do you mean the capacitance between GATE and SOURCE-DRAIN channel or SOURCE and DRAIN?
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Originally posted by kt315 View Postdo you mean the capacitance between GATE and SOURCE-DRAIN channel or SOURCE and DRAIN?
It's in the order of nF at low voltages and is in parallel with the coil. See Coss in Fig. 5 of this datasheet https://www.vishay.com/docs/91070/sihf840.pdf
I've explained it in this post https://www.geotech1.com/forums/show...576#post226576
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... may also consider the cascode switch configuration ( used in high speed high voltage switches since the valve era ) is just as fast or faster than the diode configuration. Also the series voltage drop with due selection of mosfet devices can be made lower than a series diode ... so more efficient & higher coil current. The cascode configuration mitigates the miller capacitance. NTX is a negative supply voltage.
DIODE TX
CASCODE TX
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Originally posted by moodz View Post... may also consider the cascode switch configuration ( used in high speed high voltage switches since the valve era ) is just as fast or faster than the diode configuration. Also the series voltage drop with due selection of mosfet devices can be made lower than a series diode ... so more efficient & higher coil current. The cascode configuration mitigates the miller capacitance. NTX is a negative supply voltage.
DIODE TX
[ATTACH]55639[/ATTACH]
CASCODE TX
[ATTACH]55640[/ATTACH]
Active damping tequires an exact balance of the polarization of the damping MOSFET to the energy of the coil. Even a small mismatch, such as grpund effect or a target throws the scheme off balance, requiring a complex feedback control loop.
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The cascode is not something I invented ... it’s been used to reduce capacitance for years. The upper mosfet turns off as a charge is trapped by the lower mosfets drain when it turns off .... this charge is only a few volts compared to hundreds volts trapped by the diode tx configuration. So when the lower mosfet turns off the upper one also turns off but faster due to reduced charge thus reduced capacitance.
the name cascode originates from cascaded triode and allowed early valve amplifiers to reach 100s of mhz which was not normally possible due to excess capacitance ... this was back in the 30s or 40s as far as I know.
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Originally posted by moodz View PostThe cascode is not something I invented ... it?s been used to reduce capacitance for years. The upper mosfet turns off as a charge is trapped by the lower mosfets drain when it turns off .... this charge is only a few volts compared to hundreds volts trapped by the diode tx configuration. So when the lower mosfet turns off the upper one also turns off but faster due to reduced charge thus reduced capacitance.
the name cascode originates from cascaded triode and allowed early valve amplifiers to reach 100s of mhz which was not normally possible due to excess capacitance ... this was back in the 30s or 40s as far as I know.
From the drain of the upper MOSFET the capacitance looks like two capacitors in series. Since the Cds increases by orders of magnitude at low Vds, the lower capacitor has a a value in the 1000s of nF range, while the upper one is in the 100s range, so no significant reduction takes place when in series. The simulations do not produce a significant improvement, confirming this.
What I have observed in my experiments is a physical limit as to how early it can be sampled even with a fast coil (90 uH, 35pF) because of the initial sudden drop of the drain voltage, when using a diode, that induces a crosstalk in the signal still important after the coil's transient has decayed. It looks like a target signal in the 10s of millivolts that's enough to drive the amplifier into saturation despite the coil's transient being already gone. I'm talking about a 2us transient followed by a much longer, smaller decay from the drain's voltage.
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Originally posted by Teleno View PostWhat I have observed in my experiments is a physical limit as to how early it can be sampled even with a fast coil (90 uH, 35pF) because of the initial sudden drop of the drain voltage, when using a diode, that induces a crosstalk in the signal still important after the coil's transient has decayed. It looks like a target signal in the 10s of millivolts that's enough to drive the amplifier into saturation despite the coil's transient being already gone. I'm talking about a 2us transient followed by a much longer, smaller decay from the drain's voltage.
Coil is 90uH, 35pF. MOSFET is IRF840. Series diode is a SiC Schottky with 1000V rating.
The decay of the blocked drain voltage looks like this during one PI period:
A close-up of the transient:
The orange line is there to highlight the non-linearity that shows at right at the beginning and extends into the 8us region when the coil already has decayed (2-3us). As a result it's not possible to sample as early as the coil's characteristics would theoretically allow us to.
I'm going to try an IGBT without the diode and see how it behaves. IGBTs have a tail current that might be a problem, and unlike MOSFETs they're destroyed by overvoltage.
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hmm ... well I did not want to get into a P>>ing competition ;-) but my results differ somewhat.
I am using a "real" coil ... actually a commercial PI coil ... and I get the following results. The preamp gain is approx 10000/16
the coil is damped at just over 1 microsecond and the first sample is taken at 1.5 microseconds.
I am using an IRF9640 in the front end ... its possible to get even faster using more exotic mosfets.
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Originally posted by moodz View Posthmm ... well I did not want to get into a P>>ing competition ;-) but my results differ somewhat.
I am using a "real" coil ... actually a commercial PI coil ... and I get the following results. The preamp gain is approx 10000/6
the coil is damped at just over 1 microsecond and the first sample is taken at 1.5 microseconds.
I am using an IRF9640 in the front end ... its possible to get even faster using more exotic mosfets.
[ATTACH]55649[/ATTACH]
Not trying to invent anything, just pushing the limits of the configuration in the title and see how far it can be optimized.
The simulated circuit does not produce the secondary, slower decay. It does though when I connect a 100k-200k resistor in parallel with the MOSFET, so I assume the effect is caused by the faster rate of discharge of Cds right after the peak.
Sure, you can sample earler at 2V with low gain, but what I'm trying to achieve is a pure coil decay.with no crosstalk from the blocked capacitance.
Have you ever tried an IGBT?
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Originally posted by Teleno View PostI'm not in competition mode, I'm trying to understand what happens when using a blocking diode (see the title of the thread) and why the results are worse than predicted in the simulations.
Not trying to invent anything, just pushing the limits of the configuration in the title and see how far it can be optimized.
The simulated circuit does not produce the secondary, slower decay. It does though when I connect a 100k-200k resistor in parallel with the MOSFET, so I assume the effect is caused by the faster rate of discharge of Cds right after the peak.
Sure, you can sample earler at 2V with low gain, but what I'm trying to achieve is a pure coil decay.with no crosstalk from the blocked capacitance.
Have you ever tried an IGBT?
I would not use a Shottky diode though .... the reverse leakage current is a problem.
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Originally posted by Carl-NC View PostDo you mean you want to reduce the flyback voltage? There is no flyback current.
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