Wednesday, January 30, 2013
  Why Ohm met resistance

Polistra is always cheering for traditional and human-scale measurements. She wanted to find out: Was there ever a set of natural measurements for electricity? Was there ever an English unit of potential or an American unit of resistance? Or did the original experimenters jam everything into the metric prison from the start?

The answer: Well, sort of. Briefly. In the early days of telegraphy, resistance was often measured in terms of length and width of a standard wire, and different nations had different standards. But this didn't last long, and the volt, ampere and ohm were quickly adopted as universal.

Polistra admits reluctantly that this situation makes sense. Food, farmland and fabric were used and measured systematically for thousands of years before theoreticians came along. Electricity was first used and measured by theoreticians and later passed into common use.

While looking for the nonexistent tradition, an interesting forgotten story popped out. Back in 1827, Georg Ohm developed the math of circuits correctly by using an incorrect analogy. Other 'electricians' had already reached a correct understanding of positive and negative charges; Ohm ignored this understanding and used the transmission of heat instead. Because of his incorrect analogy, his correct math was not accepted by the other scientists for many years. Alfred Mayer, writing in 1890, said:
Ohm was led to the conception of this law by assuming that the flow of electricity in a voltaic circuit is similar to the flow of heat by conduction in a rod. Also, his assumptions that the actions of two electrified particles are directly as their distance, and that the electricity is uniformly dense over each cross section of a conducting wire, were directly opposed to the laws and facts well established by Coulomb for statical electricity.

Damned theoreticians. Always the same. Always ignoring truth if it doesn't fit the latest theory.

Ohm assumed that charge was handed off step by step between the 'particles' in the wire, just as the molecular agitation of heat is handed off from one molecule to another. This led him to view resistance as a sort of velocity measurement:
That is to say, both elements reciprocally change their electric state as long as a difference continues to exist between their electroscopic forces; but this change ceases as soon as they have both attained the same electroscopic force. ... The motion is effected in most bodies so rapidly that we are seldom able to determine its changes at the various places, and on that account we are not in a condition to discover by observation the law according to which they act.

If he was observing any delay using the instruments then available, he was probably seeing the result of inductive reactance in a long coil or wire, rather than simple resistance. A low-pass RL filter can easily take a perceptible amount of time to reach full flow.

Why did Ohm's bad assumption work? Probably because it wasn't all that bad! I spent much of my life playing and working with electrical stuff: repairing, designing, building, teaching. I used Ohm and his variants and corollaries daily. I always started with the analogy of airflow or waterflow**, in which the electrons pass between the atoms of the metal at a finite speed, while the charge field acts instantly across space. In the end it doesn't matter which of these concepts is treated as a finite velocity.

Polistra and Happystar try to see Ohm's original view, using a couple of experiments.


First Polistra shows heat conduction in a rod. She puts the rod onto a 'potential difference' between cold and hot, and watches the different molecular agitations transfer at a finite speed, until the rod is at a uniform temperature.


Now Happystar applies the same concept to a (non-factual!) electric circuit, perhaps as Ohm imagined it. Using an Edison iron-nickel battery to create a potential difference, he drops a wire onto the negative end to complete the circuit. The charges transfer at a finite speed toward the center of the resistive load, until the load is at a uniform current.



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Footnote 1: **Airflow and waterflow: See my AUDIN courseware, lesson 201, for an example. Also, the battery, pulsing wires and 'resistive block' are available in my ShareCG page.


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Footnote 2: The preface to Ohm's little book nabbed my sympathy instantly:
I herewith present to the public a theory of galvanic electricity ... and shall arrange more such portions together into a whole, if this first essay shall in some degree repay the sacrifices it has cost me. The circumstances in which I have been placed have not been adapted ... to encourage me in the pursuit of novelties. I have therefore chosen for my first attempt a portion in which I have the least to [fear from] competition.

Ah, I understand only too well. I've been there too many times. My 'donate finger' got itchy, and I looked around for Georg's Paypal button ... until I realized that old Georg was probably not online right now.

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Footnote 3: Watching the movement of the red and blue in Happystar's resistive load block, my eyes catch an odd illusion. The block seems to be sagging on top and bulging on the side, but only near the right end. (Roughly under Happystar's left leg.) I guarantee there's no bulging in the digital graphics. The shape of the block is not touched by anything in the animation. No mesh adjustments, no displacement maps. Only the color gradients change, and they change symmetrically. So where does this off-center bulge come from?


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Much later update: It turns out that Georg's analogy was right.

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