I'm trying to drive a the low side of a n-channel half bridge with a 3.3V signal that is not enough to switch the MOSFET I think (sometimes it does switch and sometimes it doesn't).

schematic

I did this: http://upverter.com/nraynaud/9737d290ff152f76/half-bridge/ The high part comes from another circuit, but I built the low side on my own so I'd like some review. The 22k resistor is a pull-up because adding the circuitry complements the inputs, making everything closed when there is no inputs.

Thanks for your advice.

  • R8= 1k will limit turn on speed. R5=1k can be much smaller - say 10 Ohms. Ensure Vgs never exceeds FET Vgsmax ratings. If VCC24 = 24V etc then you get eg Vgs = 16V on top FET when on BUT up to 24V when off and about to be turned on. This is above the Vgsmax of most FETs. NPN emitter follower, emitter to FET gate, n place of R6 and R8 will give faster drive. Cap across R13 (maybe 1 NF?) will give faster drive edges. – Russell McMahon Jan 25 '13 at 22:43
  • How fast do you need the switching to happen? Are you driving something with PWM? What frequency? – Phil Frost Jan 25 '13 at 22:44
  • Russell > thanks ; can you explain the R8 speed thing please (or just give me a link) ? I think you are right, the top Vgs is 20V. – nraynaud Jan 25 '13 at 22:52
  • Phil > thanks for the edit. It's for PWM, I have not settled on a frequency yet, if you have link about the relation between my design and the max switching frequency I'd be delighted. Moreover, if somebody have a standard design that has been made by a real engineer, I'd be pleased to learn from the experts. I'm very humble on that. – nraynaud Jan 25 '13 at 22:58
up vote 11 down vote accepted

I think you will encounter two challenges in designing this. The first is getting the high side to turn on. The source of the high-side moves up and down relative to ground, so a voltage source referenced to ground won't be able to drive it without exceeding the maximum gate-to-source voltage \$V_{GS}\$. For RFG50N06, this is 20V.

The second is that you want to switch the transistors fast. Any time that the transistors spend between fully-on and fully-off will also mean both high current through and high voltage across the transistor. This means a high amount of electrical energy converted to heat, which represents an inefficiency in the system and a limit on the current your bridge can deliver to the load, since heat from these switching losses must be removed through the heatsink.

Getting the transistors to switch fast is hard because the gate driver sees a capacitive load formed by the gap between the gate and the rest of the transistor. See how the gate part of the schematic symbol for a MOSFET looks like a capacitor? It is.

So, the first thing I notice is that when you go to switch on the low side, the current must flow through R8. This is bad, because any resistance here limits how fast you can raise the gate voltage of Q2, and all that time, Q2 is wasting energy and getting hot.

The next thing I notice is that you have the gate of the high side tied (again through some resistors) to 24V. It looks like the source of Q1 is 8V. When Q1 is on, the drain won't be much below that, so the voltage from source to gate is 16V. That's getting pretty close to the absolute maximum of 20V. But consider what happens before the high-side is on. If the low-side is completely off, as Q1 turns on, its source voltage is free to rise to meet the gate voltage. But what if Q2 isn't fully off yet? What if something else is holding the source of Q1 low? Pop! You apply too much voltage at the gate and blow through the gate insulation. This is not a robust design.

Here's a gate driver I made from discrete components a while ago:

half-bridge driver schematic

The first thing all point out is C13. This provides a voltage relative to the high-side's drain, so you don't have to worry about applying too much voltage to the gate. It's essentially a charge pump; when AOUT is low, then C13 can charge through D12. When the AOUT is high, the bottom of the capacitor is lifted with it. C13 is chosen to be large enough to power the gate driver until AOUT is low again.

The next thing to notice is that for both for turn-on and turn-off, the gate current doesn't flow through any resistors except those that I've intentionally placed to slow things down (R25, R26, R15, R16). This keeps the switching losses low and the MOSFETs cool.

Why would I want to slow things down? If the source-drain voltage of a MOSFET rises too quickly, this high \$ d V/d t \$ couples through the gate capacitance and can raise the gate voltage enough to turn the MOSFET on. In a half-bridge configuration, this happens to the side that just turned off as the other side is turning on. Accidentally, the side that just turned off is turned back on, both sides are on, you've basically shorted the battery terminals together, and bad things happen. International Rectifier explains it a bit more at the end of Power MOSFET Basics.

summary of operation

Turning on:

on schematic

A high input at ALO turns on Q20. R23 is placed in the emitter, rather than on the base, so that Q20 does not saturate, and will be quicker to turn off. R21 also helps with a quick turn-off.

Most of the current through R23 comes from the collector of Q20 (by virtue of a BJT's current gain). This current must also flow through R22, raising the voltage across Q21's base-emitter. This opens the flood gates for current to flow through the nearby decoupling caps C20 and C21 (or C13, on the high side), through Q21, R25, D20, and through the gate.

As long as ALO is held high, a small current flows through R27 and R28. This in turn creates the voltage that props up the base of Q22 and Q23, keeping them off.

Turning off:

off schematic

With the ALO voltage removed, Q20 is off, cutting off the current through R22, turning off Q21, removing the source of current for R23 and R28. The gate capacitance is now free to discharge through the base-emitter diode of Q22 and R27. The current gain of Q22 multiplies this current so the turn-off can be very fast.

  • thanks for your answer, I think so much stuff is wrong in my design and a correct one uses so many parts that I will just try to find a good driver. But the reward is the journey. – nraynaud Jan 26 '13 at 6:21
  • can you please explain me why you have C20 and C21 next to each other ? I hope it's the right place for a bunch of low-level questions about your work. – nraynaud Jan 30 '13 at 11:01
  • @nraynaud having two capacitors in parallel makes them more like an ideal capacitor. A capacitor also has some series resistance and inductance; with two in parallel this resistance and inductance is decreased while the capacitance is increased. Also, C21 tends to be more effective at higher frequencies, while C20 provides a bigger reserve of energy for lower frequencies. – Phil Frost Jan 30 '13 at 12:08
  • I was using the circuit you have given here. It works provided the diode D13, D23 are removed.I did't get the use of these diode. Moreover, collector to Emitter voltage of Q10 becomes 60V when giving 30V to the DC bus. I think this circuit is suitable for low DC. Is it so? In that case can you help me with a H-bridge MOSFET driver with discrete components when the DC bus is 60V (max) – user106157 Apr 8 '16 at 8:57
  • @gang85 D13 and D23 are Schottky diodes, making Q11 and Q22 in effect Schottky transistors. They are not required, but I put them there because when Q21 is on, it's driven hard into saturation. Then when it's turned off, there's a delay. The Schottky diodes eliminate that delay. You are right about the voltage across Q10: I designed this to work at 24V. I think if you ask a new question you can get some help with the design problem of getting this to work at higher voltages. There are many ways it could be done, a bit much for a comment. – Phil Frost Apr 9 '16 at 2:38

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