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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