Finding current and charge in a RC circuit.

AI Thread Summary
The discussion focuses on finding the current and charge in a resistor-capacitor (RC) circuit connected to a direct current battery. The user applies Kirchhoff's law to formulate the differential equation governing the circuit, leading to expressions for charge and current as functions of time. Initial conditions are clarified, with the assumption of zero charge at the moment the circuit is closed. The user derives the equations for charge, q(t), and current, i(t), confirming their correctness through integration. The conversation also touches on minor issues with LaTeX formatting in the equations.
U.Renko
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Homework Statement


A resistor with resistance R and a capacitor with capacitance C are connected in series to a direct current battery ε.
find the current and charge on the circuit as function of time.

it looks more like a review of differential equations, so I'm not really sure if I should post here or in the calculus forum...feel free to move it if you think it's better.

Homework Equations



potential at resistor: V_r = Ri

potential at capacitor:V_c = \frac{q}{C}

The Attempt at a Solution



Applying one of the Kirchhoff's law:
\epsilon - Ri - \frac{q}{C} = 0
\epsilon = Ri +\frac{q}{C}
since i = \frac{dq}{dt} we can rewrite the equation as

\frac{\epsilon}{R} = \frac{dq}{dt} + \frac{q}{RC} and solve with an integration factor e^{\frac{t}{RC}}
so we have:
\frac{\epsilon}{R} e^{\frac{t}{RC}} = \frac{d}{dt}(q e^{\frac{t}{RC}})
and then:

\int \frac{\epsilon}{R} e^{\frac{t}{RC}} dt = q e^{\frac{t}{RC}}


here I'm kinda stuck:
because the problem did not give any initial conditions, should I just solve an indefinite integral or integrate from zero to an arbitrary t??

also: q e^{\frac{t}{RC}} comes from integrating \int_{a}^{b} \frac{d}{dt}(q e^{\frac{t}{RC}})dt and applying the fundamental theorem of calculus.
However, don't I need the values a and b to properly use it?
 
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The resistor and capacitor are connected in series to a battery. You can count the time from the instant when you close the circuit. At that instant you can assume zero charge on the capacitor, if it is not stated otherwise.

The differential equation for q is correct,

\frac{\epsilon}{R} = \frac{dq}{dt} + \frac{q}{RC}

Solve for q(t) with the initial condition q(0)=0. ehild
 
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hmm let's see:

\int_{0}^{t} \frac{\epsilon}{R}e^{\frac{t}{RC}}dt = qe^{\frac{t}{RC}
solving the left hand side by substitution gives:
C\epsilon\left(e^{\frac{t}{RC} -1 \right) = qe^{\frac{t}{RC}
and so:

q(t)= e^{\frac{-t}{RC}C\epsilon\left(e^{\frac{t}{RC} -1 \right)

q(t)= C\epsilon\left(1-e^{\frac{-t}{RC} \right)
and
i(t) = \frac{\epsilon}{R}e^{\frac{-t}{RC}

is that correct?
 
Last edited:
U.Renko said:
hmm let's see:

$$\int_{0}^{t} \frac {\epsilon}{R} e^{\frac{t}{RC}}dt = q e^{\frac{t}{RC}}$$
solving the left hand side by substitution gives:
$$C\epsilon \left (e^{\frac{t}{RC}} -1 \right) = qe^{\frac{t}{RC}}$$
and so:

$$q(t)= e^{\frac{-t}{RC}}C\epsilon \left (e^{\frac{t}{RC}} -1 \right)$$

$$q(t)= C \epsilon \left(1-e^{\frac{-t}{RC}} \right)$$
and
$$i(t) = \frac {\epsilon}{R}e^{\frac {-t}{RC}}$$

is that correct?

Made some corrections. Are these the equations you meant?
 
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And if so, then yes, you are correct.
 
yes, that is what I meant.

I honestly don't know where I messed up with the LaTeX though...
 
U.Renko said:
yes, that is what I meant.

I honestly don't know where I messed up with the LaTeX though...

Just missed a few brackets here and there. That's enough to break it though haha
 
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