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Re: [TCML] Spark dynamics on Jacobs Ladder



Hi Matt,

Possibly, except that Peter is correct - the EM force on the electrodes is actually repulsive and not attractive since the current is flowing in opposite directions. The magnitude of the repulsion force scales with the square of the current and is inversely proportional to the wire separation:
http://theory.uwinnipeg.ca/physics/mag/node10.html

BTW, for a graphic example of what these forces (at tens - hundreds of kA) can do to substation bus bars and standoff insulators during accidental short circuits, see:

http://www.youtube.com/watch?v=2j8D_N1v0tU

It would be interesting to compare the magnitude of the magnetic versus electrostatic forces for a typical 15/30 NST to see if they are of the same magnitude... I'll look into this a bit more.

Bert

Mddeming@xxxxxxx wrote:
Hi Gary, A simple explanation, understandable by elementary school kids, is this: A wire carrying a current has an EM field around it. The two wires carrying currents in opposite directions will thus attract each other. When the spark first forms at the bottom, the two electrodes form effectively very short wires. As the spark rises, their lengths becomes effectively longer and the attraction stronger. The maximum attraction occurs when the spark is at the top. When the spark breaks at this point, the restorative force of the spring tension of the electrodes pulls them apart again and they try to oscillate at their natural frequency. If you could get the voltage, current, spark travel time, and distance just right, you would see significant resonant gain in the movement (The pushing-a-swing analogy). The college-level explanation is here: <http://en.wikipedia.org/wiki/Lorentz_force>. Hope this helps, Matt D. In a message dated 1/18/08 11:06:32 A.M. Eastern Standard Time, Gary.Lau@xxxxxx writes:

I hope this isn't viewed as too off-topic - I'll argue that the same physics apply to TC sparks ;-)

I was giving a demonstration of various HV toys to a 4th grade class yesterday. Among the devices was a Jacobs ladder, powered by a 15/30 NST. The two 1/8" x 3 ft steel electrodes appeared to have been excited into a mechanical oscillation, bouncing towards and away from each other, at very roughly ~ 1Hz. One of the students asked my why they were moving, and I had to admit that I didn't know the source of the force that was moving them.

The period of the oscillation was much faster than the arc travel time up the electrodes. It's clear that the period was that of the free-standing rods, and that the exciting force between them varies as a function of their separation, but I don't see the source of the attraction or repulsion between them. Any theories?

Thanks,
Gary Lau
MA,  USA




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