When capacitors are connected in series, the reciprocal of the equivalent capacitance Ceq C_{\text{eq}} Ceq is the sum of the reciprocals of the individual capacitances:
1Ceq=1C1+1C2 \frac{1}{C_{\text{eq}}} = \frac{1}{C_1} + \frac{1}{C_2} Ceq1=C11+C21
Substituting the given values:
1Ceq=16.00 μF+116.0 μF \frac{1}{C_{\text{eq}}} = \frac{1}{6.00 \, \mu \mathrm{F}} + \frac{1}{16.0 \, \mu \mathrm{F}} Ceq1=6.00μF1+16.0μF1
1Ceq=16.00+116.0=16+696=2296 \frac{1}{C_{\text{eq}}} = \frac{1}{6.00} + \frac{1}{16.0} = \frac{16 + 6}{96} = \frac{22}{96} Ceq1=6.001+16.01=9616+6=9622
Ceq=9622≈4.3636 μF C_{\text{eq}} = \frac{96}{22} \approx 4.3636 \, \mu \mathrm{F} Ceq=2296≈4.3636μF
The total voltage across the series combination is the sum of the voltages across each capacitor. The charge Q Q Q on each capacitor is the same, and is given by:
Q=Ceq×V=4.3636 μF×9.00 V=39.2724 μC Q = C_{\text{eq}} \times V = 4.3636 \, \mu \mathrm{F} \times 9.00 \, \mathrm{V} = 39.2724 \, \mu \mathrm{C} Q=Ceq×V=4.3636μF×9.00V=39.2724μC
The potential difference across each capacitor is given by:
V1=QC1=39.2724 μC6.00 μF≈6.5454 V V_1 = \frac{Q}{C_1} = \frac{39.2724 \, \mu \mathrm{C}}{6.00 \, \mu \mathrm{F}} \approx 6.5454 \, \mathrm{V} V1=C1Q=6.00μF39.2724μC≈6.5454V
V2=QC2=39.2724 μC16.0 μF≈2.4545 V V_2 = \frac{Q}{C_2} = \frac{39.2724 \, \mu \mathrm{C}}{16.0 \, \mu \mathrm{F}} \approx 2.4545 \, \mathrm{V} V2=C2Q=16.0μF39.2724μC≈2.4545V
Since the capacitors are in series, the charge on each capacitor is the same:
Q1=Q2=39.2724 μC Q_1 = Q_2 = 39.2724 \, \mu \mathrm{C} Q1=Q2=39.2724μC
Ceq=4.3636 μF \boxed{C_{\text{eq}} = 4.3636 \, \mu \mathrm{F}} Ceq=4.3636μF
V1=6.5454 VV2=2.4545 V \begin{array}{l} \boxed{V_1 = 6.5454 \, \mathrm{V}} \\ \boxed{V_2 = 2.4545 \, \mathrm{V}} \end{array} V1=6.5454VV2=2.4545V
Q1=39.2724 μCQ2=39.2724 μC \begin{array}{l} \boxed{Q_1 = 39.2724 \, \mu \mathrm{C}} \\ \boxed{Q_2 = 39.2724 \, \mu \mathrm{C}} \end{array} Q1=39.2724μCQ2=39.2724μC
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