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4hv.org :: Forums :: General Science and Electronics
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Transformer B-Field Calculator

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Adam Munich
Thu Nov 08 2012, 07:26PM Print
Adam Munich Registered Member #2893 Joined: Tue Jun 01 2010, 09:25PM
Location: Cali-forn. i. a.
Posts: 2242
...Because I could barely find the formula; let alone a calculator!

Link2

Enjoy.
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Daedronus
Thu Nov 08 2012, 10:05PM
Daedronus Registered Member #2329 Joined: Tue Sept 01 2009, 08:25AM
Location:
Posts: 370
Link2

midpage?
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klugesmith
Fri Nov 09 2012, 03:01AM
klugesmith Registered Member #2099 Joined: Wed Apr 29 2009, 12:22AM
Location: Los Altos, California
Posts: 1716
Strong work, Gren.

I like that you give the formula. IMHO, formulas given without an online calculator are better than online calculators given without a formula. I've found plenty of calculators that give wrong answers, even for reasonable input values. The two in this thread seem to give the same answers.

The B-max formula is not hard to get from basic EM principles, if you work in SI units and remember that μ0 = 4pi/10^7 henries per meter. In MS Excel, you can type =4e-7*pi().
[edit]
Last night I wrote too late, and said an identical unit for μ0 was webers per volt-second. Wrong!
The SI unit of magnetic permeability is, indeed, the henry per meter.
That's identical to the "tesla per (ampere per meter)", as in μ = B / H.

But magnetic permeability has no place in the transformer core B_max formula.
That formula is an application of Faraday's law of induction: V = dΦ/dt.
Volts "per turn" = webers per second, so webers = volt-seconds.

SI flux unit: 1 weber is 1 tesla x 1 square meter; same as 10^8 maxwells.
cgs flux unit: 1 maxwell is 1 gauss x 1 square cm.
Flux change of 1 maxwell induces 10^-8 volt-seconds.


Gren's calculator gets an extra plus for having coefficients for both sine waves and square waves. Square waves have the lower RMS voltage for the same frequency and same flux swing (= integrated volt-seconds in one positive or negative half-cycle).

For |B_max| values close to saturation, you can squeeze out a bit more RMS voltage and peak voltage using "cresty" voltage waveforms. They form automatically if a sinusoidal primary voltage is too high (by, say, a factor of two), and the primary current is limited by a resistive ballast.
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