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To further my understanding of what happens when 2 circuits have a common ground could someone please explain what happens when the following 2 circuits (charged capacitor, high resistance load) :

no common ground

share a common ground

common ground

What happens to the 2 voltages and capacitor plate potentials ?

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4 Answers 4

up vote 2 down vote accepted

What Wouter van Ooijen said, but also the bottom halves of the two circuits are guaranteed to be at the same potential. You seem to be wondering why anyone would ever care about this.

To demonstrate why this important, go find a stereo or something with an audio plug coming out of it like you'd plug into an iPod or such. Turn up the volume just a bit, and touch just the tip of the connector. Hear that buzz? It's because your body is picking up all sorts of electrical fields from the electronics in your house and nature. These are at different potentials from the stereo, and it amplifies them as sound and you can hear it.

Now, touch all the parts on the plug. Squeeze so you get a good connection. The buzz is gone! Why? Because now you have a common ground. All those fields are still there, but now your body and the stereo are at the same potential, so there's no difference between you and the radio, so you don't hear anything. (Or not as much, anyway. The connection isn't infinitely conductive, so you will still hear something, if you turn the volume up more.)

So, your stereo amplifies the voltage difference between its idea of "ground" and the left and right channels on the connector. But if something (your body, an iPod, whatever) isn't connected to the stereo's ground, then the stereo will be amplifying the voltage output by the iPod and also the difference in ground between the iPod and the stereo, which is likely some crazy random noise and 60/50 Hz hum from powerlines. Giving the two a common ground reduces this difference to nearly zero, so that the two circuits can have a common reference, so they can agree what "4V" means.

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Initially the bottom halves are not at the same potential and then when they are connected they are at the same potential. So something has changed. So what are the new plate charges and capacitor voltages ? –  Funky Oordvork Jan 14 '13 at 21:27
    
@FunkyOordvork: there are only relative voltages, not absolute ones. The voltage difference between the leads of each capacitor will be unchanged. In your second schematic, I can also tell you that the voltage difference between the bottom leads of either capacitor is 0V, but in the first all I can't know. One would say they are "floating" relative to each other. They could be the same, or they could be 100V apart. We don't know, and the circuit doesn't care. –  Phil Frost Jan 14 '13 at 21:33

For the (somewhat theoretical) case you show nothing different from the not-connected case will happen, in fact nothing CAN happen because there is no (additional) closed current path.

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So will there be no movement of charge between the 2 lower capacitor plates when they are connected ? Does the fact that they have different charges (initially) not create a voltage between the lower plates ? –  Funky Oordvork Jan 14 '13 at 21:17
    
@FunkyOordvork it can't because there's nowhere it could flow. I think you should give Bill Beaty's article a read. –  Phil Frost Jan 14 '13 at 21:21
    
Okay, I just imagined what would happen if I connected 2 'water spheres' where one had its rubber plate bent twice as much as the other. Thanks Phil / Bill ! –  Funky Oordvork Jan 14 '13 at 21:51
    
Funky: unconnected capacitors have not water balloon equivalent. The capacitor equivalent of your water balloon picture would have (for instance) one side of each capacitor grounded in the first place. –  Wouter van Ooijen Jan 14 '13 at 22:08
    
Wouter: My first diagram corresponds to 2 unconnected "water spheres" where one has its rubber plate bent twice as much as the other (double the voltage). You can complete the circuit with a very thin hose (high resistance load) in both cases. –  Funky Oordvork Jan 14 '13 at 22:43

Enough electrons will flow between newly-connected plates to bring them to the same potential. From a practical perspective, though, unless something else not shown on the schematic behaves as a significant capacitance connection between the two halves of the circuit, however, the number of electrons that will have to flow to equalize the potentials will be really, really small. Really, really, really, really small.

Think of the voltage at any given point as relating to its willingness to accept or donate electrons; if two points have the same voltage, electrons will have no particular desire to favor one direction or the other. If one point has a higher voltage, electrons will prefer moving in that direction to moving in the reverse. The higher the difference in voltages, the greater the preference.

If an electron arrives on either one of a capacitor's plate, it will make every part of the capacitor be much less accepting of electrons (i.e. decrease its voltage). Conversely, every time an electron leaves one of the plates, it will make every part be much more accepting of electrons (increase the voltage). Note that if many more capacitors enter an electron than leave, both plates will have a very large negative voltage, such that electrons will jump at the opportunity to leave.

What is significant about a capacitor is that when an electron enters one plate, it causes that opposite plate's voltage to decrease slightly less than that of the plate receiving the electron. Consequently, if the balance of electrons entering one plate exceeds that of the other, the plate which receives excess electrons will start to have a more negative voltage than the plate which doesn't, but the amount of imbalance between the two plates that is required to achieve that vastly exceeds the imbalance of electrons entering or leaving the device as a whole which would be required to change both plates' voltage by that amount.

Thus, unless there is some effective capacitance or other connection between the left and right sides, the number of electrons that might have to flow between the two sides to balance out their voltages would be vanishingly insignificant.

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Next to nothing happens because the connection you have made does not create a circuit, and so current will not flow through it, except to equalize any differences caused by static electricity buildup. Static electricity buildup will appear on both plates of the capacitor: it's an excess or deficiency of electrons in the circuit as a whole. That exchange will not change the charges on the capacitors. Neither capacitor can discharge via the connection to the opposite circuit because that connection isn't a complete circuit.

What the connection means is that the two circuits now share a common reference voltage. Thus now it is meaningful to answer questions like "what is the potential difference between the top of the left resistor and the top of the right resistor".

If you add one more connection bridging the two, then you have a complete circuit. Some current can then flow through one connection and, of course, an opposite and equal current will return through the other.

A "common ground" serves this purpose: to return the currents exchanged by the other connections. It is not a true ground in the earth sense; only a common return that is called "ground" out of hubris.

Which connection is "ground" is just a convention (but of course there are design reasons for choosing a particular connection, rather than choosing arbitrarily!). We assert that the voltage on that network is 0V, and then other voltages are referenced to that.

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