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KENDRIYA VIDYALAYA, ITBP,DEHRADUN Remedial measures/revision Unit-I (Electrostatics)

โ€“ XII (PHYSICS)

Notes/Important FAQs/Graded Assignments

page -01

Part (A)-VSA & SA Questions 1. Answer the following : 1. State Coulombโ€™s law in electrostatics.

CBSE(F)-2003,(AIC)-2001

[ Ans. Coulombโ€™s law :The electrostatic force of attraction or repulsion between any two stationary point charges is directly proportional to the product of magnitude of charges and is inversely proportional to the square of the distance between them. i,e, ๐น

โˆ

๐‘ž1 ๐‘ž2

๐‘ž

โ—โ—๐‘ž2

๐‘Ÿ2 1 1 ๐‘ž1 ๐‘ž2

โ‡จ๐น = 4๐œ‹๐œ€

0

๐‘Ÿ2

๐’“

2. Write Coulombโ€™s law in vector form. What is the importance of expressing it in vector form ?CBSE (AIC)-2011

[ Ans. Coulombโ€™s law in vector form :

โƒ—โƒ—โƒ— โƒ—โƒ—โƒ— 1 ๐‘ž1 ๐‘ž2 1 ๐‘ž1 ๐‘ž2 ๐‘Ÿ 1 ๐‘ž1 ๐‘ž2 ๐‘Ÿ ๐’“ฬ‚ = = 2 2 2 4๐œ‹ ๐œ€0 ๐‘Ÿ 4๐œ‹ ๐œ€0 ๐‘Ÿ |๐‘Ÿ| 4๐œ‹ ๐œ€0 ๐‘Ÿ ๐‘Ÿ3 โƒ—โƒ—โƒ— 21 = โˆ’๐น โƒ—โƒ—โƒ— 12 = โˆ’๐’“ฬ‚12 โ‡จ๐น โƒ—โƒ—โƒ— = ๐น

ฬ‚ 21 Importance :(i) As ๐’“ Which shows that coulombโ€™s force obey Newtonโ€™s third law of motion (ii) As the Coulombโ€™s force acts along charges, so they are central forces

โƒ—โƒ—โƒ— 21 ๐‘œ๐‘Ÿ โˆ’ ๐น โƒ—โƒ—โƒ— 12, i,e, along the line joining the centres of two ๐น

3. Write any two limitations of Coulombโ€™s law. CBSE(AIC)-2001 [ Ans.(i) charges must be stationary point charges (ii) distance between the point charges ๐‘Ÿ > 10โˆ’15 ๐‘š

4. (a) Name any two basic properties of electric charge. (b) What does ๐‘ž1 + ๐‘ž2 = 0 signify in electrostatics ?CBSE(F)-2003,(AIC)-2001

[ Ans. (a) (i) Quantization of charge (ii) Conservation of charge (b) Itsignifies that charges are algebraically additive and here ๐‘ž1 &๐‘ž2 are equal and opposite

5.Is the force acting between two point electric charges q1 and q2 kept at some distance apart in air, attractive or repulsive when (a) q1 q2> 0 (b) q1 q2< 0 ? CBSE (F)-2007,2003 [ Ans. (a) when q1q2> 0,force is repulsive (b) when q1q2< 0,force is attractive

6. Two insulated charged copper spheres ๐ด and ๐ต of identical size have charges ๐‘ž๐ด and โˆ’3๐‘ž๐ด respectively. When they arebrought in contact with each other and then separated, what are the new charges on them ? CBSE (F)-2011 [ Ans. Charge on each sphere =

๐‘ž1 +๐‘ž2 2

=

๐‘ž๐ด โˆ’3๐‘ž๐ด 2

= โˆ’๐‘ž๐ด

7. Define dielectric constant of a medium in terms of force between electric charges. What is its S.I. unit ? CBSE (AI)-2015 [Ans. Dielectric constant:It is defined as the ratio of the force (๐น๐‘ฃ๐‘Ž๐‘๐‘ข๐‘ข๐‘š ) between any two point charges placed at certain distance apart in vacuum to the force (๐น๐‘š๐‘’๐‘‘๐‘–๐‘ข๐‘š ) between them when placed at equaldistance in that medium i,e, ๐พ =

๐น๐‘ฃ๐‘Ž๐‘๐‘ข๐‘ข๐‘š It has no unit ๐น๐‘š๐‘’๐‘‘๐‘–๐‘ข๐‘š

8. How does the Coulomb force between two point charges depend upon the dielectric constant of the intervening medium ? [Ans.๐น =

๐‘ž1 ๐‘ž2 1 4๐œ‹ ๐œ€0 ๐พ ๐‘Ÿ2

โ‡จ๐น โˆ ๐พ1 CBSE (AI)-2005

Coulombโ€™s force varies inversely with the dielectric constant of medium

9. Two same balls having equal positive charge โ€ฒ๐‘žโ€ฒ Coulombs are suspended by two insulating strings of equal length. What would be the effect on the force when a plastic sheet is inserted between the two ?CBSE (AI)-2014 [Ans.๐น =

๐‘ž1 ๐‘ž2 1 4๐œ‹ ๐œ€0 ๐พ ๐‘Ÿ2

โ‡จ๐น โˆ ๐พ1 But for plastic๐พ > 1hence the force between the two balls will decrease

10. Force between two point electric charges kept at a distance d apart in air is F. If the charges are kept at the same distance in water, how does the force between them change ? CBSE (AI)-2011 [Ans.๐น๐‘ค๐‘Ž๐‘ก๐‘’๐‘Ÿ =

๐น๐‘Ž๐‘–๐‘Ÿ ๐น = ๐พ 80

11. Two point charges having equal charges separated by 1๐‘šdistance experience a force of 8๐‘. What will be theforce experienced by them, if they are held in water, at the same distance ? (๐บ๐‘–๐‘ฃ๐‘’๐‘› โˆถ ๐พ๐‘ค๐‘Ž๐‘ก๐‘’๐‘Ÿ = 80 )CBSE (AIC)-2011 [Ans.๐น๐‘ค๐‘Ž๐‘ก๐‘’๐‘Ÿ =

๐น๐‘Ž๐‘–๐‘Ÿ 8 = = 0.1๐‘ ๐พ 80

==================================================================================

KENDRIYA VIDYALAYA, ITBP,DEHRADUN Remedial measures/revision Unit-I (Electrostatics)

โ€“ XII (PHYSICS)

Notes/Important FAQs/Graded Assignments

page -02

Part (A)-VSA & SA Questions 2. Answer the following : 1. Does the charge given to a metallic sphere depend on whether it is hollow or solid ? Give reason for your answer. [Ans.No, Because the charge resides only at the surface of conductorCBSE (D)-2017 2. A comb run through oneโ€™s dry hair attracts small bits of paper. Why ? What happens if the hair is wet or if it is a rainy day ? NCERT-2017 [ Ans.When a comb is run through dry hair, it gets charged due to friction. Molecules in the paper gets polarized by the charged comb resulting in a net force of attraction. If the hair is wet or it is a rainy day, friction reduces, comb does not get charged and thus it will not attract small bits of paper

3. Define electric field intensity. Write its S.I. unit. Is it a scalar or vector quantity ?CBSE (D)-2007

[ Ans. Electric field intensity :Electric field intensity at any pointis defined as the electrostatic force acting on vanishingly small unit positive test charge placed at that point โƒ—โƒ—โƒ—โƒ— โƒ—โƒ—โƒ— = lim ๐น i,e,๐‘ฌ

๐‘ž0 โ†’0 ๐‘ž0

Its. S.I. unit is ๐‘ต/๐‘ช. It is a vector quantity.

4. The electric field intensity at any point is defined as lim

๐น

๐‘ž0 โ†’0 ๐‘ž0

this expression ?CBSE (D)-2007

. What is the physical significance of the term lim in ๐‘ž0 โ†’0

[Ans.The term lim indicates that the test charge ๐‘ž0 is small enough so that its presence does not affect the ๐‘ž0 โ†’0

distribution of source charge and hence does not change the value of electric field

5. (i) What is the physical significance of electric field ? (ii) Write an expression for force acting on a test charge ๐‘ž0 placed in a uniform electric field.

CBSE (D)-2007

[Ans. (i) It gives themagnitude&direction of electric force (๐น )experienced by any charge placed at any point. (ii)๐น = ๐‘ž0 ๐ธโƒ— 6. A proton is placed in a uniform electric field directed along the positive x-axis. In which direction will it tend to move ? [Ans.+x-axis, i,e, along the direction of electric fieldCBSE (DC)-2011

7. Why must electrostatic field at the surface of a charged conductor be normal to the surface at every point? Give reason.CBSE (AI)-2015,2002,(F)-2014,(AIC)-2002 โƒ— . โƒ—โƒ—โƒ—โƒ— [Ans.๐ธ ๐‘‘๐‘Ÿ = ๐‘‘๐‘‰but at the surface of a conductor ๐‘‰ = constant โƒ—โƒ—โƒ—โƒ— โƒ— โ‡จ๐ธ. ๐‘‘๐‘Ÿ = 0โ‡จ๐ธ๐‘‘๐‘Ÿ cos ๐œƒ =0โ‡จ๐œƒ = 900 Hence electric field at the surface of a charged conductor is always normal to the surface at every point ==================================================================================

3. Answer the following : 1. Define electric potential at a point. Write its S.I. unit. Is potential a scalar or vector ?CBSE (AI)-2015

[Ans. Electric Potential (๐‘ฝ) : Electric potential at any point in an electric field may be defined as the work done by an external force in bringing a unit positive charge from infinity to that point i,e,

๐‘‰๐ด =

๐‘Šโˆž๐ด ๐‘ž0

Itโ€™s S.I. unit is J/C or Volts (V) . It is a scalar quantity.

2. Name the physical quantity whose S.I. unit is J๐ถ โˆ’1 .Is it a scalar or vector quantity ?CBSE (AI)-2010 [Ans.Potential, it is a scalar quantity

3. Why is the potential inside a hollow spherical charged conductor constant and has the same value as on its surface ? [Ans.|๐ธ|

=

๐‘‘๐‘‰ ๐‘‘๐‘Ÿ

โ‡จ๐‘‘๐‘‰ = |๐ธ|๐‘‘๐‘ŸCBSE (F)-2012,(D)-2012

As inside the hollow spherical conductor

๐ธ=0

โ‡จ๐‘‘๐‘‰ = 0โ‡จ๐‘‰ =constant

4. A hollow metal sphere of radius 10 ๐‘๐‘šis charged such that the potential on its surface is 5 ๐‘‰. What is the potential at thecentre of the sphere ? CBSE (AI)-2011 [Ans.5 ๐‘‰, because potential of a metallic sphere remains unchanged inside the sphere 5.A point charge+๐‘„ is placed at a point ๐‘‚ as shown in the figure. Is the potential difference ๐‘‰๐ด โˆ’ ๐‘‰๐ต positive, negative or zero ?

[Ans.Positive as๐‘‰ =

1

๐‘ž

4๐œ‹๐œ€0 ๐‘Ÿ

โ‡จ๐‘‰ โˆ 1๐‘Ÿ ]CBSE (D)-2016

==================================================================================

KENDRIYA VIDYALAYA, ITBP,DEHRADUN Remedial measures/revision Unit-I (Electrostatics)

โ€“ XII (PHYSICS)

Notes/Important FAQs/Graded Assignments page -03

Part (A)-VSA & SA Questions 4. Answer the following : 1. Define electric line of force/electric field line.

CBSE (D)-2005,2003

[Ans.An electric field line may be defined as the imaginary straight or curved path, along which a unit positive, isolated charge would tend to move if free to do so.

2. State any two properties of electric field lines.

CBSE (D)-2005

[Ans.(i) Electric filed lines not form closed loops. They start from positive charge and end at negative charge (ii) Tangent to any point on the electric field line gives the direction of electric field at that point (iii) No two electric field lines can intersect each other (iv) They are always normal to the surface of a conductor

3. What is the importance of electric field lines ?CBSE (AIC)-2002 [Ans.Importance :(i) Tangent to any point on the electric field line gives the direction of electric field at that point (ii) Relative closeness of electric field lines indicates the strength of electric field

4. Why do the electrostatic filed lines not form closed loops ?CBSE (AI)-2015,2014

[Ans. Due to conservative nature of electric field/ These lines start from positive charges and terminates at the negative charges

5. Why do the electric field lines never cross each other ?CBSE (AI)-2014,2005,(D)-2003 [Ans. Because if they do so, at the point of intersection two tangents can be drawn, which would represent two directions of electric field at that point, which is not possible

6. Why do the electrostatic filed lines are always normal to the surface of a conductor ?CBSE (AI)-2009,(F)-2009 [Ans.If the field lines are not normal, then electric field ๐ธโƒ— would have a tangential component which will make electrons move along the surface creating surface currents and the conductor will not be in equilibrium

7. Draw the electric field lines of an isolated point charge Q when (i) ๐‘„ > 0 and (ii) ๐‘„ < 0.CBSE (D)-2007,2003 [Ans.(i)๐‘ธ > ๐ŸŽ(ii) ๐‘ธ < ๐ŸŽ

8. (i) Depict electric field lines due to two positive charges kept at a certain distance apart. CBSE (AI)-2015,(D)-2003 (ii) Depict electric field lines due to an electric dipole or due to two opposite charges kept at a certain distance apart. [Ans. (i) (ii)

9. (i)A point charge +๐‘„ is placed in the vicinity of a conducting surface. Trace the field lines between the charge and theconducting surface. CBSE (AIC)-2017,(AI)-2015,2009 (ii) Draw the electric field lines due to uniformly charged thin spherical shell when charge on the shell is (a) positive, (b) negative [Ans.(i) (ii) (a) (ii) (b)CBSE (D)-2008

10. A metallic sphere is placed in a uniform electric field as shown in the figure. Which path is followed by the electric field lines and why ? CBSE (AI)-2010 [Ans.Path 4 Reason :Electric field lines are normal at each point of the surface and there are no electric field lines within the metallic sphere ==================================================================================

KENDRIYA VIDYALAYA, ITBP,DEHRADUN Remedial measures/revision Unit-I (Electrostatics)

โ€“ XII (PHYSICS)

Notes/Important FAQs/Graded Assignments

page -04

Part (A)-VSA & SA Questions 5. Answer the following : 1.Define dipole moment. Write its S.I. unit. Is it a scalar or vector quantity ?CBSE (AI)-2013,2011, (D)-2012 [Ans. Dipole moment :The product of magnitude of either charge of the electric dipole and the length of dipole is known as the dipole moment. i,e,|๐‘| = ๐‘ž X |2๐‘Ž| Itโ€™sS.I. unit isCoulomb X metre (๐ถ๐‘š).

It is a vector quantity

2. What is the charge of an electric dipole ?CBSE (DC)-2010

[ Ans.Zero

3. An electric dipole is placed in a uniform electric field, what is the net force acting on it ?CBSE (DC)-2001

[ Ans.Zero

4. An electric dipole of dipole moment ๐‘ โƒ—โƒ—โƒ— is placed in a uniform electric field โƒ—โƒ—โƒ— ๐ธ . Write the value of the angle between โƒ—โƒ—โƒ— โƒ—โƒ—โƒ— and๐ธ for which the torque experienced by the dipole is minimum. ๐‘ CBSE (DC)-2009 [ Ans.Zero because ๐œ = p๐ธ sin ๐œƒ = 0 5.Depict the orientation of the dipole in (i) stable, (ii) unstable equilibrium in a uniform electric field.

CBSE (D)-2017,2010

[ Ans. (i) Stable equilibrium ๐œฝ = ๐ŸŽ(ii) Unstable equilibrium ๐œฝ = ๐Ÿ๐Ÿ–๐ŸŽ

6. Find the work done in rotating the dipole from stable to unstable equilibrium in a uniform electric field. [ Ans.Forstable equilibrium, ๐œฝ = ๐ŸŽ and for unstable equilibrium๐œฝ = ๐Ÿ๐Ÿ–๐ŸŽCBSE (AI)-2016,2015,2012

โ‡จ๐‘Š = p๐ธ(cos ๐œƒ1 โˆ’ cos ๐œƒ2) = p๐ธ(cos 0 โˆ’ cos 180)

= p๐ธ [1 โˆ’ (โˆ’1)]= 2p๐ธ 7. Find the work done in rotating the dipole from unstable to stable equilibrium in a uniform electric field. [ Ans.Forunstable equilibrium๐œฝ = ๐Ÿ๐Ÿ–๐ŸŽand forstable equilibrium, ๐œฝ = ๐ŸŽCBSE (AI)-2016

โ‡จ๐‘Š = p๐ธ(cos ๐œƒ1 โˆ’ cos ๐œƒ2) = p๐ธ(cos 180 โˆ’ cos 0)

= p๐ธ [โˆ’1 โˆ’ 1]= โˆ’2p๐ธ

==================================================================================

6. Answer the following : 1. Define electric flux. Write its S.I. unit. CBSE (AIC)-2017,(AI)-2015,2012,2008,(F)-2006,(D)-2007,2006 [ Ans.Electric flux :It is defined as the total number of electric lines of force passing normally through a given surface

๐œ™๐ธ = โˆฎ ๐ธโƒ— . โƒ—โƒ—โƒ—โƒ— ๐‘‘๐‘  Itโ€™s S.I. unit is๐‘๐‘š2 /๐ถ

2. State Gaussโ€™s law in electrostatics.

CBSE (AI)-2015,2012,2007,2004,(F)-2012,(D)-2008,2006,2004

[ Ans.Gaussโ€™s Law : โ€œ Electric flux passing through any closed surface is surfaceโ€. i,e, ๐œ™๐ธ

1 ๐œ–0

times the total charge enclosed by that

๐‘ž = โˆฎ ๐ธโƒ— . โƒ—โƒ—โƒ—โƒ— ๐‘‘๐‘  = ๐œ–

0

3. A charge ๐‘ž is enclosed by a spherical surface ๐‘…. If the radius is doubled/ reduced to half, how would the electric flux through the surface change ? CBSE (AI)-2009, (AIC)-2008,(DC)-2007 [ Ans.No changeas flux does not depend on radius/ shape /size of enclosing surface

4. A charge q is placed at the centre of a cube, what is the electric flux passing through one of its faces ?

[ Ans.๐œ™ = 16 (๐œ–๐‘„ )]CBSE (AI)-2012, (F)-2010 0

5. Consider two hollow concentric spheres, S1& S2, enclosing charges 2Q & 4Q respectively as shown. (i) Find out the ratio of the electric flux through them. CBSE (AI)-2014,2002 (ii) how will the electric flux through the sphere S 1 change, if a medium of dielectric constant๐œ–๐‘Ÿ is introduced in the space inside S1 in place of air ? Deduce the necessary expression. [ Ans.(i)๐œ™1

=

๐œ™1

โ‡จ๐œ™ =

2๐‘„

2

๐œ€0

(ii)๐œ™1

2๐‘„ ๐œ–0 ๐พ

=

2๐‘„ &๐œ™2 ๐œ€0

6๐‘„

=

2๐‘„+4๐‘„ ๐œ€0

=

6๐‘„ ๐œ€0

/ ๐œ€ =1/3 0

=

2๐‘„ ๐œ–0 ๐œ–๐‘Ÿ

=================================================================================

KENDRIYA VIDYALAYA, ITBP,DEHRADUN Remedial measures/revision Unit-I (Electrostatics)

โ€“ XII (PHYSICS)

Notes/Important FAQs/Graded Assignments

page -05

Part (A)-VSA & SA Questions 7. Answer the following : 1. (i) Define electric potential energy of a system of charges.CBSE (AI)-2015 (ii) Write an expression of electric potential energy of a system of two charges. [ Ans. (i)Electric potential energy of a system of charges : It isdefined as the total amount of work done in placing the charges to their respective positions to constitute the system, by bringing them from infinity (ii)๐‘ˆ

=

1 ๐‘ž1 ๐‘ž2 4๐œ‹๐œ–0 ๐‘Ÿ

2.The figure shows field lines of a positive point charge. What will be the sign of the potential energy deference of a small negative charge between the points ๐‘„ and ๐‘ƒ. Justify your answer. CBSE (AI)-2015, (F)-2014 [Ans. Positive Reason :๐‘ˆ

=

i,e, (๐‘ผ)๐‘ธ โˆ’ (๐‘ผ)๐‘ท > 0

1 ๐‘ž1 ๐‘ž2 4๐œ‹๐œ–0 ๐‘Ÿ

P.E. of a positive charge & a negative charge is negative hence P.E. of a negative charge is more negative at P, i,e, (๐‘ผ)๐‘ธ > (๐‘ผ)๐‘ท

3. Figure shows the field lines of a negative point charge. Give the sign of the potential energy deference of a small negative charge between the points ๐ด and ๐ต. CBSE (F)-2014 [Ans.Positive Reason :๐‘ˆ

=

i,e, (๐‘ผ)๐‘จ โˆ’ (๐‘ผ)๐‘ฉ > 0 1 ๐‘ž1 ๐‘ž2 4๐œ‹๐œ–0 ๐‘Ÿ

P.E. of two negative charges is positive hence P.E. of a negative charge is more positive at A, i,e, (๐‘ผ)๐‘จ > (๐‘ผ)๐‘ฉ

4.The figure shows field lines of a positive point charge. Is the work done by the field in moving a small positive charge from ๐‘„ to ๐‘ƒ is positive or negative ? Justify your answer. CBSE (F)-2014 [Ans. Negative, Reason :๐‘‰๐‘ƒ > ๐‘‰๐‘„ โ‡จ๐‘‰๐‘ƒ โˆ’ ๐‘‰๐‘„ > 0 But๐‘‰๐‘ƒ โˆ’ ๐‘‰๐‘„

=

๐‘Š๐‘„๐‘ƒ ๐‘ž0

โ‡จ๐‘Š๐‘„๐‘ƒ > 0

โ‡จWork done by external agency is positive โ‡จWork done by electric field is negative 5. The field lines of a negative point charge are as shown in the figure. Does the kinetic energy of a small negative charge increase or decrease in going from ๐ต to ๐ด ? CBSE (AI)-2015 [Ans. K.E. decreases Reason : As the negative charge moves from B to A, it experiences more repulsion, its velocity decreases and so, its K.E. decreases ==================================================================================

8. Answer the following 1.(i) Define an equipotential surface ? CBSE (AI)-2016,2015,2002,(D)-2003 (ii) Write any two properties of an equipotential surface. [ Ans. (i) Equipotential surface : A surface drawn in an electric fieldat which every point has the same potential, is known as equipotential surface (ii) Properties : (a) No work is done in moving a test charge from one point to another over an equipotential surface (b) Electric field is always normal to the equipotential surface at every point (c) No two equipotential surfaces can intersect each other (d) Equipotential surfaces are closer in regions of strong field and farther in regions of weak field

2. โ€œFor any charge configuration, equipotential surface through a point is normal to the electric field.โ€ Justify this statement. CBSE (AI)-2016,(D)-2014 [Ans.At an equipotential surface ๐‘‰1 = ๐‘‰2 Hence work done, ๐‘Š = ๐‘ž0 (๐‘‰1 โˆ’ ๐‘‰2 ) = 0

โ‡จ

F S cos ๐œƒ = 0,

โ‡จcos ๐œƒ = 0 โ‡จ๐œƒ = 900

KENDRIYA VIDYALAYA, ITBP,DEHRADUN Remedial measures/revision Unit-I (Electrostatics)

โ€“ XII (PHYSICS)

Notes/Important FAQs/Graded Assignments

page -06

Part (A)-VSA & SA Questions 9. Answer the following : 1. No work done in moving a charge from one point to another on an equipotential surface. Why ?CBSE (AIC)-2002 [Ans.We know for any two points on an equipotential surface ๐‘‰1 = ๐‘‰2 Hence work done, ๐‘Š = ๐‘ž0 (๐‘‰1 โˆ’ ๐‘‰2 ) = 0

2. Can electric field exist tangential to an equipotential surface ? Give reason.CBSE (AI)-2016

[Ans. No, It would mean some work will be done in moving charge from one point to another on equipotential surface which is not possible

3. Why do the equipotential surfaces due to uniform electric field not intersect each other ?CBSE (F)-2013,(D)-2009 [Ans.Because if they do so then at the point of intersection there will be two values of the electric potential, which is not Possible

4. Why the equipotential surfaces about a single charge are not equidistant ?CBSE (AI)-2016,2015,(DC)-2011 OR

Why does the separation between successive equipotential surfaces get wider as the distance from the charges increases ? [Ans.|๐‘ฌ| =

โ‡จ๐‘‘๐‘Ÿ =

๐‘‘๐‘‰ ๐‘‘๐‘Ÿ

๐‘‘๐‘‰ -------------(1)CBSE |๐‘ฌ|

As the distance increases, electric field

(AI)-2016

๐ธ (=

1

๐‘ž

4๐œ‹ ๐œ€0 ๐‘Ÿ 2

)decreases therefore from (1), ๐‘‘๐‘Ÿwill be large hence

large hence equipotential surfaces get wider. Thatโ€™s why equipotential surfaces are not equidistant

5. Draw an equipotential surface in a uniform electric field.

CBSE (F)-2008,2006,(D)-2001

[Ans.

6. Draw an equipotential surface and corresponding electric field lines for a single point charge(i)+๐‘ž (๐‘ž> 0)(ii)โˆ’๐‘ž(๐‘ž< 0). [Ans. (i)๐‘ž> 0(ii) ๐‘ž< 0CBSE (AI)-2016,(F)-2006,(D)-2001

7. (i) Draw the equipotential surfaces for an electric dipole.CBSE (AI)-2015 (ii)Draw the equipotential surfaces due to two equal positive point charges placed at a certain distance. [Ans. (i) dipole(ii) equal positive chargesCBSE (AI)-2015,(D)-2010

8. A charge โ€ฒ๐‘žโ€™ is being moved from a point ๐ด above a dipole of dipole moment โ€ฒ๐‘โ€ฒ to a point ๐ต below the dipole in equatorial plane without acceleration. Find the work done in the process. CBSE (AI)-2016 [Ans. Zero, as AB is an equipotential surface]

9. What is the amount of work done in moving a point charge ๐‘„ around a circular arc of radius โ€ฒ๐‘Ÿโ€ฒ at the centre of which another point charge โ€ฒ๐‘žโ€ฒ is located ? CBSE (AI)-2016 [Ans.zero] ==================================================================================

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โ€“ XII (PHYSICS)

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page -07

Part (A)-VSA & SA Questions 10. Answer the following : 1. Define the capacitance of a conductor. Write its S .I. unit.

CBSE (AIC)-2003

[Ans.It is defined as the charge required to raise the potential of conductor by unit amount. ๐‘ž

i,e,

๐ถ=๐‘‰

Its S.I. unit is Farad (๐น)

2. Define the capacitance of a capacitor. On what factors does it depends ?CBSE (F)-2017,(DC)-2001

[Ans.Capacitance :Capacitance of a capacitor may be defined as the ratio of magnitude of charge on itseither plate to the potential difference between them. ๐‘ž

i,e,

๐ถ=๐‘‰

Factors :(i) geometrical configuration (shape, size, separation) of the system of two conductors and (ii) nature of the medium separating the two conductors

3. Define dielectric constant of a medium in terms of capacitance.

CBSE (D)-2006

[ Ans. The dielectric constant of a medium may be defined as the ratio of capacitance of capacitor completely filled with that dielectric medium to the capacitance of the same capacitor with vacuum between its plates. i,e,๐พ

๐ถ

=๐ถ

0

4. A metal plate is introduced between the plates of a charged parallel plate capacitor. What is the effect on the capacitance of the capacitor ? CBSE (F)-2009 [ Ans. Capacitance increase as the effective separation between the plates is decreased

5. (i) Define the term polarization of a dielectric. CBSE (AI)-2016,2015,(D)-2015 โƒ—โƒ—โƒ— โƒ—โƒ—โƒ— . (ii) Write a relation for polarization ๐‘ƒ of a dielectric material in the presence of an external electric field ๐ธ [ Ans. (i) Polarization of a dielectric : Induced dipolemoment per unit volume, is called polarization๐‘ƒ (ii) Relation:โƒ—โƒ—โƒ— ๐‘ƒ =

๐Œ๐’† โƒ—โƒ—๐ธ

where๐Œ๐’† is theelectric susceptibilityof the dielectric medium

6. How is the electric field due to a charged parallel plate capacitor affected when a dielectric slab is inserted between the plates fully occupying the intervening region ? CBSE (F)-2010 [ Ans. Electric field decreasesdue to dielectric polarization and becomes

๐ธ = ๐ธ0 โˆ’ ๐ธ๐‘–๐‘› =

๐ธ0 ๐พ

7. The graph shows the variation of voltage V across the plates of two capacitors A and B versus increase of charge Q stored on them. Which of the capacitors has higher capacitance ? Give reason for your answer.CBSE (D)-2004 [ Ans. B has higher capacitance Reason :๐ถ If๐‘‰

๐‘ž

=๐‘‰

=constant then ๐ถ โˆ ๐‘ž

As ๐‘ž๐ต > ๐‘ž๐ด โ‡จ๐ถ๐ต > ๐ถ๐ด 8. A parallel plate capacitor of plate area ๐ด and separation ๐‘‘ is filled with dielectrics of dielectric constants ๐พ1 and as ๐พ2 shown in the figure. Find the net capacitance of the capacitor. CBSE (F)-2011 1 1 1 1 1 ๐‘‘/2 ๐‘‘/2 [ Ans.

โ‡จ

1

๐ถ

= ๐‘‘

๐ถ1

+

๐ถ2

1

=

๐พ1 ๐œ€0 ๐ด ๐‘‘/2

1

+

๐‘‘

๐พ2 ๐œ€0 ๐ด ๐‘‘/2

=

๐พ1 ๐œ€0 ๐ด

๐พ + ๐พ2

+

2๐พ

( + ๐พ ) = 2๐œ€ ๐ด ( ๐พ1 ๐ด ๐พ

๐พ2 ๐œ€0 ๐ด

๐พ

)โ‡จ๐ถ = (๐พ1+1 ๐พ22) ๐ถ0 ๐ถ 2๐œ€0 1 2 0 1 ๐พ2 9. Two dielectric slabs of dielectric constants ๐พ1 and ๐พ2 are filled in between the two plates, each of area ๐ด, of the parallel plate capacitor as shown. Find net capacitance of the capacitor. CBSE (AI)-2005,(F)-2011 =

๐พ1 ๐œ€0 ๐ด/2 + ๐พ2๐œ€0๐‘‘๐ด/2 ๐‘‘ ๐œ€ ๐ด ๐œ€ ๐ด ๐พ +๐พ ๐พ +๐พ ๐ถ = 0 (๐พ1 + ๐พ2 ) = 0 ( 1 2) = ( 1 2) ๐ถ0 2๐‘‘ ๐‘‘ 2 2

[ Ans. ๐ถ = ๐ถ1 + ๐ถ2 =

โ‡จ

10. How will the (i) energy stored and (ii) the electric field inside the air capacitor be affected when it is completely filled with a dielectric material of dielectric constant K ? CBSE (AI)-2012 [ Ans. (i)

๐‘ž2

๐‘ž2

๐‘ž2

๐‘ˆ0 = 2๐ถ &๐‘ˆ = 2๐ถ = 2๐พ๐ถ 0

0

โ‡จ

๐‘ˆ=

๐‘ˆ0 ๐œŽ ๐œŽ (ii)๐ธ0 = &๐ธ = ๐œ€0 ๐พ๐œ€0 ๐พ

โ‡จ

๐ธ=

๐ธ0 ๐พ

==================================================================================

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Unit-I (Electrostatics)

โ€“ XII (PHYSICS)

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page -08

Part (B)-SA (II) & Long Answer Questions 1. Answer the following : 1. A charge is distributed uniformly over a ring of radius โ€ฒ๐‘Žโ€ฒ. Obtain an expression for the electric field intensity ๐ธ at a point on the axis of the ring. Hence show that for points at large distances from the ring, it behaves like a point charge. CBSE (D)-2016 [Ans.linear charge density, ๐œ†

๐‘ž

= 2๐œ‹๐‘Ž

chargeon the small element ๐‘‘๐‘™

๐‘‘๐‘ž = ๐œ†๐‘‘๐‘™ =

๐‘ž ๐‘‘๐‘™ 2๐œ‹๐‘Ž

Electric field intensity due to small element ๐‘‘๐‘™ at P

1 ๐‘‘๐‘ž 1 ๐œ†๐‘‘๐‘™ = 4๐œ‹ ๐œ€0 ๐‘Ÿ 2 4๐œ‹ ๐œ€0 ๐‘Ÿ 2 On resolving ๐‘‘๐ธ in to horizontal and vertical components the resultant electric field intensity at P is given by ๐‘‘๐ธ =

1 ๐œ†๐‘‘๐‘™ ๐‘ฅ X [ 4๐œ‹ ๐œ€0 ๐‘Ÿ2 ๐‘Ÿ

๐ธ = โˆซ ๐‘‘๐ธ cos ๐œƒ = โˆซ

โˆต cos ๐œƒ =

๐‘ฅ ๐‘Ÿ

]

๐‘ž 1 โ‡จ๐ธ = 4๐œ‹๐œ†๐œ€x ๐‘Ÿ3 โˆซ ๐‘‘๐‘™ = 4๐œ‹ ๐œ€x ๐‘Ÿ3 (2๐œ‹๐‘Ž ) (2๐œ‹๐‘Ž) = 4๐œ‹ ๐œ€

โ‡จ๐‘ฌ = ๐Ÿ’๐…๐Ÿ๐œบ

0

๐ŸŽ

๐‘ž๐‘ฅ 3 0 ๐‘Ÿ

0

๐’’๐’™ ๐Ÿ‘/๐Ÿ

(๐’™๐Ÿ +๐’‚๐Ÿ )

At the centre of the ring x= 0โ‡จ๐‘ฌ for large distances

โ‡จ๐‘ฌ =

=๐ŸŽ

๐‘ฅโ‰ซ๐‘Ž

๐Ÿ ๐‘ž ๐Ÿ’๐… ๐œบ๐ŸŽ ๐‘ฅ2

This is the electric field intensity due a point charge at distance x ==================================================================================

2. (i) An electric dipole is held in a uniform electric field. Using suitable diagram show that it does not undergo any translatory motion. Derive the expression for the torque acting on it. (ii) What would happen if the field in non-uniform ? (iii) What would happen if the external electric field ๐ธ is increasing (a) parallel to ๐‘ and (b) anti-parallel to ๐‘ ? CBSE (AI)-2016,2014,2008,(F)-2016,(DC)-2015 [ Ans. (i)Let an electric dipole of dipole moment ๐‘ is placed in a uniform electric field ๐ธโƒ— as shown in figure. Force : Force on+๐‘ž, ๐น1 = ๐‘ž๐ธ Force on โˆ’๐‘ž, ๐น2 = โˆ’๐‘ž๐ธ Hence net force on the dipole ๐น = ๐‘ž๐ธ โˆ’ ๐‘ž๐ธ = 0 Torque :Two equal and opposite forces โˆ’ ๐‘ž๐ธ and +๐‘ž๐ธ forms a couple which tries to rotate the dipole. Torquedue to this couple

๐œ = either force XโŠฅdistance=๐‘ž๐ธ x 2๐‘Ž sin ๐œƒ

x

= ๐‘ž๐ธ x 2๐‘Ž sin ๐œƒ

โ‡จ ๐œ = p๐ธ sin ๐œƒ = ๐‘โƒ—โƒ—

X โƒ—โƒ—โƒ— ๐ธ

(ii) If the electric field is non-uniform, the net force on the dipole will not be zero hence there will be the translator motion of the dipole. (iii) (a) Net force will be in the direction of increasing electric field. (b) Net force will be in the direction opposite to the increasing field ==================================================================================

3. An electric dipole is held in a uniform electric field. Write the expression for the torque acting on it. Express it in vector form and specify its direction. Identify two pairs of perpendicular vectors in the expression. [ Ans.Torque :๐œ = p๐ธ sin ๐œƒ โƒ—โƒ—โƒ— Vector form :๐œโƒ—โƒ— = โƒ—โƒ—โƒ— ๐‘ X๐ธ โƒ—โƒ—โƒ— given by Direction of ๐‰โƒ—โƒ— : Direction of torque is โŠฅ to the plane containing ๐‘ โƒ—โƒ—โƒ— and๐ธ right hand screw rule Two pairs of โŠฅvectors :(i)๐‰ โƒ—โƒ— and๐‘ โƒ—โƒ—โƒ—

โƒ—โƒ—โƒ— (ii) ๐‰ โƒ—โƒ— and ๐ธ

==================================================================================

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Unit-I (Electrostatics)

โ€“ XII (PHYSICS)

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page -09

Part (B)-SA (II) & Long Answer Questions 2. Answer the following : 1.(a) Derive an expression for the electric field E due to a dipole oflength โ€˜2aโ€™ at a point distant r from the centre of the dipole on theaxial line.CBSE (AI)-2017,2013,(D)-2015 (b) Draw a graph of E versus r for r >> a. [ Ans. Let โƒ—โƒ—โƒ—โƒ— ๐ธ1 and โƒ—โƒ—โƒ—โƒ— ๐ธ2 be the electric field at P due to โ€“ ๐‘žand +๐‘ž charges respectively then

โƒ—โƒ—โƒ—โƒ—1 | = |๐ธ ๐Ÿ’๐…๐œบ โƒ—โƒ—โƒ—โƒ—2 | &|๐ธ

๐’’

๐Ÿ along ๐ŸŽ (๐’“+๐’‚)

= ๐Ÿ’๐…๐œบ

๐’’ ๐ŸŽ (๐’“โˆ’๐’‚)

PA

๐Ÿalong

BP ๐’“

Obviously the resultant electric field intensity at P

โƒ—โƒ—โƒ—โƒ—2 | โˆ’ |๐ธ โƒ—โƒ—โƒ—โƒ—1 | = |๐ธโƒ— | = |๐ธ ๐’’ โ‡จ|๐ธโƒ—| = ๐Ÿ’๐…๐œบ

โ‡จ|๐ธโƒ—โƒ—โƒ— |

=

๐’’ ๐’’ ๐’’ ๐Ÿ ๐Ÿ ๐’’ (๐’“ + ๐’‚)๐Ÿ โˆ’ (๐’“ โˆ’ ๐’‚)๐Ÿ โˆ’ = โˆ’ = [ ] [ ] ๐Ÿ’๐…๐œบ๐ŸŽ (๐’“ โˆ’ ๐’‚)๐Ÿ ๐Ÿ’๐…๐œบ๐ŸŽ (๐’“ + ๐’‚)๐Ÿ ๐Ÿ’๐…๐œบ๐ŸŽ (๐’“ โˆ’ ๐’‚)๐Ÿ (๐’“ + ๐’‚)๐Ÿ ๐Ÿ’๐…๐œบ๐ŸŽ (๐’“๐Ÿ โˆ’ ๐’‚๐Ÿ )๐Ÿ

๐Ÿ’๐’‚๐’“ ๐Ÿ ๐ŸŽ (๐’“๐Ÿ โˆ’๐’‚๐Ÿ )

๐Ÿ

๐Ÿ๐’‘๐’“

๐Ÿ’๐… ๐œบ๐ŸŽ (๐’“๐Ÿ โˆ’ ๐’‚๐Ÿ )๐Ÿ

[ โˆต ๐‘ = 2๐‘ž๐‘Ž ]

Obviously, if ๐‘Ÿ โ‰ซ ๐‘Ž, then ๐Ÿ

๐ธ = ๐Ÿ’๐…๐œบ

๐Ÿ๐’‘๐’“ ๐ŸŽ

(๐’“๐Ÿ )

โ‡จ

๐Ÿ

๐‘ฌ=

๐Ÿ ๐Ÿ๐’‘ ๐Ÿ’๐…๐œบ๐ŸŽ ๐’“๐Ÿ‘

โƒ— is along the direction of dipole moment โƒ—โƒ—โƒ—๐‘ direction of ๐ธ ================================================================================== 2. Derive an expression for the electric field intensity at a point on the equatorial line of an electric dipole of dipole moment๐‘ โƒ—โƒ—โƒ— and length 2๐‘Ž. What is the direction of this field ?CBSE (D)-2017,(AI)-2016,2013,(F)-2015,2009 [ Ans.Let, โƒ—โƒ—โƒ—โƒ— ๐ธ1 and โƒ—โƒ—โƒ—โƒ— ๐ธ2 be the electric field intensity at at P due to โˆ’๐‘ž&+๐‘žcharges respectively, then

โƒ—โƒ—โƒ—โƒ—1 | = |๐ธ โƒ—โƒ—โƒ—โƒ—2 | = |๐ธ ๐Ÿ โ‡จ|๐ธโƒ—โƒ—โƒ—โƒ—1 | = |๐ธโƒ—โƒ—โƒ—โƒ—2 | = ๐Ÿ’๐…๐œบ

๐ŸŽ

๐Ÿ ๐’’ ๐Ÿ ๐Ÿ’๐…๐œบ๐ŸŽ โˆš ๐Ÿ ( ๐’“ + ๐’‚๐Ÿ )

๐’’ ---------(1) (๐’“๐Ÿ +๐’‚๐Ÿ )

โƒ—โƒ—โƒ—โƒ—1 and โƒ—โƒ—โƒ—โƒ— On resolving ๐ธ ๐ธ2 in horizontal and vertical components, resultant electric field intensity

|๐ธโƒ— | = ๐ธ1 cos ๐œƒ + ๐ธ2 cos ๐œƒ =2 ๐ธ1 cos ๐œƒ โ‡จ|๐ธโƒ—| =2 ๐Ÿ ๐Ÿ ๐’’ ๐Ÿ ๐Ÿ๐‘Ž ๐Ÿ[ โˆต cos ๐œƒ =

โ‡จ|๐ธโƒ—| =

๐Ÿ’๐…๐œบ๐ŸŽ (๐’“ +๐’‚ ) โˆš๐’“ +๐’‚ ๐Ÿ ๐Ÿ๐’’๐’‚ ๐Ÿ’๐…๐œบ๐ŸŽ ๐Ÿ ๐Ÿ ๐Ÿ‘/๐Ÿ (๐’“ +๐’‚ )

๐Ÿ โ‡จ|๐ธโƒ—| = ๐Ÿ’๐…๐œบ

๐ŸŽ

๐’‘ [ (๐’“๐Ÿ +๐’‚๐Ÿ )๐Ÿ‘/๐Ÿ

Obviously, if ๐‘Ÿ

โ‰ซ ๐‘Ž, then

โˆต ๐‘ = 2๐‘ž๐‘Ž ]

|๐ธโƒ— | =

๐Ÿ ๐’‘ ๐Ÿ’๐…๐œบ๐ŸŽ ๐’“๐Ÿ‘

๐‘Ž โˆš๐’“๐Ÿ +๐’‚๐Ÿ

โƒ— is opposite to that of dipole moment ๐‘ direction of ๐ธ โƒ—โƒ—โƒ—

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โ€“ XII (PHYSICS)

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page -10

Part (B)-SA (II) & Long Answer Questions 3. Answer the following : 1. Derive an expression for the potential at a point along the axial line of a short dipole. For this dipole draw a plot showing the variation of potential ๐‘‰versus ๐‘Ÿ,where ๐‘Ÿ(๐‘Ÿ โ‰ซ 2๐‘Ž), is the distance from the point charge โˆ’๐‘žalong the line joining the two charges.CBSE (AI)-2015, (D)-2008,2007 [ Ans. Let ๐‘‰1 and ๐‘‰2 be the electric potential at P due toโ€“ ๐‘ž and +๐‘ž charges respectively then

๐‘‰1 = &๐‘‰2

= ๐Ÿ’๐…๐œบ

๐’’ ๐ŸŽ (๐’“ โˆ’ ๐’‚)

โˆ’๐’’ ๐Ÿ’๐…๐œบ๐ŸŽ (๐’“ + ๐’‚)

๐’“

Resultant electric potential at P

โˆ’๐’’ ๐’’ ๐’’ ๐Ÿ ๐Ÿ ๐’’ ๐’“ + ๐’‚ โˆ’ (๐’“ โˆ’ ๐’‚) + = โˆ’ [ ] [ ]= (๐’“๐Ÿ โˆ’ ๐’‚๐Ÿ ) ๐Ÿ’๐…๐œบ๐ŸŽ (๐’“ + ๐’‚) ๐Ÿ’๐…๐œบ๐ŸŽ (๐’“ โˆ’ ๐’‚) ๐Ÿ’๐…๐œบ๐ŸŽ (๐’“ โˆ’ ๐’‚) (๐’“ + ๐’‚) ๐Ÿ’๐…๐œบ๐ŸŽ

๐‘‰ = ๐‘‰1 + ๐‘‰2 = ๐Ÿ โ‡จ๐‘‰ = ๐Ÿ’๐…๐œบ

๐ŸŽ

๐Ÿ๐’’๐’‚ (๐’“๐Ÿ โˆ’ ๐’‚๐Ÿ )

๐Ÿ

โ‡จ๐‘‰ = ๐Ÿ’๐…๐œบ

๐’‘ ๐ŸŽ

[ โˆต ๐‘ = 2๐‘ž๐‘Ž ]

(๐’“๐Ÿ โˆ’ ๐’‚๐Ÿ )

Obviously, if ๐‘Ÿ โ‰ซ ๐‘Ž, then

๐‘ฝ=

๐Ÿ ๐’‘ ๐Ÿ’๐…๐œบ๐ŸŽ ๐’“๐Ÿ

================================================================================== 4. (i) Derive the expression for the potential energy of an electric dipole of dipole moment ๐‘ โƒ—โƒ—โƒ— placed in a uniform electric field โƒ—โƒ—โƒ— ๐ธ.

(ii) Find out the orientation of the dipole when it is in (a) stable equilibrium (b) unstable equilibrium. CBSE (AI)-2016,2015,2012 [ Ans. (i)Two equal and opposite forces โˆ’ ๐‘ž๐ธ and +๐‘ž๐ธ forms a couple whichtries to rotate the dipole.Torquedue to this couple

๐œ =either force XโŠฅ distance= ๐‘ž๐ธ x 2๐‘Ž sin ๐œƒ ๐œ= ๐‘๐ธ sin ๐œƒ

Work done in rotating the dipole through an angle ๐‘‘๐œƒ

๐‘‘๐‘Š = ๐œ๐‘‘๐œƒ = p๐ธ sin ๐œƒ ๐‘‘๐œƒ โ‡จ๐‘Š = โˆซ๐œƒ๐œƒ2 p๐ธ sin ๐œƒ ๐‘‘๐œƒ = p๐ธ โˆซ๐œƒ๐œƒ2 sin ๐œƒ ๐‘‘๐œƒ = p๐ธ[โˆ’cos ๐œƒ]๐œƒ๐œƒ21 1

1

x

โ‡จ๐‘Š = p๐ธ(cos ๐œƒ1 โˆ’ cos ๐œƒ2 )-------(1)

When ๐œƒ1 = 900and ๐œƒ2 =๐œƒ, then ๐‘Š = ๐‘ˆ

โ‡จ ๐‘ˆ= p๐ธ(cos 900 โˆ’ cos ๐œƒ) = p๐ธ(0 โˆ’ cos ๐œƒ)= โˆ’๐ฉ๐‘ฌ ๐œ๐จ๐ฌ ๐œฝ โ‡จ ๐’–(๐œฝ) = โˆ’๐’‘โƒ—โƒ—โƒ— .๐‘ฌโƒ—โƒ—โƒ— (ii)(a) When ๐œƒ = 00 , ๐‘ˆ = โˆ’p๐ธ cos 0 = โˆ’p๐ธ In this case P.E. is minimum hence it is the orientation of stable equilibrium. (b)When ๐œƒ= 1800 , ๐‘ˆ = โˆ’p๐ธ cos 180 = + p๐ธ In this case P.E. is maximum hence it is the orientation of unstable equilibrium. ==================================================================================

5.(i) Draw 3 equipotential surfaces corresponding to a field that uniformly increases in magnitude but remains constant along z-direction.CBSE (AI)-2016,2009,(F)-2008 (ii) How are these surfaces different from that of a constant electric field along z- direction ? [Ans. (i)

(ii)

Difference :In the first case, as the magnitude of field increases, equipotential surfaces get closer In the second case, equipotential surfaces are equidistant planes parallel to XY planes

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6. Answer the following : 1. (i) Derive an expression for electric potential energy of a system of two point charges. (ii) Three point charges ๐‘ž1 , ๐‘ž2 and ๐‘ž3 are kept respectively at points ๐ด, ๐ต and ๐ถ as shown in the figure. Derive the expression for the electric potential energy of the system. CBSE (AI)-2015

[ Ans.Electric potential energy of a system of two point charges :

๐‘Š1 = 0

1 ๐‘ž1 1 ๐‘ž1 ๐‘ž2 ๐‘Š2 = ๐‘‰1 ๐‘‹๐‘ž2 = ( ) ๐‘‹ ๐‘ž2 = 4๐œ‹๐œ€0 ๐‘Ÿ 4๐œ‹๐œ€0 ๐‘Ÿ

โ‡จ๐‘ˆ = ๐‘Š1 + ๐‘Š2 = 0 + 4๐œ‹๐œ€1

0

๐‘ž1 ๐‘ž2 ๐‘Ÿ

1

= 4๐œ‹๐œ€

0

๐‘ž1 ๐‘ž2 ๐‘Ÿ

(ii) Electric potential energy of a system of three point charges :

๐‘Š1 = 0

1 ๐‘ž1 ๐‘ž2 4๐œ‹๐œ€0 ๐‘Ÿ12 1 ๐‘ž2 ๐‘ž3 1 ๐‘ž3 ๐‘ž1 ๐‘Š3 = + 4๐œ‹๐œ€0 ๐‘Ÿ23 4๐œ‹๐œ€0 ๐‘Ÿ31 โ‡จ๐‘ˆ = ๐‘Š1 + ๐‘Š2 + ๐‘Š3 = 0 + 1 ๐‘ž1๐‘ž2 + 1 ๐‘ž2๐‘ž3 + ๐‘Š2 =

โ‡จ๐‘ˆ = 4๐œ‹๐œ€1

0

[

๐‘ž1 ๐‘ž2 ๐‘Ÿ12

+

๐‘ž2 ๐‘ž3 ๐‘Ÿ23

+

4๐œ‹๐œ€0 ๐‘Ÿ12 ๐‘ž3 ๐‘ž1 ] ๐‘Ÿ31

4๐œ‹๐œ€0 ๐‘Ÿ23

1 ๐‘ž3 ๐‘ž1 4๐œ‹๐œ€0 ๐‘Ÿ31

==============================================================================

2. (i) What is a dielectric ? Give one example. CBSE (AI)-2016,(D)-2015,(F)-2006 (ii) Distinguish with the help of a suitable diagram, the difference in the behaviour of a conductor and a dielectric placed in an external electric field. How does polarized dielectric modify the original external filed ? [ Ans. (i) Dielectric : Dielectrics are non-conducting substances which allows electric induction to take place through them but do not allow the flow of charge through them. for example : Air, glass, mica (ii) In a conductor, in the presence of external electric field the free charge carriers move and charge distribution in the conductor adjusts itself in such a way that the net electric field within the conductor becomes zero. i,e, ๐ธ = ๐ŸŽ In a dielectric, external electric field induces net dipole moment by stretching or re-orienting molecules. The electric field due to this induced dipole moment opposes the external field but does not exactly cancel it. As a result net electric field is reduced.

๐ธ = ๐‘ฌ๐ŸŽ โˆ’ ๐‘ฌ๐’Š๐’ =

๐ธ0 ๐พ

==============================================================================

3. Define the term โ€˜dielectric strengthโ€™. What does this term signify ? What is its value for (a) air (b) vacuum ? CBSE (AIC)-2015

[ Ans. (i) Dielectric strength : The maximum electric field that a dielectric medium can withstandwithout break-down (of its insulating property) is called its dielectricstrength. Significance :This signifies the maximum value of electric field, up to which the dielectric can safely play its role (ii) (a) for air it is about 3 ๐‘‹ 106 ๐‘‰๐‘šโˆ’1 (b) for vacuum it is infinity ============================================================================

4. What is electrostatic shielding ? How is this property used in actual practice ? Is the potential in the cavity of a charged conductor zero ? CBSE (AI)-2016 [ Ans. Electrostatic shielding : Whatever be the charge and field configuration outside, any cavity in a conductor remains shielded from outside electric influence: thefield inside the cavity is always zero. This is known as electrostatic shielding. Use :The effect can be madeuse of in protecting sensitive instruments from outside electrical influence by enclosing them in a hollow conductor.

Potential inside the cavity is not zero. It is constant ==================================================================================

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Part (B)-SA (II) & Long Answer Questions 7 .Answer the following : 1. Using Gaussโ€™s law, derive an expression for the electric field intensity due to an infinitely long, straight wire of linear charge density๐œ† C/m. CBSE (AIC)-2017,(AI)-2007,2006,2005,(D)-2009,04 [ Ans.Charge enclosed by Gaussian surface,

๐‘ž = ๐œ†๐‘™

At the part I and II of Gaussian surface ๐ธโƒ— and ๐‘›ฬ‚ are โŠฅ, so flux through surfaces I and II is zero. By Gaussโ€™s law, โˆฎ โƒ—โƒ—โƒ— ๐ธ. โƒ—โƒ—โƒ—โƒ— ๐‘‘๐‘ 

=

๐’’ ๐œบ๐ŸŽ

โ‡จโˆฎ ๐ธ๐‘‘๐‘ ๐‘๐‘œ๐‘ 0 = ๐œบ๐’’ ๐ŸŽ โ‡จ๐ธ โˆฎ ๐‘‘๐‘  = ๐œบ๐’’ ๐ŸŽ

โ‡จ๐ธ(2๐œ‹๐‘Ÿ๐‘™) = ๐œ†๐œ– ๐‘™ โ‡จ๐‘ฌ = ๐Ÿ๐…๐œบ๐€

0

๐ŸŽ๐’“

15. Using Gaussโ€™s law, obtain the expression for electric field intensity at a point due to an infinitely large, plane sheet of charge of charge density๐œŽ C/m2. How is the field directed if the sheet is (i) positively charged (ii) negatively charged? CBSE (AI)-2015,2010,2005,2004,(D)-2012,2009,06,(DC)-2002,01,(F)-2003 [ Ans.Let us consider a Gaussian surface as shown. At the curved part of Gaussian surface ๐ธโƒ— and ๐‘›ฬ‚ are โŠฅ, so flux through curved surface is zero.

โƒ—โƒ—โƒ—โƒ— โƒ—โƒ—โƒ— ๐‘‘๐‘  By Gaussโ€™s law,โˆฎ ๐ธ.

โ‡จโˆฎ ๐ธ๐‘‘๐‘ ๐‘๐‘œ๐‘ 0 = ๐œบ๐’’ ๐ŸŽ โ‡จ๐ธ โˆฎ ๐‘‘๐‘  = ๐œบ๐’’ ๐ŸŽ ๐’’ โ‡จ๐ธ(2๐ด) = ๐œบ

=

๐’’ ๐œบ๐ŸŽ

๐ŸŽ

โ‡จ๐‘ฌ =

๐’’ ๐Ÿ๐œบ๐ŸŽ๐‘จ

๐ˆ

= ๐Ÿ๐œบ

๐ŸŽ

Direction of field :(i) If the sheet is positively charged the field is directed away from it (ii) If sheet is negatively charged the field is direct towards it

17. Using Gaussโ€™s law, deduce the expression for the electric field due to uniformly charged spherical conducting shell of radius๐‘… at a point (i) outside and (ii) inside the shell. Plot a graph showing variation of electric field as a function of r > R and r< R. CBSE (AI)-2015,2013,2007,2004,(D)-2011,2009,2008,2006,2004 [ Ans.(i) Outside the shell (๐’“ > ๐‘…) Let us consider the Gaussian surface as shown by Gaussโ€™s law,

๐’’ ๐ธ. โƒ—โƒ—โƒ—โƒ— ๐‘‘๐‘  = ๐œบ โˆฎ โƒ—โƒ—โƒ—

โ‡จโˆฎ ๐ธ๐‘‘๐‘ ๐‘๐‘œ๐‘ 0 = ๐œบ๐’’ ๐ŸŽ โ‡จ๐ธ โˆฎ ๐‘‘๐‘  = ๐œบ๐’’ ๐ŸŽ โ‡จ๐ธ(4๐œ‹๐‘Ÿ2) = ๐œ–๐‘ž0 ๐Ÿ ๐’’ โ‡จ๐‘ฌ =๐Ÿ’๐…๐œบ ๐’“๐Ÿ

๐ŸŽ

๐ŸŽ

(ii) Inside the shell (๐’“ < ๐‘…) Let us consider the Gaussian surface as shown By Gaussโ€™s law

โƒ—โƒ—โƒ—โƒ— = โƒ—โƒ—โƒ— ๐‘‘๐‘  โˆฎ ๐ธ.

๐’’ ๐œบ๐ŸŽ

But, charge inside the spherical shell,i,e, q = 0

โ‡จโˆฎ ๐ธ๐‘‘๐‘ ๐‘๐‘œ๐‘  0 = 0 โ‡จ๐‘ฌ = ๐ŸŽ

==================================================================================

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8. Answer the following : 1. What is a capacitor? Deduce an expression for the capacitance of a parallel plate capacitor with air as the medium between the plates. CBSE (F)-2017,2006,(AI)-2003,2001,(DC)-2005,2004 [ Ans. Capacitor :It is an arrangement required to increase the capacity of a conductor so that a large amount of charge can be stored in it without changing its dimensions Capacitance of โˆฅ plate capacitor :let us consider a parallel plate capacitorfilled with a medium of dielectric constant K as shown Electric field between the plates

๐ธ=

๐œŽ ๐‘ž = ๐œ€0 ๐พ ๐œ€0 ๐พ๐ด

โ‡จpotential difference between the plates ๐‘‰=๐ธ๐‘‘=

โ‡จ๐ถ = ๐‘‰๐‘ž =

๐‘ž ๐‘ž๐‘‘ ๐œ€0 ๐พ๐ด

=๐‘ฒ

๐‘ž๐‘‘ ๐œ€0 ๐พ๐ด

๐œบ๐ŸŽ ๐‘จ ๐’…

If air is as the medium between the plates then,

โ‡จ๐‘ช๐ŸŽ =

๐พ=1

๐œบ๐ŸŽ ๐‘จ ๐’…

2. A dielectric slab of thickness โ€˜tโ€™ is introduced without touching between the plates of a parallel plate capacitor separated by a distance โ€˜dโ€™ (t < d). Derive an expression for the capacitance of the capacitor. [ Ans. Electric field between the plates in airCBSE (AIC)-2005,2001

๐ธ0 = Electric field in dielectric slab

๐ธ = ๐‘ฌ๐ŸŽ โˆ’ ๐‘ฌ๐’‘

=

๐‘ž ๐œ€0 ๐ด

๐ธ0 โˆ’

๐ˆ๐’‘ ๐ธ0 ๐‘ž = = ๐œบ๐ŸŽ ๐พ ๐œ€0 ๐พ๐ด

โ‡จpotential difference between the plates ๐‘‰ = ๐ธ0 (๐‘‘ โˆ’ ๐‘ก) +

โ‡จ๐ถ = ๐‘‰๐‘ž = โ‡จ๐‘ช =

๐‘ž

๐ธ0

๐‘ก ๐‘ž ๐‘ก ๐‘ก = ๐ธ0 [(๐‘‘ โˆ’ ๐‘ก) + ] = [(๐‘‘ โˆ’ ๐‘ก) + ] ๐พ ๐พ ๐œ€0 ๐ด ๐พ

๐‘ž ๐‘ก [(๐‘‘โˆ’๐‘ก)+ ] ๐œ€0 ๐ด ๐พ

๐œบ๐ŸŽ ๐‘จ

๐’• (๐’…โˆ’๐’•)+๐‘ฒ

3. Why does the capacitance of a parallel plate capacitor increase on introduction of a dielectric in between its plates ? [ Ans. Due to dielectric polarization, an electric field is induced intheCBSE (F)-2006 dielectric oppositetoexternal electric field. Hence net electric field decreases to

๐ธ = ๐‘ฌ๐ŸŽ โˆ’ ๐‘ฌ๐’Š๐’ = ๐ธ0 โˆ’ It reduces potential difference

โ‡จ๐ถ =

๐‘ž0 ๐‘‰

=

๐‘ž0 ๐‘‰0 /๐พ

= ๐พ(

๐‘ž0

๐‘‰0

๐ˆ๐’‘ ๐ธ0 = ๐œบ๐ŸŽ ๐พ

to ๐‘‰ = ๐‘ฌ๐’… = ๐ธ๐พ0 ๐‘‘ = ๐‘‰๐พ0

) = ๐พ๐ถ0

Hence capacitance increases K times

4. A slab of material of dielectric constant ๐พ has the same area as that of the plates of a parallel plate capacitor but hasthe thickness 3d/4, where d is the separation between the plates. Find out the expression for its capacitance

when the slab is inserted between the plates of the capacitor.CBSE (F)-2017,2010,(AI)-2013,NCERT-2017 [ Ans.

๐ธ0 ๐พ

๐‘‰ = ๐ธ0 (๐‘‘ โˆ’ ๐‘ก) +

๐‘ก = ๐ธ0 [(๐‘‘ โˆ’ 3๐‘‘/4) + ๐ถ=

3๐‘‘/4 ] ๐พ

=

๐ธ0 ๐‘‘ 3 (1 + ๐พ) 4

=

๐‘‰0 ๐พ + 3 ( ๐พ ) 4

๐‘ž0 ๐‘ž0 4๐พ ๐‘ž0 4๐พ = ๐‘‰ ๐พ+3 = = ๐ถ0 0 ๐‘‰ ( ) (๐พ + 3) ๐‘‰0 (๐พ + 3) 4

๐พ

==================================================================================

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Part (B)-SA (II) & Long Answer Questions 9. Answer the following : 1

1. Prove that the total electrostatic energy stored in a parallel plate capacitor is ๐ถ๐‘‰2 . Hence derive an expression 2

for energy density of the capacitor. How does the stored energy change if air is replaced by medium of dielectric constant โ€˜Kโ€™ ? CBSE (AI)-2015,2012,2008,2002,(F)-2013,2006,(D)-2006,2002 [ Ans. Energy stored in a capacitor : When a capacitor is charged by a battery, work is done by the battery at the expense of its chemical energy. This work done is stored between the plates as electrostatic potential energy Small work done in giving a charge ๐‘‘๐‘ž ๐‘ž ๐ถ

๐‘‘๐‘Š = V X ๐‘‘๐‘ž = ๐‘‘๐‘ž

โ‡จ

Total work done in giving a charge Q to the capacitor ๐‘ธ

1

๐‘ž2

1

๐‘„2

๐‘Š = ๐ถ โˆซ๐ŸŽ ๐’’ ๐‘‘๐‘ž = ๐ถ [ 2 ]๐‘„0 = 2๐ถ

โ‡จ๐‘ผ =๐‘„2๐ถ= (๐ถ๐‘‰) 2๐ถ

2

2

Energy density:

๐’– = ๐‘‰๐‘œ๐‘™๐‘ข๐‘š๐‘’ = 2๐ด ๐‘‘ = 2

๐Ÿ

= ๐Ÿ ๐‚๐‘ฝ๐Ÿ 1

๐‘ˆ

1 ๐œ€0 ๐ด ( )(๐ธ๐‘‘)2 ๐‘‘

C๐‘‰2

๐ด๐‘‘

1

1

= 2 ๐œ€0 ๐ธ 2

๐’– = 2 ๐œ€0 ๐ธ2

โ‡จ

If air is replaced by a medium of dielectric constant ๐พ then 1

๐‘‰ 2

1

๐‘ผโ€ฒ= 2 Cโ€ฒ(๐‘‰โ€ฒ)2 = 2 ๐พC (๐พ) =

1 ๐ถ๐‘‰ 2 ๐‘ˆ =๐พ 2 ๐พ

==============================================================================

2. Three capacitors of capacitances ๐ถ1 , ๐ถ2 &๐ถ3 are connected (a) in series (b) in parallel. Show that the energy stored in the series combination is the same as that in the parallel combination.CBSE (AI)-2003 [ Ans. (i) In series,๐‘ˆ๐‘ 

โ‡จ

1

1

๐‘ 

1

๐Ÿ

๐‘ 

๐‘ˆ๐‘  = ๐‘ˆ1 + ๐‘ˆ2 + ๐‘ˆ3

(ii) In parallel,

โ‡จ

๐‘„2

๐Ÿ

๐Ÿ

1 ๐‘„2

1 ๐‘„2

1 ๐‘„2

1

2

3

= 2๐ถ = 2 ๐‘„ 2 (๐ถ ) = 2 ๐‘„ 2 (๐‘ช + ๐‘ช + ๐‘ช ) = 2 ๐ถ + 2 ๐ถ + 2 ๐ถ

1

๐Ÿ

1

๐Ÿ

๐Ÿ‘

1

1

1

๐‘ˆ๐‘ƒ = 2 ๐ถ๐‘ƒ ๐‘‰ 2 = 2 (๐ถ1 + ๐ถ2 + ๐ถ3 )๐‘‰ 2 = 2 ๐ถ1 ๐‘‰ 2 + 2 ๐ถ1 ๐‘‰ 2 + 2 ๐ถ1 ๐‘‰ 2

๐‘ˆ๐‘ƒ = ๐‘ˆ1 + ๐‘ˆ2 + ๐‘ˆ3

===============================================================================

3. A network of four capacitors each of 10 ๐œ‡๐น capacitance is connected to a 500 ๐‘‰ supply as shown in the figure. Determine theCBSE (AI)-2015 (i) equivalent capacitance of the network and (ii) charge on each capacitor [ Ans. (i)

1 ๐ถโ€ฒ

1

1

1

1

2

3

1

1

1

3

= ๐ถ + ๐ถ + ๐ถ = 10 + 10 + 10 = 10โ‡จ๐ถ โ€ฒ =

โ‡จequivalent capacitance, ๐ถ = ๐ถ โ€ฒ + ๐ถ4 = 10 +10 = 3

40 3

10 3

๐œ‡๐น

๐œ‡๐น

(ii) charge on ๐ถ4 , ๐‘ž4 = ๐ถ4 X ๐‘‰ = 10X10โˆ’6 ๐‘‹ 500 = 5X10โˆ’3 ๐ถ โ€ฒ

๐‘ž1 = ๐‘ž2 = ๐‘ž3 = ๐ถ X ๐‘‰ =

10 โˆ’6 5 โˆ’3 X10 ๐‘‹ 500 = X10 ๐ถ 3 3

4. Find the equivalent capacitance of the network shown in the figure, when each capacitor is of 1 ๐œ‡๐น. When the ends ๐‘‹ and๐‘Œ are connected to a 6 ๐‘‰ battery, find out (i) the charge and (ii) energy stored in the network. ๐‘ช๐Ÿ

[ Ans.

๐‘ช๐Ÿ

=

๐‘ช๐Ÿ‘ ๐‘ช๐Ÿ’

โ‡จ๐Ÿ๐Ÿ = ๐Ÿ๐ŸCBSE (AI)-2015,(AIC)-2003,(D)-2001

this is the condition of balance so there will be no current in ๐ถ5 Now ๐ถ1 &๐ถ2 are in series

โ‡จ๐ถ12

๐ถ ๐ถ = 1 2 ๐ถ1+ ๐ถ2

= 11 X+11 =

1/2๐œ‡๐น

๐ถ3 &๐ถ4 are in series, ๐ถ3 ๐ถ4 ๐ถ3 + ๐ถ4

= 11 X+11 = 1/2๐œ‡๐น

โ‡จ๐ถ34 =

โ‡จ๐ถ = ๐ถ12 + ๐ถ34 = 12 + 12 = 1 ๐œ‡๐น

โ‡จ(i) ๐‘ž = ๐ถ๐‘‰ = 1 X 6 = 6๐œ‡๐ถ (ii)๐‘ˆ = 12 ๐‘ž๐‘‰ = 12 X 1 X 10โˆ’6X 6 = 31 X 10โˆ’6

๐ฝ

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Part (B)-SA (II) & Long Answer Questions 10. Answer the following : 1. Given the components of an electric field as ๐ธ๐‘ฅ = ๐›ผ๐‘ฅ, ๐ธ๐‘ฆ = 0 and ๐ธ๐‘ง = 0, where ๐›ผ is dimensional constant. Calculate the flux through the cube of side โ€˜aโ€™ as shown in the figure and the effective charge inside the cube. CBSE (AI)-2015,(F)-2012 [ Ans.(i)

๐œ™ = ๐œ™๐ฟ + ๐œ™๐‘… = ๐ธ๐‘ฅ ๐‘‘๐‘  cos 180 + ๐ธ๐‘ฅ ๐‘‘๐‘  cos 0 โ‡จ๐œ™ = (๐›ผ๐‘Ž)๐‘Ž2 (โˆ’1) + [๐›ผ (๐‘Ž + ๐‘Ž)]๐‘Ž2 (1) = โˆ’๐›ผ๐‘Ž3 + 2๐›ผ๐‘Ž3

โ‡จ๐œ™ = ๐›ผ๐‘Ž3 ๐‘ž (ii) ๐œ™ = โ‡จ๐‘ž = ๐œ€0 ๐œ™ = ๐œ€0 ๐›ผ๐‘Ž3 ๐œ€ 0

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2. Given a uniform electric field ๐„ = 6 X 103 ๐‘–ฬ‚ N/C, Find the flux of this field through a square of 10 Cm on a side whose plane is parallel to Y-Z plane. What would be the flux through the same square if the plane makes a 300 angle with the x- axis ?CBSE (D)-2014 [ Ans.Given :๐„ = 6 X 103 ๐‘–ฬ‚ N/C, ๐‘Ž = 10 ๐‘๐‘š = 10๐‘‹10โˆ’2 ๐‘š, ๐œ™ = ? In first case,๐œ™ = ๐ธ ๐‘‘๐‘  cos 0 = 6 X 103 X (10 ๐‘‹ 10โˆ’2 )2 = 60 N m2/C In second case,๐œ™

= ๐ธ ๐‘‘๐‘  cos(90 โˆ’ 30) = ๐ธ ๐‘‘๐‘  cos 60 = 6 X 103 X (10 X 10โˆ’2 )2 X

1 2

= 30 N m2/C

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3. Two point charges 4๐œ‡C and +1 ๐œ‡C are separated by a distance of 2 m in air.Find the point on the line-joining charges at which the net electric field of thesystem is zero.CBSE (AIC)-2017 1 ๐‘ž1 4๐œ‹๐œ–0 ๐‘Ÿ12

[Ans.

1

= 4๐œ‹๐œ–

๐‘ž2 2 0 ๐‘Ÿ2

4

1

โ‡จ๐‘ฅ2 = (2โˆ’๐‘ฅ)2โ‡จ2(2 โˆ’ ๐‘ฅ) = ๐‘ฅโ‡จ๐‘ฅ = 43 ๐‘š

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4. Two point charges 20๐‘‹10โˆ’6 ๐ถ and โˆ’4๐‘‹10โˆ’6 ๐ถ are separated by a distance of 50 ๐‘๐‘š in air. Find(i) the point on the line joining the charges, where the electrostatic potential is zero. (ii) calculate the electrostatic potential energy of the system. CBSE (AI)-2008 [Ans. (i) (ii)๐‘ˆ

1

= 4๐œ‹๐œ€

1 ๐‘ž1 4๐œ‹๐œ–0 ๐‘Ÿ1

๐‘ž1 ๐‘ž2 ๐‘Ÿ 0

1

+ 4๐œ‹๐œ–

๐‘ž2 0 ๐‘Ÿ2

20๐‘‹10โˆ’6

= 0โ‡จ

= โˆ’9๐‘‹109 X

+

๐‘ฅ 20X10โˆ’6 X4X10โˆ’6 50๐‘‹ 10โˆ’2

โˆ’4๐‘‹10โˆ’6 (50โˆ’๐‘ฅ)

20

4

= 0โ‡จ ๐‘ฅ = (50โˆ’๐‘ฅ)โ‡จ๐‘ฅ =

250 6

= 41 ๐‘๐‘š

= โˆ’1.44 J

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5. Show that if we connect the smaller and the outer sphere by a wire, the charge ๐‘ž on the former will always flow to the latter, independent of how large ๐‘„ is. CBSE (F)-2015,(AI)-2009 [Ans. Potential at a point on the inner sphere

๐‘‰1 =

1 ๐‘ž 1 ๐‘„ + 4๐œ‹๐œ€0 ๐‘Ÿ 4๐œ‹๐œ€0 ๐‘…

Potential at a point on the spherical shell

1 ๐‘ž 1 ๐‘„ + 4๐œ‹๐œ€0 ๐‘… 4๐œ‹๐œ€0 ๐‘… ๐‘ž ๐‘„ ๐‘ž ๐‘…โˆ’๐‘Ÿ [๐‘Ÿ โˆ’ ๐‘… ] = 4๐œ‹๐œ€ [ ๐‘Ÿ๐‘… ] ๐‘‰2 =

1

โ‡จ ๐‘‰1 โˆ’ ๐‘‰2 = 4๐œ‹๐œ€

0

0

โ‡จ ๐‘‰1 โˆ’ ๐‘‰2 > 0โ‡จ ๐‘‰1 > ๐‘‰2, hence the charge will flow from inner sphere to outer shell ]

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6. Calculate the work done to dissociate the system of three charges placed on the vertices of an equilateral triangle of side 10 cm as shown in figure. Here ๐‘ž = 1.6 ๐‘‹ 10โˆ’10 ๐ถ. CBSE (AI)-2016,2013, (D)-2008 [ Ans. Required work done = โˆ’ potential energy of the system

๐‘Š=โˆ’

1 โ‡จ๐‘Š =โˆ’ 4๐œ‹๐œ–

0

โ‡จ๐‘Š =9๐‘‹109

1 ๐‘ž1 ๐‘ž2 ๐‘ž2 ๐‘ž3 ๐‘ž3 ๐‘ž1 + + [ ] 4๐œ‹๐œ€0 ๐‘Ÿ12 ๐‘Ÿ23 ๐‘Ÿ31 1 ๐‘ž(โˆ’4๐‘ž) (โˆ’4q)(2q) q (2q) =โˆ’ [ + + ] 4๐œ‹๐œ–0 ๐‘Ž a a

[โˆ’

4๐‘ž2 ๐‘Ž

โˆ’

8๐‘ž2 ๐‘Ž

+

2๐‘ž2 ]= ๐‘Ž

โˆ’10 2

10 ๐‘‹ (1.6 ๐‘‹ 10

โˆ’2

10๐‘‹ 10

)

+

1

10๐‘ž 2

4๐œ‹๐œ–0

๐‘Ž

= 2.304๐‘‹10โˆ’8 J

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