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#1
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| Hi What would be an appropriate figure for the speed of an electrical signal? If there is no constant one, what factors does it depend on (how long would it take a signal to go through a 1 km cable). Danny |
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#2
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| "Danny" <[Only registered users see links. ]> wrote in message news:BZELb.493$[Only registered users see links. ].net... Through a continuous cable with no junctions you can normally expect something of the order of 0.5c. For 1km of cable this gives a transit time of 6.7 microseconds or so. If you have a continuous spectrum of frequencies there will be some dispersion where the speed is frequency-dependent, the main effect of which will be to smooth out sharp edges in the signal. The math is quite complex, depending on cable geometry as well as proximity to other cables and conducting surfaces. -- Paul V. S. Townsend Interchange the alphabetic elements to reply |
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#3
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| "Danny" <[Only registered users see links. ]> wrote in message news:BZELb.493$[Only registered users see links. ].net... There are *two* different answers to that question, and which one is correct depends on what you are *thinking of* when you use the word "electricity." There is an analogy here that may help - air. The speed of sound (mechanical energy) in air is pretty fast - about 300 m/second, and it depends on the temperature of the air, the humidity, and several other things. The speed of the individual molecules in air depends on the weight of the molecule and the air pressure and temperature, varies over a broad range, and the average is 1400 m/sec for oxygen (molecular weight 32) at 25° C and 1 atm. The speed of the bulk movement of air ("wind") is variable and typically runs less than 10% of the speed of sound. If you think of "electricity" as the movement of *electrical energy* through the wire, then it is pretty fast - equal to the speed of light c divided by the index of refraction n(f) of the metal for waves *of that particular frequency f* - the index of refraction is frequency-dependent. For example, the value of n(0) is 3.16 for lithium, which gives us a speed of about c/n(0) = 95,000 km/sec for electricity in lithium - a significant fraction of the speed of light. Theoretical arguments set the velocity of *the bulk motion of electrons* (electron wind) at much lower speeds (meters per second), but measuring those speeds is very difficult: [Only registered users see links. ] OTOH, the motion of "individual electrons" (treated as particles like the molecules in air, which itself is problematical) is typically much higher, but not as fast as the motion of electrical energy: [Only registered users see links. ] For more information on electrical current see the following: [Only registered users see links. ] Tom Davidson Richmond, VA |
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#4
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| Hi Another thing i was thinking, what if i remove the signal source before the signal has reached the end of the line, will the signal carry on to the end, or will it just stop dead and never reach the end? Danny tadchem wrote: |
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#5
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| "Danny" <[Only registered users see links. ]> wrote in message news:2RQLb.74$[Only registered users see links. ].net... That will depend on what's at the end of the line. Suppose the line simply ends in mid-air with an open circuit. Now there can be no current through an open circuit, and what will happen is that the signal will be "reflected" by the open-circuit, with reversed current (so that the currents of the original signal and its reflection cancel). This reflection will travel back up the line, possibly interfering with following signals or, if the other end of the line is also an open-circuit, bouncing back and being seen as another signal. The other extreme type of termination (equally bad) is a short-circuit. Here it's the voltage that has to be zero, so again there will be a reflection, this time with reversed voltage. The ideal termination is somewhere in between. The ideal cable is one that is infinitely long, so it never reaches any termination and the question does not arise. In practice, the cable characteristics can be analysed (again, the math is quite complicated) and the final result is that an infinite length of cable would appear as a pure electrical resistance, the precise value depending on cable geometry and (to a lesser extent) signal frequency. The resistance value is usually referred to as the "characteristic impedance" of the cable. The important point is that the math works both ways. An infinite length of cable looks like a particular electrical resistance. A particular electrical resistance looks like an infinite length of cable. If the cable is terminated with its own characteristic impedance, there will be no signal bounce - the termination absorbs both the voltage and the current perfectly as though the cable were infinitely long. -- Paul V. S. Townsend Interchange the alphabetic elements to reply |
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#6
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#7
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| "Danny" <[Only registered users see links. ]> wrote in message news:2RQLb.74$[Only registered users see links. ].net... If you fire a gun and put it back into the holster before the bullet gets to the target, will the bullet *continue* towards the target after the gun has been holstered? Tom Davidson Richmond, VA |
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#8
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| "Prai Jei" <[Only registered users see links. ].uk> wrote in message news:btop8e$ih8$[Only registered users see links. ].pol.co.uk... <snip> can following Please review your alternating current (AC) theory. A capacitor/condensor is an open circuit. It carries AC and transients quite well, but it has a high impedance to direct currents (DC). Danny's signal is a transient. It will continue quite well. Tom Davidson Richmond, VA |
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| electricity , speed |
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