Charging a parallel plate capacitor

In summary, the conversation discusses charging parallel plate capacitors and the concept of fully charging a capacitor. It also mentions the use of a resistor in series and how it affects the charging process. The equation for calculating the potential difference across the capacitor is also mentioned. Finally, a resource for more information on charging capacitors is provided.
  • #1
al_201314
116
0
Hi guys,

I've been reading the forums and finally I have something to post :smile:

I've got a question regarding charging parallel plate capacitors. Take this for example:

Connect a 6 Volt power supply to a resistor of 2Mohm and in series with a 15uF capacitor initially uncharged, with a current of 0.0000018A flowing through.

A simple calculation would show that the P.D across the capacitor is 2.4V. The question then goes on to ask what is the new p.d across the capacitor when it is fully charged and reduced to 5uF without any loss of charges and the answer is 16.8V

I figured in order to get the answer the charges in the capacitor must be that of 6V x 15uF. My question is that how then would the capacitor gets charged up to the maximum of 6V (how would one know the max is 6V?) with the presence of the resistor?

I can't really grasp the concept here hope someone can help me out with the explanation and sorry for being so long winded can't find an easier way to put it across!

Thanks
 
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  • #2
V(capacitor) = V(source, 6 volts in this instance)*(1-e^-(t/rc)).

Theoretically, the potential difference across the capacitor will never reach the source voltage, but after a very very long time, it will be close enough that you won't be able to measure the difference anyway.

In electronics, after five or so time constants (r*c) they call it good and say the capacitor is fully charged. Plugging in the numbers, at that time the capacitor is charged up to 99 percent of the source voltage. For this particular circuit the time required would be somewhat less than three minutes.

Leave it hooked up for a day, and the difference between the source voltage and that across the capacitor is something to the order of 10^-54 or so.
 
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  • #3
Thanks for the reply Hammie... pardon me but could you elaborate on how the capacitor could charge up close to the source voltage when in this case there's a resistor in series leaving a p.d of only 2.4V across the capacitor?

Thanks!
 
  • #4
al_201314 said:
Thanks for the reply Hammie... pardon me but could you elaborate on how the capacitor could charge up close to the source voltage when in this case there's a resistor in series leaving a p.d of only 2.4V across the capacitor?

Thanks!
The current through the resistor is maximum initially, when the capacitor is uncharged and the voltage across the resistor is maximum. The current decays exponentially as the voltage on the cap increases with a decaying exponential shape. The final current through the resistor after a long time is zero, and the voltage on the capacitor equals the source voltage.

Remember that the equation for the current into a capacitor that is charging is I = C dV/dt. The higher the current, the faster the capacitor charges. Solve this equation to see the exponential equation for the capacitor voltage versus time when charged through a series resistor.
 
  • #5
Connect a 6 Volt power supply to a resistor of 2Mohm and in series with a 15uF capacitor initially uncharged, with a current of 0.0000018A flowing through.

You are correct, the voltage across the capacitor is 2.4 volts, but at a particular time. The voltage will approach six volts, at a much greater time than this.

The question then goes on:

The question then goes on to ask what is the new p.d across the capacitor WHEN IT IS FULLY CHARGED and reduced to 5uF without any loss of charges and the answer is 16.8V

before the capacitor is reduced to 5 uf, its potential difference is (or is as good as..) six volts, it is said to be fully charged.

This may be more than you want to know about charging capacitors, but look here..

http://www.ac.wwu.edu/~vawter/PhysicsNet/Topics/DC-Current/RCSeries.html
 
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  • #6
Thanks for the responses much appreciated!
 

Related to Charging a parallel plate capacitor

What is a parallel plate capacitor?

A parallel plate capacitor is a device used to store electrical charge. It consists of two metal plates separated by an insulating material, known as a dielectric. When a voltage is applied to the plates, opposite charges are stored on each plate, creating an electric field between them.

How do you charge a parallel plate capacitor?

To charge a parallel plate capacitor, you must connect it to a power source, such as a battery. The positive terminal of the power source should be connected to one plate of the capacitor, and the negative terminal to the other plate. This will create an electric field between the plates, causing one plate to become positively charged and the other to become negatively charged.

What factors affect the charging of a parallel plate capacitor?

The charging of a parallel plate capacitor is affected by several factors, including the capacitance of the capacitor, the voltage applied, and the material and distance of the dielectric between the plates. The larger the capacitance and voltage, the more charge can be stored on the capacitor, while a thinner or higher-permittivity dielectric will allow for a stronger electric field and thus more charge storage.

How does a parallel plate capacitor store charge?

A parallel plate capacitor stores charge by creating an electric field between its plates. When a voltage is applied, electrons are pushed and pulled towards the respective plates, leaving one plate with a surplus of electrons (negative charge) and the other with a deficit of electrons (positive charge). The charged plates are then separated by the dielectric, preventing the charges from neutralizing.

What is the equation for the capacitance of a parallel plate capacitor?

The capacitance (C) of a parallel plate capacitor is given by the equation C = εA/d, where ε is the permittivity of the dielectric material, A is the area of the plates, and d is the distance between the plates. This means that the capacitance is directly proportional to the area of the plates and the permittivity of the dielectric, and inversely proportional to the distance between the plates.

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