The relationship between the rise time (\(t_r\)) of a device (like a BJT or an amplifier) and its upper 3dB cutoff frequency (\(f_H\)) or bandwidth (BW) is approximately given by: \[ t_r \approx \frac{0.35}{f_H} \]
The transition frequency (\(f_T\)) of a BJT is related to its high-frequency performance and is often considered as a measure of its bandwidth capability. In many contexts, especially for a single-pole response approximation, \(f_H\) can be related to \(f_T\). However, a more direct relation for transition frequency involves \(f_T = \text{gain} \times \text{bandwidth}\).
If we assume that the rise time is primarily limited by the dominant high-frequency pole, then \(f_H\) can be considered a measure of the bandwidth. The transition frequency \(f_T\) is the frequency at which the short-circuit common-emitter current gain (\(\beta(j\omega)\) or \(h_{fe}(j\omega)\)) drops to unity (0 dB).
The relation \(t_r \cdot BW \approx 0.35\) is commonly used. If we consider \(f_T\) to be the relevant bandwidth here: \[ f_T \approx \frac{0.35}{t_r} \]
Given \(t_r = 3.5\) micro seconds = \(3.5 \times 10^{-6}\) seconds.
\[ f_T \approx \frac{0.35}{3.5 \times 10^{-6} \text{ s}} = \frac{0.35}{3.5} \times 10^6 \text{ Hz} = 0.1 \times 10^6 \text{ Hz} = 100 \times 10^3 \text{ Hz} = 100 \text{ kHz} \]
This matches option (d).
Final Answer: \[ \boxed{100 \text{ kHz}} \]