Path: utzoo!utgpu!news-server.csri.toronto.edu!cs.utexas.edu!usc!zaphod.mps.ohio-state.edu!wuarchive!emory!athena.cs.uga.edu!mcovingt From: mcovingt@athena.cs.uga.edu (Michael A. Covington) Newsgroups: sci.electronics Subject: Re: 80386. Message-ID: <1991Jan16.161646.9446@athena.cs.uga.edu> Date: 16 Jan 91 16:16:46 GMT References: <1990Dec18.234020.2491@uoft02.utoledo.edu> <4400001@hpsgwp.sgp.hp.com> <1991Jan14.205104.2829526@locus.com> Organization: University of Georgia, Athens Lines: 29 In article <1991Jan14.205104.2829526@locus.com> dana@locus.com (Dana H. Myers) writes: > >Since we are assuming the power is disspated in capacitance, we'll >use the simple form of capacitive reactance: >...etc... Er... Power is not dissipated in capacitance. No such thing. Only resistance can dissipate power. Here's how CMOS dissipation works. A CMOS chip dissipates power resistively while transitioning from one state to the other, and while charging the input capacitance of another chip. (That's how capacitance got into it... the capacitance does not dissipate power, but it provides current flow through a resistance.) The time taken to make a transition, and the time taken to charge an input capacitance, are constant for any given set of chips. So is the amount of power dissipated per transition. Clock frequency is then (proportional to) number of transitions per second. I would maintain that *both* current *and* power are proportional to frequency (not the square of frequency). Odd, but plausible once you realize we are talking about varying the duty cycle, not the voltage or current. 73 de N4TMI