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nossren
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Homework Statement
Assume you have a fully charged capacitor with initial condition [itex]V(0) = V_0[/itex] connected in series to two resistors [itex]R_1[/itex] and [itex]R_2[/itex]. Derive an expression for the voltage over the capacitor with respect to time.
Homework Equations
1. Kirchhoff's voltage law [itex]\sum_n V_n = 0[/itex]
2. Ohm's law: [itex]V=RI[/itex]
3. Capacitance of capacitor: [itex]C = \frac{Q}{V}[/itex]
4. Current [itex]I = \frac{dQ}{dt}[/itex]
The Attempt at a Solution
If I "go" in the direction of the current, then the potential difference over both resistors are negative whereas it is positive over the capacitor, hence
[tex]V(t) - V_{R_{1}} - V_{R_{2}} = 0 = V(t) - R_1 I - R_2 I[/tex].
Which I can rewrite using the time derivative of Q (3 and 4 from above)
[tex]= V(t) - (R_1 + R_2)\frac{dQ}{dt} = V(t) - (R_1 + R_2)C\frac{dV(t)}{dt} = 0 \implies \frac{1}{(R_1 + R_2)C}V(t) - \frac{dV(t)}{dt} = 0[/tex].
By solving this differential equation, I get
[tex]V(t) = V_0e^\frac{t}{(R_1+R_2)C}[/tex]
which is wrong, because the voltage should decrease over time, so a more logical solution would be
[tex]V(t) = V_0e^{-\frac{t}{(R_1+R_2)C}}[/tex].
Is there something I have overlooked? Is Kirchhoff's law setup incorrectly (sign conventions)?
Any help is appreciated.