Robert A. Millikan's photoelectric effect experiment yielded a slope of \( 4.12 \times 10^{-15} \, \text{Vs} \) for the cut-off voltage versus frequency plot. This allows us to determine Planck's constant (\( h \)).
The photoelectric effect is governed by:
\[ eV_{\text{cut-off}} = h u - \phi \] where:
The plot of \( V_{\text{cut-off}} \) against \( u \) is linear. Rearranging the photoelectric equation yields:
\[ V_{\text{cut-off}} = \frac{h}{e} u - \frac{\phi}{e} \]
This is in the form \( y = mx + c \), with:
Therefore, the slope \( m = \frac{h}{e} \), enabling Planck's constant calculation from the given slope.
Given slope \( m = 4.12 \times 10^{-15} \, \text{Vs} \) and \( e = 1.6 \times 10^{-19} \, \text{C} \). Using:
\[ \frac{h}{e} = 4.12 \times 10^{-15} \, \text{Vs} \]
Solving for \( h \):
\[ h = 4.12 \times 10^{-15} \times 1.6 \times 10^{-19} \, \text{Js} \]
\[ h = 6.592 \times 10^{-34} \, \text{Js} \]
Planck's constant \( h \) is approximately \({6.59 \times 10^{-34}} \, \text{Js}\).