John Curl's Blowtorch preamplifier part II

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What insulator thickness? How to relate that to the 168 Ohm used? Do you mean cable diameter?

As another said, the insulation thickness will determine the inductance of the pair. Really thin insulation can get cylindrical wires down to about 150 nH per foot. Really thick, the value goes over 200 nH per foot.

Here are the equations:

Thank you John.

If I am reading and doing the math correctly it appears that length of wire has nothing to do with this value.
Absolutely correct.

Not sure how that would work with something like the twisted braided wire such as Kimber 4TC type of wire, is that a completely different set of equations?
No, same equations, just more difficult. For this app, just measure the capacitance and inductance per foot, Z = sqr(L/C). If you use multiple pairs, consider the impedance as the wires paralleled. This works well as long as the pairs are independently twisted. A quadstar cable is the most number of conductors that can be twisted together while maintaining magnetic orthogonality, it will have about half the impedance, or 50 to 75 ohms. A cat5e with the four combined solids and stripes will have 25 ohms.

Edit: when measuring a cable's L and C, do a sanity check using the equation L(nH/ft)C(pf/ft) = 1034 EDC. If you get a value of EDC that is less than 1, you've made a testing error, most likely inductance. You should get a value between 3 and absolute maximum 10 if the conductors are really far apart. And the cable prop velocity will be Vc/sqr(EDC), hence the can't be less than 1 thing...no superluminal signals here.

For most practical purposes a 2W 100 Ohm resistor will work. While I have not tried formal double blind tests its usually a pretty obvious improvement (change). If you have something like Cobra cable or Analysis plus (or another really low Z cable) you will need to figure it out. One way is to drive the cable with a fast rise pulse watching with a scope and trying different values until the reflection is gone. This won't be correct for audio frequencies but at audio frequencies the cables' impedance is less of an issue than its lumped R, L & C.

The only thing I'd mention here is be wary of wirewound and NI resistors. While an NI in theory is bifilar and non inductive, it still has a settling time due to the actual length of the element. I've no idea how that would affect frequencies under a gig..

Audibly how does putting this shunt resistor across the cable affect the sound? What is changing besides what the amplifier is seeing on the load end?
It dampens out the rf stuff. It may increase phase margin of the amp, if the amp is a hot one.

The only place where to put it, in the real world application, is the end of the speaker cable.
Agreed.

This is with coaxial RG58 cable.
See the resonances as seen at generator-out due to reflections at the cable end and the effect of resistive termination at cable end.
Generator's nominal Output impedance 50 Ohm

George
Excellent work. thank you. I loved the baselining at the end..and the labels on the first three. The interesting thing to note is the interleaving of dip frequencies between load>z and load<z.
edit: I missed the longer length of cable on the bottom, I thought it was a frequency change due to opposite reflection coefficient...kept my error in the post, just pinked it.
George, try to put a divider like 50/5 ohm to the generator output. Then you will drive the cable from <5 ohm impedance. You will get gross impedance mismatch. Then the effect of the terminating resistor will be even much more pronounced.
Excellent suggestion.

You guys are awesome..made my day.

jn
 
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Yep. Correct.
I’ve done it as I am working on the issue.
Jn has put me on fire and I am in the preliminary steps.
I will start a thread, I will post a link when I am ready.
Thanks again.

George
>Edit:The pics above is just to show the effect of termination and the shifting down in freq of the resonances as the length of the cable increases

George, why don't you write an article and submit it to jan?

jn
 
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Excellent work. thank you. I loved the baselining at the end..and the labels on the first three. The interesting thing to note is the interleaving of dip frequencies between load>z and load<z.
edit: I missed the longer length of cable on the bottom, I thought it was a frequency change due to opposite reflection coefficient...kept my error in the post, just pinked it.
jn

jn Thank you.
I think you should un-pink that sentense. See 2.4m/10 Ohm and 2.4m/200 Ohm. Comparable depth of notches but at different frequencies (this too to be explored).

As for an article, I would be honored but Jan wouldn’t be.
He does well keeping the standards of his magazine high.

There are many prohibiting reasons for not thinking over an article, the main one is that I don’t master the issue, I am studying it (and it shows :D ).

Between you and me, why don’t you…? ;)

George
 
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jn Thank you.
I think you should un-pink that sentense. See 2.4m/10 Ohm and 2.4m/200 Ohm. Comparable depth of notches but at different frequencies (this too to be explored).
Ah, I see it now. My bad.. Sounds like that drill seargent phrase..

edit: the interleaving resonance frequencies caused by the changed reflection coefficient sign is consistent with what I recall.
As for an article, I would be honored but Jan wouldn’t be.
He does well keeping the standards of his magazine high.
Which is why I recommended you write one.

Between you and me, why don’t you…? ;)

George
Perhaps a collaboration between several? So many here bring so much to the table.

jn
 
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Here is the book title.
 

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It is important to study the 'advantages' of Teflon vs cheaper plastics to actually make an informed decision. Most big labs use both Teflon wire and caps in LARGE quantities. They DO have the money, but that is not the only reason that they use Teflon to such a high proportion, compared to other insulators.
 
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Yes, it is quite easy to design and implement a poor active speaker too.

I find no difficulty in putting theory into practice with DSP based active crossover and EQ.

Passive crossovers are highly limited in controlling load presented by drivers.

Way too much time goes into thinking about what is happening on the dark side of speaker transducers rather then working with what comes out of them on the light side in using them most effectively.

Transfer function at voice coil leads is not transfer function of acoustic output.

With any amplifier and any transducer worth using in a speaker system very little information is lost to noise and non-linear distortion. Amplitude and phase of spectral components are merely rearranged in the acoustic output.

I've sure noticed a HUGE improvement going active DSP bi/tri amping.

Is this all phase related because when I hear a Danley synergy I felt the improvements were also similar.

Bare with me as I'm no EE.

I dunno what it is but it's something I can hear and I've noticed a similar psycho-acoustic affect between an LR2 and LR4.

Perhaps it's the full period time delay inherent is 360 LR4?
 
It is important to study the 'advantages' of Teflon vs cheaper plastics to actually make an informed decision. Most big labs use both Teflon wire and caps in LARGE quantities. They DO have the money, but that is not the only reason that they use Teflon to such a high proportion, compared to other insulators.

One big lab doesn't. Teflon tends to creep too much, has bad radiation resistance, and doesn't retain it's flexibility at 4.5K.

However, we do have roughly 1,300 power supplies with single digit ppm stability that we designed in house and farmed the assembly out, using some "horrific" D/A stuff...when I get a chance, I'll ask the designers what kind of caps they used for the high resolution analog stuff.

jn
 
Good reading is found here: Current-Driving of Loudspeakers by Esa Merilainen. yr 2010 340 pages.

"Eliminating Major Distortion and Interference Effects by the Physically Correct Operation Method".

Thx-RNMarsh

How does it make reference to characteristic impedance of speaker cable?

How is that resistive zobel affecting the upstream amplifier's performance?

How does this affect Z?

Z is minimum safe load impedance right?

Bare with me I'm an amateur with high school physics and no formal EE education.
 
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