M
Michael Robinson
Guest
A lot of people have built the circuit in this Home Power article.
http://alton-moore.net/graphics/desulfator.pdf
There's also an active discussion forum
http://leadacidbatterydesulfation.yuku.com/
In my opinion it's an elegant design, very creative, and maybe it could be
made even better.
Here is an equivalent circuit using an n-fet and reversing the polarity
overall (view in proportional font).
Nothing new there.
D1
,------+->|-+------,
| | | |
| ( ) |
| L1 ( ) L2 |
| ( ) |
| ( ) -----
| | | ---
| '--+-' -----
_| | ---
--||_ ---- |
| ---- C4 |
| | |
'---------+--------'
L1 and L2 are separate inductors. They are not linked.
I arranged them in parallel to illustrate something:
why not use magnetically coupled windings?
,------, ,------,
| | | |
| *( || )* |
| ( || ) |
| 1 ( || ) 2 |
| ( || ) -----
| | | ---
| '--+-' -----
_| | ---
--||_ ---- |
| ---- C4 |
| | |
'---------+--------'
The same pulse that appears at winding 1 when the mosfet turns off will
appear at winding 2.
This means you can pulse the battery without having to wait for a diode to
come out of reverse bias and start conducting.
(Of course, in a physical circuit you could have stray inductance and
imperfect coupling between the windings
so I might include D1, but I left it out of the drawing to get the idea
across.)
This brings up another question about an effect that I think magnetically
linked windings would have.
Would coupling the windings with the indicated polarity reduce ripple on the
capacitor, as compared to the original circuit?
I think that when the mosfet is on, current is ramping up in winding 1, and
the "back emf" in winding 1
that opposes the impressed voltage will be reflected into winding 2 and push
current into the capacitor node at the same time
winding 1 is drawing circuit from that node. Is my analysis correct?
http://alton-moore.net/graphics/desulfator.pdf
There's also an active discussion forum
http://leadacidbatterydesulfation.yuku.com/
In my opinion it's an elegant design, very creative, and maybe it could be
made even better.
Here is an equivalent circuit using an n-fet and reversing the polarity
overall (view in proportional font).
Nothing new there.
D1
,------+->|-+------,
| | | |
| ( ) |
| L1 ( ) L2 |
| ( ) |
| ( ) -----
| | | ---
| '--+-' -----
_| | ---
--||_ ---- |
| ---- C4 |
| | |
'---------+--------'
L1 and L2 are separate inductors. They are not linked.
I arranged them in parallel to illustrate something:
why not use magnetically coupled windings?
,------, ,------,
| | | |
| *( || )* |
| ( || ) |
| 1 ( || ) 2 |
| ( || ) -----
| | | ---
| '--+-' -----
_| | ---
--||_ ---- |
| ---- C4 |
| | |
'---------+--------'
The same pulse that appears at winding 1 when the mosfet turns off will
appear at winding 2.
This means you can pulse the battery without having to wait for a diode to
come out of reverse bias and start conducting.
(Of course, in a physical circuit you could have stray inductance and
imperfect coupling between the windings
so I might include D1, but I left it out of the drawing to get the idea
across.)
This brings up another question about an effect that I think magnetically
linked windings would have.
Would coupling the windings with the indicated polarity reduce ripple on the
capacitor, as compared to the original circuit?
I think that when the mosfet is on, current is ramping up in winding 1, and
the "back emf" in winding 1
that opposes the impressed voltage will be reflected into winding 2 and push
current into the capacitor node at the same time
winding 1 is drawing circuit from that node. Is my analysis correct?