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Discrete Semiconductor Devices and Circuits

Class A BJT Amplifiers


62 questions By Tony R. Kuphaldt

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  • Question 55 of 62

    Explain each of the mathematical approximations for this typical common-emitter amplifier circuit (with a bypass capacitor):

    $$A_V \approx \frac{R_C||R_{load}}{r'_e}$$

    $$Z_{in} \approx R_1 || R_2 || (\beta+1)r’_e$$

    $$Z_{out} \approx R_C$$

    What does each term in each expression represent, and why do they relate to one another as shown?

    Reveal answer
  • Question 56 of 62

    Explain each of the mathematical approximations for this typical common-emitter amplifier circuit (with the dynamic emitter resistance ßwamped” by RE):

    $$A_V \approx \frac{R_C||R_{load}}{r'_e+R_E}$$

    $$Z_{in} \approx R_1||R_2||(\beta+1)(r’_e+R_E)$$

    $$Z_{out} \approx R_C$$

    What does each term in each expression represent, and why do they relate to one another as shown?

    Reveal answer
  • Question 57 of 62

    A common set of equations for calculating input and output impedances of bypassed common-emitter amplifier circuits is as follows:

    $$Z_{in} \approx R_1||R_2||(\beta+1)r’_e$$

    $$Z_{out} \approx R_C$$

    If precision is not required, we may greatly simplify the first equation by assuming the transistor to be ideal; i.e. having an infinite current gain (β = ∞). Re-write the first equation accordingly, and explain how you simplified it.

    Reveal answer

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