Repeat Problem 67 for the same two capacitors but with them now connected in parallel.

Short Answer

Expert verified
  1. Equivalent capacitance is10.0μF
  2. Charge q1is1.20×10-3C
  3. Potential difference on capacitor 1 is 200 V
  4. Charge q2is 8×10-4C.
  5. Potential differenceV2 on capacitor 2 is 200 V

Step by step solution

01

The given data

a) Capacitance,C1=6.00μF

b) Capacitance,C2=4.00μF

c) Potential of battery,V=200V

d) Here given capacitors in parallel.

02

Understanding the concept of the equivalent capacitance

We first find the equivalent capacitance of the parallel combination and then using the relation of charge and capacitance we find the charge on each capacitor and the potential difference across it.

Formulae:

The equivalent capacitance of a parallel connection of capacitors,

Cequivalent=Ci …(i)

The charge stored between the plates of the capacitor,q=CV …(ii)

03

(a) Calculation of the equivalent capacitance

Since two capacitors are in parallel their equivalent capacitance is given using the equation (i) by,

Ceq=6.00μF+4.00μF=10.0μF

Hence, the value of the capacitance is 10.0μF.

04

(b) Calculation of the charge, q1

Since the two capacitors are now parallel, the potential difference across both the capacitors is same but charge is different.

Thus, the value of the charge of capacitor 1 is given using equation (ii) as:

q1=6.00μF×200V=1200μC=1.2×10-3C

Hence, the value of the charge is 1.20×10-3C.

05

(c) Calculation of the potential difference, V1

Since the two capacitors are now parallel, the potential difference across both the capacitors is same. That is given by,

V1=V=200V

Hence, the value of the potential difference is 200V.

06

(d) Calculation of the charge, q2

The charge onC2 is given using the data in equation (ii) as follows:

q2=4.00μF×200V=8×10-4C

Hence, the value of the charge is 8×10-4C.

07

(e) Calculation of the potential difference,V2

Since the two capacitors are now parallel the potential difference across both the capacitors is same.

Hence, the value of the potential difference across capacitor 2 is 200V.

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Most popular questions from this chapter

In Fig. 25-36, the capacitances areC1=1.0μFand C2=3.0μF, and both capacitors are charged to a potential difference ofV=100Vbut with opposite polarity as shown. Switches S1 and S2 are now closed. (a) What is now the potential difference between points aand b? What now is the charge on (b) capacitor 1 and (c) capacitor 2?

A parallel plate capacitor has a capacitance of 100pF , a plate area of , and a mica dielectric (k=5.4) completely filling the space between the plates. At 50 V potential difference,(a) Calculate the electric field magnitude E in the mica? (b) Calculate the magnitude of free charge on the plates (c) Calculate the magnitude of induced surface charge on the mica.

Figure 25-22 shows an open switch, a battery of potential difference, a current-measuring meter A, and three identical uncharged capacitors of capacitance C. When the switch is closed and the circuit reaches equilibrium, what is (a) the potential difference across each capacitor and (b) the charge on the left plate of each capacitor? (c) During charging, what net charge passes through the meter?

You have many 2.0μFcapacitors, each capable of withstanding 200 Vwithout undergoing electrical breakdown (in which they conduct charge instead of storing it). How would you assemble a combination having an equivalent capacitance of (a)0.40μFand (b)1.2μF, each combination capable of withstanding 1000 V?

Figure 25-54 shows capacitor 1 (C1=8.00μF), capacitor 2 (C2=6.00μF), and capacitor 3(C3=8.00μF) connected to a 12.0 V battery. When switch S is closed so as to connect uncharged capacitor 4 (C4=6.00μF), (a) how much charge passes through point Pfrom the battery and (b) how much charge shows up on capacitor 4? (c) Explain the discrepancy in those two results.

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