PNP junction transistor

The PNP junction transistor pictorial presentation is:

pnp junction transistor picture

VEE forward-biases emitter-base pn junction, electrons in base flow to emitter. Emitter base junction property is low impedance and low voltage drop but collector base junction is reverse-biased with high impedance. Current in the emitter circuit is emitter current while current in the collector circuit is collector current. Collector current comprised of emitter current and collector base current, ICBO. The emitter current has constant of proportionality α or αIE.

Both currents αIE and ICBO . This is written as IC =  αIE + ICBO . Apply KCL to this transistor yields

IE = IB + IC

β

From IE = IB + IC , IB = IE - IC. But  IC =  αIE + ICBO rearrange α we get

hFE parameter discovered

The ratio α/(1-α) represents β.

Emitter Base Junction

pnp junction transistor picture

Apply KVL to emitter base loop the emitter current is IE = (VEE - VEB)/ Re . Simplify circuit that voltage collector dependence is negligible and dependence of emitter current on collector base voltage is postponed then emitter-base circuit is exactly same as the analysis of diode circuits.

Emitter base characteristic

Voltage threshold or VEBQ is about 0.7 for silicon transistor. When VEE = 4 volts and Re = 1 kΩ. Note that VBE varies between 0.7 and 0.9 volts depends on base current.

DC with oscillator

Insert oscillator vi in series with dc source VEE. The ac signal is vi = Vim cosωt . The presentation picture is

Emitter base equivalent circuit

Figure One

inserting dynamic resistance 2 ohm and VBE = 0.5 volts

Collector Base Junction

Collector Base junction is bring into consideration after plotting the common-base output characteristics. Such a  figure consider below:

common base output characteristics

For values VCB less than 0.5 volts the curve plotted above is a family of straight line equation given by

IC = αIE + ICBO

Convert this equation into its equivalent yields:

common base equivalent circuitis

Active elements like transistor has emitter current transmitted to collector current thus αIE is a dependant source. To avoid the nonlinear region to the left of iC axis it is necessary that VCB less than 0.5 volts at all times.

Large signal model

Figure two

Common base equivalent circuit

In the circuit above α = 1, ICBO = 0, VEE = 2 volts, Re = 1 kΩ, VCC = 50 volts, RC = 20 kΩ and a 1 volt peak sinusoidal source is connected in series with VEE.

For emitter-base circuit, the junction is forward biased as long as Vim < 1.3 volts. The transistor amplifies input ac voltage and resulting voltage gain is AO = Vcbm/Vim = 20/1 = 20.

Current amplification

A change in emitter current in pnp transistor produces a change of approximately the same amount of collector current iC and smaller change in base current a factor of 1 - α. To achieve current amplification the change is initiated in the base current not in the emitter current. It assumes that β = α/(1-α) does not vary with base current. Neglecting ICBO, we have iC = βiB . In a typical range of 1 to 100 mA, hfe is approximately equal to β, independent of any changes in collector current.

Current amplification circuit

Current amplification circuit is made so that base-emitter junction is forward-biased and collector-base junction reverse-biased. The picture presentation is

Basic transistor amplifier

The derivation involved in this circuit is made based on Kirchoff's Voltage Law

Derivation for finding collector current

Previous | Next

Emitter Base Junction

The emitter-base junction of pnp silicon transistor in the common-base configuration can be represented by a  0.5 volts battery in series with 10 ohm resistance and an ideal diode.

a. Find VEBQ for Re = 1000 ohm and VEE = 6 volts.

b. Repeat for Vim = 2 volts.

Combine dynamic resistance concept with DC with oscillator we get figure one.

Consider that f = 6oHz and t = 1.

a. Using KVL around the emitter-base loop yields:

6V - 0.5 = IEQ x (1000 + 10)

IEQ = 5.5 / 1010 = 5.4 x 10 -3

Vrd = IEQ x rd = 5.4 mA x 10 = 54 mV

Therefore VEBQ = 500 mV + 54 mV = 554 mV

b.    Using KVL around emitter-base loop when inserting oscillator.

total emitter current

Vrd = 7.4 mA x 10 = 74 mV

VEBQ = 500 + 74 = 574 mV

PNP transistor low frequency large signal circuit

An example of a large signal model is shown as Figure 2. Find iE and VCB.

PNP transistor low frequency large signal circuit