Charge a Capacitor: Qualitative & Quantitative Explanations

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    Capacitor Charging
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Discussion Overview

The discussion revolves around the charging of a capacitor, particularly focusing on the qualitative and quantitative aspects when a capacitor is connected directly to a battery without any resistance in between. Participants explore theoretical implications, mathematical formulations, and practical considerations related to this scenario.

Discussion Character

  • Exploratory
  • Technical explanation
  • Debate/contested

Main Points Raised

  • One participant describes the standard charging process of a capacitor using the equation V = iR + Q/C and questions the scenario when a capacitor is connected directly to a battery.
  • Another participant suggests that there is always some resistance in the wire and proposes considering an RC circuit with a very small resistance.
  • A participant challenges the idea of resistance, asking what happens if the wire has zero resistance, emphasizing the need for clarification on this point.
  • It is proposed that if a capacitor charges instantaneously, an "infinite" current would flow for an infinitesimally short time, leading to a charge Q=E/C, where E is the emf of the battery.
  • Some participants discuss the application of Kirchhoff's law in the context of an ideal battery and capacitor circuit, questioning the implications of energy radiated as electromagnetic waves.
  • One participant mentions that the voltage on the wire/capacitor would rise very quickly, potentially generating high-frequency signals and radio waves.
  • Another participant notes that passing a high current through a wire in a magnetic field could result in observable forces, drawing a parallel to motor operation.

Areas of Agreement / Disagreement

Participants express multiple competing views regarding the implications of connecting a capacitor directly to a battery, particularly concerning the role of resistance and the behavior of current. The discussion remains unresolved, with no consensus on the theoretical outcomes.

Contextual Notes

Limitations include assumptions about ideal components (zero resistance, ideal battery, ideal capacitor) and the implications of these assumptions on real-world scenarios. The discussion does not resolve the mathematical steps or the physical interpretations involved.

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I understand the situation when we charge a capacitor using a battery and a resistor placed in between serially placed ! V = iR + Q/C where we write i = dQ/dt
whereas,
V is voltage of battery
R is resistance of resistor
Q is charge on capacitor
C is capacitance of capacitor
i is current
But what happens when we connect a capacitor directly to a battery , nothing in between ??
Can somebody explain this qualitatively and also quantitatively !
 
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There is always some resistance in the wire. So just take the RC circuit you already know and make R very small.
 
But what if the wire connecting the battery and the capacitor is of zero resistance
That my question actually ! !
 
The capacitor will charge instantaneously. An "infinite" current will flow for no time (zero time interval) so that it caries a charge Q=E/C where E is the emf of the battery.
But this does not describe what happens when you connect a (real) battery to a (real) capacitor.
 
Shreyas Samudra said:
But what if the wire connecting the battery and the capacitor is of zero resistance
That my question actually ! !
Just take the RC circuit that you already understand, calculate whatever quantity you are interested in, and then take the limit as R goes to 0. It will give you mathematically what nasu described above.
 
Actually i want to ask how do we apply krichhoff' s law for a circuit having only a battery(ideal, of zero resistance) and a capacitor
I got to know something like -energy radiated out in form of EM waves, as of a reference in my textbook
but that is not in detail , so can somebody please elaborate on that
 
E=Q/C
 
Shreyas Samudra said:
Actually i want to ask how do we apply krichhoff' s law for a circuit having only a battery(ideal, of zero resistance) and a capacitor
I got to know something like -energy radiated out in form of EM waves, as of a reference in my textbook
but that is not in detail , so can somebody please elaborate on that
What do you get if you use the approach I already suggested above?
 
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Shreyas Samudra said:
Actually i want to ask how do we apply krichhoff' s law for a circuit having only a battery(ideal, of zero resistance) and a capacitor.

That's a bit like asking what happens if you apply an infinitely large force to an immovable object. In the real world the capacitor will also have some resistance and inductance.

If you connect an ideal battery to an ideal capacitor using ideal wire the current would be infinite. However the capacitor would also charge up in zero time so the infinitely large current would only flow for an infinitely short time.

I got to know something like -energy radiated out in form of EM waves, as of a reference in my textbook
but that is not in detail , so can somebody please elaborate on that

How best to explain? .. The voltage on the wire/capacitor would rise very fast in the situation you describe. That's equivalent to having a very high frequency signal on the wire. In general the higher the frequency the shorter the aerial you need to easily launch a radio wave. So yes you would get a burst of radio waves. An AM radio receiver would probably pick it up as a click or thump.

Other interesting things might happen. For example if you pass a high current through a wire in a magnetic field it will experience a force. After all that's how a motor works. You propose passing an infinite current through a wire in the Earth's magnetic field.
 

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