- Planck’s constant: $\text{h}=\frac{\text{lm}}{2\text{n}}$
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and $\nu_2^2$ are the velocities of the emitted electrons for radiations of frequencies v1 > v and v2 > v respectively. So, $\text{h}\nu_1=\text{h}\nu+\frac{1}{2}\text{mv}^2_1\dots(\text{i})$
and $\text{h}\nu_2=\text{h}\nu+\frac{1}{2}\text{mv}^2_2\dots(\text{ii})$
From equation (i) and (ii), we get
$\text{h}(\nu_2-\nu_1)=\frac{1}{2}\text{m}(\text{v}^2_2-\text{v}^2_1)$
$\therefore\ \text{h}=\frac{\frac{1}{2}\text{m}(\text{v}^2_2-\text{v}^2_1)}{(\nu_2-\nu_1)}$
Slope of $\text{v}^2_\text{max}$ vs frequency graph is,
$\tan\theta=\frac{\text{v}^2_2-\text{v}^2_1}{(\nu_2-\nu_1)}$
$\therefore\ \text{h}=\frac{1}{2}\text{m}.\tan\theta$
From graph
$\tan\theta=\frac{1}{\text{n}}$ So, $\text{h}=\frac{1}{2}\text{m}\Big(\frac{\text{l}}{\text{n}}\Big)\dots(\text{iii})$
- From graph, the work function of the material is,
w = hn ...(iv)
From equations (iii) and (iv), we get
$\text{w}=\frac{1}{2}\text{m}\Big(\frac{\text{l}}{\text{n}}\Big)\times\text{n}=\frac{1}{2}\text{ml}$