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On Mar 12, 1:37*pm, K7ITM wrote:
On Mar 12, 9:24*am, "JC" wrote: In a lossy coax the lost energy is, I suppose, heating up the dielectric. To try *to visualize that I stripped off 30 cm of dielectric from an old RG58 cable and put it in a 900 W 2450 MHz standard microwave oven together with a 100cc cup of water as dummy load. 2 minutes after switching on the water was boiling but the polyethylene was only slightly *warmer due to the proximity to the boiling water., Can I conclude that RG58 dielectric has no loss at 2350 MHz ? Certainly not ( it is well known that all the PE food containers used in such ovens are not heated ), but what is wrong in this test ? how does it differ from the dielectric heated in an actual operating lossy cable ? JC Others have set you straight about most of the loss being due to heating the conductors (I^2*R loss) rather than dielectric loss. *Look in the thread "Two coax as substitute for open line" thread for my posting on 25 February; it contains a formula for line loss that lets you see how the two loss mechanisms stack up as a function of impedance, frequency, conductor size and dielectric loss tangent. An interesting point to note: *If you buy line of a certain impedance and diameter, you'll note that if the line uses solid polyethylene dielectric its loss is higher than line of otherwise the same construction using foam polyethylene dielectric. *The reason for that is NOT that the foam dielectric is less lossy, but rather that the lower effective relative dielectric constant of the foam requires a larger diameter center conductor to get the same impedance, and the larger center conductor has lower loss. If you assume copper conductors and dielectric with a dissipation factor of 0.0002 (which should be close to what either polyethylene or PTFE of high quality is, up to a few GHz), you'll find that RG-213 size coax with a 0.285" outer conductor ID and solid 0.081" inner conductor (appropriate for solid polyethylene 50 ohm line) yields the following _approximate_ losses, in dB/100ft: * * * * * Total * * Copper * * Dielectric 1MHz * * *0.138 * * 0.137 * * *0.001 10MHz * * 0.437 * * 0.433 * * *0.004 100MHz * *1.383 * * 1.370 * * *0.013 200MHz * *1.957 * * 1.938 * * *0.018 500MHz * *3.094 * * 3.064 * * *0.030 1GHz * * *4.376 * * 4.334 * * *0.042 2GHz * * *6.188 * * 6.129 * * *0.059 5GHz * * *9.784 * * 9.690 * * *0.094 You can see that even at 5GHz, the dielectric loss in this particular line is quite small compared with the copper loss. *It would be appropriate to use a bit higher dielectric dissipation factor in the GHz region, but even if it's ten times as large as what I used here, the dielectric loss is less than 10% of the total, at 5GHz. *The calculation I used here is idealized, but the non-idealities tend to be unrelated to dielectric loss: *things like conductors that aren't smooth copper (braid; stranded center conductor) and small variations in impedance along the line that cause additional apparent and real losses. *It does depend on the dielectric not becoming "contaminated," but modern cable construction seems to do a good job minimizing that, if you use the cable in reasonable environments. Cheers, Tom Oh, crap. Let's try that again. I looked at the table above and it did NOT look right. Wondered why the ratio of copper to dielectric loss didn't get worse with increasing frequency. Made a mistake in the spreadsheet that calculated it. Should have spotted it before I posted it. This is probably better: Total Copper Dielectric 1MHz 0.138 0.137 0.001 10MHz 0.442 0.433 0.008 100MHz 1.454 1.370 0.084 200MHz 2.105 1.938 0.167 500MHz 3.482 3.064 0.418 1GHz 5.169 4.334 0.836 2GHz 7.800 6.129 1.671 5GHz 13.869 9.690 4.179 So the contribution of dielectric loss by the time you get to 5GHz is significant, but not dominant if the dielectric is high quality and uncontaminated. |
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