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I agree equivalent circuits are invalid when it comes to calculating either
efficiency or internal power loss. The circuit in my example was the ACTUAL circuit, i.e., a 10 volt source with a series 50 ohm resistor, not a Thevenin nor a Norton equivalent. With this restriction, I don't see anything wrong with my statement. Depending on what the ACTUAL circuit is in a power amplifier, I believe the current drawn can either increase of decrease when the load is removed. Ron W5DXP wrote: Ron wrote: It helps me understand reflected power to think of a 50 ohm source of 10 volts connected to a half wave lossless line. In this situation the line can be removed from the equation and the load can be considered connected directly to the 50 ohm 10 volt source. If the load R is either a short or open circuit, there will be zero power transferred to the load, but there will be a big difference in the power dissipated in the source, two watts with the short and zero watts with the open. Not with a Norton source. :-) Quoting _Fields_and_Waves_in_Communication_ Electronics_, by Ramo, Whinnery, & Van Duzer, page 721: "It must be emphasized, as in any Thevenin equivalent circuit, that the equivalent circuit was derived to tell what happens in the *LOAD* under different load conditions, and significance cannot be automatically attached to a calculation of power loss in the internal impedance of the equivalent circuit." Seems your above assertion violates that sage admonition. |
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