jim hardy said:
...
I'm pretty sure if you consider the amp-turns per inch of airgap in the magnetic circuit of your microphone you'll find the Δflux from ribbon current is infinitesimal compared with the flux from your magnet.
In other words it's calculable; but I think it's so small as to be not measurable and an old hand would likely say 'don't worry about it'..
only way to be sure in measure it.
Carl Pugh addressed this in posts 9 and 11.
Yes, Carl, you and some other guys told me that the fluctuations of flux are very little comparing to flux from magnegnet and should be ignored.
But I have some feeling that something is not right in this comparison. Let me explain you why.
Example.
Atmospheric pressure is big, heavy - 14.7psi at sea level.
Pressure of mosquito wings is infinitesimal compared with the atmospheric pressure. It is probably 1mln times less.
However, we can hear mosquito quite well from distance 1-2m.
Huge atmospheric pressure does not hide infinitesimal fluctuations of itself.
This is what I mean by still asking "will flux in core fluctuate impacted by ribbon? how much (%) energy will be lost on these fluctuations of flux?"
It is like how much energy mosquito looses on making sound around itself instead of directing this energy on flight, counteracting with gravity and wind. :)
(Yes, making waves can take big portion of energy, that is why ship hull engineers try to elimitate them.)
So, the question is not in comparisson a mosquito and the Earth athmosfere, but rather getting understanding about efficiency of mosquito itself.
jim hardy said:
The little transformer has many more turns and no air gap. That's where the flux from your ribbon current will be significant - inside the transformer where you want it.
If it's a worry perhaps you could use nonconductive ceramic magnets for pole pieces?
Or place a few turns of tiny wire in the airgap and measure Δflux with an oscilloscope.
ceramic magnets will not produce that amount of flux that can be concentrated by Fe Co core.
I plan to use laminated core. By two reasons: 1 - it is more technological for me. 2 - it can be used to fight (possible) Eddy currents.
jim hardy said:
Is it moot anyway? Since eddy currents in iron oppose a change in flux it seems to me they're helping you cancel out what in a motor would be called "Armature Reaction".
"Armature reaction" is modulation of field flux by armature current.
Yes, this idea is used in loudspeakers. They put Faraday ring there exactly for this.
I am thinking about this too. It is not that complex, elongated copper ring around each pole.
jim hardy said:
Maybe that's why you don't see laminations in the pole pieces of old microphones. Something to ask on a microphone design forum.
:) This is exactly what I hoped to find an answer here, on
physics forum. I hope people here know electromagnetics better. ;)
jim hardy said:
Also I point out - a motor has two large mmf's that interact to produce lots of torque.
You have one huge mmf(magnet) and one infinitesimal mmf(current in the ribbon) that you'd prefer don't interact.
How many amp-turns are required to push your 1 tesla through your air gap?
1/1000th as many amps through your 1 turn ribbon will affect your flux by a part in a thousand.
That puts a number on it for you.
I looked at TI's application guide and they recommend this opamp for a microphone transformer replacement, but I think they mean the one at preamp input:
http://www.ti.com/lit/ds/sbos003/sbos003.pdfA
microphone design forum.
Time for some experimenting.
It looks like that.
jim hardy said:
I haven't heard you mention your acoustic design. This ribbon has inertia and stiffness, and you want it to move with feeble variations in air pressure... F=MA ...
Look at its output when subjected to square wave sound at various frequencies and with a range of resistive loads..
The lighter ribbon is the more signal level it produces. Amasingly frequency response does not depend on ribbon mass. It is because mechanic inertia is square of movement and electric output is square of movement as well.
They compensate each other, but overall level decreases if mass increases.
Because of this ribbons are very thin - ~2 micron.
Highest frequency that ribbon can take depends on width and depth of baffles on each side of ribbon. These baffles are formed usually by poles, sometimes by magnets too. 0.5x0.5" baffles will allow max ~8KHz
(explanation and calculator is here
http://www.diyaudiocomponents.com/ribboninfo.php?sub=3).
But, decreasing width of baffles lowers sensitivity because it decreases pressure gradient.