Kirchhoff's Law with Capacitors: Voltage, Resistance & Charge

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Discussion Overview

The discussion revolves around the application of Kirchhoff's law in circuits involving capacitors, particularly focusing on the equations governing discharging capacitors and the implications of different sign conventions in circuit analysis.

Discussion Character

  • Technical explanation
  • Conceptual clarification
  • Debate/contested

Main Points Raised

  • One participant expresses confusion regarding the application of Kirchhoff's law with capacitors, noting the difference in sign between the equations for a battery and a discharging capacitor.
  • Another participant mentions that during capacitor discharge, the current decreases the charge, leading to a specific relationship between current and voltage.
  • A participant reiterates the initial confusion and introduces the concept of passive and active sign conventions, suggesting that the choice of convention does not affect the underlying physics.
  • One participant proposes that understanding actual current flow can simplify the analysis, arguing that focusing on the physics rather than conventional rules may reduce confusion.

Areas of Agreement / Disagreement

Participants express varying levels of confusion and differing perspectives on the application of sign conventions, indicating that the discussion remains unresolved with multiple competing views on how to interpret Kirchhoff's law in the context of capacitors.

Contextual Notes

There are limitations regarding the assumptions made about current flow and the definitions of passive and active sign conventions, which may not be universally agreed upon among participants.

Silviu
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Hello! I am bit confused about kirchhoffs law with capacitors. So if I have a battery and resistance, I obtain V-RI=0. But from what I read, if I have a capacitor and resistance (so discharging capacitor), the equation reads
R(dq/dt) + q/c = 0, which is equivalent to RI + q/c =0. Why in this case we have "+" between terms, if the capacitor acts like a battery?
 
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If the capacitor discharges, the current lowers the charge, so ##I = - dV/dt = -{1\over C}{dq\over dt}##
 
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Silviu said:
Hello! I am bit confused about kirchhoffs law with capacitors. So if I have a battery and resistance, I obtain V-RI=0. But from what I read, if I have a capacitor and resistance (so discharging capacitor), the equation reads
R(dq/dt) + q/c = 0, which is equivalent to RI + q/c =0. Why in this case we have "+" between terms, if the capacitor acts like a battery?
In addition to the above, it could also come from using the passive sign convention for the capacitor and the active sign convention for the battery. The convention used doesn't affect any of the physics.

The passive sign convention means that a positive current goes from the positive side to the negative side so P=IV is the power received by the element. The active sign convention means that a positive current goes from the negative side to the positive side so P=IV is the power produced by the element.
 
To get the right sign, it's much easier to think in terms of actual current flow. E.g., a positive current towards the positively charged plate of the capacitor leads to an increasing voltage. It's much simpler to think about the physics than learn the quite complicated conventional rules by engineers, which usually leads to confuse themselves ;-).
 

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