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On Mar 19, 12:00*pm, Cecil Moore wrote:
Keith Dysart wrote: I am not sure why you focus on the infinitesimally small times when "the instantaneous source power equals zero". :-) :-) That was my exact reaction when you wanted to focus on the infinitesimally small times associated with instantaneous powers. :-) :-) You are to blame for that focus, not I. It only takes one example to prove your claims wrong. Could you state the claim that you think you are proving wrong? I didn't want to focus on instantaneous power at all but you insisted. Now that your own techniques are being used to prove you wrong, you are objecting. If you wish to have your equalities apply at only selected points within the cycle, that works for me. It only fails when you make the assertion that for the circuit under consideration, the energy in the reflected wave is dissipated in the source resistor. At the time when the instantaneous source power is zero, the only other sources of energy in the entire network is reflected energy and interference energy. That's a fact of physics. You have gotten caught superposing powers, something that every sophomore EE knows not to do. Could you kindly show me where? The two expressions in which I have summed power are Ps(t) = Prs(t) + Pg(t) and Pg(t) = Pf.g(t) + Pr.g(t) You have not previously indicated that either of these are incorrect. Please take this opportunity. I repeat: The only time that power can be directly added is when there is *ZERO INTERFERENCE*. The test for zero interference is: (V1^2 + V2^2) = (V1 + V2)^2 Surely you overstate. Powers can be directly added whenever you have a system with ports adding and removing energy from the system. Conservation of energy says that the sum of the energy being stored in the system is equal to the sums of all the ins and outs at the ports. There are no conditions on the ports adding or removing energy. ...Keith |
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