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#1
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Reg Edwards wrote:
The condition for which Zo of a transmission line is always purely resistive (Zo = Ro) is extremely simple. It is - G = C * R / L Wonder why Ramo and Whinnery say that's an approximation for low-loss lines? If the R+jwL angle is equal to the G+jwC angle, doesn't that make Z0 purely resistive? -- 73, Cecil http://www.qsl.net/w5dxp |
#2
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Cecil,
Try it. I believe you will find that your equality requirement on angles reduces to precisely the simple equation offer by Reg. 73, Gene W4SZ Cecil Moore wrote: Reg Edwards wrote: The condition for which Zo of a transmission line is always purely resistive (Zo = Ro) is extremely simple. It is - G = C * R / L Wonder why Ramo and Whinnery say that's an approximation for low-loss lines? If the R+jwL angle is equal to the G+jwC angle, doesn't that make Z0 purely resistive? -- 73, Cecil http://www.qsl.net/w5dxp |
#3
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Gene Fuller wrote:
Try it. I believe you will find that your equality requirement on angles reduces to precisely the simple equation offer by Reg. Exactly! That's why I wonder why Ramo and Whinnery said it's an approximation. Wonder why Ramo and Whinnery say that's an approximation for low-loss lines? If the R+jwL angle is equal to the G+jwC angle, doesn't that make Z0 purely resistive? -- 73, Cecil http://www.qsl.net/w5dxp |
#4
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Cecil,
They were undoubtedly confused by their models, and they could not deal with reality. 73, Gene W4SZ Cecil Moore wrote: Gene Fuller wrote: Try it. I believe you will find that your equality requirement on angles reduces to precisely the simple equation offer by Reg. Exactly! That's why I wonder why Ramo and Whinnery said it's an approximation. Wonder why Ramo and Whinnery say that's an approximation for low-loss lines? If the R+jwL angle is equal to the G+jwC angle, doesn't that make Z0 purely resistive? -- 73, Cecil http://www.qsl.net/w5dxp |
#5
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Gene Fuller wrote:
They were undoubtedly confused by their models, and they could not deal with reality. Thanks Gene, I really appreciate it when you contribute something techincal. -- 73, Cecil http://www.qsl.net/w5dxp |
#6
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![]() Gene Fuller wrote: Cecil, They were undoubtedly confused by their models, and they could not deal with reality. 73, Gene W4SZ I guess one could infer that that if G / C R / L, and R + jwL G + jwC, then perhaps there are losses. I would only add that there are probably also small currents in shunt distributed along the line. 73, ac6xg Cecil Moore wrote: Gene Fuller wrote: Try it. I believe you will find that your equality requirement on angles reduces to precisely the simple equation offer by Reg. Exactly! That's why I wonder why Ramo and Whinnery said it's an approximation. Wonder why Ramo and Whinnery say that's an approximation for low-loss lines? If the R+jwL angle is equal to the G+jwC angle, doesn't that make Z0 purely resistive? -- 73, Cecil http://www.qsl.net/w5dxp |
#7
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Jim Kelley wrote:
I guess one could infer that that if G / C R / L, and R + jwL G + jwC, then perhaps there are losses. I would only add that there are probably also small currents in shunt distributed along the line. If R 0 and G 0, then there are losses. The only time a line is lossless is when R = G = 0 which, according to Reg, is only in my wet dreams about circles on Smith Charts. :-) For real world transmission lines at HF, (usually) R/Z0 G*Z0. When I was a member of the high speed cable group at Intel, I remember test leads designed for R/Z0=G*Z0 but they were expensive special order devices. We apparently are more successful at designing very good dielectrics than in finding an economically feasible conductor with a couple of magnitudes less resistance than copper. Thus our ordinary transmission lines have a lot more series resistance than shunt conductance, especially open-wire transmission lines in free space. :-) -- 73, Cecil http://www.qsl.net/w5dxp |
#8
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Cecil,
Do you s'pose that if the equality is perfect for zero-loss lines then maybe it is an useful approximation for low-loss lines? Do you really think R&W were proposing that this simple relationship is more appropriate for low loss lines than for zero loss lines? 73, Gene W4SZ Cecil Moore wrote: Gene Fuller wrote: Try it. I believe you will find that your equality requirement on angles reduces to precisely the simple equation offer by Reg. Exactly! That's why I wonder why Ramo and Whinnery said it's an approximation. Wonder why Ramo and Whinnery say that's an approximation for low-loss lines? If the R+jwL angle is equal to the G+jwC angle, doesn't that make Z0 purely resistive? -- 73, Cecil http://www.qsl.net/w5dxp |
#9
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Gene Fuller wrote:
Do you s'pose that if the equality is perfect for zero-loss lines then maybe it is an useful approximation for low-loss lines? Do you really think R&W were proposing that this simple relationship is more appropriate for low loss lines than for zero loss lines? Nope, exactly the opposite. Apparently, they were proposing that this simple relationship doesn't hold for highly lossy lines. Chipman also has something to say about highly lossy lines. -- 73, Cecil http://www.qsl.net/w5dxp |
#10
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![]() Who the heck are Ramo and Whinnery. Never heard of them! Presumably, because you refer to them, they are or were people who make or made a living out of re-iterating old wive's tales in book-form. It was obvious I introduced G = C * R / L simply to show that a line's Zo can be purely resistive even when it is NOT lossless. It can have any loss you like. Apparently you have not yet grasped the idea. And, despite what R and W or YOU may have to say on the subject, it is an exact expression at all frequencies from DC to almost infinity. My only references are Ohm, Ampere and Volta who I'm sure you have heard of. But no hard feelings. ;o) Tonight I'm on Chilean, dry, 2004, MontGras, Reserve Chardonnay. I didn't choose it myself. My loving daughter does my shopping. But it's quite a pleasant, refreshing plonk. ---- Regards, Reg. ============================================ "Cecil Moore" wrote Reg Edwards wrote: The condition for which Zo of a transmission line is always purely resistive (Zo = Ro) is extremely simple. It is - G = C * R / L Wonder why Ramo and Whinnery say that's an approximation for low-loss lines? If the R+jwL angle is equal to the G+jwC angle, doesn't that make Z0 purely resistive? -- 73, Cecil |