Energy to charge capacitor and stored energy

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    Capacitor Charge Energy
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Discussion Overview

The discussion revolves around the energy dynamics involved in charging a capacitor using a battery, specifically focusing on the energy supplied by the battery, the energy stored in the capacitor, and the losses incurred during the process. The scope includes theoretical considerations, mathematical reasoning, and conceptual clarifications related to energy transfer in electrical circuits.

Discussion Character

  • Technical explanation
  • Conceptual clarification
  • Debate/contested
  • Mathematical reasoning

Main Points Raised

  • One participant states that a capacitor stores half the energy supplied by the battery, with the other half lost to resistance in the wires.
  • Another participant challenges this claim, suggesting that the relationship between energy loss and resistance is not straightforward and depends on the circuit configuration.
  • A different viewpoint is presented, arguing that losses can be minimized by adding inductance to the circuit.
  • One participant explains that the energy supplied by the battery is Q x V, while the energy stored in the capacitor is 0.5Q x V, and identifies three potential sources of energy loss during charging.
  • Another participant emphasizes the importance of modeling the wire as a resistor in series with the capacitor to accurately account for energy losses.
  • There is a mention of the role of parasitic resistance during the discharge phase of the capacitor affecting overall energy efficiency.

Areas of Agreement / Disagreement

Participants express differing views on the nature of energy loss during the charging process, with no consensus reached on the mechanisms or the extent of these losses. Some participants agree on the basic principles of energy storage in capacitors, while others contest specific claims regarding energy dissipation.

Contextual Notes

Participants discuss various assumptions related to resistance, circuit configurations, and the ideal behavior of components, indicating that the discussion is influenced by these factors and may not apply universally.

Who May Find This Useful

This discussion may be of interest to individuals studying electrical engineering, physics, or anyone looking to understand the principles of energy transfer in capacitive circuits.

sridhar10chitta
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I use a 1V battery to charge a capacitor of capacity 1.602x10raised to -19 Farad (1.602x10raised to -19 coulomb is the electric charge of a single electron).
What is the energy spent by the battery and the energy stored in the capacitor ?
 
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There's a formula for energy stored in capacitor which you'll need here. You can assume that there is no energy loss, ie. energy in capacitor = energy provided by battery.
 
The capacitor stores half the energy supplied by the battery. Remaining half is lost in the resistance (resistance of wires used) as I*I*R. The energy lost in the resistance is independent of value or resistance and depends primarily on the capacitance.
 
vinayakbhat82 said:
The capacitor stores half the energy supplied by the battery. Remaining half is lost in the resistance (resistance of wires used) as I*I*R. The energy lost in the resistance is independent of value or resistance and depends primarily on the capacitance.

This is not true. One could easily imagine a situation where you have a very large capacitor connected to a power source by a very resistive wire. The ideal case would have the resistance of the wire be zero whereby all the power received would be equal to the power delivered. But if half the power is always dissipated by the wire regardless of resistance, then this is a discontinuous relationship. I think you are thinking about the power delivered using an AC signal in a reactive circuit.

If he wants to account for the power lost due to ohmic losses then he can model the wire as a resistor in series with the capacitor and solve the new differential equation or use the appropriate transform to find the current relationship and then integrate over time to find the power delivered by the power source and the power dissipated by the resistor.
 
Born2bwire said:
vinayakbhat82 said:
The capacitor stores half the energy supplied by the battery. Remaining half is lost in the resistance (resistance of wires used) as I*I*R. The energy lost in the resistance is independent of value or resistance and depends primarily on the capacitance.
This is not true.
I think it is true. However, the losses can be decreased by adding inductance. There is a good explanation here: http://www.smpstech.com/charge.htm
 
Born2bwire said:
This is not true. One could easily imagine a situation where you have a very large capacitor connected to a power source by a very resistive wire. The ideal case would have the resistance of the wire be zero whereby all the power received would be equal to the power delivered. But if half the power is always dissipated by the wire regardless of resistance, then this is a discontinuous relationship. I think you are thinking about the power delivered using an AC signal in a reactive circuit.

If he wants to account for the power lost due to ohmic losses then he can model the wire as a resistor in series with the capacitor and solve the new differential equation or use the appropriate transform to find the current relationship and then integrate over time to find the power delivered by the power source and the power dissipated by the resistor.



As I understand, the statement made by me earlier is indeed true. Immaterial of values of capacitor and resistors, the capacitor would store half the energy supplied by the battery. The power delivered by the battery in charging a capacitor of value 'C' to voltage 'V' is C*V^2. The energy stored in the capacitor is (C*V^2)/2. The difference energy i.e. (C*V^2)/2 is dissipated in the resistor. Even in case of a very large capacitor and very small resistor (as described by you), the initial current would be very high due to low resistor and would remain high for pretty long due to big capacitor which would mean high value of (I^2)*R (Here I is instantaneous current integrated over time). The current would exponentially decrease as the capacitor charges, with time constant RC. Can you please clarify the "discontinuous relationship" being referred?
 
TurtleMeister said:
I think it is true. However, the losses can be decreased by adding inductance. There is a good explanation here: http://www.smpstech.com/charge.htm

I'll have to work it out then by hand when I have some time then.

EDIT: Oh yeah it is, funny that.

P_{res} = IV = \int^\infty_0dt\frac{V_0^2}{R}\left(1-e^{-t/\tau_0}\right)e^{-t/\tau_0} \\<br /> = \left.\frac{V_0^2}{R}\left[-\tau_0e^{-t/\tau_0} + \frac{\tau_0}{2}e^{-2t/\tau_0}\right]\right|_0^\infty \\<br /> = \frac{V_0^2\tau_0}{2R} = \frac{V_0^2C}{2}

Well then, you learn something new everyday.
 
Last edited:
Thanks all of you. It is clear that there will be a loss in the wire...one electron or not...
Sridhar
 
See, there is a basic difference between capacitor and cell. A cell supplies charge at constant potential, while the capacitor, transfers the charge at variable potentials, so in case of capacitor the formula is derived using integration.

while transfering charge q at potential V a cell does work qV, while in transfering charge q to a capacitor such that potential changes from 0 to V is 1/2 qV.
it is clear that while charging, half of energy is lost, at the same time, no charge is lost.
 
  • #10
TurtleMeister said:
I think it is true. However, the losses can be decreased by adding inductance. There is a good explanation here: http://www.smpstech.com/charge.htm

The energy loss is most likely present in the discharge phase of the capacitor, where the parasitic resistance in line with the load "steals" energy.

----------------
heh...after some simulations, in more complex circuits (like our beloved SMPSs) , the resistance present when charging a capacitor plays a big role in the efficiency of the circuit.
 
Last edited:
  • #11
If the resistance of wire and all is zero. Then will the energy supplied by battery = energy gained by capacitor = 1/2 CV^2 ??
 
  • #12
The energy supplied by the battery is Q x V.
The energy stored on the capacitor is 0.5Q x V
Energy can be lost in 3ways
1) resistance of the wire (this can be made =0)
2) any sparking at the switch(this can be made =0)
3) electro magnetic radiation from the connecting wires as the current changes during the charging (or discharging) (This cannot be made = 0)
Whenever coronet changes electro magnetic radiation occurs. The radiation could be radio waves and can be detected using a radio... It is crackling interference
 

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