Skaperen said:
there is no A1-B2. i am wondering if a charged capacitor can be treated as having an electrostatic charge. not the whole capacitor, just one terminal on each (A2 and B1).
Any atomic material can carry an electrostatic charge. Each side of the capacitors you described will have charge - so there are four sides A1, A2, B1, and B2. Since these are rated at 12V, the differences between A1 and A2 will normally be no greater than 12V - and so with B1 and B2.
In my previous post, I described an "ideal" voltage meter. For the situation you have described, a meter could be made that is close enough to ideal to show the effects I will describe:
1) You charge both A and B to 9V. Since this is a 0.1F capacitors, these are actually very substantial charges. If you were to accidently drop a piece of aluminum foil across the terminals, the result would be explosive with the rapid evaporation of some of the aluminum.
2) You set both capacitors down onto a glass plate in a room with a relative humidity of 0% and measure the voltages A1-A2 and B1-B2. Both are 9V.
3) Before you make the next measurement, let's think about the charges for a moment. In the simplest case, each capacitor consists of two conducting elements. There could also be a conductive "can" holding them, and to keep things simple, we will presume that the "can" is connected to the terminal 1. Each of those two elements has some charge value which represents the number of excess or deficient electrons. As these two capacitors sit on the glass plate, there is a can-to-can (A1-B1) capacitance. But this is such a small capacitance (I said 1 fF earlier) that your typical meter would be unable to measure it.
4) So now you pull out your specially engineered voltmeter. This is a very high-impedance, low-capacitance device and is therefore very susceptible to ESD damage. You would probably need about 30 minutes of study to get good readings from it without destroying it. We will give it a voltage rating of 2KV. When you connect it from A1 to B2, it reads 9V. Between B1 and A2, it also reads 9V. Any normal meter would read 0V - but normal meters act as conductors across such trite charges.
5) You momentarily allow B1 to come into contact with a sweater which immediately draws some electrons away from it.
6) Your take new readings: A1 to A2: still 9V; B1 to B2: still 9V; A1 to B1: 1000V; A1 to B2: 1009V; A2 to B1: 991V.
7) Now you move one of the capacitors to a new location on the glass plate. You have not changed the charge, but the capacitance is down to 0.2fF.
8) You repeat the measurements and destroy your meter in the process. (ooops)