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Answer #1

We transformed the original ciruit combining the capacitors to obtain a LC circuit with

one capacitor as shown on the below image:

Where \frac{1}{C_{eq}} = \frac{1}{C_1} + \frac{1}{C_2} \rightarrow C_{eq} = \frac{C_1 * C_2}{C_1 + C_2} = 171,42 \mu F

Applying Kirchoff's loop rule to the circuit we obtain

-\frac{q}{C_{eq}} - L \frac{d i}{d t} = 0 , but i = \frac{d q}{d t} therefore \frac{d^2 q}{d t^2} = - \frac{1}{L C_{eq}} q

The solution of the diferential equation is an armonic function

q(t) = Q_{max} cos(\omega t + \phi), where \omega = \sqrt{\frac{1}{LC_{eq}}} .

SInce i = \frac{d q}{d t} , then i (t) = - I_{max} sin(\omega t + \phi) , where I_{max} = \omega Q_{max} .

The circuit resonant frecquency is \omega = \sqrt{\frac{1}{L C_{eq}}} = 165.88 \frac{1}{s} .

Applying this initial condition t = 0 s, \, q(0) = 0, I (0) = I_L(0) to

q(t) \, and \, I(t) we obtain \phi = \frac{3 \pi}{2}, \, and \, Q_{max} = \frac{I_{max}}{\omega}

The charge in the capacitor C_{eq} in t = 22.1 ms is

q(22.1 ms) = \frac{135*10^{-3} A}{165.88 s^{-1}} cos[(165.88 s^{-1}*22.1*10^{-3}) + \frac{3 \pi}{2}]

q(22.1 ms) = - 4.07*10^{-4} \, C

Since C_1 \, and \, C_2 are in parallel Q_1 = Q_2 = q(22.1 ms) = -4.07*10^{-4} C.

The potential difference between b and c is V_b - V_c = \frac{q}{C_{eq}} = -\frac{ 4.07*10^{-4} \, C}{171,42*10^{-6} F} = - 2.37 V

To find the capacitor C_1 maximum charge we consider that:

Q_{eq \, max} = Q_{1 \, max} = Q_{2 \, max} = \frac{I_{max}}{\omega} = \frac{135 *10^{-3} A}{165.88 s^{-1}} = 8.14*10^{-4} C

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