The amp rating on a P-channel MOSFET is a case-temperature promise, not a board reality — and the higher the sticker, the bigger the gap between the two.
A -30A DFN part and a -50A DFN part from the same family can publish thermal envelopes that look backwards: the bigger die carries the tighter 35W ceiling, and the smaller die carries the better RθJC.
This post walks the NCE 30P line — SOP-8 25A, DFN 30A, TO-252 30A, DFN 50A — and shows where the current rating actually comes from, what a real board delivers, and the honest crossover to N-ch.
The sticker current is measured at TC = 25°C with the case held there — a heatsink of infinite size, in other words.
Board reality is different. The junction temperature is set by the power you burn times the thermal path from die to air, and the path is the package, the pad, the copper, and the airflow — in that order.
Now the fine print that few people read: the on-resistance rows are measured at currents far below the stickers.
The 50A part's 7mΩ is tested at -10A. The 30A DFN's 10mΩ is tested at -15A. The 30A TO-252's 18mΩ is tested at -20A. None is measured anywhere near its own sticker.
Why does that matter? At the sticker current the die is near its limit and the measurement is not repeatable at pulse widths. The rows describe die quality, not 50A conduction.
The same -30V rail, three packages, three ways for heat to leave the die — and the datasheets disagree on which envelope each one gets.
| NCE30P25S (SOP-8) | NCE30P30K (TO-252-2L) | NCE30P30G (DFN5×6-8L) | NCE30P50G (DFN 5x6) | |
|---|---|---|---|---|
| Sticker current | -25A | -30A | -30A | -50A |
| RDS(on) max @ 10V | 9mΩ (test -15A) | 18mΩ (test -20A) | 10mΩ (test -15A) | 7mΩ (test -10A) |
| Qg | 98.9nC | 31.2nC | 81.3nC | 84nC |
| PD @ TC 25°C | — | 60W | 80W | 35W |
| RθJC | — | 2.5°C/W | 1.56°C/W | 3.6°C/W |
| TJ max | 150°C | 175°C | 150°C | 150°C |
| EAS published | no row | 169mJ | no row | 300mJ |
Read the last three rows twice: the 50A part carries the tightest envelope of the three big dies, and the TO-252 part runs the hottest junction ceiling.
That is not a typo. It is package attribution — each datasheet is internally consistent, and each tells a different story about what the die is for.
Three heat exits: the SO-8 part sheds heat through five thin leads — that is the wall near ~10A continuous. The TO-252 tab and the DFN pad both hand the heat to the copper; the difference is assembly and inspection, not physics.
Worst-case conduction loss at your current is I² times the max RDS(on) — use the max row, not the typ.
At 20A: the 50G burns 2.8W, the G 4.0W, the K 7.2W. At 30A: 6.3W, 9.0W, 16.2W.
Now take the junction math with the published envelope: at 30A the G's 9.0W against RθJC 1.56°C/W means the junction runs 14°C above the case before a watt leaves the copper.
That sounds small — until you remember the case sits at whatever your board's copper, vias and airflow deliver, which no datasheet row tells you.
P-ch high-side switching is a convenience: the gate drive references the rail, no level-shift IC, no bootstrap. The price is roughly double the RDS(on) per die dollar of an N-ch.
From what we see across Shenzhen lots (2025–2026), the crossover shows up in reorders: boards that pass about 20-25A continuous stop reordering P-ch and start asking about N-ch plus a driver.
Our own line makes the point: the NCE30H10K — an N-ch, 30V, 100A, 5.5mΩ, TO-252 — carries the current class the P-ch parts struggle to name.
What does that driver actually cost? About a dollar of BOM — and it's the cheapest half-loss you'll ever buy at this current class.
So the rule of thumb: P-ch below ~20A continuous, surge-tolerant; N-ch plus a high-side driver above it. The driver costs a dollar of BOM and buys half the conduction loss.
We batch-test every 30P lot at the datasheet's own points — not at the sticker. A -30A part gets tested at -15A or -20A per its row, and the milliohm max is the pass line.
What that catches, in practice: relabeled smaller dies. A 30A die relabeled as the 50A part fails the 7mΩ row at -10A; a 25S relabeled as a 30P30G fails the 4.5V row. The test conditions are the counterfeit detector.
Across lots (2025–2026) we also see the honest questions repeat: "can it really do 30A?" is almost always followed by the real question — "what does my board actually deliver?"
The answer is the same every time: measure it. Thermocouple on the pad, a current probe on the load, and the datasheet math on paper — that combination settles more arguments than any spec sheet.
A: Yes, when the pad delivers — and the envelope says how much of the job is yours. The G's 80W at RθJC 1.56°C/W is a case rating; the junction stays cool only if the pad, pours, vias and airflow move the watts. On a good 2oz board with airflow, 20-25A continuous is a defensible design; measure with a thermocouple before production.
A: Datasheet package attribution — and a design statement. The 50G lists RθJC 3.6°C/W with 35W at TJ 150°C; the 30P30G lists 1.56°C/W with 80W. Both are internally consistent. The practical reading: the 50G is specced for surge duty — pulse energy and duty set its junction temperature, not continuous watts.
A: Above roughly 20-25A continuous — that is the honest crossover. P-ch die economics give roughly double the RDS(on) per dollar of an N-ch. Add a high-side driver to an N-ch and the loss halves for about a dollar of BOM. P-ch stays the right answer for simplicity and surge duty below that line.
A: No — test at the datasheet's own test current. The rows are guaranteed at -10A, -15A or -20A depending on the die, not at -30A or -50A. Testing at the datasheet point catches relabeled dies; testing at the sticker just measures a die past its pulse-test region.
A: The DFN pad wins on paper; the TO-252 tab wins in the rework bay. The G's RθJC 1.56°C/W beats the K's 2.5, but the tab is inspectable, hand-solderable, and shares a land pattern with the whole N-ch TO-252 line. Pick by your assembly reality, not by the smaller number alone.
A: Yes, for single events — with the pulse-width caveat in the note. IDM is limited by junction temperature, so it is a stall-and-inrush budget, not a switching design target. Size your repeated pulsing against thermal impedance, not the sticker.





