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BSM150GB120DLC Infineon 1200V 150A Dual IGBT Module

BSM150GB120DLC IGBT Module In-stock / Infineon: 1200V 150A half-bridge switch, 2.1V VCE(sat), 2500V isolation. 90-day warranty, BESS & PCS applications. Global fast shipping. Get quote.

· Categories: IGBT
· Manufacturer: Infineon
· Price: US$ 35 In-Stock Offer
· Date Code: Please Verify on Quote
. Available Qty: 509
90-Day Warranty
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Content last revised on August 28, 2026

Desaturation (VCE(sat)) Short-Circuit Protection & Soft Turn-Off

In commercial and industrial Battery Energy Storage Systems (BESS) and Power Conversion Systems (PCS), the Infineon BSM150GB120DLC operates in harsh electrical environments where DC-link short circuits (Type I) and load faults under full conduction (Type II) can emerge. The module provides a rated collector-emitter breakdown voltage of VCES = 1200V and a continuous collector current rating of IC = 150A (at TC = 80°C), with a peak capability of ICRM = 300A. Under severe short-circuit conditions, the collector current rises sharply, pulling the operating point out of the saturation region into the active linear region where collector-emitter saturation voltage VCE(sat) escalates rapidly from its typical 2.1V conduction level.

According to standard short-circuit safe operating area (SCSOA) requirements detailed across the Infineon IGBT Modules Overview, the maximum withstand time tsc must not exceed 10 µs. Protection circuitry must utilize desaturation detection diodes coupled directly to the module collector to monitor this voltage rise. When VCE exceeds a programmed threshold (typically 6.5V to 7.5V), the driver must initiate a controlled, two-stage soft turn-off (2-Step Turn-Off). Abrupt gate shutdown under short-circuit currents creates excessive inductive voltage spikes dictated by ΔVCE = -Lsigma · (di/dt). By gradually discharging the input capacitance via a high-impedance path, soft turn-off suppresses catastrophic overvoltage excursions across the 1200V bus structure.

Active Miller Clamp Implementation & Parasitic Turn-On Prevention

The half-bridge configuration of the BSM150GB120DLC exhibits rapid switching dynamics, characterized by a typical turn-on rise time of tr = 0.06 µs and a turn-off fall time of tf = 0.08 µs under nominal gate resistance (RG = 5.6 Ω). During hard-switching transitions in high-power PCS bridges, high dv/dt transients generated across the complementary switch induce a displacement current through the parasitic gate-collector Miller capacitance (Cres / Cgc):

IMiller = Cgc · (dv/dt)

This transient displacement current flows through the external gate resistor and internal gate impedance, developing a positive potential across the gate-emitter terminal. If this induced voltage surpasses the gate threshold voltage VGE(th) (specified between 4.5V and 6.5V at Tvj = 25°C), the inactive IGBT undergoes parasitic cross-conduction (shoot-through), causing extreme thermal dissipation and potential DC-bus destruction.

To eliminate shoot-through risks without requiring complex negative power rails (-8V or -15V), design engineers implement an Active Miller Clamp. Once the gate discharge voltage drops below approximately 2.0V during turn-off, an internal clamp transistor transitions into a low-impedance state, tying the gate directly to the emitter return rail. For systems requiring lower power distribution or multi-phase auxiliary power stages, related bridge designs such as the BSM75GD120DLC provide sixpack topologies with similar voltage isolation parameters.

PCB Gate Loop Layout Symmetry & Kelvin Emitter Routing Rules

The high-current commutations inside PCS inverter stages create strong magnetic fields that can couple into sensitive gate drive traces. The BSM150GB120DLC features dedicated auxiliary Kelvin emitter terminals designed to decouple the high di/dt power return path from the low-power gate drive loop. Stray emitter inductance (LE) in the main current path produces an opposing voltage VL = LE · (di/dt) that directly counteracts applied gate signals, leading to unwanted switching delays and gate oscillation.

  • Kelvin Return Separation: Connect the gate driver ground strictly to the module auxiliary emitter terminal. Never bridge the auxiliary emitter to the main high-current DC power bus on the PCB layer.
  • Differential Loop Minimization: Route the gate and Kelvin emitter traces as tightly coupled differential pairs or stacked microstrip lines on adjacent PCB layers to cancel stray magnetic flux and minimize loop inductance Lsigma.
  • Symmetrical Impedance: Ensure identical trace lengths and matching series gate resistors for both high-side and low-side switch channels to preserve dynamic switching balance.

In complex multi-stage conversion topologies containing front-end rectifiers or auxiliary stages, components like the FP40R12KT3G are frequently evaluated alongside dual-pack configurations to streamline subsystem partitioning. For deeper engineering diagnostics and structural testing guidelines regarding parasitic loop mitigation, consult the technical methodologies outlined in the Field Engineer’s Handbook.

Bi-Directional DC-DC Buck-Boost Conversion & Battery Cycling Thermal Management

In commercial BESS installations, the bidirectional DC-DC stage manages continuous energy flow between variable battery pack voltages and the stabilized intermediate DC link. During high C-rate charging (Buck mode) and discharging (Boost mode), the BSM150GB120DLC undergoes repetitive power cycling that causes cyclic thermal expansion across internal materials.

Parameter Symbol Test Conditions Value Unit
Collector-Emitter Voltage VCES Tvj = 25°C 1200 V
Continuous Collector Current IC TC = 80°C 150 A
Saturation Voltage VCE(sat) IC = 150A, VGE = 15V, Tvj = 25°C 2.1 (typ) / 2.6 (max) V
Thermal Resistance, Junction to Case Rth(j-c) Per IGBT element 0.10 K/W
Thermal Resistance, Case to Heatsink Rth(c-h) Per module, λgrease = 1 W/(m·K) 0.03 K/W
Insulation Test Voltage VISOL RMS, f = 50 Hz, t = 1 min 2500 V

Thermal calculations must account for the junction-to-case thermal resistance (Rth(j-c) = 0.10 K/W per IGBT switch) and case-to-heatsink resistance (Rth(c-h) = 0.03 K/W per module). The total junction temperature is calculated via:

Tj = Ta + Ptotal · (Rth(j-c) + Rth(c-h) + Rth(h-a))

Managing the junction temperature delta (ΔTj) during peak shaving cycles reduces mechanical stress on wire bonds and DBC ceramic substrates, ensuring stable thermal equilibrium and high operational margins under sustained 150A conduction states.

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