The IRFZ44N is a workhorse. 55V, 49A, 17.5mΩ RDS(on) in a TO-220 package - it shows up in DC motor drivers, SMPS primaries, battery protection boards, and half the DIY inverter and Tesla coil projects on YouTube. It's cheap, it's everywhere, and for 12–24V high-current switching, it's hard to beat on paper.
But the IRFZ44N has a gate drive problem that catches hobbyists and engineers alike. Its Vgs(th) of 2–4V means a 3.3V or 5V microcontroller GPIO cannot fully turn it on. At 5V gate drive, the IRFZ44N might pass 20A instead of its rated 49A - and the RDS(on) is far above the 17.5mΩ spec. The MOSFET runs hot, efficiency tanks, and field failures follow.
If you're driving the gate from a microcontroller, the IRLZ44N is the solution - same voltage and current class, but logic-level gate (Vgs(th) 1–2V) that fully enhances at 5V. If you want better specs in the same footprint, the STP60NF06 (STMicro, 60V/60A/10.5mΩ) drops RDS(on) by 40%. If you need voltage headroom above 55V, the IRF540N (100V) is the standard upgrade - at the cost of higher RDS(on) and lower current. This guide covers all of them.
All three are N-channel power MOSFETs in the TO-220 package. The IRLZ44N is the logic-level variant - the single most important distinction for anyone driving a gate from a microcontroller. The STP60NF06 is the performance upgrade.
| Parameter | IRFZ44N | IRLZ44N | STP60NF06 |
|---|---|---|---|
| Manufacturer | Infineon / Multi-source | Infineon / Multi-source | STMicroelectronics |
| Type | Standard Level | Logic Level | Standard Level |
| Vds (max) | 55V | 55V | 60V |
| Id Continuous @ 25°C | 49A | 47A | 60A |
| RDS(on) @ Vgs=10V | 17.5mΩ | 22mΩ | 10.5mΩ |
| RDS(on) @ Vgs=5V | Not specified - partially on | ~28mΩ | Not specified - partially on |
| Vgs(th) Range | 2.0–4.0V | 1.0–2.0V | 2.0–4.0V |
| Vgs (max) | ±20V | ±20V | ±20V |
| Gate Charge Qg (typ) | 63 nC | 48 nC | 44 nC |
| Input Capacitance Ciss | 1,470 pF | 1,700 pF | 1,470 pF |
| Rise / Fall Time | 60 ns / 45 ns | 140 ns / 70 ns | 60 ns / 40 ns |
| Pd (max @ 25°C) | 94W | 83W | 110W |
| Package | TO-220 | TO-220 | TO-220 |
| Pinout | G-D-S (1-2-3) | G-D-S (1-2-3) | G-D-S (1-2-3) |
| Status | Active | Active | Active |
| Price Reference | $0.30–0.60/unit | $0.40–0.80/unit | $0.50–0.90/unit |
| Part Number | Manufacturer | Vds | Id (max) | RDS(on) @ 10V | Vgs(th) | Pin-Compatible? | Status | Notes |
|---|---|---|---|---|---|---|---|---|
| IRLZ44N | Infineon | 55V | 47A | 22mΩ | 1.0–2.0V | Yes - TO-220 G-D-S | Active | Logic-level. Fully on at 5V gate drive. Best for MCU direct drive. |
| STP60NF06 | STMicro | 60V | 60A | 10.5mΩ | 2.0–4.0V | Yes - TO-220 G-D-S | Active | Best RDS(on). 60V headroom. Fast switching. |
| FQP50N06 | onsemi | 60V | 50A | 14mΩ | 2.0–4.0V | Yes - TO-220 G-D-S | Active | Balanced cost/performance. 10–15% cheaper than STP60NF06. |
| IRFZ44NPBF | Infineon | 55V | 49A | 17.5mΩ | 2.0–4.0V | Yes - TO-220 G-D-S | Active | Pb-free version. Same die, same specs. |
| HRFZ44N | onsemi | 55V | 49A | 17.5mΩ | 2.0–4.0V | Yes - TO-220 G-D-S | Active | onsemi's equivalent. Same specs. |
| AUIRFZ44N | Infineon | 55V | 49A | 17.5mΩ | 2.0–4.0V | Yes - TO-220 G-D-S | Active | Automotive grade. AEC-Q101 qualified. |
| IRFZ44 (non-N) | Multi-source | 60V | 55A | 16.5mΩ | 2.0–4.0V | Yes - TO-220 G-D-S | Active | Slightly better specs. Slower switching (97/57 ns). |
| IRF540N | Infineon / Multi-source | 100V | 33A | 44mΩ | 2.0–4.0V | Yes - TO-220 G-D-S | Active | 100V rating. Lower current, higher RDS(on). Cheaper. |
| STP55NF06 | STMicro | 60V | 55A | ~19mΩ | 2.0–4.0V | Yes - TO-220 G-D-S | Active | Close match. Slightly higher RDS(on) than IRFZ44N. |
| IRFZ46NPBF | Infineon | 55V | 53A | ~18mΩ | 2.0–4.0V | Yes - TO-220 G-D-S | Active | 4A more current. Minor upgrade. |
This is the most common IRFZ44N problem on StackExchange and Arduino forums, and it deserves a section of its own.
The IRFZ44N datasheet specifies RDS(on) = 17.5mΩ at Vgs = 10V. At Vgs = 5V - the voltage from an Arduino or ESP32 GPIO - RDS(on) is not specified. The MOSFET is not fully enhanced. In practice, at 5V gate drive, RDS(on) is roughly 30–60mΩ (varies unit-to-unit) and the MOSFET can only pass about 20–25A before exceeding its thermal limits. At 3.3V, it's even worse - the gate voltage is barely above the 2–4V threshold. The MOSFET may only pass a few amps before hitting its RDS(on) thermal wall.
The symptom is always the same: "My MOSFET gets burning hot at only 10A - the datasheet says 49A!" The datasheet's 49A rating assumes you're driving the gate to 10V and keeping the case at 25°C. Neither is true on a hobbyist bench. A TO-220 without a heatsink has a junction-to-ambient thermal resistance of ~62°C/W. At just 5A with RDS(on)=50mΩ (the real value at Vgs=5V), that's 1.25W dissipation → 77°C temperature rise above ambient. The MOSFET is at 100°C and climbing.
The fix: use the IRLZ44N. At Vgs=5V, its RDS(on) is specified at ~28mΩ - still higher than the 10V spec, but characterized and guaranteed. For 3.3V systems, even the IRLZ44N is marginal - use a gate driver to translate 3.3V to 10V, or step up to a MOSFET with sub-1V threshold like the IRLB8721 (30V/62A, Vgs(th) 1.0–2.0V, RDS(on) specified at Vgs=4.5V).
Catastrophic drain-source short. Most common in switching circuits (inverters, Tesla coils, induction heaters, SMPS). The failure sequence: a voltage spike on the drain exceeds the 55V Vds rating → the drain-source junction avalanches → localized heating melts the silicon → a permanent short forms between all three terminals. Once a single MOSFET fails this way, every replacement fails the same way - because the circuit, not the part, is the problem.
Check: (a) add a proper snubber (R-C or RCD) across the drain-source to clamp switching spikes, (b) verify your layout minimizes drain trace inductance - long traces create larger voltage overshoots, (c) measure the actual drain voltage with a scope during switching - you might be seeing 80–100V spikes that your multimeter averages away.
The gate is a capacitor. Once charged, it has no discharge path if your drive circuit is high-impedance when "off." The MOSFET remains conducting until the gate charge slowly leaks away - which can take seconds. Always include a 10k–100kΩ resistor from gate to source. This provides a guaranteed discharge path. Without it, the MOSFET can turn on during MCU startup (when GPIOs are floating) or stay on after the MCU enters sleep mode. This is the #1 layout mistake in IRFZ44N circuits on StackExchange.
Uneven current sharing. During switching transitions, the MOSFET with the lower Vgs(th) turns on first and carries more current during the critical high-dissipation crossover period. Over many cycles, that device runs hotter, its Vgs(th) drops further (negative tempco), and the imbalance worsens. Fixes: (a) use individual gate resistors (10–22Ω) for each MOSFET - never tie gates directly together, (b) thermally couple the MOSFETs on the same heatsink so they track each other's temperature, (c) add small source degeneration resistors (0.01–0.1Ω) if current imbalance persists in steady-state.
ZVS (zero-voltage switching) circuits are unforgiving. Common mistakes with the IRFZ44N in these circuits: (a) 5V Zeners on the gates - these are too low. The IRFZ44N's Vgs(max) is ±20V, and a 5V Zener clips the gate drive, preventing full enhancement. Use 12–15V Zeners, or remove them entirely if the supply is below 15V. (b) Gate resistors too small - 220Ω lets the gate current spike and can cause parasitic oscillation. Use 470Ω–1kΩ. (c) Missing asymmetry resistor - a ZVS oscillator needs a slight imbalance to start reliably. Add a 10kΩ resistor across one gate-source to create a guaranteed startup path. Without it, both MOSFETs can sit in the linear region and cook.
Automotive voltage is not 12V - it's 13.8–14.4V with the alternator running, and load-dump transients can spike to 40–60V for hundreds of milliseconds. The IRFZ44N's 55V rating survives a typical load-dump, but the margin is thin. Worse: if your gate drive is a resistor divider from the battery, the gate voltage rises with the battery. At 14.4V with a 10V Zener clamp, the gate sits at 10V - fine. But if the Zener is missing or fails open, the gate hits 14.4V, which is within the ±20V limit but beyond what the drain can handle with inductive kickback stacked on top. For automotive, use the AUIRFZ44N (AEC-Q101 qualified) or step up to a 75–100V MOSFET.
| Parameter | Details |
|---|---|
| Best MCU-Direct Replacement | IRLZ44N (TO-220, 55V, 47A, Logic-Level, Infineon) |
| Best Performance Upgrade | STP60NF06 (TO-220, 60V, 60A, 10.5mΩ, STMicro) |
| Best Value (Performance per Dollar) | FQP50N06 (TO-220, 60V, 50A, 14mΩ, onsemi) |
| Best Automotive Grade | AUIRFZ44N (TO-220, 55V, 49A, AEC-Q101, Infineon) |
| Condition | New, original manufacturer packaging |
| Lead Time | In stock, ship from Shenzhen |
| Packing | Tube (50/standard tube for TO-220) |
Contact ICMASS for current pricing on your specific quantity. We stock IRFZ44N, IRLZ44N, STP60NF06, FQP50N06, IRF540N, and AUIRFZ44N with full manufacturer traceability. Volume pricing for TO-220 power MOSFETs typically ranges from $0.30–$0.90/unit depending on part number and quantity. Need to validate a gate drive design or check a substitution for production? We can supply sample quantities and engineering support.
A: Yes - same TO-220 package, same G-D-S pinout, same 55V rating. The IRLZ44N gives up 2A of current (47A vs 49A) and has slightly higher RDS(on) at 10V (22mΩ vs 17.5mΩ). What you gain: full enhancement at 5V gate drive. If you're switching from a microcontroller, this trade is worth it every time.
A: The 49A rating assumes 10V gate drive and the case held at 25°C. At 5V gate drive (typical microcontroller GPIO), RDS(on) rises to ~30–60mΩ. At 10A through 50mΩ, that's 5W dissipation. Without a heatsink (RθJA = 62°C/W), junction temperature hits 310°C - the MOSFET destroys itself. Use the IRLZ44N for 5V gate drive, or add a gate driver to deliver 10V to the gate.
A: 10V for the datasheet RDS(on) of 17.5mΩ. At 8V, it's mostly on but RDS(on) is higher (~20–25mΩ). At 5V, the MOSFET is in the linear region - RDS(on) is uncharacterized and can be 30–60mΩ. At 3.3V, most units don't turn on reliably. For any production design, drive the gate to 10–12V through a dedicated gate driver or a push-pull transistor stage.
A: The IRFZ44 (non-N) is the older version. It has slightly better raw specs - 60V Vds, 55A Id, 16.5mΩ RDS(on) - but slower switching (rise/fall 97/57 ns vs the N-version's 60/45 ns). The IRFZ44N is more widely available and preferred for new designs where switching speed matters. For DC on/off switching, the two are interchangeable.
A: It depends on current. At 5A with proper 10V gate drive (RDS(on)=17.5mΩ): Pd = 0.44W, temp rise = 27°C - fine without a heatsink. At 15A: Pd = 3.9W, temp rise = 244°C - needs a heatsink. At 30A: Pd = 15.8W - needs a substantial heatsink with forced air. The math: Pd = I² × RDS(on) × 1.5 (temperature coefficient at 100°C). If Pd × RθJA > 75°C rise from ambient, add a heatsink.
A: Not directly. The ESP32's 3.3V GPIO is below the IRFZ44N's Vgs(th) of 2–4V for many units. Even if the MOSFET partially turns on, RDS(on) at Vgs=3.3V can be hundreds of milliohms. Use a logic-level MOSFET (IRLZ44N at minimum, or IRLB8721 for better 3.3V performance), or add a 3.3V→10V gate driver stage. A simple NPN transistor + pull-up resistor to 12V works as a cheap level-shifting gate driver.
A: Drain voltage spikes exceeding 55V during switching, caused by parasitic inductance in the PCB traces and transformer leakage inductance. The spike duration is nanoseconds - a multimeter won't see it, but a scope will. Solutions: minimize high-current loop area on the PCB, add an RCD snubber across the drain-source, use a MOSFET with a higher Vds rating (IRF540N at 100V), or add a TVS diode clamp from drain to gate (with a series resistor to limit current). A 47V TVS from drain to gate with a 100Ω series resistor can save MOSFETs during development.
A: Three rules. (1) Individual gate resistors: 10–22Ω per MOSFET, never tie gates directly together - this prevents parasitic oscillation between parallel gates. (2) Thermal coupling: mount all MOSFETs on the same heatsink with thermal paste. As one heats up, its neighbors heat up too, keeping Vgs(th) tracking. (3) Layout symmetry: keep source and drain trace lengths equal for all paralleled MOSFETs. Asymmetric layout → asymmetric inductance → asymmetric current sharing during switching edges. For steady-state sharing, the positive tempco of RDS(on) helps - as a MOSFET heats up, its RDS(on) rises, pushing current to cooler devices. But that mechanism only works in DC; switching transitions are dominated by layout and Vgs(th) matching.





