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Carl Mungan asked this:
Suppose I connect two capacitors in series across a battery. Label the four
capacitor plates from left to right as A, B, C, and D. Okay, suppose A is
connected to the positive terminal of the battery, so out goes charge +Q to
it, and compensating charge off D, leaving -Q on it. My question is: why
does the charge on B and C have to be -Q and +Q, respectively?
If the isolated circuit consisting of plates B and C and the wire between
them is initially uncharged, then the sum of the charges presumably has to
remain zero. But why couldn't I get -1.1Q and +1.1Q on these two plates,
say? Why *exactly* -/+Q? Is it always exact: what if plates A and B have
different shapes? Or what if I imagine distorting the wire between plates B
and C, so that B and C are both portions of some larger object, say the two
ends of a solid rectangular block, or even a sphere? Surely at some point
the answer will no longer be -/+Q. At what point - in other words, what
assumptions go into the usual derivation? I've looked in several textbooks
and it's presented as though -/+Q is patently obvious. Carl
...
The original questioner was interested to know why the charge at point
B and C have to be numerically equal, as quoted above.
...
What difficulty?
The difficulty of erroneously assigning equal charge on connected plates of
series caps.
...
I may have mentioned recently that I do NOT subscribe to the
orthodox ( I deliberately do not say "old-fashioned") view
that there are "natural laws" that scientists discover;
I find it much more productive to suppose that there are man-made models -
any of which may be more or less suitable to any particular case.
This has the particular virtue that when physicists comfortably think they
are dealing on a 'more-fundamental' level, I can as easily see the flaws in
their models as in any other man made elaboration.
...
Let u = [mu] = 10^(-6)
Q_1 = 30 uC (Q_A = -30 uC, Q_B = +30 uC), Q_2 = 60 uC (Q_C = +60 uC,
Q_D = -60 uC)
So you can now easily admit a case where Qb is not numerically equal to Qc
This was the crux of Carl's question, was it not?
...
It was Cockroft and Walton who defined this arrangement for a
voltage multiplier in the earliest accelerator experiments.
They were physicists as I recall.
But I don't suppose their names are known to teachers hereabouts.
(On careful deliberation, I have deleted the putative reason I offered
for this. I hope you will accept this as a tribute to your private coaching
in how to prevent public shows of sniping)