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![]() "Dave" wrote in message news:q7u8j.6941$xd.2942@trndny03... "Roger" wrote in message . .. Richard Clark wrote: On Thu, 13 Dec 2007 08:40:53 -0800, Roger wrote: And just for completeness... The fundamental equations also work when: - the signal is not sinusoidal, e.g. pulse, step, square, ... - rather than a load at one end, there is a source at each end - the sources at each end produce different arbitrary functions - the arbitrary functions at each end are DC sources It is highly instructive to compute the forward and reverse voltage and current (and then power) for a line with the same DC voltage applied to each end. ...Keith ...Keith Interesting! The important thing is to get answers that agree with our experiments. I have done some computations for DC voltage applied to transmission lines. The real surprise for me came when I realized that transmission line impedance could be expressed as a function of capacitance and the wave velocity. Z0 = 1/cC where c is the velocity of the wave and C is the capacitance of the transmission line per unit length. Hi Roger, This last round has piqued my interest when we dipped into DC. Those "formulas" would lead us to a DC wave velocity? 73's Richard Clark, KB7QHC Hi Richard, Here are two links to pages that cover the derivation of the formula Zo = 1/cC and much more. http://www.speedingedge.com/PDF-File..._Impedance.pdf http://www.ece.uci.edu/docs/hspice/h...001_2-269.html Here is the way I proposed to Kevin Schmidt nearly seven years ago after seeing him use the formula on a web page: *ASSUME*: 1) An electrical wave travels at the speed of light, c 2) A 'perfect' voltage source without impedance, V 3) A 'perfect' transmission line having no resistance but uniform capacitance per unit length, C *CONDITIONS AND SOLUTION* The perfect voltage source has one terminal connected to the transmission line prior to beginning the experiment. The experiment begins by connecting the second terminal to the transmission line. The voltage source drives an electrical wave down the transmission line at the speed of light. Because of the limitation of speed, the wave travels in the shape of a square wave containing all frequencies required to create a square wave. The square wave travels down the transmission line at the speed of light (c). After time (T), the wave has traveled distance cT down the transmission line, and has charged the distributed capacity CcT of the line to voltage V over that distance. The total charge Q on the distributed capacitor is VCcT. Current (I) is expressed as charge Q per unit time. Therefore the current into the transmission line can be expressed as I = Q/T = VCcT / T = VCc Impedance (Zo) is the ratio of voltage (V) to current (I). Therefore the impedance can be expressed as Zo = V / I = V / VCc = 1/Cc We can generalize this by using the velocity of the electrical wave rather than the speed of light, which allows the formula to be applied to transmission line with velocities slower than the speed of light. Of course, only the wave front and wave end of a DC wave can be measured to have a velocity. 73, Roger, W7WKB the OBVIOUS error is that the step when the second terminal is connected DOES NOT travel down the line at c, it travels at some smaller percentage of c given by the velocity factor of the line. That IS what I said. Think of the velocity as a moving wall, with the capacitor charged behind the wall, uncharged in front of the moving wall. The second OBVIOUS error is the terminology 'DC wave'. you are measuring the propagation velocity of a step function. this is a well defined fields and waves 101 homework problem, not to be confused with the much more common 'sinusoidal stead state' solution that most other arguments on this group assume but don't understand. Be real. This experiment can be performed, and the DC switched as frequently as desired. How square the wave front will be depends upon real world factors. Go to a transmission line characteristics table and use the formula to compare Zo, capacity per length, and line velocity. It will amaze you. 73, Roger, W7WKB |
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