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Question
双极性结型晶体管的伏安特性:[...]
Answer
  • 发射极(Emitter):\(\begin{align}I_{E}&=I_{S}\left(e^{\frac{qV_{BE}}{KT}}-1\right)\approx I_{S}e^{\frac{qV_{BE}}{KT}}=I_{S}e^{\frac{V_{BE}}{V_{T}}}\\&=I_{C}+I_{B}=(\beta+1)I_{B}\end{align}\)
  • 集极(Collector):\(\begin{align}I_{C}&=\alpha I_{E}=\alpha I_{S}e^{\frac{V_{BE}}{V_{T}}}\\&=\beta I_{B}\end{align}\)
  • 基极(Base):\(I_{B}=I_{E}-I_{C}=(1-\alpha)I_{E}=(1-\alpha)I_{S}e^{\frac{V_{BE}}{V_{T}}}\)

Question
双极性结型晶体管的伏安特性:[...]
Answer
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Question
双极性结型晶体管的伏安特性:[...]
Answer
  • 发射极(Emitter):\(\begin{align}I_{E}&=I_{S}\left(e^{\frac{qV_{BE}}{KT}}-1\right)\approx I_{S}e^{\frac{qV_{BE}}{KT}}=I_{S}e^{\frac{V_{BE}}{V_{T}}}\\&=I_{C}+I_{B}=(\beta+1)I_{B}\end{align}\)
  • 集极(Collector):\(\begin{align}I_{C}&=\alpha I_{E}=\alpha I_{S}e^{\frac{V_{BE}}{V_{T}}}\\&=\beta I_{B}\end{align}\)
  • 基极(Base):\(I_{B}=I_{E}-I_{C}=(1-\alpha)I_{E}=(1-\alpha)I_{S}e^{\frac{V_{BE}}{V_{T}}}\)

Summary

statusnot learnedmeasured difficulty37% [default]last interval [days]               
repetition number in this series0memorised on               scheduled repetition               
scheduled repetition interval               last repetition or drill

Details

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