Step 1: Define the saturation condition.A BJT is saturated when fully on. In this state, the collector-emitter voltage reaches its minimum, \(V_{CEsat}\), and the collector current is limited by external circuit components.
Step 2: Calculate the saturation collector current (\(I_{Csat}\)).Apply Kirchhoff's Voltage Law (KVL) to the collector-emitter loop:\[ V_{CC} = I_C R_C + V_{CE} \]At saturation, \(V_{CE} = V_{CEsat}\). Therefore:\[ I_{Csat} = \frac{V_{CC} - V_{CEsat}}{R_C} \]Substitute the provided values:\[ I_{Csat} = \frac{3 V - 0.2 V}{1 k\Omega} = \frac{2.8 V}{1000 \Omega} = 2.8 \text{ mA} \]
Step 3: Calculate the minimum base current required (\(I_{Bmin}\)).To ensure saturation, the base current must be sufficient to support the saturation collector current. This relationship depends on the transistor's current gain, \(\beta\):\[ I_C = \beta I_B \implies I_B = \frac{I_C}{\beta} \]The minimum base current to achieve saturation is:\[ I_{Bmin} = \frac{I_{Csat}}{\beta} = \frac{2.8 \text{ mA}}{50} = 0.056 \text{ mA} \]Convert to microamperes: \(0.056 \text{ mA} = 56 \text{ } \mu A\).