Kirchoff's Loop Rule as applied to Capacitors?

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Homework Help Overview

The discussion centers around the application of Kirchhoff's Loop Rule in circuits that include capacitors and resistors. The original poster expresses confusion regarding the relationship between the loop rule, potential differences, and capacitors, noting a lack of examples that incorporate these elements together.

Discussion Character

  • Exploratory, Conceptual clarification, Assumption checking

Approaches and Questions Raised

  • Participants explore the application of Kirchhoff's Loop Rule to capacitors, with some referencing the fundamental laws governing capacitors. Questions arise about the behavior of current in relation to capacitors when they are fully charged and the implications of steady state conditions.

Discussion Status

The discussion is ongoing, with participants providing insights into the relationship between Kirchhoff's Loop Rule and capacitors. There is a recognition of different scenarios affecting current flow in capacitors, and some participants are questioning the definitions and assumptions related to steady state and equilibrium.

Contextual Notes

Participants are navigating concepts related to RC circuits and the conditions under which current flow ceases in capacitors. The original poster's inquiry reflects a search for clarity on how these principles are applied in practical examples.

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Homework Statement



How does the loop rule apply to capacitors? I can't find any examples of circuits containing capacitors and resistors where the loop rule is used. I know the loop rule measures potential differences, but I'm not quite sure if that has anything to do with capacitors? All the examples are 0 = V - IR - IR, etc.


Homework Equations





The Attempt at a Solution

 
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Yes, the loop rule is used with capacitors all the time. The element law for a capacitor is v=q/C. In more advanced (calculus-based) courses this is written i=C\frac{dv}{dt}. Solving this for the voltage, one obtains:

v=\frac{1}{C}\int_{t_0}^ti(\tau)d\tau+v(t_0)
 
all the basics of RC circuits (RL and RLC circuits too) come from a basic application of Kirchoff's Loop principle.
 
So when finding currents, the branch that a capacitor is on (in terms of current) is 0, right? since when a capacitor is full, no current flows.
 
not necessarily. it depends on the situation. Since charging rate = current, current=0 if and only if the charge of the capacitor is constant. This happens when the capacitor has been (dis)charging for a long time, or when the circuit reaches steady state.
 
Last edited:
the problem says that the currents reach equilibrium. isn't that steady state?
 

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