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I've been finding a lot of popular press coverage distressing. Maybe I should keep some sort of journal of my specific objections.

Here are a couple of bad habits which come to mind:

I got to celebrate the new year in Massachusetts with Eric and Kate, for what I think was my eighth straight year celebrating with Eric. I also saw a bunch of cool people whom I rarely see except at Eric's new year's party, and got a visit from Rachel and Vasilios, who graciously drove for hours and hours.

I did a countdown program in Python, using Tkinter. It's normally done with HyperCard, but Eric couldn't get HyperCard running right away, so I tried out Tkinter. I have to admit that I don't know an enormous amount of Tkinter, but it's pretty straightforward to get started with it. The most difficult part is probably the geometry management and packing stuff.

We thought we might be able to get the countdown to start a fire (as we'd hoped in previous years) -- lighting a candle, for example. Unfortunately, I couldn't get my solid-state relay to trigger from my laptop's parallel port, and I didn't have a voltmeter or LEDs or anything else to use for debugging purposes. So the computer control was out this year. We did try an experiment later on to see about the possibility of igniting something with electricity. Our experimental result is this: if you connect eight 9-volt batteries in series (which is very easy to do because of how the connectors are designed), a fairly large spark is produced by the 72-volt potential across the resulting gap when battery leads are brought close together. This spark is sufficient to ignite a small piece of cardboard wetted with 91% isopropyl alcohol.

A much simpler technique would be to get a thin wire like those used in cigarette lighters in cars, and connect this to a relatively small DC voltage. The wire should become hot enough to ignite things (like cigarettes). There is some detail about matching the internal resistance of the power source in order to maximize the power dissipated through the wire.

The theory here is pretty simple. Suppose that we want to cause heat by connecting a wire in series with a battery. Assume that the battery's total voltage is V, and the internal resistance of this source is Rs, the resistance of the wire is Rw. Then the total series resistance is Rs+Rw, current I=V/(Rs+Rw), power in the wire Pw=I*Vw=V^2*Rw/(Rs+Rw)^2. I did take dPw/dRw by hand (I'm ashamed to say it's the first derivative I've taken in a year or two), and found it to be V^2[(Rs+Rw)^2-2Rw(Rs+Rw)]/(Rs+Rw)^2, which has a zero when Rs=Rw. This implies that the wire will become hot most quickly when its resistance is exactly equal to the internal resistance of the battery.

(In that case, of course, the battery will also dissipate power at the same rate as the wire, so the battery may become rather hot as well.)

There's a much more general result, or technique, known to electrical engineers, and it's called impedance matching. I never got far into alternating currents in my physics class, so I didn't learn too much detail about impedances.

I'm glad I got to be here for the new year. I'll be back in California soon.

Happy new year!


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Contact: Seth David Schoen