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Solutions to some interesting problems on Electrostatics of I.E. Irodov

Solutions to some interesting problems on Electrostatics of I.E. Irodov

ieirodov

I have often seen students seeing solutions for I.E. Irodov problems .. well its not wrong thing to look at solutions if you have tried yourself , but in all the books i have seen solutions are just given for sake of solution .. they do not focus on building concepts . And i got a chance to give some insight into concepts when i was invited by IITBANDA team to prepare an article for it .

I am adding a Disclaimer : i have taken problems from I.E. Irodov books( this is necessary as i have seen many materials copying questions from the book and do not giving due credits to them) .

One more thing If you really want to gain concept solving problems , then I.E. Irodov is must even though questions in iit are not of that level that used to come in late nineties but the concepts are same and you can only make concepts while analyzing & solving problems .

3.132

What amount of heat will be generated in the circuit shown in after the switch Sw is shifted from position I to position 2?.

clip_image002

Sol : Let us find first charge distribution, when switch is connected to 1

c and co in parallel

clip_image004 … (1)

clip_image006

Let us apply Kirchhoff’s law in the loop shown in fig.

clip_image008 … (2)

Solving (1) and (2)

clip_image010

clip_image012

clip_image014

If we carefully observe the ck + 1 and ck + 2. The only difference between two circuit is charge of polarity of the battery.

So, on change of polarity of battery, the charges on both the plate of each capacitor will just change in polarity.

Here we have to find that in charge redistribution how much charge has flown through the battery clip_image016.

clip_image018

When switch is connected to 2

A charge qo will flow from left most capacitor and pass through the battery and get deposited on middle capacitor.

Some amount of charge will flow from rightmost capacitor and get deposited on the middle capacitor but in this process, it does not have to pass through the battery.

Now, work done by the battery is equal to product of charge transferred and emf of the battery

Here, qo charge has passed through the battery

So, work done by battery on the system is equal of increase in electrostatic energy stored in the circuit and heat generated.

clip_image020

clip_image022 is work done by battery on the circuit

clip_image024 is work done by battery on the circuit

clip_image026 is het generated in the circuit

Now, clip_image028

Since, polarity of charges on capacitor has changed only, the magnitude of charge have remained unchanged. So, the electrostatic energy will not change clip_image030

clip_image026[1] Hence, clip_image033

So, heat generated clip_image035

3.133

What amount of heat will be generated in the circuit shown in after the switch Sw is shifted from position 1 to position 2?

clip_image037

When Sw is connected to 1 charge on capacitor c is

clip_image039

clip_image041

Electrostatic energy stored on capacitor

clip_image043

When Sw is shifted to 2

Charge on capacitor will change to clip_image045. Battery clip_image047 is out of the circuit and has no significance now.

clip_image049

Charge which has passed through the capacitor is equal to clip_image051.

Work done by battery on the system

clip_image022[1] = charge transferred × clip_image054

= clip_image056

Now, electrostatic energy stored in circuit

clip_image058

Change in electrostatic energy of circuit

clip_image060

= clip_image062

As in last question

clip_image064 Heat generated clip_image066

Q. 3.134  A  system Consists of two thin concentric metal shells of radii R1 and R2 with corresponding charges q1 & q2 .Find the self-energy values W1 & W2  of each shell , the interaction energy of the two shell w12 & total energy ?

Self energy of inner shell

(Refer to the article on work and energy in electrostatics)

clip_image070

clip_image072

Self energy of outer shell

clip_image074

Now, we have to calculate electrostatic interaction energy of the two shells.

If the electrostatic potential due to first charge configuration is same at each and every point where second charge is distributed then electrostatic interaction energy between two shells will be given by electrostatic potential due to first charge distribution at the point where second charge is distributed multiplied by total magnitude of second charge. Its vice–versa is also true

So, clip_image076

where clip_image078 is potential due to shell on the second shell and clip_image080 is potential due to second shell on first shell.

3135

Volume charge density

clip_image084

clip_image086

Electric field inside the

clip_image088

= clip_image090

Electric field outsides the sphere

clip_image092

To electrostatic energy is given by

clip_image094

= clip_image096

= clip_image098

First term W1 denote the electrostatic energy inside the charge distribution and second term W2 denotes the electrostatic energy outside the charge distribution.

clip_image100

= clip_image102

clip_image104

= clip_image106

So, the electrostatic self energy of ball

clip_image108

Ratio of the energy w1, stored in the ball to the energy w2 pervading the surrounding space

clip_image110

3136

Electric field inside the dielectric

clip_image114

clip_image116

Electrostatic energy stored inside the dielectric

clip_image118

= clip_image120

= clip_image122

= clip_image124

3.137  A spherical Shell of Radius R1 with uniform charge q is expanded to a radius R2 . Find the work performed by the electric force in this process ?

Sol : Electrostatic energy of spherical shell of radius R,

clip_image128

clip_image130

work performed by the electric forces is at the cost of electrostatic energy

clip_image132

So, work done electric forces

= clip_image134

= clip_image136

3.138 A spherical shell of radius R 1 with a uniform charge q hasa point charge q0 at its centre. Find the work performed by the electric forces during the shell expansion fromradius R1 to radius R2

W1 = Self energy of point charge = 0

W2 = Self energy of charge spericalshell = clip_image138

clip_image140

W12 = Electrostatic energy between point charge and charged spherical shell = potential due to point charge at the charged spherical sheel × charge on spherical shell

= clip_image142

Total electrostatic energy = clip_image144

= clip_image146

= clip_image148

Work performed by the electric forces during the shell expansion from radius clip_image150 to radius clip_image152

clip_image154

process?
3.t42. Inside a parallel-plate capacitor there is a plate parallel
to the outer plates, whose thickness is equal to l = 0.60 of the gap
width. When the plate is absent the capacitor capacitance equals
c —– 20 nF. First, the capacitor was connected in parallel to a cons-
tant voltage source producing V = 200 V, then it was disconnected
from it, after which the plate was slowly removed from the gap.
Find the work performed during the removal, if the plate is
(a) made of metal; (b) made of glass.

process?

3.142. Inside a parallel-plate capacitor there is a plate parallel to the outer plates, whose thickness is equal to l = 0.60 of the gap width. When the plate is absent the capacitor capacitance equals c —– 20 nF. First, the capacitor was connected in parallel to a constant voltage source producing V = 200 V, then it was disconnected from it, after which the plate was slowly removed from the gap.Find the work performed during the removal, if the plate is

(a) made of metal; (b) made of glass.

clip_image158

Capacitance of capacitor without plate = C (given)

Capacitance of capacitor of with plate

clip_image160

= clip_image162

When capacitor is connected to constant voltage source producing voltage v, it will get immediately charged to c’v when voltage source is disconnected, capacitor will become isolated and its charge will remain constant when plate is removed, external agency has to do work against the electric forces as shown in fig.

clip_image164

When dielectric is placed two capacitor plates, it get polarized and surface charges appear on dielectric plate. These surface charges are pulled by charges on capacitor plates. So external agency pulling the dielectric plate has to apply force to pull the dielectric plate and do work on the system. The work done by external agency will be stored as electrostatic energy in capacitor. In this process, the charge on capacitor will remain constant because capacitor is isolated.

Work done by external agency in pulling the capacitor can be found out by taking difference of electrostatic energy of capacitor without plate and that of with plate

clip_image166

where q = c’v

clip_image168

clip_image170

This is the case when dielectric is made of glass and clip_image172 is dielectric constant of glass.

If dielectric is made of metal, we just have to make clip_image174 in our final answer.

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6 Responses to “Solutions to some interesting problems on Electrostatics of I.E. Irodov”

  1. himanshu svt says:

    I WANT TO KNOW THE METHOD HOW TO SOLVE MAGNETOSTATIC PROBLEMS

  2. ravi says:

    this article is really lovely

  3. deepak says:

    very nice but there is a mistake que 3 130 in calculation of delta u

  4. deepak says:

    sry que 3 130

  5. ganesh says:

    time to solve i e book for iit target std.

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