
To solve this problem, we need to understand the relation between stopping potential, frequency of incident light, and Planck's constant. The photoelectric effect is described by Einstein's photoelectric equation:
\(K.E._\text{max} = h v - \phi\),
where:
The stopping potential \(V_0\) is related to the maximum kinetic energy by:
\(e V_0 = K.E._\text{max}\),
where \(e\) is the charge of the electron. Substituting \(K.E._\text{max}\) from Einstein's equation:
\(e V_0 = h v - \phi\)
Rearranging, we get:
\(V_0 = \frac{h}{e} v - \frac{\phi}{e}\)
This is in the form of a straight line \(y = mx + c\), where:
Thus, Planck's constant \(h\) is given by:
\(h = e \times (\text{slope of the line})\)
Therefore, the correct answer is: product of slope of the line and charge on the electron.
