Discharging capacitor in RC circuit, confusing path

AI Thread Summary
The discussion focuses on analyzing an RC circuit involving a capacitor and resistors R1 and R2. For part (a), the potential difference across the capacitor is determined by considering the charging behavior and the arrangement of resistors in the circuit. In part (b), confusion arises regarding the direction of current flow during the capacitor's discharge after the battery is disconnected, with emphasis on the effective resistance of the circuit. The current direction is clarified by understanding the voltage across the capacitor terminals, which dictates how the current flows as it discharges. Overall, the key points revolve around understanding the circuit configuration and the behavior of current and voltage in an RC discharge scenario.
horsedeg
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Homework Statement


The circuit in the figure below has been connected for a long time. Let R1 = 8.20 Ω and R2 = 4.40 Ω.
28-p-037-alt.gif

(a) What is the potential difference across the capacitor?
(b) If the battery is disconnected from the circuit, over what time interval does the capacitor discharge to one-eighth its initial voltage?

Homework Equations


V=IR
Q=CV
Derived equations for current/voltage over time in discharging case

The Attempt at a Solution


(a) wasn't hard. I think normally, if this capacitor was fully in series with the resistors, then the potential difference across the capacitor would be equal to the voltage across the battery. However, in this case, it's not in series. Once the capacitor becomes fully charged, the current in the middle branch stops completely and the capacitor acts as an infinite resistor, but it keeps going everywhere else. Then the 1.00 Ω resistor and R2 are in series. I can use that to solve for the current across that left branch containing those two resistors while the capacitor is fully charged, because parallel devices have equal voltage drops, so I can use V=IR (or 10.0 = I*[1.00Ω + R2]), and then do so similarly for the right branch to find the other current. Then I can use Kirchoff's loop rule in that upper triangle to solve for the difference of potential across the capacitor.

(b) doesn't make a lot of sense to me. First, which way would the resulting current be? To the left because of the fact that there's less resistance coming from that direction so the + would be on the left of the capacitor?

The part that I understand the least, though, is that apparently the Reff actually becomes a combination of all of the resistors. Somehow they can be combined like this. This first and second pictures make perfect sense, but I don't understand the rest.
28-p-037-mi.gif
 
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When the capacitor discharges with the battery disconnected, the circuit is quite simple: R1 is in series with the 1 ohm resistor, and R2 is in series with the 2 ohm resistor. The two series chains are in parallel so the total resistance can easily be computed. One other hint for this part: Can you write the equation of the voltage across the capacitor and/or the current as the capacitor discharges?
 
Charles Link said:
When the capacitor discharges with the battery disconnected, the circuit is quite simple: R1 is in series with the 1 ohm resistor, and R2 is in series with the 2 ohm resistor. The two series chains are in parallel so the total resistance can easily be computed. One other hint for this part: Can you write the equation of the voltage across the capacitor and/or the current as the capacitor discharges?
I guess I can somewhat see how it's in series, but this doesn't make much sense to me.
upload_2016-12-10_20-31-41.png

This is basically an equivalent circuit after the voltage source is removed, but I can't make sense of this. They're in series, but what happens to the current? Does it go back towards the capacitor?
 
horsedeg said:
First, which way would the resulting current be?
In (a) you determined the voltage of the capacitor terminals, so you know which is more positive and by how much. This is what determines the direction of current as it discharges, with current leaving one plate to return via the external circuit to the other plate.
 
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