Energy of Capacitor in RC Circuit

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SUMMARY

The discussion focuses on the energy dynamics in an RC circuit comprising a battery, switch, resistor, and capacitor. When the switch is closed, the capacitor charges over time, ultimately storing only half of the energy supplied by the battery. The equations involved include the voltage across the capacitor, V(t) = V_0(1-e^{-t/\tau}), and the energy stored in the capacitor, U = 1/2CV^2. The total energy delivered by the battery is established as C V_0^2, confirming that the energy stored in the capacitor is indeed half of the total energy supplied.

PREREQUISITES
  • Understanding of RC circuit components (battery, resistor, capacitor)
  • Familiarity with Kirchhoff's laws, particularly Kirchhoff's current and loop laws
  • Knowledge of calculus, specifically integration and differentiation
  • Basic grasp of electrical energy equations, including U = 1/2CV^2
NEXT STEPS
  • Study the derivation of the time constant in RC circuits
  • Explore energy conservation principles in electrical circuits
  • Learn about the impact of resistor values on charging time in RC circuits
  • Investigate the behavior of capacitors in AC circuits
USEFUL FOR

Electrical engineering students, physics learners, and anyone interested in understanding the energy transfer and storage in RC circuits.

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Homework Statement


The circuit consists of a battery, switch, resistor, and capacitor connected in a loop in series. When the switch is closed at time t=0, a time-dependent current flows out of the battery and charges the capacitor. The capacitor is fully charged at time t=infinity. Show that only half of this energy supplied by the battery ends up being stored in the fully charged capacitor.

Homework Equations


V(t)=V_0(1-e^{-t/\tau}
U=1/2CV^2
P=IV=V^2/R=\dot{E}

The Attempt at a Solution


U(\infty)=1/2CV_0^2=\frac{QV_0}{2}=\frac{V_0^2}{2}

I'm confused about where my extra factor of V0 is coming from. Do I need to use the power equation?
 
Last edited:
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\frac { Q V_0 } {2}

is the correct expression for the energy stored in the capacitor. The next step is wrong.

Try to show that the total energy delivered by the battery is twice as large.
 
Energy supplied by battery up to any point is qVo
here q is total charge supplied up to that point

use this and qVo/2 for capacitor at t = ∞
 
The instantaneous power delivered to a component is given by

I * V

where the I is the current through the component, and V is the voltage across the component.

Note that the current through the resistor and capacitor are the same, because of Kirchoff's current law:

<br /> I(t) = \frac{dQ(t)}{dt} = C \frac{dV(t)}{dt}<br />

where Q(t) is the charge on the capacitor at a time t, and the voltage V_R across the resistor plus the voltage V_C across the resistor is:

<br /> V(t) = V_R + V_C = V_o <br />

Since the voltage across the capacitor and resistor always sums to V_o (Kirchoff loop law).

The total energy delivered to the component is given by the time integral of this expression, since power is the time derivative of the energy. So the total energy delivered to the RC circuit is
<br /> C \int_0^{t_o} \frac{d V(t)}{d t} V_o d t<br />

The fundamental law of calculus says this is equal to:

<br /> C V_o \left( V(t_o) - V(0) \right)<br />

There is no initial voltage across the capacitor so V(0) = 0. t_o is infinite so V(t_o) = V_o. So the total energy expended to charge the capacitor is:

<br /> C V_o^2<br />

Which is twice the energy stored in the capacitor.
 
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