Answer:
a) Q1=Q2=480μC V1=240V V2=60V
b) Q1=96μC Q2=384μC V1=V2=48V
c) Q1=Q2=0C V1=V2=0V
Explanation:
Let C1 = 2μC and C2=8μC
For part (a) of this problem, we know that charge in a series circuit, is the same in C1 and C2. Having this in mind, we can calculate equivalent capacitance first:
[tex]C=\frac{1}{\frac{1}{C1} +\frac{1}{C2} } = 1.6\mu C[/tex]
[tex]Q_{T} = V_{T}*C_{T} = 480\mu C[/tex]
[tex]V1 = \frac{Q1}{C1}=240V[/tex]
[tex]V2 = \frac{Q2}{C2}=60V[/tex]
For part (b), the capacitors are in parallel now. In this condition, the voltage is the same for both capacitors:
[tex]V1=V2[/tex] So, [tex]\frac{Q1}{C1} = \frac{Q2}{C2}[/tex]
Total charge is the same calculated for part (a), so:
[tex]\frac{Qt - Q2}{C1} = \frac{Q2}{C2}[/tex] Solving for Q2:
Q2 = 384μC Q1 = 96μC.
Therefore:
V1=V2=48V
For part (c), both capacitors would discharge, since their total voltage of 300V would by applied to a wire (R=0Ω). There would flow a huge amount of current for a short period of time, and capacitors would be completely discharged. Q1=Q2=0C V1=V2=0V