Mosaic
Well-Known Member
Hi all:
I have a simple flywheel snubber Schottky across a 12V Lead Acid batt I am experimenting with. Pulsing from a 36V capacitor bank.
The battery's DC-R is around 25mΩ and AC-R is 15mΩ.
The battery is accepting 4A avg and holding at about 16V.
My concern is that the flywheel schottky snubber seems to be permitting up to 15+V kickback for several µS as measured across the terminals of the flywheel schottky.
Why is this?
This is the 50SQ80 spec sheet.
https://www.farnell.com/datasheets/3251.pdf
The V/µS of the voltage kickback is 500V/µS, well below that of the Schottky @ 10KV/µS
See the scope waveforms annotated below. The blue trace is the current flow to the battery as measured by a CT.
EDIT:
BTW I am investigating using the inductive kickback to depolarize the cells to improve the pulse charge acceptance. You can see that the positive going pulse width is significantly reduced with this method for a fixed avg current acceptance!
I have a simple flywheel snubber Schottky across a 12V Lead Acid batt I am experimenting with. Pulsing from a 36V capacitor bank.
The battery's DC-R is around 25mΩ and AC-R is 15mΩ.
The battery is accepting 4A avg and holding at about 16V.
My concern is that the flywheel schottky snubber seems to be permitting up to 15+V kickback for several µS as measured across the terminals of the flywheel schottky.
Why is this?
This is the 50SQ80 spec sheet.
https://www.farnell.com/datasheets/3251.pdf
The V/µS of the voltage kickback is 500V/µS, well below that of the Schottky @ 10KV/µS
See the scope waveforms annotated below. The blue trace is the current flow to the battery as measured by a CT.
EDIT:
BTW I am investigating using the inductive kickback to depolarize the cells to improve the pulse charge acceptance. You can see that the positive going pulse width is significantly reduced with this method for a fixed avg current acceptance!
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