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SQM Replication Project Update
22-05-05.
This weekend I tried a different
approach. I heated the magnets and
used more capacitors. I started
heating the magnets to around 200
Degrees Celsius and putting them
straight in the Conditioning Coils
chamber. I have been using a
capacitor bank of 21500uf at 200
Volts and thought about the math of
the pulsing a bit more. This is the
math for current pulsing and
discharge to the conditioning coil:
The equation is: U = 1/2 CV^2
The capacitor bank charges to: 200
Volts
200x200 x .0215 = 860, / 2 = 430
Joules
After discharge the capacitor ends
up containing: 15 Volts
15 x 15 x .0215 = 4.8375, / 2 =
2.41875 Joules
When the Capacitor discharges,
427.58125 joules discharge into the
Conditioning Coil.
200 x 200 = 40000
40000 times .0215 = 860
860 / 2 = 430 Watts Dissipation
The math of the pulsing of the last
Conditioning attempt is with a
1500uf capacitor:
The capacitor charges to: 200 Volts
200x200 x .0015 = 60, / 2 = 30
Joules
And it ends up containing: 20 Volts
20 x 20 x .0015 = 0.6 / 2 = 0.3
Joules
When the Capacitor discharges, 29.7
joules discharge into the
Conditioning Coil.
200 x 200 = 40000
40000 times .0015 = 60
60 / 2 = 30 Watts Dissipation
With this information the
conditioning process seems to be a
bit of a waste of time when you look
at the power to magnetise the
magnets in the first place. Most
magnetisers will start at around 800
Joules and go up to thousands of
Joules. So to make any real
conventional changes to the magnets
the power or energy levels seem to
be far to low. I must say with
heating the magnets I have
demagnetised the Anisotropic magnets
quite a lot by pulsing with the
method I have used today but do not
appear to have changed the field
pattern in the magnets using the
magnetisation film paper (Magna
View) all that much. However there
is a small change in the field
pattern and the magnets don't have
close thin field lines and one
magnet has a sharp spike in the
middle.
This is a picture of the magnets
unaltered by the Conditioning.
This is a picture of the magnets
after the conditioning.
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