Discharging a capacitor -- Calculate the current as a function of time

In summary, the conversation discusses the correct calculation of task b, which involves interpreting an open switch as an infinitely large resistor and using Kirchhoff's rules to find the current in the circuit. The negative sign in front of the current indicates the direction of the current, but it can be chosen arbitrarily. The discussion also touches on the distribution of charges on the capacitor and the relevance of positive or negative signs in the context of the question.
  • #1
Lambda96
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Homework Statement
Calculate the current as a function of time when discharging the capacitor
Relevant Equations
none
Hi,

I am not sure if I have calculated the task b correctly.

Bildschirmfoto 2023-04-26 um 15.25.39.png

I always interpret an open switch as an infinitely large resistor, which is why no current is flowing through this "resistor". So there is no current in the red circle, as it was the case in task part a, but only in the blue circle.

Bildschirmfoto 2023-05-05 um 12.00.57.png


Since the resistors are connected in series, I combined them into one, so ##R_g=R_1+R_3## Then I set up Kirchhoff's rules ##\frac{q}{C}=-R_g I## after that I rewrote the current as follows ##\frac{dq}{dt}## and put it into the equation ##\frac{q}{C}=-R_g \frac{dq}{dt}## and rewrote it as follows and integrated it afterwards.

$$-\frac{1}{R_g C}dt=\frac{1}{q}dq$$
$$ \int_{0}^{t} -\frac{1}{R_g C}dt= \int_{Q_0}^{Q} \frac{1}{q} dq $$
$$-\frac{t}{R_g C}=\ln(\frac{Q}{Q_0})$$
Solve the equation for Q: ##Q=Q_0e^{-\frac{t}{R_g C}}##

To get the current now, I simply derived the equation for the charge with respect to time.

$$I(s)=\frac{dQ}{dt}=-\frac{Q_0}{R_g C}e^{-\frac{t}{R_g C}}$$
 
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  • #2
This would be correct if you have calculated ##Q_0## correctly from part (a).

What does the negative sign in front of the current mean? Is the direction of the current clockwise or counterclockwise?
 
  • #3
Thanks kuruman for looking over my calculation 👍 The minus sign came from the derivative of the function for the charge.

For the charge ##Q## I got the following in task a ##Q(t)=\epsilon C(1-e^{-\frac{t}{R_g C}})##

##Q_0## would then be reached at time ##T##, so ##Q_0(T)=\epsilon C(1-e^{-\frac{T}{R_g C}})##

##\epsilon## is the voltage of the battery

But if I read the circuit diagram correctly, when charging the capacitor, the left side of the capacitor would be positive and the right side negative. If now the switch ##S_1## is closed and ##S_2## is opened, the positive charges would move to the negative charges, whereby the current would move clockwise and should then be positive, or have I misunderstood the plan and the distribution of the charges on the capacitor?
 
  • #4
The signs of the current or charge are not really relevant for what the question asks. And there is no absolute rule for taking the current positive or negative. Clockwise does not mean positive unless you choose to be so.
 
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FAQ: Discharging a capacitor -- Calculate the current as a function of time

What is the formula for the current as a function of time when discharging a capacitor through a resistor?

The current as a function of time when discharging a capacitor through a resistor is given by the formula: \( I(t) = \frac{V_0}{R} e^{-\frac{t}{RC}} \), where \( V_0 \) is the initial voltage across the capacitor, \( R \) is the resistance, \( C \) is the capacitance, and \( t \) is the time.

How does the time constant (τ) affect the discharging process of a capacitor?

The time constant (τ) is defined as \( \tau = RC \). It represents the time it takes for the current (or voltage) to decrease to approximately 36.8% of its initial value. A larger time constant means the capacitor discharges more slowly, while a smaller time constant means it discharges more quickly.

What happens to the current over time during the discharging of a capacitor?

During the discharging of a capacitor, the current decreases exponentially over time. Initially, the current is at its maximum value, \( \frac{V_0}{R} \), and it approaches zero as time goes to infinity.

Can you explain the physical significance of the exponential decay in the current during capacitor discharge?

The exponential decay in the current during capacitor discharge signifies that the rate at which charge leaves the capacitor decreases over time. This is because the voltage across the capacitor (which drives the current) also decreases exponentially, reducing the driving force for the current as the capacitor discharges.

How can you experimentally determine the time constant (τ) of a capacitor-resistor circuit?

To experimentally determine the time constant (τ) of a capacitor-resistor circuit, you can measure the voltage across the capacitor at different times during the discharge process. Plot the natural logarithm of the voltage versus time, and the slope of the resulting straight line will be \(-\frac{1}{RC}\). From the slope, you can determine the time constant τ.

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