
Mudcat
Senior Audioholic
Subsequent to my recent post on the measured LCR parameters of Carol 12 gauge 4 conductor cable, I measured a 6 foot section of Alpha Wire 85104CY. This is a 10awg 4 conductor shielded cable. Each conductor is 658 strands of 38 awg wire. And it is really expensive at $15/foot wholesale (I found what I was told was about 100 foot, but when measured turned out to be closer to 48 feet - no one to complain to because it was a garage sale and they moved, but still I only paid $25) .
I tested this cable three ways, and always the same two conductors. The first number will be the two conductors with the other two conductors open, the second number will be with the other two conductors shorted, and the third number - if any, will be with the outer jacket and shield removed and only the inner jacket covering the conductors.
Anyway the data you are all looking for. All results are per foot.
DCR = 0.0033 - 0.0033 (ohms)
RAC@100Hz = 0.0025 - 0.0022 (ohms)
RAC@120Hz = 0.0025 - 0.0022 (ohms)
RAC@1000Hz = 0.0022 - 0.0028 (ohms)
RAC@10000Hz = 0.0141 - 0.0146 (ohms)
Cp@100Hz = 45.65 - 45.4 - 31.3 (picofarads)
Cp@120Hz = 45.2 - 45.13 - 31 (picofarads)
Cp@1000Hz = 41.95 - 41.79 - 28.2 (picofarads)
Cp@10000Hz = 38.1 - 37.95 - 26.4 (picofarads)
Ls@100Hz = 0.24 - 0.259 (uH)
Ls@120Hz = 0.21 - 0.257 (uH)
Ls@1000Hz = 0.21 - 0.21 (uH)
Ls@10000Hz = 0.215 - 0.218 (uH)
Notice that I only measure the capacitance after I removed the shield. Also notice that the capacitance went way down after the shield was removed. So, is there an electrophysicist out there who can anlyze this data and explain why the capacitance droped after removing the shield when all else remained the same, and explain the minor differenced when the unused conductors were shorted oppposed to open?
I tested this cable three ways, and always the same two conductors. The first number will be the two conductors with the other two conductors open, the second number will be with the other two conductors shorted, and the third number - if any, will be with the outer jacket and shield removed and only the inner jacket covering the conductors.
Anyway the data you are all looking for. All results are per foot.
DCR = 0.0033 - 0.0033 (ohms)
RAC@100Hz = 0.0025 - 0.0022 (ohms)
RAC@120Hz = 0.0025 - 0.0022 (ohms)
RAC@1000Hz = 0.0022 - 0.0028 (ohms)
RAC@10000Hz = 0.0141 - 0.0146 (ohms)
Cp@100Hz = 45.65 - 45.4 - 31.3 (picofarads)
Cp@120Hz = 45.2 - 45.13 - 31 (picofarads)
Cp@1000Hz = 41.95 - 41.79 - 28.2 (picofarads)
Cp@10000Hz = 38.1 - 37.95 - 26.4 (picofarads)
Ls@100Hz = 0.24 - 0.259 (uH)
Ls@120Hz = 0.21 - 0.257 (uH)
Ls@1000Hz = 0.21 - 0.21 (uH)
Ls@10000Hz = 0.215 - 0.218 (uH)
Notice that I only measure the capacitance after I removed the shield. Also notice that the capacitance went way down after the shield was removed. So, is there an electrophysicist out there who can anlyze this data and explain why the capacitance droped after removing the shield when all else remained the same, and explain the minor differenced when the unused conductors were shorted oppposed to open?