Concept:
The small-signal transconductance (\(g_m\)) of a Bipolar Junction Transistor (BJT) measures the sensitivity of the collector current output response relative to changes in the base-emitter input voltage. In the Common Emitter (CE) configuration, transconductance depends directly on the DC bias collector current (\(I_C\)) and the thermal voltage (\(V_T\)):
\[
g_m = \frac{I_C}{V_T}
\]
where \(V_T = \frac{\bar{k}T}{q}\) is the thermal voltage, which is approximately equal to 25 mV (or 26 mV) at standard room temperature.
Step 1: Identify the given values and convert units to standard form.
The parameters provided are:
• DC Collector current (\(I_C\)) = \(2.4\text{ mA} = 2.4 \times 10^{-3}\text{ A}\)
• Thermal voltage (\(V_T\)) = \(25\text{ mV} = 25 \times 10^{-3}\text{ V}\)
• Current gain factor (\(\beta\)) = 120
Step 2: Calculate the small-signal transconductance (\(g_m\)).
Substitute the values into the transconductance formula:
\[
g_m = \frac{2.4 \times 10^{-3}\text{ A}}{25 \times 10^{-3}\text{ V}}
\]
The \(10^{-3}\) scale terms in the numerator and denominator cancel out directly:
\[
g_m = \frac{2.4}{25}\text{ Siemens (S)}
\]
To evaluate this division easily, multiply both the numerator and the denominator by 4:
\[
g_m = \frac{2.4 \times 4}{25 \times 4} = \frac{9.6}{100} = 0.096\text{ S}
\]
Thus, the small-signal transconductance of the BJT is equal to 0.096 S, matching option (C).