Step 1: Understand the effect of a dielectric on a capacitor.
When a dielectric material is inserted between the plates of a charged capacitor, it becomes polarized, and an induced charge appears on its surfaces. This induced charge creates an electric field that opposes the original electric field due to the charges on the capacitor plates. The net electric field inside the dielectric is reduced, and consequently, the potential difference across the plates decreases, while the charge on the plates remains the same (if the capacitor is isolated).
Step 2: Relate the induced charge to the free charge and the dielectric constant.
Let \( Q \) be the free charge on the capacitor plates, and \( Q_i \) be the magnitude of the induced charge on each face of the dielectric slab. The relationship between these charges and the dielectric constant \( K \) of the material is given by:
\[
Q_i = Q \left(1 - \frac{1}{K}\right)
\]
Step 3: Substitute the given values into the formula.
We are given:
Free charge on the capacitor plates, \( Q = 5 \times 10^{-6} \, C \)
Induced charge on one face of the dielectric slab, \( Q_i = 4 \times 10^{-6} \, C \)
Substituting these values into the formula:
\[
4 \times 10^{-6} = 5 \times 10^{-6} \left(1 - \frac{1}{K}\right)
\]
Step 4: Solve for the dielectric constant \( K \).
Divide both sides by \( 5 \times 10^{-6} \):
\[
\frac{4 \times 10^{-6}}{5 \times 10^{-6}} = 1 - \frac{1}{K}
\]
\[
\frac{4}{5} = 1 - \frac{1}{K}
\]
Rearrange the equation to solve for \( \frac{1}{K} \):
\[
\frac{1}{K} = 1 - \frac{4}{5}
\]
\[
\frac{1}{K} = \frac{5}{5} - \frac{4}{5}
\]
\[
\frac{1}{K} = \frac{1}{5}
\]
Now, solve for \( K \):
\[
K = 5
\]
The dielectric constant of the slab is 5.