Modeling conservation of charge

In summary, a group of physics students designed an experiment to test the model of conservation of charge. They charged a capacitor (C1 = 5600 micro F) with a voltage of 10 volts. Then they added a second capacitor (C2 = 1400 micro F) in the circuit and measured the voltage across C1 (2 volts). They also calculated the charges on the capacitors and concluded that charge is conserved if q_0 = q_1 + q_2. However, the correct answer is that all the charges are equal (q_0 = q_1 = q_2) and the charge on the system decreases as the capacitance decreases when capacitors are connected in series. The students also
  • #1
SparkimusPrime
35
0
A group of physics students designed the following experiment to test the model of conservation of charge.

a) They first charged a capacitor C1 = 5600 micro F by applying a voltage V_0 = 10 volts (as shown in attachment Exam 2 - Problem 2 - Part a.JPG)

b) Then the connected a second capacitor of C2 = 1400 micro F in the circuit (as shown in Exam 2 - Problem 2 - Part b.JPG). They measured the voltage across C1 using a voltmeter. The reading of V_1 = 2 volts.

c) Then they calculated charge q_0 in the capacitor C1 in the circuit in part a and charges q_1 and q_2 in part b. Finally, they tried to compare the value of q_0 with the value of q_1 + q_2. They concluded that charge is conserved if q_0 = q_1 + q_2. Otherwise charge is not conserved.

The correct answer is supposed to be that all the charges are equal (q_0 = q_1 = q_2). But I get answers agreeing with the assessment of the experiment:

q_0 = C1 * V_0 = (10) * (5600) = 5.6e4 micro C

As shown in the figure, the total capacitance of the system decreases, because the capacitors are placed in series:

1 / C_total = 1 / C_1 + 1 / C_2
C_total = 1120 micro F

So the charge on the system should be decreased similarly (as the electric force between the plates decreases so too should the charge on the individual capacitors and thus the system). So it seems to me, by inspection that there should by such a relationship as expressed in the experiment.

If the voltage across C1 (in part b) is 2 volts, the charge on that capacitor should be:

C1 * V_1 = (5600)*(2) = 11200 micro C

Clearly less than the original charge. Of course this may be where my error occurs, I'm taking the charge across a single capacitor in a series, can I treat it as if it were alone or do I have to consider the entire system?

Also as an aside, I don't think the LaTeX system is working correctly. I tried to denote some Greek symbols (mu and delta) via latex and it showed some very strange behavior:

\mu
This would work correctly as long as it was at the top of the post.

\Delta
This would work correctly as long as there was another latex symbol that wasn't a delta above it. Otherwise it would display as a mu.

Subscripts simply wouldn't work at all. V_0 for example is supposed to display a V subscript 0, but it displayed nothing.

The code was gleaned from this site

Edit:

Apparently I can't attach more than one image, nor can I attach an image after I've removed it. I'll reply to this thread with the appropriate images.
 
Last edited:
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  • #2
part a:
 

Attachments

  • exam 2 - problem 2 - part a.jpg
    exam 2 - problem 2 - part a.jpg
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  • #3
part b:

Edit:

If someone knows how to do this more elegantly please, enlighten me.
 

Attachments

  • exam 2 - problem 2 - part b.jpg
    exam 2 - problem 2 - part b.jpg
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  • #4
It's been a while since I studied capacitors, but I'll give this a shot.

The correct answer is supposed to be that all the charges are equal ([tex]q_0 = q_1 = q_2[/tex])
Are you sure this is the correct answer? It's obvious that [tex]q_1 = q_2[/tex] but I don't think it also equals the charge of the first capacitor when it was alone.

Ignoring for a minute that the number of capacitors changes, let's just look at the total capacity of the system as a whole in the two case. In (a) the capacity of the system is:
[tex]C_a = C_1[/tex]
In (b) the capacity is of two capacitors connected in series, i.e:
[tex]C_b = \frac{1}{\frac{1}{C_1} + \frac{1}{C_2}}[/tex]

It's easy to see that [tex]C_a > C_b[/tex]. Since the voltage in both cases is equal [tex]V_a = V_b[/tex], and [tex]q = VC[/tex], the charge must change and [tex]q_a > q_b[/tex]. So the charge quantity on the capacitors does change. In words, the voltage stays the same but the capacity of the system changes, and therefore the charge quantity has to change.
 
  • #5
It's easy to see that . Since the voltage in both cases is equal , and , the charge must change and . So the charge quantity on the capacitors does change. In words, the voltage stays the same but the capacity of the system changes, and therefore the charge quantity has to change.

Yes, it seems to me that this should be the answer. Maybe it is a misprint, all the evidence seems to point that way.

Calculating the charges on the two capacitors:

Q_1 = C1 * V_1 = 5600*2 = 11200
Q_2 = C2 * V_1 = 1400*8 = 11200

It seems that the charges on the capacitors are equal, but that they don't equal the total charge on the system with just one capacitor (part a). Almost half as much charge on the system in part b as in part a, which jives with my intuition about the capacitence and therefore the charge decreasing. Have I missed anything?
 
  • #6
Argh, I am so stupid.

When talking about capacitors, we are not talking about the total charge of them. We are talking about the charge they hold in one of their plates. On one plate they hold +q charge, and on the other plate they have -q charge. So in total... they have no charge at all. :smile: So there is no conflict with the preservation of charge, it is just divided differently.
 
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  • #7
When talking about capacitors, we are not talking about the total charge of them. We are talking about the charge they hold in one of their plates. On one plate they hold +q charge, and on the other plate they have -q charge. So in total... they have no charge at all.

I know there is charge present on each plate of a capacitor, as they store charge (by definition). The charges are equal and opposite and it is the electric forces generated by that charge that allows said charge to be stored. Taken as a system and preserving the signs, yes there is no net charge on the capacitor, given that it has reached electrostatic equilibrium.

So there is no conflict with the preservation of charge, it is just divided differently.

So is my conclusion correct?

Peter
 
  • #8
What is your conclusion? If it is what you posted in the last post then yes, it is correct.
 

1. What is the conservation of charge?

The conservation of charge is a fundamental principle in physics that states that the total electric charge in a closed system remains constant over time. This means that charge cannot be created or destroyed, but can only be transferred from one object to another.

2. How is the conservation of charge modeled?

The conservation of charge is typically modeled using mathematical equations, such as the continuity equation and the Gauss's law, which describe the flow and distribution of charge in a system. These equations help to explain and predict the behavior of electric charge in various situations.

3. Why is the conservation of charge important?

The conservation of charge is important because it is a fundamental law of nature that governs the behavior of electric charge. It allows us to understand and predict the behavior of electrically charged particles and their interactions, and has many practical applications in fields such as electronics, engineering, and chemistry.

4. Can the conservation of charge be violated?

No, the conservation of charge is a fundamental law of nature and has been rigorously tested and proven to hold true in all known physical systems. Any apparent violation of this law is usually due to errors in measurement or incomplete understanding of the system.

5. How does the conservation of charge relate to other conservation laws?

The conservation of charge is closely related to other conservation laws, such as the conservation of energy and the conservation of momentum. These laws are all based on the principle of conservation, which states that certain physical quantities cannot be created or destroyed, but can only be transferred or converted into other forms.

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