Transient Capacitance Analysis: DC Source, Resistor & Capacitor

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Discussion Overview

The discussion revolves around the transient analysis of a circuit comprising a DC voltage source, a resistor, and a capacitor in parallel. Participants explore the behavior of voltage across the resistor and capacitor over time, as well as the implications of Kirchhoff's voltage law in this context.

Discussion Character

  • Exploratory
  • Technical explanation
  • Debate/contested

Main Points Raised

  • One participant questions how the voltage drop across the resistor changes with that of the capacitor, noting that they are in parallel and thus should share the same voltage.
  • Another participant points out that the initial conditions of the circuit lead to infinite current for an infinitely short time until the capacitor charges to the voltage of the source.
  • Concerns are raised about the applicability of Kirchhoff's voltage law in this scenario, particularly regarding the behavior of an ideal DC source and the changing potential difference across the capacitor.
  • Some participants suggest that real-world components introduce parasitic effects, such as internal resistance and inductance, which can affect circuit behavior and compliance with Kirchhoff's laws.
  • There is a discussion about the implications of models yielding infinite values for voltages or currents, with suggestions that such models may need to be revised to reflect real-world conditions.
  • A later reply introduces the idea of undefined equations or division by zero in certain scenarios, questioning whether the loop equation leads to infinity in this case.

Areas of Agreement / Disagreement

Participants express differing views on the implications of ideal versus real-world components, with no consensus on how to reconcile the observed behavior with Kirchhoff's laws. The discussion remains unresolved regarding the validity of the models used and their applicability to real circuits.

Contextual Notes

Participants note that many components exhibit parasitic effects that can complicate analysis, particularly under transient conditions or at high frequencies. The discussion highlights the limitations of ideal circuit models in capturing real-world behavior.

Sidney
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When analyzing the transient development of a circuit containing a DC voltage source, capacitor and resistor in parallel, how might one explain the fact that 1. the voltage drop across the resistor changes with that of the capacitor. 2. The first loop containing the capacitor and DC source seem not to obey kirchhoff's voltage law (as the ideal DC source is fixed but the capacitor p.d changes with time)
 
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I can't understand your questions without a picture. Please sketch one and use the UPLOAD button to post it.
 
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Your circuit, as drawn, will have infinite current for infinitely short time until the capacitor is charged to the voltage of the voltage source. Then the voltage across the resistor is equal to the voltage across the capacitor.

This will, of course, change if you use a real world voltage source. Real world voltage sources have series resistance, peak current, and transient response characteristics. And real world circuits have wires with finite resistance, capacitance, and inductance. And real world capacitors have internal resistance and inductance.
 
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Here is a good rule you can use. Ohms Law, and Kirckoffs Laes allows us to make models of real world circuits. But whenever they give answers of infinity for voltages or currents, it means that the model is no good and that we must change it in ways such as @jrmichleim said.
 
Sidney said:
When analyzing the transient development of a circuit containing a DC voltage source, capacitor and resistor in parallel, how might one explain the fact that 1. the voltage drop across the resistor changes with that of the capacitor.

The R and C are in parallel. They are connected between the same two nodes therefore they must have the same voltage.
2. The first loop containing the capacitor and DC source seem not to obey kirchhoff's voltage law (as the ideal DC source is fixed but the capacitor p.d changes with time)

What others have said.

You have identified a situation where a circuit model differs from the real world. In the real world batteries, wires and capacitors all have some internal resistance. If you add those resistors to the circuit you will see it can and does meet KVL.

Most components have unwanted parasitic effects. Capacitors also have some inductance. Inductors have some capacitance. Some resistors have both. Batteries aren't ideal voltages sources. Wires have resistance, capacitance and inductance. The list goes on..

In many cases these so-called parasitics are not significant and can be ignored, but not always. In general you have to watch out at high frequencies or transient conditions, or at high or low currents and voltages.
 
anorlunda said:
But whenever they give answers of infinity for voltages or currents, it means that the model is no good and that we must change it in ways such as @jrmichleim said.

Does the loop equation give an answer of infinitely in this case? I think what you get is an undefined equation or more specifically a division by zero. Obviously, the conclusion and action one takes to correct the situation is the same either way.

A system that could give infinity as an answer would be something like: find the quiescent point of ideal constant current source charging an ideal capacitor. (At least I think so. I recall the formal definition of quiescent point as voltages, currents at t=infinity for constant inputs but I might be wrong about that.)
 
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