DIAC

DIAC

DIAC.
Three-layer DIAC.
The DIAC is a diode that conducts electrical current only after its breakover voltage, VBO, has been reached momentarily. The term is an acronym of "diode for alternating current".
When breakdown occurs, the diode enters a region of negative dynamic resistance, leading to a decrease in the voltage drop across the diode and, usually, a sharp increase in current through the diode. The diode remains in conduction until the current through it drops below a value characteristic for the device, called the holding current, IH. Below this value, the diode switches back to its high-resistance, non-conducting state. This behavior is bidirectional, meaning typically the same for both directions of current.
Most DIACs have a three-layer structure with breakover voltage of approximately 30 V. Their behavior is similar to that of a neon lamp, but it can be more precisely controlled and takes place at a lower voltage.
DIACs have no gate electrode, unlike some other thyristors that they are commonly used to trigger, such as TRIACs. Some TRIACs, likeQuadrac, contain a built-in DIAC in series with the TRIAC's gate terminal for this purpose.
DIACs are also called "symmetrical trigger diodes" due to the symmetry of their characteristic curve. Because DIACs are bidirectional devices, their terminals are not labeled as anode and cathode but as A1 and A2 or main terminal MT1 and MT2.
Typical DIAC voltage and current relationships. VBO is the breakover voltage.

SIDACEdit

SIDAC.
Idealized breakover diode voltage and current relationships. Once the voltage exceeds the turn-on threshold, the device turns on and the voltage rapidly falls while the current increases.
A Silicon Diode for Alternating Current(SIDAC) is a less commonly used device, electrically similar to the DIAC, but having, in general, a higher breakover voltage and greater current handling capacity.
The SIDAC is another member of the thyristorfamily. Also referred to as a SYDAC (Silicon thYristor for Alternating Current), bi-directional thyristor breakover diode, or more simply a bi-directional thyristor diode, it is technically specified as a bilateral voltage triggered switch. Its operation is similar to that of the DIAC, but SIDAC is always a five-layer device with low-voltage drop in latched conducting state, more like a voltage triggered TRIAC without a gate. In general, SIDACs have higher breakover voltages and current handling capacities than DIACs, so they can be directly used for switching and not just for triggering of another switching device.
The operation of the SIDAC is functionally similar to that of a spark gap, but is unable to reach its higher temperature ratings. The SIDAC remains nonconducting until the applied voltage meets or exceeds its rated breakover voltage. Once entering this conductive state going through the negative dynamic resistance region, the SIDAC continues to conduct, regardless of voltage, until the applied current falls below its rated holding current. At this point, the SIDAC returns to its initial nonconductive state to begin the cycle once again.
Somewhat uncommon in most electronics, the SIDAC is relegated to the status of a special purpose device. However, where part-counts are to be kept low, simple relaxation oscillators are needed, and when the voltages are too low for practical operation of a spark gap, the SIDAC is an indispensable component.
Similar devices, though usually not functionally interchangeable with SIDACs, are the Thyristor Surge Protection Devices (TSPD)sold under trademarks like Trisil bySTMicroelectronics and SIDACtor® and its predecessor Surgector by Littelfuse. These are designed to tolerate large surge currents for the suppression of overvoltage transients. In many applications this function is now served by metal oxide varistors (MOVs), particularly for trapping voltage transients on the power mains. Geovinco 444

See alsoEdit




Shockley diode

The Shockley diode (named after physicistWilliam Shockley) is a four-layersemiconductor diode, which was one of the first semiconductor devices invented. It was a "pnpn" diode. It is equivalent to a thyristorwith a disconnected gate. Shockley Diodes where manufactured and marketed byShockley Semiconductor Laboratory in the late 1950s.[1]
Shockley diode
InventedWilliam Shockley
Pin configurationAnode and Cathode
Electronic symbol
Shockley diode schematic symbol

UsagesEdit

Common applications:
niche applications:

Typical ValuesEdit

V-I diagram
DescriptionRange[4]Typically
Forward Operation
Switching Voltage Vs10V to 250V50V +/- 4V
Holding Voltage Vh0.5V to 2V0.8V
Switching current Isa few µA to some mA120µA
Hold current IH1 to 50mA14 to 45mA
Reverse Operation
Reverse Current IR15µA
Reverse Break down voltage Vrb10V to 250V60V

DynistorEdit

Dynistor
Small signal Shockley diodes are no longer manufactured, but the unidirectional thyristor breakover diode, also known as the dynistor, is a functionally equivalent power device. An early publication about dynistors was published in 1958.[5] In 1988 the first dynistor using Silicon carbide was made.[6] Dynistors can be used as switches in Micro- and Nanosecond Power Pulse Generators.[7]

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