John Curl's Blowtorch preamplifier part II

Status
Not open for further replies.
Ran an open loop & closed loop set up & lead calibration test just a few days ago.

Have tried different arrangements but usually don't have leads close & parallel while calibrating because it is not always possible while testing - but thx for the reminder.

Ls Cs & Rs are three different functions with the option of a selectable secondary function displayed also.

So Rs results I showed were not piggy backed on an Ls result.

If Rs is lower than DCR I have been ignoring it.
 
Dan

Is this what you wanted ?
 

Attachments

  • four choke values into 8R.jpg
    four choke values into 8R.jpg
    266.5 KB · Views: 208
  • Results into 8R.jpg
    Results into 8R.jpg
    185.5 KB · Views: 194
Ran an open loop & closed loop set up & lead calibration test just a few days ago.

Have tried different arrangements but usually don't have leads close & parallel while calibrating because it is not always possible while testing - but thx for the reminder.

Ls Cs & Rs are three different functions with the option of a selectable secondary function displayed also.

So Rs results I showed were not piggy backed on an Ls result.

If Rs is lower than DCR I have been ignoring it.
Ah, ok. I'd do the same.

jn
 
I just put two graphs in a new personal gallery, showing how some inductors in the 200-300uH range react both in air and against a copper PCB plane. It's interesting to see how nearby conductive surfaces change both the losses and the overall inductance. Something to be aware of should you be using air core coils and need exact values.

jn
 
Member
Joined 2002
Paid Member
I just put two graphs in a new personal gallery,
jn

Jn
Thanks again. In this diagram:


with the inductors close to copper, R increases linearly with frequency from 2kHz and up.
With the inductors in free air, from 9kHz to 50kHz, R increases faster with frequency and from 50kHz and above the rate droops.
I would expect the opposite, a linear increase of R with cores on air and a nonlinear increase with cores close to copper plate due to the extra eddy currents in the copper.
Where is my fault?

George
 
Jn
Thanks again. In this diagram:


with the inductors close to copper, R increases linearly with frequency from 2kHz and up.
With the inductors in free air, from 9kHz to 50kHz, R increases faster with frequency and from 50kHz and above the rate droops.
I would expect the opposite, a linear increase of R with cores on air and a nonlinear increase with cores close to copper plate due to the extra eddy currents in the copper.
Where is my fault?

George

Your fault?? None.

I've no idea how to analytically model it. Remember, as the eddies fight the rate of change, it excludes field. If the conductor were inside the winds where field lines were forced, it'll act differently. Exclusion of the field would reduce the losses.

The meter lumps eddy current losses and IR losses into Rs by it's nature of calculations. I assume it does an rms calculation of the powers that are in phase and 90 degrees out. As long as we don't try to extend too far into the high dissipation area, I guess we can use simple models. But if we try to extrapolate too far, we'll probably leave reality.

Bottom line, I'm just the messenger here. One of the guys here could certainly develop an analytical model that'll be accurate to ten decimal places. But I'm also confident I won't be able to follow it past the first half page of equations.

jn
 
Status
Not open for further replies.