For a Common Emitter (CE) transistor amplifier, the current amplification factor \( \beta \) (also denoted as \( h_{fe} \)) is defined as the ratio of the collector current \( I_C \) to the base current \( I_B \):
$$ \beta = \frac{I_C}{I_B} $$
We are given \( \beta = 59 \).
The emitter current \( I_E \) is the sum of the base current \( I_B \) and the collector current \( I_C \):
$$ I_E = I_B + I_C $$
We are given \( I_E = 6.
6 \) mA.
We can express \( I_C \) in terms of \( I_B \) and \( \beta \):
$$ I_C = \beta I_B = 59 I_B $$
Substitute this into the equation for \( I_E \):
$$ I_E = I_B + 59 I_B = 60 I_B $$
Now, we can solve for the base current \( I_B \):
$$ I_B = \frac{I_E}{60} = \frac{6.
6 \text{ mA}}{60} $$
$$ I_B = \frac{6.
6}{60} \text{ mA} = 0.
11 \text{ mA} $$
The base current is \( 0.
11 \) mA.