Problem #1
How many 1.00 μF capacitors must be connected in parallel to store a charge of 1.00 C with a potential of 110 V across the capacitors?Answer;
Known:
Capacitances N capasitor is C = 1.00 μF, with N is the number of capacitors
potential across the capacitors is V = 110 V
charge, q = 1.00 C
Hence the number of parallel arranged capacitors is given by
NC = q/V
N = q/VC = 1.00 C/(1.00 x 10─6 F x 110 V) = 9091 capacitors
Problem #2
Each of the uncharged capacitors in Fig. 01 has a capacitance of 25.0 μF. A potential difference of V = 4200 V is established when the switch is closed. How many coulombs of charge then pass through meter A?
Fig.01 |
Capacitors connected in parallel can be replaced with an equivalent capacitor that has the same total charge q and the same potential difference V as the actual capacitors.
The total capasitance CP of the parallel caacitors of C given by
CP = 3C
CP = 3 x 25.0 μF = 75 μF
Then
qA = CPV = (75μF)(4200 V) = 315 mC
Problem #3
Figure 02 shows a variable “air gap” capacitor for manual tuning. Alternate plates are connected together; one group of plates is fixed in position, and the other group is capable of rotation. Consider a capacitor of n = 8 plates of alternating polarity, each plate having area A = 1.25 cm2 and separated from adjacent plates by distance d = 3.40 mm. What is the maximum capacitance of the device?
Fig.02 |
Known:
number of identical capacitors, n = 8
each plate having area A = 1.25 cm2 = 1.25 x 10-4 m2
distance d = 3.40 mm = 3.40 x 10-3 m
For maximum capacitance the two groups of plates must face each other with maximum area. In this case the whole capacitor consists of (n – 1) identical single capacitors connected in parallel. Each capacitor has surface area A and plate separation d so its capacitance is given by
C0 = e0A/d.
Thus, the total capacitance of the combination is
C = (n – 1)C0 = (n – 1)(e0A/d)
= (8 – 1)(8.85 x 10-12 C2/N.m2)(1.25 x 10-4 m2)/(3.40 x 10-3 m)
C = 2.72 x 10-12 F = 2.71 μF
Problem #4
In Fig. 03, the capacitances are C1 = 1.0 μF and C2 = 3.0 μF, and both capacitors are charged to a potential difference of V = 100 V but with opposite polarity as shown. Switches S1 and S2 are now closed. (a) What is now the potential difference between points a and b? What now is the charge on capacitor (b) 1 and (c) 2?
Fig.03 |
The charge on each cap. before switches are closed is;
Q1 = C1V0 = 100 μF x 100 V = 104 μC
Q2 = C2V0 = 300 μF x 100 V = 3 x 104 μC
When the switches are closed the charge redistributes into q1 and q2 but the total charge is less because of the initial reverse polarity. The total is;
q1 + q2 = Q2 – Q1
C1V + C2V = C2V0 - C1V0
V = (C2 – C1)V0/(C2 + C1)
= (3.0 μF – 1 0 μF)100 V/(3.0 μF + 1.0 μF)
V = 50 Volt
This is the final voltage across either capacitor (they are in parallel) which is also the voltage Vab, so
Vab = 50 Volt
(b) the charge on capacitor 1 is
Q1 = C1V0 = 100 μF x 50 V = 5 x 103 μC = 5 mC
(b) the charge on capacitor 2 is
Q1 = C1V0 = 300 μF x 50 V = 15 x 103 μC = 15 mC
Problem #5
In Fig. 04, V = 10 V, C1 = 10 μF, and C2 = C3 = 20 μF. Switch S is first thrown to the left side until capacitor 1 reaches equilibrium. Then the switch is thrown to the right. When equilibrium is again reached, how much charge is on capacitor 1?
Answer:
Switch to left
Initial charge on C1
Q1 = C1V0 = 10 μF x 10 V = 100 μF
capacitor C2 and C3 are in parallel
C23 = C2 + C3 = 40 μF
Switch to right
Charge is conserved:
Q = Q1 + Q23
C1V0 = C1V1 + C23V23 with V1 = V23 = V, then
C1V0 = C1V + C23V
V = C1V0/( C1 + C23) = (10 μF)(10 V)/(10 μF + 40 μF) = 2.0 V = V1 = V23
So that
Q1 = C1V = 10 μF x 2.0 V = 20 μC and
Q23 = C23V = 40 μF x 2.0 V = 80 μC
Problem #6
In Fig. 05, two parallel-plate capacitors (with air between the plates) are connected to a battery. Capacitor 1 has a plate area of 1.5 cm2 and an electric field (between its plates) of magnitude 2000 V/m. Capacitor 2 has a plate area of 0.70 cm2 and an electric field of magnitude 1500 V/m. What is the total charge on the two capacitors?
Answer:
Known:
Capacitor 1 has a plate area, A1 = 1.5 cm2 = 1.5 x 10─4 m2
electric field in capacitor 1, E1 = 2000 V/m
Capacitor 2 has a plate area, A2 = 0.7 cm2 = 7 x 10─5 m2
electric field in capacitor 1, E2 = 1500 V/m
the capacitance of each capacitor is
C1 = ϵ0A1/d1
C2 = ϵ0A2/d2
The relationship between the electric field and electric potential is given by
E = V/d, then V = Ed
the electric charge on each capacitor is
Q1 = C1V = (ϵ0A1/d1)E1d1 = ϵ0A1E1 and
Q2 = C2V = (ϵ0A2/d2)E2d2 = ϵ0A2E2
then, the total charge on the capacitor is
Q = Q1 + Q2 = ϵ0(A1E1 + A2E2)
Q = 8.85 x 10-12 C2/N.m2[(1.5 x 10─4 m2 x 2000 V/m + (0.7 x 10─4 m2 x 1500 V/m)
Q = 3.58 pC
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