Question on capacitors in an RC circuit

AI Thread Summary
In an RC circuit with initially uncharged capacitors, they behave like wires, leading to confusion about potential at points a and b when the circuit is powered. When a 24V source is applied with the switch open, current flows, and the capacitors start charging, resulting in a measurable potential at those points. If a resistor is placed directly after the battery, the voltage drop across this resistor affects the remaining voltage available for the circuit. The potential at points a and b can be determined by measuring the voltage across the resistor and capacitor, considering the voltage drop from the resistor. Understanding these dynamics clarifies the behavior of the circuit during initial charging.
BlueCerealBox
Messages
4
Reaction score
0

Homework Statement


All information is given in the picture posted

Homework Equations


V=IR , Q=CV

The Attempt at a Solution


What I don't understand is , when the capacitors are initially uncharged , they should just be treated as wires , if this is the case , then the entire circuit is shorted. So why would there be a potential at points a and b?
 

Attachments

  • Capacitors.jpg
    Capacitors.jpg
    49 KB · Views: 421
Physics news on Phys.org
So why would there be a potential at points a and b?

Assume for a moment that the ##24V## source is shorted to zero (put a wire there) and the switch is open. So all you have is a circuit with some components and nothing going on. There is no potential at any point, and no current to be measured at all. This is reasonable because we have no power supply yet.

Now suppose we apply the ##24V## source to the circuit with the switch open. Immediately, current will begin to flow through the circuit and the capacitors will begin charging up. This implies ##V = IR \neq 0## and ##V = \frac{q}{C} \neq 0##. So we can deduce there must be a potential at points ##a## and ##b##. In fact, because the resistors and capacitors are in parallel, we know the ##24V## must drop across both branches.
 
Zondrina said:
Assume for a moment that the ##24V## source is shorted to zero (put a wire there) and the switch is open. So all you have is a circuit with some components and nothing going on. There is no potential at any point, and no current to be measured at all. This is reasonable because we have no power supply yet.

Now suppose we apply the ##24V## source to the circuit with the switch open. Immediately, current will begin to flow through the circuit and the capacitors will begin charging up. This implies ##V = IR \neq 0## and ##V = \frac{q}{C} \neq 0##. So we can deduce there must be a potential at points ##a## and ##b##. In fact, because the resistors and capacitors are in parallel, we know the ##24V## must drop across both branches.

So it's only for this special case? If I were to put a resistor directly after the battery source , would the following case still apply?
 
BlueCerealBox said:
So it's only for this special case? If I were to put a resistor directly after the battery source , would the following case still apply?

I don't believe there's anything too special about it.

If you were to place a resistor directly after the battery source (it could be the internal resistance of the battery for example) then the calculations would change somewhat. Some of the voltage would drop across this resistance. Call the amount of voltage dropped across this resistance ##V_B## for a moment.

Then, when we first apply the ##24V## source, we know the voltage remaining after the ##V_B## drop is ##24V - V_B##.

This remaining ##24V - V_B## would then be lost across both parallel branches. We can measure the potential at points ##a## and ##b## by measuring the voltage across the ##4.4 \Omega## resistor and the ##0.24 \mu F## capacitor respectively.

This is assuming the switch is open at the time.
 
Ah ok. I think I somewhat understand it now. Thanks for the help!
 
Kindly see the attached pdf. My attempt to solve it, is in it. I'm wondering if my solution is right. My idea is this: At any point of time, the ball may be assumed to be at an incline which is at an angle of θ(kindly see both the pics in the pdf file). The value of θ will continuously change and so will the value of friction. I'm not able to figure out, why my solution is wrong, if it is wrong .
Thread 'Voltmeter readings for this circuit with switches'
TL;DR Summary: I would like to know the voltmeter readings on the two resistors separately in the picture in the following cases , When one of the keys is closed When both of them are opened (Knowing that the battery has negligible internal resistance) My thoughts for the first case , one of them must be 12 volt while the other is 0 The second case we'll I think both voltmeter readings should be 12 volt since they are both parallel to the battery and they involve the key within what the...

Similar threads

Back
Top