The photoelectric equation is stated as:
\[ KE_{\text{max}} = hu - \phi \]
Here, \( KE_{\text{max}} \) represents the maximum kinetic energy of emitted electrons, \( h \) is Planck's constant, \( u \) is the frequency of the incident light, and \( \phi \) is the work function of the metal.
The maximum kinetic energy can also be expressed using the stopping potential \( V_0 \) as:
\[ KE_{\text{max}} = eV_0 \]
where \( e \) is the elementary charge.
By equating the two expressions for \( KE_{\text{max}} \):
\[ eV_0 = hu - \phi \]
This equation can be rearranged to:
\[ V_0 = \frac{h}{e} u - \frac{\phi}{e} \]
When compared to the standard linear equation \( y = mx + c \), the slope \( m \) is identified as:
\[ m = \frac{h}{e} \]
Therefore, the charge of an electron \( e \) can be determined as:
\[ e = \frac{h}{m} \]
Consequently, the correct answer is \( \frac{h}{m} \).