Mosaic
Well-Known Member
Hi all:
I was experimenting with the effects of a yellow 220µH toroid (shorted and unshorted) with a high current pulse 14AWG passing thru the centre toward the load.
I could use some help with the principle in play here.
Pls note the attached scope images. (constant avg current = 1.8A)
1: Toroid coil NOT shorted - note the blue trace current spike (40A/V) @ 224A peak, also the pulse width is 20µS

2)Same as 1 WITH the 220µH toroid shorted. Blue trace pk current is now 256A and the P.width is shortened to maintain the 1.8A avg.
The yellow voltage trace exhibits more (post pulse) kick back ringing harmonics and amplitude

3) Here is item 1 zoomed to observe the risetime (50nS), a bit of jitter.

4)Item 2 zoomed to observe the rise time, I observe a 'cleaner', less jittery signal.

Empircally, it would seem that the shorted toroid improves the pulse fidelity, current rise time and generates richer ringing harmonics. Also , noting the yellow V trace...the positive endpoint V of the capacitive pulse is the same in both 1 & 2 implying the charge moved is the same, but in less time! Wouldn't that imply that the 14AWG parasitic inductance is mitigated in some manner?
My question is what combination of electrical principles are at work here; Lenz's law seems applicable but how does it improve the behaviour of the pulse signal in the pulse conductor to give a 14% improved peak pulse and reduced jitter?
Edit: I took some more images of the pulse signal at the load (battery) which will include all cabling impedance losses. The first set of images were direct from the PCB output. The voltage scale is adjusted to compensate for the loss in amplitudes.
5) Same as 1 @ the load terminals:
6) Same as 2 @ the load terminals:
7) zoom of #5
8) Zoom of #6

I was experimenting with the effects of a yellow 220µH toroid (shorted and unshorted) with a high current pulse 14AWG passing thru the centre toward the load.
I could use some help with the principle in play here.
Pls note the attached scope images. (constant avg current = 1.8A)
1: Toroid coil NOT shorted - note the blue trace current spike (40A/V) @ 224A peak, also the pulse width is 20µS

2)Same as 1 WITH the 220µH toroid shorted. Blue trace pk current is now 256A and the P.width is shortened to maintain the 1.8A avg.
The yellow voltage trace exhibits more (post pulse) kick back ringing harmonics and amplitude

3) Here is item 1 zoomed to observe the risetime (50nS), a bit of jitter.

4)Item 2 zoomed to observe the rise time, I observe a 'cleaner', less jittery signal.

Empircally, it would seem that the shorted toroid improves the pulse fidelity, current rise time and generates richer ringing harmonics. Also , noting the yellow V trace...the positive endpoint V of the capacitive pulse is the same in both 1 & 2 implying the charge moved is the same, but in less time! Wouldn't that imply that the 14AWG parasitic inductance is mitigated in some manner?
My question is what combination of electrical principles are at work here; Lenz's law seems applicable but how does it improve the behaviour of the pulse signal in the pulse conductor to give a 14% improved peak pulse and reduced jitter?
Edit: I took some more images of the pulse signal at the load (battery) which will include all cabling impedance losses. The first set of images were direct from the PCB output. The voltage scale is adjusted to compensate for the loss in amplitudes.
5) Same as 1 @ the load terminals:

6) Same as 2 @ the load terminals:

7) zoom of #5

8) Zoom of #6

Last edited: