Step 1: Expression for the capacitance of a parallel plate capacitor.
The capacitance of a parallel plate capacitor without a dielectric is given by:
\[
C_0 = \frac{\varepsilon_0 A}{d}
\]
where:
- \( \varepsilon_0 \) is the permittivity of free space,
- \( A \) is the area of each plate,
- \( d \) is the separation between the plates.
When a dielectric material with dielectric constant \( \kappa \) is inserted between the plates, the capacitance increases by a factor of \( \kappa \), and the capacitance becomes:
\[
C = \kappa C_0 = \frac{\kappa \varepsilon_0 A}{d}
\]
Step 2: Induced charge on the dielectric slab.
Let the total charge on the capacitor be \( Q = 100 \, \mu \text{C} \). The electric field \( E \) inside the capacitor is related to the charge \( Q \) and the capacitance \( C \) by:
\[
E = \frac{Q}{C}
\]
For the dielectric material inserted, the induced charge \( Q_{\text{induced}} \) on the dielectric slab is given by:
\[
Q_{\text{induced}} = \left( \kappa - 1 \right) \times Q
\]
Substituting the given values:
\[
Q_{\text{induced}} = \left( 2.0 - 1 \right) \times 100 \, \mu\text{C} = 1 \times 100 \, \mu\text{C} = 100 \, \mu\text{C}
\]
Step 3: Conclusion.
The induced charge on the dielectric slab in the capacitor is \( 100 \, \mu\text{C} \).