Step 1: Understand the original capacitor
Given:
- Plate area = \( A \)
- Plate separation = \( d = 2\,m \)
- Original capacitance \( C = 4\,\mu F \)
This is for air/vacuum between the plates (dielectric constant \( K = 1 \)).
Using the formula:
\[
C = \frac{\varepsilon_0 A}{d}
\]
From this, \( \frac{\varepsilon_0 A}{2} = 4\,\mu F \)
Step 2: New setup with partial dielectric
Half the space is filled with dielectric \( K = 3 \), and the other half is air.
So the system behaves like two capacitors connected in parallel, each with plate area \( A \), but different separations:
- Capacitor 1 (with dielectric): \( d_1 = 1\,m \), \( K = 3 \)
- Capacitor 2 (without dielectric): \( d_2 = 1\,m \), \( K = 1 \)
Step 3: Calculate individual capacitances
Let’s find \( \varepsilon_0 A \) from the original setup:
\[
\frac{\varepsilon_0 A}{2} = 4\,\mu F \Rightarrow \varepsilon_0 A = 8\,\mu F
\]
Now compute the two capacitances:
- With dielectric:
\[
C_1 = \frac{K \varepsilon_0 A}{d_1} = \frac{3 \times 8}{1} = 24\,\mu F
\]
- Without dielectric:
\[
C_2 = \frac{\varepsilon_0 A}{d_2} = \frac{8}{1} = 8\,\mu F
\]
Step 4: Combine the two capacitors
These two are in series along the vertical axis (since dielectric fills half the separation, not half the area).
So equivalent capacitance:
\[
\frac{1}{C_{\text{eq}}} = \frac{1}{C_1} + \frac{1}{C_2} = \frac{1}{24} + \frac{1}{8} = \frac{1 + 3}{24} = \frac{4}{24}
\Rightarrow C_{\text{eq}} = \frac{24}{4} = 6\,\mu F
\]
Final Answer: 6μF