Adjustment of Q with frequency.

Grin, Well it makes it easy to go from radians/sec to cycles/sec. So an RC time of 1us is about 100kHz corner freq. So easy to pick an R or C to go into a circuit.

Oh thanks, but that's not necessary. I don't use skin depth very often.

George H.

Reply to
George Herold
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Yes, and you should listen to R. Macy.

Q as a function of frequency:

Q(w) = w*L/(R_DC + ((w_0*L/Q_0) - R_DC)*sqrt(w/w_0))

w = 2*pi*f

R-DC := DC resistance

Subscript "_0" means the frequency at which you know the Q.

The presumption is that you are operating below any frequency where the self resonating capacitor has substantive effect. That is, you are in the "sweet range" of an air core inductor.

Q = w*L/R_total

Generally, R_total = R_DC + R_skin + R_core + R_dielectric + R_radiate

For what I gave you, it is only R_DC & R_skin (R_dielectric lumped in)

Generally too, *everything* is a function of frequency except R_DC, by definition. So the formula, again, is bounded to the "sweet range" of an air core inductor.

Reply to
Simon S Aysdie

Gee, there was fifth different answer!

"multiply R by sqrt(2)" Well I know that's wrong, no frequency term. I'm sorry you got involved at all. Let alone a second time, with a no response post. Why did you waste your time? Mikek

btw, What is your answer?

Reply to
amdx

I am.

Thanks for that.

I always thought interwinding capacitance had an effect on Q. The higher the interwinding capacitance the lower the Q. Maybe very low with a 1/4" dia. 5 turn coil, but what about a 200uH coil with 15pf interwinding capacitance. Is there something there or do I have it all wrong? Thanks, Mikek

Reply to
amdx

self resonating capacitor has substantive effect. That is, you are in the "sweet range" of an air core inductor.

definition. So the formula, again, is bounded to the "sweet range" of an a ir core inductor.

Interwinding capacitance has an effect on Q if it is substantial for the fr equency of operation. I mean, at self resonance, the Q is zero. If the va lue "L" (Henrys) of the inductor is *not* "flat-ish" in your range of opera tion, then it is having an effect.

But like I said, you have to figure out how substantive the interwinding ca pacitance is for the frequency of operation. For filter type work, using t he inductor where interwinding capacitance is substantive is a no-no. You should be using inductors where their values are "flat-ish."

200 uH is pretty big for an air core. But maybe you never said it is air c ore. I can't remember.
Reply to
Simon S Aysdie

Sorry, I don't want to confuse things here, the coils I'm discussing for the 110 Mhz filter are are around 100nH, 1/4" id. 5 turns.

I have worked with AM BCB coils that were large, 3" x 3" and had

240uH of inductance and 8pf to 15pf of interwinding capacitance.

I think I've worked through the math, I'll check it and then post it. Thanks, Mikek

Reply to
amdx

Q(w) = 6.28*100Meg*105nH/(.002+((6.28*50Meg*105nH/80)-.002)* sqrt(100/50))

Q(w) = 65.94 /(.002+ (.412125 -.002)*sqrt 2)

Q(w) = 65.94 /(.002+ .410125 * 1.414)

Q(w) = 65.94 /(.002+ .57991675 )

Q(w) = 65.94 / .58191675

Q(w) = 113.3

The measured Q of the 105nH coil was 80 at 50 MHz.

Using this formula, the calculated Q is 113.3 at 100MHz.

I appreciate the exercise, time for a drink!

Mikek

Hope the font works.

Reply to
amdx

Add 50% in your head and it's within about 6%, closer than many caps.

Best regards, Spehro Pefhany

--
"it's the network..."                          "The Journey is the reward" 
speff@interlog.com             Info for manufacturers: http://www.trexon.com 
Embedded software/hardware/analog  Info for designers:  http://www.speff.com
Reply to
Spehro Pefhany

My answer is that you appear to be a lost cause.

Reply to
John S

And again you wasted your time with a non helpful response.

btw, what is your answer?

Mikek

Reply to
amdx

No, I didn't waste my time. The object was to get you to waste your time.

Reply to
John S

btw, what is your answer?

Reply to
amdx

My answer is that you appear to be a lost cause. Still haven't learned to read, have you?

Reply to
John S

Boys! Please... stop it! Show some restraint. Maybe this coming New Year we can all make a pledge to be nicer. I often write something in response and then look at it.. do I really need to post this.. and then throw it away.

George H.

Reply to
George Herold

You're right, George. I failed to restrain myself so I hereby apologize to Mikek and the group.

Cheers to all.

Reply to
John S

Sounds about right. Look at the Q v f plots for the Coilcraft "Midi Spring" inductors. That graph suggests your calculation is reasonable.

No problem.

Um, I have google. Just terrible.

Reply to
Simon S Aysdie

Thanks, I'm just here to learn enough do a few electronic projects. I didn't learn the math 40 years ago when I should have. I lean on people here to help.

So, I note the sqrt(2) gives me an answer of Q = 113.13

Very close to the long formula,

Q(w) = w*L/(R_DC + ((w_0*L/Q_0) - R_DC)*sqrt(w/w_0))

Using this formula, the calculated Q is 113.3 at 100MHz.

But I understand the long formula has more utility. Mikek

PS. I'm usually the one trying to stop the sparing between Thompson and Larkin.

Reply to
amdx

Say what?

Jamie

Reply to
Maynard A. Philbrook Jr.

Actually Robert Macy said "usually sqrt(f/f0) times the losses". I said sqrt(2) because, IIRC, the R was measured at 50MHz and the estimate was to be for 100MHz. So, R*sqrt(100/50) is the same as R*sqrt(2). Don't use sqrt(2) unless your frequencies are 2:1. The long equation is the correct one to use for most any two arbitrary frequencies. Keep in mind that these are approximations. There are many factors which affect all this.

Cheers.

Reply to
John S

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