Appeared in: 2026 (3 sets)
A graph between the frequency of incident radiation ($\nu$) and the corresponding stopping potential ($V_0$) for a metal is a straight line. Let $\alpha$ and $\beta$ be the value of the slope and the value of the intercept on the $V_0$-axis respectively. Then, according to Einstein's photoelectric equation $\left(\frac{\beta}{\alpha}\right)$ is :
(A) $\nu_0$
(B) $\frac{1}{\nu_0}$
(C) $e\nu_0$
(D) $\frac{\nu_0}{h}$