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Re: Capacitor energy experiment



Once again, I'm lost.

It seems to me that the real issue is how we define work.
Now we've gotten into a discussion about where the energy
goes when we charge a capacitor. These are two separate
issues, it seems to me.

Let's suppose that the energy associated with the capacitor
is QV (or Q^2/C, from the definition of C=Q/V). Capacitor
A has charge Q. It is then connected to capacitor B with
the same capacitance C. The charge Q is split between
the two capacitors. What is the energy associated with
capacitors A and B after being connected? Feel free to
assume steady-state, oscillations, etc., whatever you'd like.

Is the energy after being connected the same as that before
being connected? Does it depend upon the assumption of
steady-state, oscillations, etc.?

Finally, do we get a different answer if we assume the
energy associated with the capacitor is 0.5QV instead
of QV?

____________________________________________
Robert Cohen; rcohen@po-box.esu.edu; 570-422-3428; http://www.esu.edu/~bbq
Physics, East Stroudsburg Univ., E. Stroudsburg, PA 18301

-----Original Message-----
From: David Rutherford [mailto:drutherford@SOFTCOM.NET]
Sent: Wednesday, February 05, 2003 6:40 PM
To: PHYS-L@lists.nau.edu
Subject: Re: Capacitor energy experiment


Ludwik Kowalski wrote:

My description of the experiment with the air capacitor
was not complete. There should be an electronic switch
so that charging is done in a different loop that discharging.
The electronic switch would perform the same function as
a mechanical switch but much more rapidly, for example,
every 0.1 ms. Then the calorimeter would measure the
"amount of heat" generated in N discharges, each
delivering only 0.5*C*V^2 of thermal energy.

The point of my experiment is to show that for Ec ~ 0, that is for the
energy Ec << 1/2 CV^2 dissipated while charging the capacitor, the
thermal energy dissipated while discharging the capacitor will be Ed ~
CV^2. For Ec = 0, I predict that you would get Ed = CV^2, not 1/2
CV^2, as predicted conventionally, therefore the energy stored on the
capacitor after charging and before discharging would be CV^2, not 1/2
CV^2, as predicted conventionally. That would disprove one of the most
basic laws of physics - the energy of a distribution of charges.

Unless I'm mistaken, the experiment you're describing is old hat.
There's nothing new to be discovered doing the experiment your way. If
I'm incorrect in assuming that your way is the same old thing, please
explain to me why it's not.