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Answer: \(\alpha_{DC} = \dfrac{I_C}{I_E}\), \(\beta_{DC} = \dfrac{I_C}{I_B}\); \(\beta_{DC} = \dfrac{\alpha_{DC}}{1 - \alpha_{DC}}\) and \(\alpha_{DC} = \dfrac{\beta_{DC}}{1 + \beta_{DC}}\).

\(\alpha_{DC}\) (common base d.c. current gain) is the ratio of the collector current to the emitter current: \(\alpha_{DC} = \dfrac{I_C}{I_E}\). Its value is slightly less than 1.

\(\beta_{DC}\) (common emitter d.c. current gain) is the ratio of the collector current to the base current: \(\beta_{DC} = \dfrac{I_C}{I_B}\). It is large (typically 50 to 300).

Relation: In a transistor, \(I_E = I_B + I_C\).

Dividing by \(I_C\): \(\dfrac{I_E}{I_C} = \dfrac{I_B}{I_C} + 1\), i.e. \(\dfrac{1}{\alpha_{DC}} = \dfrac{1}{\beta_{DC}} + 1\).

So \(\dfrac{1}{\beta_{DC}} = \dfrac{1}{\alpha_{DC}} - 1 = \dfrac{1 - \alpha_{DC}}{\alpha_{DC}}\), giving \(\beta_{DC} = \dfrac{\alpha_{DC}}{1 - \alpha_{DC}}\).

Similarly, \(\dfrac{1}{\alpha_{DC}} = \dfrac{1 + \beta_{DC}}{\beta_{DC}}\), so \(\alpha_{DC} = \dfrac{\beta_{DC}}{1 + \beta_{DC}}\).

Doubtly AI · 29 Oct 2026 AI-generated · not yet verified Report
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