With a constant charge \( Q \), capacitance \( C = \frac{\varepsilon_0 A}{d} \) without dielectric, and
\( C' = \frac{K \varepsilon_0 A}{d} \) with dielectric (\( K > 1 \)). When the dielectric is fully
inserted, \( C \) increases, reducing \( V = \frac{Q}{C} \). If the slab is partially removed, the
effective capacitance decreases (as less dielectric area contributes \( K \)), approaching the air value.
Since \( Q \) is constant, a decrease in \( C \) leads to an increase in \( V \), as \( V = \frac{Q}{C}
\).
The electric field becomes non-uniform
The effective capacitance decreases
The charge on the plates increases
The dielectric induces more charges