05-04-2012, 10:19 AM
Transistor Current Components
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In the figure we show the various components which flow across the forward-based emitter junction and the reverse-biased collector junction. The emitter current IE consists of hole current IpE (holes crossing from the emitter into base) and electron current InE (electron crossing from base into the emitter). The ratio of hole to electron currents, IpE / InE, crossing the emitter junction is proportional to the ratio of the conductivity of the p material to that of the n material. In the commercial transistor the doping of the emitter is made much larger than the doping of the base. This future ensures (in a p-n-p transistor) that the emitter current consists almost entirely of the holes. Such a situation is desired since the current which results from electrons crossing the emitter junction from base to emitter does not contribute carriers which can reach the collector.
Not all the holes crossing the emitter junction JE reach the collector junction Jc because some of them combine with the electrons in the n – type base. If Ipc is the hole current at Jc, there must be a bulk recombination current IpE - I¬pC leaving the base, as indicated in figure. (actually, electrons enter the base region through the base lead to supply those charges which have been lost by recombination with the holes injected into the base across JE).
Emitter Efficiency:- (γ)
The emitter, or injection, efficiency γ is defined as
γ ≡ Current of injected carriers at JE
Total emitter current
In the case of a p-n-p transistor we have
γ = IpE = IpE
IpE + InE IE
Where IpE is the injected hole diffusion current at emitter junction and InE is the injected electron diffusion current at emitter junction.
Transport Factor:- (β*)
The transport factor β* is defined as
β* ≡ injected carrier current reaching Jc
injected carrier current at JE
In the case of a p-n-p transistor we have
β* = IpC / IpE