V₀₁ is delayed by 2 μs relative to V_i, and V₀₂ is a triangular waveform.

V₀₁ is not delayed relative to V_i, and V₀₂ is a trapezoidal waveform.

V₀₁ is not delayed relative to Vi, and V₀₂ is a triangular waveform.

V₀₁ is delayed by 1 μs relative to V_i, and V₀₂ is a trapezoidal waveform.

$29R$ and $1/(2\pi \sqrt{6}RC)$

$2R$ and $1/(2\pi RC)$

$29R$ and $1/(2\pi RC)$

$2R$ and $1/(2\pi \sqrt{6}RC)$

$g_{m2}R_D$

$\frac{g_{m2} R_D \left( R_B + \frac{1}{g_{m1}} \right)}{R_B + \frac{1}{g_{m1}} + R_S}$

$\frac{g_{m2} R_D \left( R_B + \frac{1}{g_{m1}} + R_S \right)}{R_B + \frac{1}{g_{m1}}}$

$\frac{g_{m2} R_D \left( \frac{1}{g_{m1}} \right)}{\frac{1}{g_{m1}} + R_S}$

Under high-level injection condition in forward active mode, $\beta$ will decrease with increase in the magnitude of collector current.

Under low-level injection condition in forward active mode, where the current at the emitter-base junction is dominated by recombination-generation process, $\beta$ will decrease with increase in the magnitude of collector current.

$\beta$ will be lower when the BJT is in saturation region compared to when it is in active region.

A higher value of $\beta$ will lead to a lower value of the collector-to-emitter breakdown voltage.