Energy to charge capacitor and stored energy

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    Capacitor Charge Energy
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SUMMARY

The discussion centers on the energy dynamics involved in charging a capacitor with a 1V battery and a capacitance of 1.602x10-19 Farads. It is established that the energy stored in the capacitor is half of the energy supplied by the battery, with the remaining energy dissipated as heat due to resistance in the wires. Participants debate the validity of this assertion, emphasizing that energy loss is influenced by the resistance of the wire and the characteristics of the circuit, particularly in reactive AC circuits. The conversation also touches on the impact of inductance on energy loss during charging.

PREREQUISITES
  • Understanding of capacitor charging equations, specifically the formula for energy stored in a capacitor: E = (1/2)CV2.
  • Knowledge of electrical resistance and its impact on energy dissipation, particularly Ohm's Law (I2R losses).
  • Familiarity with reactive circuits and the role of inductance in energy transfer.
  • Basic principles of electromagnetic radiation and its effects during current changes.
NEXT STEPS
  • Study the derivation of energy stored in capacitors and the implications of resistance in charging circuits.
  • Learn about the effects of inductance on energy efficiency in capacitor charging.
  • Explore advanced circuit simulations to analyze energy loss in complex circuits like Switch Mode Power Supplies (SMPS).
  • Investigate the principles of electromagnetic radiation and its detection in electrical circuits.
USEFUL FOR

Electrical engineers, physics students, and anyone interested in understanding the principles of capacitor charging, energy loss in circuits, and the effects of resistance and inductance on energy efficiency.

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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