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EE130/230A Discussion  14 EE130/230A Discussion  14

EE130/230A Discussion 14 - PowerPoint Presentation

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EE130/230A Discussion 14 - PPT Presentation

Peng Zheng 1 Game Plan for IV Derivation Solve the minoritycarrier diffusion equation in each quasineutral region to obtain excess minoritycarrier profiles different set of boundary conditions for each region ID: 759733

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Slide1

EE130/230A Discussion 14

Peng Zheng

1

Slide2

“Game Plan” for I-V Derivation

Solve the minority-carrier diffusion equation in each quasi-neutral region to obtain excess minority-carrier profilesdifferent set of boundary conditions for each regionFind minority-carrier diffusion currents at depletion region edgesAdd hole & electron components together  terminal currents

EE130/230A Fall 2013

Lecture 26, Slide

2

Slide3

BJT Terminal Currents

We know:Therefore:

EE130/230A Fall 2013

Lecture 26, Slide

3

Slide4

BJT with Narrow Base

In practice, we make W << LB to achieve high current gain. Then, since we have:

EE130/230A Fall 2013

Lecture 26, Slide

4

R. F.

Pierret

,

Semiconductor Device Fundamentals

, Fig. 11.2

Slide5

Ebers-Moll Model

The Ebers-Moll model is a large-signal equivalent circuit which describes both the active and saturation regions of BJT operation.Use this model to calculate IB and IC given VBE and VBC

increasing

(npn) or

VEC (pnp)

EE130/230A Fall 2013

Lecture 26, Slide 5

C. C. Hu,

Modern Semiconductor Devices for Integrated Circuits

, Figure 8-2

Slide6

If only VEB is applied (VCB = 0):

If only

V

CB is applied (VEB = 0): :

a

R

: reverse common base gainaF : forward common base gain

I

C

V

CB

V

EB

I

B

E

B

C

Reciprocity relationship

:

EE130/230A Fall 2013

Lecture 26, Slide

6

Slide7

In the general case, both

V

EB and VCB are non-zero:

IE: E-B diode current + fraction of C-B diode current that makes it to the E-B junction

I

C

: C-B diode current + fraction of E-B diode current that makes it to the C-B junction

Large-signal equivalent circuit for a pnp BJT

EE130/230A Fall 2013

Lecture 26, Slide

7

R. F.

Pierret, Semiconductor Device Fundamentals, Fig. 11.3

Slide8

High gain (bdc >> 1) One-sided emitter junction, so emitter efficiency g  1Emitter doped much more heavily than base (NE >> NB) Narrow base, so base transport factor aT  1Quasi-neutral base width << minority-carrier diffusion length (W << LB)IC determined only by IB (IC  function of VCE,VCB) One-sided collector junction, so quasi-neutral base width W does not change drastically with changes in VCE (VCB)Based doped more heavily than collector (NB > NC)(W = WB – xnEB – xnCB for PNP BJT)

Summary: BJT Performance Requirements

EE130/230A Fall 2013

Lecture 26, Slide

8

Slide9

Questions regarding the MOSFET design project?

9

Good luck to Quiz#6!