Power Electronics: Power Semiconductor Devices, Commutation, and Controlled Rectifiers

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Flashcards covering power semiconductor devices (BJT, SCR, TRIAC, DIAC), triggering methods, commutation classes (Class A to F), dynamic switching characteristics, circuit protections, and controlled rectifier equations based on lecture notes.

Last updated 3:52 AM on 10/8/26
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18 Terms

1
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Circuit configuration of an RC gate triggering circuit for an SCR

An AC voltage source connected to the load and thyristor, with a parallel gate-control network consisting of a variable resistor RR, a capacitor CC, and two diodes: diode D1D_1 in series with the gate terminal and diode D2D_2 connected across the gate-cathode junction.

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Conduction path and operating mechanism of an RC gate triggering circuit

During the positive half-cycle, capacitor CC charges through the variable resistor RR until the capacitor voltage reaches the threshold required to inject gate current through diode D1D_1, triggering the SCR. During the negative half-cycle, diode D2D_2 charges capacitor CC negatively to protect the gate-cathode junction from excessive reverse breakdown, while D1D_1 prevents reverse current flow into the gate.

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Circuit configuration of Class A (Self / Resonant / Load) commutation

A DC source (VdcV_{dc}) connected to an underdamped RLCRLC circuit where the commutating elements—inductor LL and capacitor CC—are connected either in series with load resistance RR or with load RR connected in parallel across capacitor CC.

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<p>Conduction path and operating mechanism of Class A commutation</p>

Conduction path and operating mechanism of Class A commutation

When the SCR is triggered, forward current flows through the resonant path Vdc+→SCR→L→C→R→Vdc−V_{dc}^+ \rightarrow \text{SCR} \rightarrow L \rightarrow C \rightarrow R \rightarrow V_{dc}^-. Due to the underdamped resonant response, capacitor CC charges to a voltage exceeding the supply voltage, naturally driving the oscillatory current to zero and reverse-biasing the SCR to turn it off.

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Circuit configuration of Class B (Resonant-Pulse / Current) commutation

A DC supply voltage connected in series with load resistor RR and the main SCR, while a separate resonant commutating LCLC branch is connected directly in parallel across the main SCR.

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Conduction path and operating mechanism of Class B commutation

The capacitor initially charges to VdcV_{dc} with upper plate positive. Triggering the SCR establishes the load current path Vdc+→R→SCR→Vdc−V_{dc}^+ \rightarrow R \rightarrow \text{SCR} \rightarrow V_{dc}^- while discharging the capacitor through the resonant path C+→L→SCR→C−C^+ \rightarrow L \rightarrow \text{SCR} \rightarrow C^-. Once the resonant current reverses polarity, the discharge current opposes and exceeds the forward load current (Ic>ILI_c > I_L), forcing the SCR anode current below holding current to turn it off.

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Circuit configuration of Class C (Complementary) commutation

A DC voltage source supplying two parallel branches: the main thyristor (SCR1SCR_1) in series with load resistor R1R_1, and a complementary thyristor (SCR2SCR_2) in series with resistor R2R_2, with a commutating capacitor CC connected across the anodes of both thyristors.

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Conduction path and operating mechanism of Class C commutation

Triggering SCR1SCR_1 completes the load path E+→R1→SCR1→E−E^+ \rightarrow R_1 \rightarrow SCR_1 \rightarrow E^- and charges capacitor CC via path E+→R2→C+→C−→SCR1→E−E^+ \rightarrow R_2 \rightarrow C^+ \rightarrow C^- \rightarrow SCR_1 \rightarrow E^-. When SCR2SCR_2 is triggered, the positive terminal of CC is grounded through SCR2SCR_2, applying a negative transient voltage across SCR1SCR_1 to commutate it off while SCR2SCR_2 conducts.

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Circuit configuration of Class D (Auxiliary) commutation

A power circuit with a main thyristor (SCR1SCR_1) and load resistor RR across a DC source, accompanied by an auxiliary commutation circuit comprising an auxiliary thyristor (SCR2SCR_2), a commutating capacitor CC, an inductor LL, and an antiparallel discharge diode DD.

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Conduction path and operating mechanism of Class D commutation

Auxiliary SCR2SCR_2 is fired first to charge capacitor CC via path E+→C+→C−→SCR2→R→E−E^+ \rightarrow C^+ \rightarrow C^- \rightarrow SCR_2 \rightarrow R \rightarrow E^-. Main SCR1SCR_1 is then triggered to power the load and reverse the capacitor charge via the resonant loop C+→SCR1→L→D→C−C^+ \rightarrow SCR_1 \rightarrow L \rightarrow D \rightarrow C^-. Re-triggering SCR2SCR_2 discharges CC through C+→SCR2→SCR1→C−C^+ \rightarrow SCR_2 \rightarrow SCR_1 \rightarrow C^-, opposing the forward load current to force SCR1SCR_1 off.

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<p>Circuit configuration of Class E (External Pulse) commutation</p>

Circuit configuration of Class E (External Pulse) commutation

A main DC circuit with a thyristor and load connected to a DC supply, interfaced with an external pulse generator that supplies a pulse transformer whose secondary winding is connected across the main SCR via a commutating capacitor CC.

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Conduction path and operating mechanism of Class E commutation

While the main SCR carries forward load current, a high-frequency turn-off pulse is applied to the primary of the pulse transformer. The induced voltage across the secondary winding applies a reverse-bias voltage across the SCR via capacitor CC, driving the thyristor anode current below holding current for a duration exceeding turn-off time (tqt_q).

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<p>Circuit configuration of an SCR snubber circuit for dynamic protection</p>

Circuit configuration of an SCR snubber circuit for dynamic protection

A protective network consisting of a series damping resistor RsR_s and capacitor CsC_s connected directly in parallel across the thyristor, alongside a small inductor LsL_s connected in series with the thyristor.

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Conduction path and operating mechanism of an SCR snubber circuit

When an abrupt voltage transient occurs, uncharged capacitor CsC_s behaves as a temporary short, diverting transient current away from the SCR via path Vs+→Rs→Cs→LoadV_s^+ \rightarrow R_s \rightarrow C_s \rightarrow \text{Load} to suppress dvdt\frac{dv}{dt}. Inductor LsL_s limits the rate of anode current rise (didt\frac{di}{dt}), while RsR_s dissipates stored energy and limits discharge current when the SCR turns on.

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Circuit configuration of a single-phase half-wave controlled rectifier with resistive load

An alternating sinusoidal voltage source (vs=Vmsin⁡(ωt)v_s = V_m \sin(\omega t)) connected in series with a single thyristor (SCR) and a purely resistive load RR.

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Conduction path and operating mechanism of a single-phase half-wave controlled rectifier with resistive load

During the positive half-cycle (0≤ωt≤π0 \le \omega t \le \pi), the thyristor is forward biased and triggered at delay angle α\alpha, conducting load current along vs+→SCR→R→vs−v_s^+ \rightarrow \text{SCR} \rightarrow R \rightarrow v_s^-. At ωt=π\omega t = \pi, the source voltage falls to zero, bringing the anode current to zero and naturally turning off the SCR due to natural line commutation throughout the negative half-cycle.

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Circuit configuration of a single-phase half-wave controlled rectifier with an R-L load

A sinusoidal AC voltage source (vs=Vmsin⁡(ωt)v_s = V_m \sin(\omega t)) connected in series with a single Silicon Controlled Rectifier and a series combination of a load resistor RR and inductor LL.

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Conduction path and operating mechanism of a single-phase half-wave controlled rectifier with an R-L load

When triggered at firing angle α\alpha, current flows along path vs+→SCR→R→L→vs−v_s^+ \rightarrow \text{SCR} \rightarrow R \rightarrow L \rightarrow v_s^-, storing energy in inductor LL. When the AC source reverses at ωt=π\omega t = \pi, the collapsing magnetic field in inductor LL induces a positive voltage (LdidtL \frac{di}{dt}) that maintains forward current conduction until extinction angle β\beta (β>π\beta > \pi), where current drops to zero and commutates the SCR off.