UJT

Unijunction transistor

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Transistor UJT

Unijunction transistors
Type	active
Pin configuration	B2, B1, Emitter
Electronic symbol

A unijunction transistor (UJT) is a three-lead electronic semiconductor device with only one junction that acts exclusively as an electrically controlled switch.

The UJT is not used as a linear amplifier. It is used in free-running oscillators, synchronized or triggered oscillators, and pulse generation circuits at low to moderate frequencies (hundreds of kilohertz). It is widely used in the triggering circuits for silicon controlled rectifiers. The low cost per unit, combined with its unique characteristic, have warranted its use in a wide variety of applications like oscillators, pulse generators, saw-tooth generators, triggering circuits, phase control, timing circuits, and voltage- or current-regulated supplies.^[1] The original unijunction transistor types are now considered obsolete; but a later multi-layer device, the programmable unijunction transistor (PUT), is still widely available.

Contents

  [hide] 

• 1Types
• 2Applications
• 3Construction of a UJT
• 4Device operation
• 5Invention
• 6References
• 7External links

Types[edit]

Graph of UJT characteristic curve, emitter-base1 voltage as a function of emitter current, showing current-controlled negative resistance (downward-sloping region)

There are three types of unijunction transistors:

1. The original unijunction transistor, or UJT, is a simple device that is essentially a bar of n-type semiconductor material into which p-type material has been diffused somewhere along its length, fixing the device parameter ${\displaystyle \eta }$ (the "intrinsic stand-off ratio"). The 2N2646 model is the most commonly used version of the UJT.
2. The complementary unijunction transistor, or CUJT, that is a bar of p-type semiconductor material into which n-type material has been diffused somewhere along its length, defining the device parameter ${\displaystyle \eta }$. The 2N6114 model is one version of the CUJT.
3. The programmable unijunction transistor or PUT, is a multi-junction device that, with two external resistors, displays similar characteristics to the UJT. It is a close cousin to the thyristor and like the thyristor consists of four p-n layers. It has an anode and a cathode connected to the first and the last layer, and a gate connected to one of the inner layers. PUTs are not directly interchangeable with conventional UJTs but perform a similar function. In a proper circuit configuration with two "programming" resistors for setting the parameter ${\displaystyle \eta }$, they behave like a conventional UJT. The 2N6027, 2N6028^[2] and BRY39 models are examples of such devices.

Applications[edit]

Unijunction transistor circuits were popular in hobbyist electronics circuits in the 1960s and 1970s because they allowed simple oscillators to be built using just one active device. For example, they were used for relaxation oscillators in variable-rate strobe lights.^[3] Later, as integrated circuits became more popular, oscillators such as the 555 timer IC became more commonly used.

In addition to its use as the active device in relaxation oscillators, one of the most important applications of UJTs or PUTs is to trigger thyristors (silicon controlled rectifiers (SCR), TRIAC, etc.). A DC voltage can be used to control a UJT or PUT circuit such that the "on-period" increases with an increase in the DC control voltage. This application is important for large AC current control.

UJTs can also be used to measure magnetic flux. The hall effect modulates the voltage at the PN junction. This affects the frequency of UJT relaxation oscillators.^[4] This only works with UJTs. PUTs do not exhibit this phenomenon.

Construction of a UJT[edit]

Structure of a p-type UJT

The UJT has three terminals: an emitter (E) and two bases (B₁ and B₂) and so is sometimes known a "double-base diode". The base is formed by lightly doped n-type bar of silicon. Two ohmic contacts B₁ and B₂ are attached at its ends. The emitter is of p-type and it is heavily doped; this single PN junction gives the device its name. The resistance between B1 and B2 when the emitter is open-circuit is called interbase resistance. The emitter junction is usually located closer to base-2(B2) than base-1(B1) so that the device is not symmetrical, because symmetrical unit does not provide optimum electrical characteristics for most of the applications.

If no potential difference exists between its emitter and either of its base leads, an extremely small current flows from B₁ to B₂. On the other hand, if an adequately large voltage relative to its base leads, known as the 'trigger voltage', is applied to its emitter, then a very large current will flow from its emitter and join the current flowing from B₁ to B₂, which would create a larger B₂ output current.

The schematic diagram symbol for a unijunction transistor represents the emitter lead with an arrow, showing the direction of conventional current flow when the emitter-base junction is conducting a current. A complementary UJT would use a p-type base and an n-type emitter, and operates the same as the n-type base device but with all voltage polarities reversed.

The structure of a UJT is similar to that of an N-channel JFET, but p-type (gate) material surrounds the N-type (channel) material in a JFET, and the gate surface is larger than the emitter junction of UJT. A UJT is operated with emitter junction forward- biased while the JFET is normally operated with the gate junction reverse-biased. It is a current controlled negative resistance device.

Device operation[edit]

The device has a unique characteristic that when it is triggered, its emitter current increases regeneratively until it is restricted by emitter power supply. It exhibits a negative resistance characteristic and so it can be employed as an oscillator.

The UJT is biased with a positive voltage between the two bases. This causes a potential drop along the length of the device. When the emitter voltage is driven approximately one diode voltage above the voltage at the point where the P diffusion (emitter) is, current will begin to flow from the emitter into the base region. Because the base region is very lightly doped, the additional current (actually charges in the base region) causes conductivity modulation which reduces the resistance of the portion of the base between the emitter junction and the B2 terminal. This reduction in resistance means that the emitter junction is more forward biased, and so even more current is injected. Overall, the effect is a negative resistance at the emitter terminal. This is what makes the UJT useful, especially in simple oscillator circuits.