SCR and THYRISTOR SILICON CONTROLLED RECTIFIERS (SCR) A silicon controlled rectifier is a semiconductor device that acts as a true electronic switch. it can change alternating current and at the same time can control the amount of power fed to the load. SCR combines the features of a rectifier and a transistor.
CONSTRUCTION When a pn junction is added to a junction transistor the resulting three pn junction device is called a SCR. ordinary rectifier (pn) and a junction transistor (npn) combined in one unit to form pnpn device. three terminals are taken : one from the outer p type material called anode a second from the outer n type material called cathode K and the third from the base of transistor called Gate. GSCR is a solid state equivalent of thyratron. the gate anode and cathode of SCR correspond to the grid plate and cathode of thyratron SCR is called thyristor
WORKING Load is connected in series with anode the anode is always kept at positive potential w.r.t cathode. WHEN GATE IS OPEN
No voltage applied to the gate, j2 is reverse biased while j1 and j3 are FB . J1 and J3 is just in npn transistor with base open .no current flows through the load RL and SCR is cut off. if the applied voltage is gradually increased a stage is reached when RB junction J2 breakdown .the
SCR now conducts heavily and is said to be ON state. the applied voltage at which SCR conducts heavily without gate voltage is called Break over Voltage. WHEN GATE IS POSITIVE W.R.T CATHODE.
The SCR can be made to conduct heavily at smaller applied voltage by applying small positive potential to the gate.J3 is FB and J2 is RB the electron from n type material start moving across J3 towards left holes from p type toward right. electrons from j3 are attracted across junction J2 and gate current starts flowing. as soon as gate current flows anode current increases. the increased anode current in turn makes more electrons available at J2 breakdown and SCR starts conducting heavily. the gate looses all control if the gate voltage is removed anode current does not decrease at all. The only way to stop conduction is to reduce the applied voltage to zero. BREAKOVER VOLTAGE I t is the minimum forward voltage gate being open at which SCR starts conducting heavily i.e turned on PEAK REVERSE VOLTAGE( PRV) It is the maximum reverse voltage applied to an SCR without conducting in the reverse direction. HOLDING CURRENT It is the maximum anode current gate being open at which SCR is turned off from on conditions. FORWARD CURRENT RATING It is the maximum anode current that an SCR is capable of passing without destruction CIRCUIT FUSING RATING It is the product of of square of forward surge current and the time of duration of the surge
VI CHARACTERISTICS OF SCR
FORWARD CHARCTERISTICS When anode is +ve w.r.t cathode the curve between V & I is called Forward characteristics. OABC is the forward characteristics of the SCR at Ig =0. if the supplied voltage is increased from zero point A is reached .SCR starts conducting voltage across SCR suddenly drops (dotted curve AB) most of supply voltage appears across RL REVERSE CHARCTERISTICS When anode is –ve w.r.t.cathode the curve b/w V&I is known as reverse characteristics reverse voltage come across SCR when it is operated with ac supply reverse voltage is increased anode current remains small avalanche breakdown occurs and SCR starts conducting heavily is known as reverse breakdown voltage SCR as a switch SCR Half and Full wave rectifier
Application SCR as a static contactor SCR for power control SCR for speed control of d. c. shunt motor Over light detector
Triggering (Turn on) Methods of Thyristor: Triggering: The turning on Process of the SCR is known as Triggering. In other words, turning the SCR from ForwardBlocking state to ForwardConduction state is known as Triggering.The various methods of SCR triggering are discussed here.
The various SCR triggering methods are x x x x x
Forward Voltage Triggering Thermal or Temperature Triggering Radiation or Light triggering dv/dt Triggering Gate Triggering
(a) Forward Voltage Triggering: x x x x
In this mode, an additional forward voltage is applied between anode and cathode. When the anode terminal is positive with respect to cathode(VAK) , Junction J1 and J3 is forward biased and junction J2 is reverse biased. No current flows due to depletion region in J2 is reverse biased (except leakage current). As VAK is further increased, at a voltage VBO (Forward Break Over Voltage) the junction J2 undergoes avalanche breakdown and so a current flows and the device tends to turn ON(even when gate is open)
(b) Thermal (or) Temperature Triggering: x x x
The width of depletion layer of SCR decreases with increase in junction temperature. Therefore in SCR when VAR is very near its breakdown voltage, the device is triggered by increasing the junction temperature. By increasing the junction temperature the reverse biased junction collapses thus the device starts to conduct.
(c) Radiation Triggering (or) Light Triggering: x x x x
For light triggered SCRs a special terminal niche is made inside the inner P layer instead of gate terminal. When light is allowed to strike this terminal, free charge carriers are generated. When intensity of light becomes more than a normal value, the thyristor starts conducting. This type of SCRs are called as LASCR
(d) dv/dt Triggering: x x x
When the device is forward biased, J1 and J3 are forward biased, J2 is reverse biased. Junction J2 behaves as a capacitor, due to the charges existing across the junction. If voltage across the device is V, the charge by Q and capacitance by C then, ic=dQ/dt Q=CV ic=d(CV)/dt C.dV/dt+V.dC/dt as dC/dt = 0
ic = C.dV/dt x
Therefore when the rate of change of voltage across the device becomes large, the device may turn ON, even if the voltage across the device is small.
(e) Gate Triggering: x x x x
This is most widely used SCR triggering method. Applying a positive voltage between gate and cathode can Turn ON a forward biased thyristor. When a positive voltage is applied at the gate terminal, charge carriers are injected in the inner Player, thereby reducing the depletion layer thickness. As the applied voltage increases, the carrier injection increases, therefore the voltage at which forward breakover occurs decreases.
COMMUTATION OF SCR The term commutation basically means the transfer of current from one path to another. It is not possible for a thyristor to turn itself O F F t h e circuit in which it is connected must reduce the thyristor current to zero to enable it to turn off ‘COMMUTATION’ is the term to describe the methodsof achieving this.Broadly classified into two methods: 1.NATURAL COMMUTATION 2.FORCED COMMUTATION NATURAL COMMUTATION This widely used method of commutation makes use of thealternating, reversing nature of a.c voltage to effect the currentt r a n s f e r . A s t h e c u r r e n t p a s s e s through natural zero, a reversev o l t a g e w i l l s i m u l t a n e o u s l y a p p e a r across the device. This i m m e d i a t e l y t u r n s o f f t h e d e v i c e . T h i s p r o c e s s i s c a l l e d a s natural commutation since no external circuit is required for this purpose. FORCED COMMUTATION In case of dc circuits, for switching off the thyristors, the f o r w a r d c u r r e n t s h o u l d b e f o r c e d t o b e z e r o b y m e a n s o f s o m e external circuits. The process is called forced commutation. C L A S S I F I C A T I O N O F F R O C E D C O M M U T A T I O N TECHNIQUES: T h e c l a s s i f i c a t i o n i s b a s e d o n t h e a r r a n g e m e n t o f commutating components and the manner in which zero currentis obtained in the SCR.The six distinct classes by which the SCR can be turned off are: Class A Self commutated by a resonating load Class B Self commutated by a LC circuit Class C C or LC switched by another load carrying SCR Complementary commutation Class D C or LC switched by an auxiliary SCR Auxiliary commutation Class E An external pulse source for commutationExternal pulse commutation Class F AC line commutation Class A, Self commutated by resonating the load
•When the SCR is triggered, anode current flows and charges up C with the dot as positive. •The LCR form a second order underdamped circuit. The current through the SCR builds up and completes a half cycle. •When the inductor current will then attempt to flow through the SCR in the reverse direction and the SCR will be turned off. Class B, Self commutated by an LC circuit
•T h e C a p a c i t o r C c h a r g e s u p i n t h e d o t a s p o s i t i v e before a gate pulse is applied to the SCR. When SCR istriggered, the resulting current has two components. •T h e c o n s t a n t l o a d c u r r e n t I f l o w s t h r o u g h R L l o a d . T h i s i s e n s u r e d b y t h e l a r g e r e a c t a n c e i n s e r i e s w i t h the load and the freewheeling diode clamping it. •A s i n u s o i d a l c u r r e n t f l o w s t h r o u g h t h e r e s o n a n t L C circuit to chargeup C with the dot as negative at the end of the half cycle.
•T h i s c u r r e n t w i l l t h e n r e v e r s e a n d f l o w t h r o u g h t h e SCR in opposition to the load current for a small fraction of t h e n e g a t i v e s w i n g t i l l t h e t o t a l c u r r e n t t h r o u g h t h e S C R becomes zero. •T h e S C R w i l l t u r n o f f w h e n t h e r e s o n a n t – c i r c u i t (reverse) current is just greater than the load current. •T h e S C R i s t u r n e d o f f i f t h e S C R r e m a i n s r e v e r s e d biased for t q> t off , a n d t h e r a t e o f r i s e o f t h e r e a p p l i e d voltage