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The voltage across the capacitor has a phase angle of 106750 exactly 900 less than the phase angle of the circuit current. The capacitance describes how much charge can be stored on one plate of a capacitor for a given push voltage drop.

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Basically a capacitor will charge to the input dc level however it will mathematically never happen since capacitors charge at a certain rate the voltage drop across a capacitor will follow the r.

Voltage drop by capacitor. Applying kirchhoffs voltage law v is equal to the voltage drop across the resistor r. A very stretchy flexible membrane corresponds to a higher capacitance than a stiff membrane. And conversely the capacitor with the greater capacitance value will drop less voltage across it.
According to this formula the capacitor with the lower capacitance value will drop more voltage across it. A small capacitance value will result in a larger voltage while a large value of capacitance will result in a smaller voltage drop. This output voltage which is the voltage that is dropped across capacitor c2 is calculated by the formula vout vin c1c1 c2.
As the charge q is equal and constant the voltage drop across the capacitor is determined by the value of the capacitor only as v q c. For a discharging capacitor the voltage across the capacitor v discharges towards 0. This tells us that the capacitors voltage and current are still 900 out of phase with each other.
The current i through the resistor is rewritten as above and substituted in equation 1. By integrating and rearranging the above equation we get.

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