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Class 12-science H C VERMA Solutions Physics Chapter 8 - Gauss' Law

Gauss' Law Exercise 141

Solution 1

  

  (As given plane is parallel to YZ plane)

And flux is given as :

  

  

  

Solution 2

Linear charge density,

  

And charge enclose inside is given as:

  

  

  

Solution 3

Electric field is uniform and given plane is perpendicular to it. Thus it is an equipotential surface with no net current on that surface. So, net charge is :

Q = 0

Solution 4

  

If  

  

  

  

  

  

  

  

Also,  

  

  

  

Solution 5

By Gauss Law:

  

At centre of cube:

  (For six surfaces)

  

Solution 6

Let us assume a cubical surface of side 'a'. So charge will be at centre of the cube and flux through one surface of cube is given as:

  

  

Solution 7

  

 

By gauss's law sphere experiences flux only by charge present inside sphere and not by charge present outside sphere.

  

  

  

Solution 8

In case of sphere flux is given as:

  

In case of hemisphere,

  

Solution 9

Volume charge density =   

We know,

  

Also,

  

  

  

  

Solution 10

(a) We know,

  

  

  

(b) Now,

  

  

  

Also,

  

  

  

Solution 11

  

  

  

Charge enclosed by sphere of radius  is :

  

  

By Gauss law,

  

  

  

Gauss' Law Exercise 142

Solution 12

By Property of induction charge induced at inner surface   and outer surface . +Q

(a) Surface charge density at inner surface   

Surface charge density at outer surface   

(b) When q is added then there is no effect on inner surface charge density

  

But when q is added outer surface charge density becomes,

  

(c) Let us assume an area inside sphere which is at   distance from centre of sphere.

  

  

  

Solution 13

(a) Electric field ,

  

  

  

(b) Total Charge Q =   

  

Electric field ,

  

  

  

Solution 14

We know,

  

  

  

  

  

Solution 15

For cylinder

  

Also, Force

  

  

  

  

  

  

  

Solution 16

We know,

  

  

(Total charge As nQ =   where,   is volume charge density)

  

Solution 17

We know,

  

  

  

  

Solution 18

We know in case of charge conducting sheet:

  

And Force is :

  

=  

  0.45 N

Solution 19

According to given figure:

  

And

  

Also

  

  

From (1) and (2)

  

  

  

  

  

Solution 20

(a) In equilibrium,

  

  

  

(b) For this, acceleration is included. Thus,

  

  

  

  

Solution 21

We know,

  

  

  

Now, electric field is given as:

  

And

  

Also

  

  

  

  

  

  

Solution 22

(a) For any point on left plate, electric flux is not present as it is outside the system. Hence, electric field,

E = 0

(b) For charge present in between plates, it experiences force towards negative plate, which is given as:

  

  

  

  

(c) For any point of right plate no electric flux is present as it is outside the system. Hence, electric field is given as:

E = 0

Solution 23

(a) Electric field at left end   

And Electric field at right end   

As the electric field is balanced

  

And   

  

  

  

(b) From above part,

 (for left part)

  

As   is charged plate   electric field is directed towards left.

(c) Here,   is charged plate so it acts as only source of electric field. Thus, electric field is directed from left to right and is given as:

  

(d) Similar to above part, Y acts as positive plate thus it repels, so electric field is directed towards right and is given as:

  

Solution 24

Net electric field at point P is:

  

  

Solving we get,

  

And, Net charge on right of right plate is:

  

  

  

 

  

 

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