A1: An NPN may have 3 states, which can be linearly modeled as:
- Cutoff: BE junction is reverse biased
- $i_B=0$, $i_C=0$
- $v_{BE}<v_{D0}$
- Active: BE junction is forward biased, BC junction is reverse biased
- $v_{BE}=v_{D0}$, $i_B \geq 0$
- $i_C=\beta i_B$, $v_{CE}\geq v_{D0}$
- Saturation*: BE junction is forward biased, BC junction is forward biased
- $v_{BE}=v_{D0}$, $i_B \geq 0$
- $v_{CE}=v_{sat}$, $i_C < \beta i_B$
*There are actually 3 subcategories of saturation: soft saturation, near cutoff saturation, and deep saturation. Here, we'll use saturation to mean deep saturation.
For a PNP, flip the order of the subscript letters for voltages and remember that current directions reverse (relative to the NPN)
For silicon, $v_{sat}=0.2V$
Q2: How can I solve BJT circuits?
A2: To specify the 6 BJT parameters, recall that you only need to find 2 currents and 2 voltages. For example, you might choose to calculate:
- $v_{BE}$
- $v_{CE}$
- $i_{B}$
- $i_{C}$
- Write down the KVL equation for the BE and CE voltages.
- Assume BJT is off: set $i_B=0$ and $i_C=0$. Check this assumption using the BE-KVL.
- If it follows that $v_BE<v_{D0}$, your assumption is correct. You can then use the CE-KVL to solve for $v_{CE}$
- Otherwise, the BJT has a forward biased BE junction. Set $v_BE=0.7$ to compute $i_B$
- Assume the BJT is active: set $i_C=\beta i_B$. Check this assumption using the CE-KVL.
- If it follows that $v_{CE} \geq v_{D0}$, your assumption is correct
- Otherwise, the BJT must be in saturation
- The BJT is in saturation: set $v_{CE}=v_{sat}$.
- Use the CE-KVL to find $i_C$.
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