Step 1: State the relations for a Common Emitter (CE) configuration.
In a transistor, the emitter current ($I_E$), collector current ($I_C$), and base current ($I_B$) are related by:
\[
I_E = I_C + I_B.
\]
The current amplification factor in the CE configuration is $\beta$, which is the ratio of the collector current to the base current:
\[
\beta = \frac{I_C}{I_B}.
\]
Step 2: Relate the emitter current to the base current using $\beta$.
From the definition of $\beta$, we have $I_C = \beta I_B$.
Substitute this into the emitter current relation:
\[
I_E = (\beta I_B) + I_B = (\beta+1)I_B.
\]
This gives the base current as:
\[
I_B = \frac{I_E}{\beta+1}.
\]
Step 3: Substitute the given values.
We are given the current amplification factor $\beta = 80$.
The emitter current is $I_E = 2.43 \text{ mA} = 2.43 \times 10^{-3} \text{ A}$.
\[
I_B = \frac{2.43 \text{ mA}}{80 + 1} = \frac{2.43 \text{ mA}}{81}.
\]
Step 4: Calculate the numerical value of the base current.
The fraction $\frac{2.43}{81}$ can be calculated:
\[
\frac{2.43}{81} = \frac{243}{8100}.
\]
Since $81 \times 3 = 243$, we have:
\[
I_B = \frac{3}{100} \text{ mA} = 0.03 \text{ mA}.
\]
Step 5: Convert the result to $\mu$A.
Since $1 \text{ mA} = 1000 \mu\text{A}$:
\[
I_B = 0.03 \times 1000 \mu\text{A} = 30 \mu\text{A}.
\]
\[
\boxed{I_B = 30 \mu\text{A}}.
\]