junction transistor tetrode - определение. Что такое junction transistor tetrode
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Что (кто) такое junction transistor tetrode - определение

FIRST TYPE OF BIPOLAR JUNCTION TRANSISTOR MADE
Grown junction transistor
  • An NPN grown-junction transistor with the cover removed to show the germanium ingot and the base wire.

bipolar transistor         
  • Approximated Ebers&ndash;Moll model for an NPN transistor in the forward active mode. The collector diode is reverse-biased so ''I''<sub>CD</sub> is virtually zero. Most of the emitter diode current (''α''<sub>F</sub> is nearly 1) is drawn from the collector, providing the amplification of the base current.
  • Generalized h-parameter model of an NPN BJT.<br />''Replace '''x''' with '''e''', '''b''' or '''c''' for CE, CB and CC topologies respectively.''
  • 3D model of bipolar transistor
  • Symbol for NPN bipolar transistor with current flow direction
  • depleted regions]].
  •  url=https://archive.org/details/microelectronicc0000sedr/page/903
 }}</ref> ''I''<sub>B</sub>, ''I''<sub>C</sub> and ''I''<sub>E</sub> are the base, collector and emitter currents; ''I''<sub>CD</sub> and ''I''<sub>ED</sub> are the collector and emitter diode currents; ''α''<sub>F</sub> and ''α''<sub>R</sub> are the forward and reverse common-base current gains.
  • Ebers&ndash;Moll model for a PNP transistor
  • Hybrid-pi model
  • Simplified cross section of a planar ''NPN'' bipolar junction transistor
  • Structure and use of NPN transistor. Arrow according to schematic.
  • [[Band diagram]] for NPN transistor in active mode, showing injection of electrons from emitter to base, and their overshoot into the collector
  • [[Band diagram]] for NPN transistor at equilibrium
TRANSISTOR THAT USES BOTH ELECTRONS AND HOLES AS CHARGE CARRIERS
BJT; P-n-p transistor; N-p-n transistor; Bjt; Bipolar junction transistors; Bipolar Junction Transistor; Collector current; Bjt transistor; Emitter, base, and collector; Ebers-Moll; PNP (transistor polarity); Ebers-Moll model; PNP transistor; NPN transistor; Transistor beta; Ebers–Moll model; Bipolar transistor; Bipolar transistors; Power BJT; Junction transistor; P–n–p transistor; N–p–n transistor; H-parameter model; Emitter, base and collector; Emitter current; VBIC
<electronics> A transistor made from a sandwich of n- and p-type semiconductor material: either npn or pnp. The middle section is known as the "base" and the other two as the "collector" and "emitter". When used as an amplifying element, the base to emitter junction is in a "forward-biased" (conducting) condition, and the base to collector junction is "reverse-biased" or non-conducting. Small changes in the base to emitter current (the input signal) cause either holes (for pnp devices) or free electrons (for npn) to enter the base from the emitter. The attracting voltage of the collector causes the majority of these charges to cross into and be collected by the collector, resulting in amplification. Contrast field effect transistor. (1995-10-04)
BJT         
  • Approximated Ebers&ndash;Moll model for an NPN transistor in the forward active mode. The collector diode is reverse-biased so ''I''<sub>CD</sub> is virtually zero. Most of the emitter diode current (''α''<sub>F</sub> is nearly 1) is drawn from the collector, providing the amplification of the base current.
  • Generalized h-parameter model of an NPN BJT.<br />''Replace '''x''' with '''e''', '''b''' or '''c''' for CE, CB and CC topologies respectively.''
  • 3D model of bipolar transistor
  • Symbol for NPN bipolar transistor with current flow direction
  • depleted regions]].
  •  url=https://archive.org/details/microelectronicc0000sedr/page/903
 }}</ref> ''I''<sub>B</sub>, ''I''<sub>C</sub> and ''I''<sub>E</sub> are the base, collector and emitter currents; ''I''<sub>CD</sub> and ''I''<sub>ED</sub> are the collector and emitter diode currents; ''α''<sub>F</sub> and ''α''<sub>R</sub> are the forward and reverse common-base current gains.
  • Ebers&ndash;Moll model for a PNP transistor
  • Hybrid-pi model
  • Simplified cross section of a planar ''NPN'' bipolar junction transistor
  • Structure and use of NPN transistor. Arrow according to schematic.
  • [[Band diagram]] for NPN transistor in active mode, showing injection of electrons from emitter to base, and their overshoot into the collector
  • [[Band diagram]] for NPN transistor at equilibrium
TRANSISTOR THAT USES BOTH ELECTRONS AND HOLES AS CHARGE CARRIERS
BJT; P-n-p transistor; N-p-n transistor; Bjt; Bipolar junction transistors; Bipolar Junction Transistor; Collector current; Bjt transistor; Emitter, base, and collector; Ebers-Moll; PNP (transistor polarity); Ebers-Moll model; PNP transistor; NPN transistor; Transistor beta; Ebers–Moll model; Bipolar transistor; Bipolar transistors; Power BJT; Junction transistor; P–n–p transistor; N–p–n transistor; H-parameter model; Emitter, base and collector; Emitter current; VBIC
Bipolar Junction Transistor (Reference: IC)
Bipolar junction transistor         
  • Approximated Ebers&ndash;Moll model for an NPN transistor in the forward active mode. The collector diode is reverse-biased so ''I''<sub>CD</sub> is virtually zero. Most of the emitter diode current (''α''<sub>F</sub> is nearly 1) is drawn from the collector, providing the amplification of the base current.
  • Generalized h-parameter model of an NPN BJT.<br />''Replace '''x''' with '''e''', '''b''' or '''c''' for CE, CB and CC topologies respectively.''
  • 3D model of bipolar transistor
  • Symbol for NPN bipolar transistor with current flow direction
  • depleted regions]].
  •  url=https://archive.org/details/microelectronicc0000sedr/page/903
 }}</ref> ''I''<sub>B</sub>, ''I''<sub>C</sub> and ''I''<sub>E</sub> are the base, collector and emitter currents; ''I''<sub>CD</sub> and ''I''<sub>ED</sub> are the collector and emitter diode currents; ''α''<sub>F</sub> and ''α''<sub>R</sub> are the forward and reverse common-base current gains.
  • Ebers&ndash;Moll model for a PNP transistor
  • Hybrid-pi model
  • Simplified cross section of a planar ''NPN'' bipolar junction transistor
  • Structure and use of NPN transistor. Arrow according to schematic.
  • [[Band diagram]] for NPN transistor in active mode, showing injection of electrons from emitter to base, and their overshoot into the collector
  • [[Band diagram]] for NPN transistor at equilibrium
TRANSISTOR THAT USES BOTH ELECTRONS AND HOLES AS CHARGE CARRIERS
BJT; P-n-p transistor; N-p-n transistor; Bjt; Bipolar junction transistors; Bipolar Junction Transistor; Collector current; Bjt transistor; Emitter, base, and collector; Ebers-Moll; PNP (transistor polarity); Ebers-Moll model; PNP transistor; NPN transistor; Transistor beta; Ebers–Moll model; Bipolar transistor; Bipolar transistors; Power BJT; Junction transistor; P–n–p transistor; N–p–n transistor; H-parameter model; Emitter, base and collector; Emitter current; VBIC
A bipolar junction transistor (BJT) is a type of transistor that uses both electrons and electron holes as charge carriers. In contrast, a unipolar transistor, such as a field-effect transistor, uses only one kind of charge carrier.

Википедия

Grown-junction transistor

The grown-junction transistor was the first type of bipolar junction transistor made. It was invented by William Shockley at Bell Labs on June 23, 1948 (patent filed June 26, 1948), six months after the first bipolar point-contact transistor. The first germanium prototypes were made in 1949. Bell Labs announced Shockley’s grown-junction transistor on July 4, 1951.

An NPN grown-junction transistor is made of a single crystal of semiconductor material which has two PN junctions grown into it. During the growth process, a seed crystal is slowly pulled from a bath of molten semiconductor, which then grows into a rod-shaped crystal (boule). The molten semiconductor is doped N-type at the start. At a predetermined moment in the growth process a small pellet of a P-type dopant is added, almost immediately followed by a somewhat larger pellet of an N-type dopant. These dopants dissolve in the molten semiconductor changing the type of semiconductor subsequently grown. The resulting crystal has a thin layer of P-type material sandwiched between sections of N-type material. This P-type layer may be as little as a thousandth of an inch (25 μm) thick. The crystal is sliced, leaving the thin P-type layer in the center of the slice, then cut into bars. Each bar is made into a transistor by soldering its N-type ends to supporting and conducting leads, then welding a very fine gold lead to the central P-type layer, and finally encasing in a hermetically sealed can. A similar process, using the opposite dopants, makes a PNP grown-junction transistor.

The most difficult part of this process is welding the gold wire to the base layer, as the wire may have a larger diameter than the thickness of the base. To facilitate this operation, the gold wire is pointed or flattened until the end is thinner than the base layer. The tip of the gold wire is slid along the bar until electrical resistance measurement shows it is in contact with the base layer. At this time a pulse of current is applied, welding the wire in place. Unfortunately sometimes the weld is too large or slightly off center in the base layer. To avoid shorting the transistor, the gold wire is alloyed with a small amount of the same type dopant as used in the base. This causes the base layer to become slightly thicker at the point of the weld.

Grown-junction transistors rarely operated at frequencies above the audio range, due to their relatively thick base layers. Growing thin base layers was very hard to control and welding the wire to the base became harder the thinner it got. Higher-frequency operation could be obtained by welding a second wire on the opposite side of the base, making a tetrode transistor, and using special biasing on this second base connection.