Energy lost charging a capacitor - can someone check my calculations.

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Homework Help Overview

The original poster attempts to demonstrate that not all of the energy supplied by a power supply is stored in a capacitor when charging occurs through a resistor. The problem involves analyzing the energy transfer in an RC circuit, focusing on the energy dissipated in the resistor versus the energy stored in the capacitor.

Discussion Character

  • Exploratory, Mathematical reasoning, Assumption checking

Approaches and Questions Raised

  • Participants discuss the integration of power over time to find energy transferred to both the capacitor and resistor. The original poster expresses doubt about their calculations and seeks clarification on the relationship between the energies involved.

Discussion Status

Some participants provide feedback on the original poster's calculations, with one pointing out a potential error in integration. Another participant offers an alternative expression for the energy in the capacitor, leading to a discussion about the limit as time approaches infinity. There is no explicit consensus on the correctness of the original poster's approach, but guidance has been offered regarding the limits and integration.

Contextual Notes

The original poster is working under the constraints of a homework assignment, which may impose specific methods or assumptions that are not fully detailed in the discussion.

MalachiK
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Homework Statement


I'm trying to show that not all (half) of the energy supplied by the power supply ends up in the capacitor when the capacitor is charged through a resistor. I've looked at some of the other threads on these sorts of topics and I'd thought I'd have a go at working through it myself. The treatments of this problem that I've seen seem to consider the work done moving each charge element through a potnetial differnece but I thought I could do this another way. Anyway, it's not going well and I'd appreciate any advice.

Homework Equations



I've included these in the working below...

The Attempt at a Solution


It seems to me that you can start by considering the power transferred to C and to R over a given time interval and then integrate to get the energy transferred in this time.

At first, all of the p.d. is dropped across R. Let's call this V0. We can also call the initial current I0. None of the p.d. is dropped across the cap at first.

After time t, the p.d. across R is V0e-t/RC and the p.d. across the cap is V0(1-e-t/RC). The current is I0e-t/RC.

At ant time t, the power delivered to the resistor is V(t)I(t). So after some time T, the energy lost as heat in the resistor should be V0I0\int^T_0e-2t/RC dt

Setting Vo Io as Po and with some calculating I get...

ER=(2Po/RC)(1 - e-2T/RC)

It also occurred to me that the total energy delivered to the circuit would be \int^T_0Vo Io e-t/RC dt [the total p.d. across the circuit doesn't change, only the way it is shared out changes. The current falls with time.]Evaluating this gives me
ET = (Po/RC)(1 - e-T/RC)So far so good (unless I've made some stupid mistake!) Now for the energy to the capacitor. Following the same reasoning as before I get that...

EC= Po \int^T_0 e-t/RC - e-2t/RC dt

Evaluating this gives me

EC = (Po/RC)(2e-2T/RC -e-T/RC - 1)Now I'm doubtful of this result because it looks like it's got too many terms in it, but on the other hand, when I calculate EC = ET - ER I get the same result so at least if I'm wrong I'm internally consistent!

At this point my algebra fails me and I can't see how I can compare my expressions for each of the energies to show something like EC = 0.5 ET. Is this because there's something seriously wrong with my thinking?
 
Last edited:
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\int e^{at} dt is not equal to a e^{at}


You want the energy for time from 0 to infinity, so you have to take the limit for t->inf,
wich should be easy as all the exponentials become 0.
 
For the capacitor, I get

P_c = \int_0^T I_o e^{-\frac{t}{\tau}} V_o \left(1 - e^{-\frac{t}{\tau}}\right) dt

P_c = -\frac{1}{2} \tau I_o V_o \left(2 e^{-\frac{T}{\tau}} - e^{-\frac{2T}{\tau}} - 1 \right)

P_c = \frac{1}{2} \tau I_o V_o \left(1 - e^{-\frac{2T}{\tau}} + e^{-\frac{T}{\tau}} \right)

Now, τ = RC, so

P_c = \frac{1}{2} R C I_o V_o \left(1 - e^{-\frac{2T}{\tau}} + e^{-\frac{T}{\tau}} \right)

But R Io = Vo, so

P_c = \frac{1}{2} C V_o^2 \left(1 - e^{-\frac{2T}{\tau}} + e^{-\frac{T}{\tau}} \right)

In the limit as T → ∞ this becomes

P_c = \frac{1}{2} C V_o^2
 
Last edited:
Doh! I am a moron.

Thanks for the help.
 

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