Descripción: La puerta es el terminal equivalente a la base del BJT (Bipolar Junction Transistor), de cuyo funcionamiento se diferencia, ya que en el FET, el voltaje aplicado entre la puerta y la fuente control...
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Ericsson Mobility ParametersFull description
Full description
Transistor “h” and “y” Parameters Basic Circuits There are three basic transistor circuits. They are called according to that electrode (emitter, base, col-lector) which is common to both input and output circuit.
If expressed in matrix form we obtain:
( ( ( ( v1 i2
i1 = (h) v 2
(h) =
( ( h ih r
h fh o
Explanation of h-Parameters Input impedance (shorted output, v 2 = 0) Common Emitter
hi =
v1 i1
Reverse voltage transfer ratio (open input, i 1 = 0) hr =
v1 i1
Small signal current gain (shorted output, v 2 = 0)
Common Base
hf =
i2 i1
Output admittance (open input, i 1 = 0) i2 ho = v 2
Common Collector
Properties of the three basic circuits: Common Emitter
Common Base
Common Collector
Input impedance
medium
small
high
Output impedance
medium
high
small
Current gain
high
less than 1
high
Upper frequency limit
l ow
hi g h
l ow
Four-Pole Four-Pole Symbols of h-Matrix A transistor can be considered considered as an active active four-pole network. When driven with small low-frequency signals its properties can be described by the four characteristic values of the h-matrix (hybrid), which are assumed to be real. v1 = hi · i1 + hr · v2 Transistor four pole
v1 = hi · i1 + hr · v2
A frequentl frequently y used used abbre abbreviati viation on is is the the determinant: ∆h = h i · h o - hr · h f
For all three basic circuit configurations the circuit illustrated below represents the equivalent four-pole circuit using h-parameters.
In the transistor data sheets the h-parameters are usually quoted for the common emitter configuration and for a given operating point (bias). The latter is determined by the collector voltage, the emitter or collector current and by the ambient temperature. For different operating points, correction factors are needed which can be gathered from the relevant curves. For common base or common collector transistor stage calculations, the appropriate h-parameters are ascertained from those of the common emitter configuration by using the following conversion formulas.
Common Emitter
Common Base
Common Collector
Input impedance
h ie
hie hib = 1 + h fe
hic = hie
Reverse voltage transfer ratio
h re
hie · hoe hrb = 1 + h - hre fe
hrc = 1 - h re
Small Signal current gain
h fe
hfe hfb = - 1 + h
-hfc = 1 + hfe
Output admittance
h oe
hoe hob = 1 + h fe
Calculation of a Tranistor Stage
Transistor four pole
Whereas the network behaviour of lowfrequency transistors could be described by using the h-matrix (hybrid), the y-matrix (admittance) is usually employed for high frequency transistors.
Transistor four pole
v1 hi + R L · ∆h = i1 1 + h o · RL
i1 = yi · v1 + yr · v2 i2 = yf · i1 + yo · v2
Output impedance Z2 =
hoc = hoe
Four-Pole Symbols of y-Matrix
Input impedance Z1 =
fe
v2 hi + R G = i2 ∆h + h o · RG
In matrix form we obtain:
( ( ( ( ( ( i1
Current gain
i2
i2 hf GC = = i1 1 + h o · RL
= (y)
V1
V2
(y) =
yi yr
yf yo
The y-parameters are complex values which can be expressed as
Voltage gain
yik = gik + jbik with bik = ωCik or with bωikL= -
v2 -hf · RL Gv = = v1 h i + R L · ∆h
1
ik
Often, the following notation is expedient:
Power gain
yik = 1 y ik 1 exp jϕik 2
Gp =
v 2 · i2 hf · RL = v1 · i1 (1 + ho · RL) (h i + R L · ∆h)
Maximum available power gain, input and output matched with R G opt resp. RL opt Gp max =
(
2 hf ∆h + hi · ho
(
By adding the suffix e, b, or c it is possible to indicate to which of the three basic circuit configurations the parameters are valid. Explanation of y-Parameters Input admittance (shorted output, v 2 = 0) yi =
i1 v1
RG opt =
hi · ∆h ho
Reverse Transconductance (shorted input, v 2 = 0)
RL opt =
hi ho · ∆h
yr =
i1 v2
Forward Transconductance (shorted output, v 2 = 0) yf =
Maximum available power gain, input and output matched with R G opt resp. RL opt