NCERT Solutions For Class 12 Physics Chapter 1 has been provided here on this page. All the relevant information along with NCERT Class 12 Physics Chapter 1 Exercise Solutions can be found here in a detailed manner. This chapter introduces the most basic topics from the world of electric charge and Gauss’s Law to the students. Therefore, it is necessary to study and understand the topics in this NCERT Solutions For Class 12 Physics. We hope this NCERT Class 12 Physics Chapter 1 Solutions will be helpful for the students and the applicants preparing for other competitive exams. Candidates can find answers to all their problems with the help of NCERT Solutions For Class 12 Physics Chapter 1 at the end of this page.
NCERT Solutions For Class 12 Physics Chapter 1- Electric Charges And Fields
Topic-wise overview for NCERT Solutions For Class 12 Physics Chapter 1 Electric Charges And Fields are given in the following table.
| Section Name | Topics |
| 1 | Electric Charges And Fields |
| 1.1 | Introduction |
| 1.2 | Electric Charge |
| 1.3 | Conductors and Insulators |
| 1.4 | Charging by Induction |
| 1.5 | Basic Properties of Electric Charge |
| 1.6 | Coulomb’s Law |
| 1.7 | Forces between Multiple Charges |
| 1.8 | Electric Field |
| 1.9 | Electric Field Lines |
| 1.10 | Electric Flux |
| 1.11 | Electric Dipole |
| 1.12 | Dipole in a Uniform External Field |
| 1.13 | Continuous Charge Distribution |
| 1.14 | Gauss’s Law |
| 1.15 | Applications of Gauss’s Law |
Class 12 Physics NCERT Solutions Chapter 1 :
Question 1.1:
What is the force between two small charged spheres having charges of 2 × 10−7 C and 3 × 10−7 C placed 30 cm apart in the air?
Solution:
Repulsive force of magnitude 6 × 10−3 N
Charge on the first sphere, q1 = 2 × 10−7 C
Charge on the second sphere, q2 = 3 × 10−7 C
Distance between the spheres, r = 30 cm = 0.3 m
The electrostatic force between the spheres is given by the relation,
Where ∈0 = Permittivity of free space.
Then,
Therefore, the force between the two small charged spheres is 6 × 10−3 N. The charges are of the same nature. So, the force between them will be repulsive.
Question 1.2:
The electrostatic force on a small sphere of charge of 0.4 μC due to another small sphere of charge of − 0.8 μC in the air is 0.2 N.
(a) What is the distance between the two spheres?
(b) What is the force on the second sphere due to the first?
Solution:
(a) Electrostatic force on the first sphere, F = 0.2 N
Charge on this sphere, q1 = 0.4 μC = 0.4 × 10−6 C
Charge on the second sphere, q2 = − 0.8 μC = − 0.8 × 10−6 C
The electrostatic force between the spheres is given by the relation,
Where ∈0 = Permittivity of free space.
r² = q1q24π∈0F = 9×109×0.4×10-6× 0.8×10-6x 0.2 = 144×10-4x r
⇒ r = 144×10-4 = 0.12 m. (b) Both the spheres attract each other with the same force. Hence, the force on the second sphere due to the first is also 0.2 N.
Question 1.3:
Check that the ratio ke2/G memoemp is dimensionless. Lookup a Table of Physical Constants and determine the value of this ratio. What does the ratio signify?
Solution:
The Given ratio is 
where,
G = Gravitational constant
Its unit is N m2 kg−2.
me and mp = Masses of electron and proton.
Their unit is kg.
e = Electric charge.
Its unit is C.
∈0 = Permittivity of free space
Its unit is N m2 C−2.
Therefore, the unit of the given ratio is,
Hence, the given ratio is dimensionless.
e = 1.6 × 10−19 C
G = 6.67 × 10−11 N m2 kg-2
me= 9.1 × 10−31 kg
mp = 1.66 × 10−27 kg
So, the numerical value of the given ratio is
This is the ratio of electric force to the gravitational force between a proton and an electron, keeping the distance between them constant.
Question 1.4:
(a) Explain the meaning of the statement ‘electric charge of a body is quantized’.
(b) Why can one ignore quantization of electric charge when dealing with macroscopic i.e., large-scale charges?
Solution:
(a) Electric charge of a body is quantized. This means that only an integral (1, 2, …., n) number of electrons can be transferred from one body to the other. Charges are not transferred infractions. Hence, a body possesses total charge only in integral multiples of electric charge.
(b) In macroscopic or large-scale charges, the charges used are huge as compared to the magnitude of electric charge. Hence, quantization of electric charge is of no use on a macroscopic scale. Therefore, it is ignored and it is considered that the electric charge is continuous.
Question 1.5:
When a glass rod is rubbed with a silk cloth, charges appear on both. A similar phenomenon is observed with many other pairs of bodies. Explain how this observation is consistent with the law of conservation of charge.
Solution:
Rubbing produces charges of equal magnitude but opposite nature on the two bodies because charges are created in pairs. This phenomenon of charging is called charging by friction. The net charge on the system of two rubbed bodies is zero. This is because equal amounts sent of opposite charges annihilate each other. When a glass rod is rubbed with a silk cloth, opposite-natured charges appear on both the bodies. This phenomenon is consistent with the law of conservation of energy. A similar phenomenon is observed with many other pairs of bodies.
Question 1.6:
Four-point charges qA = 2 μC, qB = −5 μC, qC = 2 μC, and qD = −5 μC are located at the corners of a square ABCD of side 10 cm. What is the force on a charge of 1 μC placed at the center of the square?
Solution:
The given figure shows a square of a side 10 cm with four charges placed at its corners. O is the center of the square.
Where,
(Sides) AB = BC = CD = AD = 10 cm
(Diagonals) AC = BD = cm
AO = OC = DO = OB = cm
A charge of amount 1μC is placed at point O.
Force of repulsion between charges placed at corner A and center O is equal in magnitude but opposite in direction relative to the force of repulsion between the charges placed at corner C and center O. Hence, they will cancel each other. Similarly, the force of attraction between charges placed at corner B and center O is equal in magnitude but opposite in direction relative to the force of attraction between the charges placed at corner D and center O. Hence, they will also cancel each other. Therefore, the net force caused by the four charges placed at the corner of the square on the 1 μC charge at center O is zero.
Question 1.7:
(a) An electrostatic field line is a continuous curve. That is, a field line cannot have sudden breaks. Why not?
(b) Explain why two field lines never cross each other at any point?
Solution:
(a) An electrostatic field line is a continuous curve because a charge experiences a continuous force when traced in an electrostatic field. The field line cannot have sudden breaks because the charge moves continuously and does not jump from one point to the other.
(b) If two field lines cross each other at a point, then electric field intensity will show two directions at that point. It is not possible. Hence, two field lines never cross each other.
Question 1.8:
Two-point charges qA = 3 μC and Bq = −3 μC are located 20 cm apart in vacuum.
(a) What is the electric field at the midpoint O of the line AB joining the two charges?
(b) If a negative test charge of magnitude 1.5 × 10−9 C is placed at this point, what is the force experienced by the test charge?
Solution:
(a) The situation is represented in the given figure. O is the mid-point of line AB.
Distance between the two charges, AB = 20 cm
∴AO = OB = 10 cm
The net electric field at point O = E
The electric field at point O is caused by a +3μC charge,
E1 = 
along OB.
Where,
∈∘ = Permittivity of free space
The magnitude of the electric field at point O is caused a by −3μC charge,
along OB.
Therefore, the electric field at mid-point O is 5.4 × 106 N C−1 along OB.
= 5.4 × 106 N/C along OB
(b) A test charge of amount 1.5 × 10−9 C is placed at mid-point O.
q = 1.5 × 10−9 C
Force experienced by the test charge = F
∴F = qE
= 1.5 × 10−9 × 5.4 × 106
= 8.1 × 10−3 N
The force is directed along line OA. This is because the negative test charge is repelled by the charge placed at point B but attracted towards point A.
Therefore, the force experienced by the test charge is 8.1 × 10−3 N along with OA.
Question 1.9:
A system has two charges qA = 2.5 × 10−7 C and qB = −2.5 × 10−7 C located at points A: (0, 0, − 15 cm) and B: (0, 0, + 15 cm), respectively. What is the total charge and electric dipole moment of the system?
Solution:
Both the charges can be located in a coordinate frame of reference as shown in the given figure.
At A, the amount of charge, qA = 2.5 × 10−7C
At B, the amount of charge, qB = −2.5 × 10−7 C
The total charge of the system,
q = qA + qB
= 2.5 × 107 C − 2.5 × 10−7 C
= 0
Distance between two charges at points A and B,
d = 15 + 15 = 30 cm = 0.3 m
Electric dipole moment of the system is given by,
p = qA × d = qB × d
= 2.5 × 10−7 × 0.3
= 7.5 × 10−8 C m along the positive z-axis
Therefore, the electric dipole moment of the system is 7.5 × 10−8 C m along the positive z−axis.
Question 1.10
An electric dipole with a dipole moment 4 × 10−9 C m is aligned at 30° with the direction of a uniform electric field of magnitude 5 × 104 N C−1. Calculate the magnitude of the torque acting on the dipole.
Solution:
Electric dipole moment, p = 4 × 10−9 C m
Angle made by p with a uniform electric field, θ = 30°
Electric field, E = 5 × 104 N C−1
The torque acting on the dipole is given by the relation,
τ = pE sinθ
Therefore, the magnitude of the torque acting on the dipole is 10−4 N m.
Question 1.11:
A polythene piece rubbed with wool is found to have a negative charge of 3 × 10−7 C.
(a) Estimate the number of electrons transferred (from which to which?)
(b) Is there a transfer of mass from wool to polythene?
Solution:
(a) When polythene is rubbed against wool, several electrons get transferred from wool to polythene. Hence, the wool becomes positively charged and polythene becomes negatively charged.
Amount of charge on the polythene piece, q = −3 × 10−7 C
Amount of charge on an electron, e = −1.6 × 10−19 C
Number of electrons transferred from wool to polythene = n
n can be calculated using the relation,
q = ne
=> n=q ∕ e
= 1.87 × 1012
Therefore, the number of electrons transferred from wool to polythene n = 1.87 × 1012.
(b) Yes. There is a transfer of mass taking place. This is because an electron has mass,
me = 9.1 × 10−3 kg
Total mass transferred to polythene from wool,
m = me × n
= 9.1 × 10−31 × 1.85 × 1012
= 1.706 × 10−18 kg
Therefore, a negligible mass has been transferred from polythene to wool.
Question 1.12:
(a) Two insulated charged copper spheres A and B have their centers separated by a distance of 50 cm. What is the mutual force of electrostatic repulsion if the charge on each is 6.5 × 10−7 C? The radii of A and B are negligible compared to the distance of separation.
(b) What is the force of repulsion if each sphere is charged double the above amount, and the distance between them is halved?
Solution:
(a) Charge on sphere A, QA = Charge on sphere B, qB = 6.5 × 10−7 C
Distance between the spheres, r = 50 cm = 0.5 m
Force of repulsion between the two spheres,
Where,
∈0 = Free space permittivity
= 9 × 109 N m2 C−2
= 1.52 × 10−2 N
Therefore, the force between the two spheres is 1.52 × 10−2 N. Therefore, the force between the two spheres is 1.52 × 10−2 N.
(b) After doubling the charge, charge on sphere A, qA = Charge on sphere B, qB = 2 × 6.5 × 10−7 C = 1.3 × 10−6 C
The distance between the spheres is halved.
Force of repulsion between the two spheres,
= 16 × 1.52 × 10−2
= 0.243 N
Therefore, the force between the two spheres is 0.243 N.
Question 1.13:
Suppose the spheres A and B in Exercise 1.12 have identical sizes. A third sphere of the same size but uncharged is brought in contact with the first, then brought in contact with the second, and finally removed from both. What is the new force of repulsion between A and B?
Solution:
Distance between the spheres, A and B, r = 0.5 m
Initially, the charge on each sphere, q = 6.5 × 10−7 C
When sphere A is touched with an uncharged sphere C,
amount of charge from A will transfer to sphere C. Hence, the charge on each of the spheres, A and C, is
When sphere C with charge is brought in contact with sphere B with charge q, total charges on the system will divide into two halves given as,
Each sphere will share each half. Hence, the charge on each of the spheres, C and B, is
.
Force of repulsion between sphere A having charge and sphere B having charge
Therefore, the force of attraction between the two spheres is 5.703 × 10−3 N.
Question 1.14:
Figure 1.33 shows tracks of three charged particles in a uniform electrostatic field. Give the signs of the three charges. Which particle has the highest charge the mass ratio?
Solution:
Opposite charges attract each other and the same charges repel each other. It can be observed that particles 1 and 2 both move towards the positively charged plate and repel away from the negatively charged plate. Hence, these two particles are negatively charged. It can also be observed that particle 3 moves towards the negatively charged plate and repels away from the positively charged plate. Hence, particle 3 is positively charged.
The charge to mass ratio (emf) is directly proportional to the displacement or amount of deflection for a given velocity. Since the deflection of particle 3 is the maximum, it has the highest charge to mass ratio.
Question 1.15:
Consider a uniform electric field E = 3 × 103 îN/C. (a) What is the flux of this field through a square of 10 cm on a side whose plane is parallel to the yz plane? (b) What is the flux through the same square if the normal to its plane makes a 60° angle with the x-axis?
Solution:
(a) Electric field intensity,
= 3 × 103 î N/C
The magnitude of electric field intensity,
= 3 × 103 N/C
Side of the square, s = 10 cm = 0.1 m
Area of the square, A = s2 = 0.01 m2
The plane of the square is parallel to the y-z plane. Hence, the angle between the unit vector normal to the plane and electric field, θ = 0°
Flux (Φ) through the plane is given by the relation,
Φ =
= 3 × 103 × 0.01 × cos0°
= 30 N m2/C
(b) Plane makes an angle of 60° with the x-axis. Hence, θ = 60°
Flux, Φ =
= 3 × 103 × 0.01 × cos60°
= = 15 N m2/C
Question 1.16:
What is the net flux of the uniform electric field of Exercise 1.15 through a cube of side 20 cm oriented so that its faces are parallel to the coordinate planes?
Solutions:
All the faces of a cube are parallel to the coordinate axes. Therefore, the number of field lines entering the cube is equal to the number of field lines piercing out of the cube. As a result, net flux through the cube is zero.
Question 1.17:
Careful measurement of the electric field at the surface of a black box indicates that the net outward flux through the surface of the box is 8.0 × 103 N m2/C. (a) What is the net charge inside the box? (b) If the net outward flux through the surface of the box were zero, could you conclude that there were no charges inside the box? Why or Why not?
Solution:
(a) Net outward flux through the surface of the box, Φ = 8.0 × 103 N m2/C
For a body containing net charge q, flux is given by the relation, 
∈0 = Permittivity of free space
= 8.854 × 10−12 N−1C2 m−2
q = ∈0Φ
= 8.854 × 10−12 × 8.0 × 103
= 7.08 × 10−8
= 0.07 μC
Therefore, the net charge inside the box is 0.07 μC.
(b) No
Net flux piercing out through a body depends on the net charge contained in the body. If the net flux is zero, then it can be inferred that net the charge inside the body is zero. The body may have an equal amount of positive and negative charges.
Question 1.18:
A point charge +10 μC is a distance of 5 cm directly above the center of a square of side 10 cm, as shown in Fig. 1.34. What is the magnitude of the electric flux through the square? (Hint: Think of the square as one face of a cube with an edge of 10 cm.)
Solution:
The square can be considered as one face of a cube with an edge of 10 cm with a center where charge q is placed. According to Gauss’s theorem for a cube, total electric flux is through all its six faces.
Hence, electric flux through one face of the cube i.e., through the square,
Where,
∈0 = Permittivity of free space
= 8.854 × 10−12 N−1C2 m−2
q = 10 μC = 10 × 10−6 C
1.88 × 105 N m2 C−1
Therefore, electric flux through the square is 1.88 × 105 N m2 C−1.
Question 1.19:
A point charge of 2.0 μC is at the center of a cube is a Gaussian surface of 9.0 cm on the edge. What is the net electric flux through the surface?
Solution:
Net electric flux (ΦNet) through the cubic surface is given by,
Where,
∈0 = Permittivity of free space
= 8.854 × 10−12 N−1C2 m−2
q = Net charge contained inside the cube = 2.0 μC = 2 × 10−6 C
= 2.26 × 105 N m2 C−1
The net electric flux through the surface is 2.26 × 105 N m2 C−1.
Question 1.20:
A point charge causes an electric flux of −1.0 × 103 Nm2/C to pass through a spherical Gaussian surface of a 10.0 cm radius centered on the charge. (a) If the radius of the Gaussian surface were doubled, how much flux would pass through the surface? (b) What is the value of the point charge?
Solution:
(a) Electric flux, Φ = −1.0 × 103 N m2/C
The radius of the Gaussian surface,
r = 10.0 cm
Electric flux piercing out through a surface depends on the net charge enclosed inside a body. It does not depend on the size of the body. If the radius of the Gaussian surface is doubled, then the flux passing through the surface remains the same i.e., −103 N m2/C.
(b) Electric flux is given by the relation,
Where,
q = net charge enclosed by the spherical surface
∈0 = Permittivity of free space = 8.854 × 10−12 N−1C2 m−2
= −1.0 × 103 × 8.854 × 10−12
= −8.854 × 10−9 C
= −8.854 nC
Therefore, the value of the point charge is −8.854 nC.
Question 1.21:
A conducting sphere of radius 10 cm has an unknown charge. If the electric field 20 cm from the center of the sphere is 1.5 × 103 N/C and points radially inward, what is the net charge on the sphere?
Solution:
Electric field intensity (E) at a distance (d) from the center of a sphere containing net charge q is given by the relation,
Where,
q = Net charge = 1.5 × 103 N/C
d = Distance from the center = 20 cm = 0.2 m
∈0 = Permittivity of free space
and, = 9 × 109 N m2 C−2
= 6.67 × 109 C
= 6.67 nC
Therefore, the net charge on the sphere is 6.67 nC.
Question 1.22:
A uniformly charged conducting sphere of 2.4 m in diameter has a surface charge density of 80.0 μC/m2. (a) Find the charge on the sphere. (b) What is the total electric flux leaving the surface of the sphere?
Solution:
(a) Diameter of the sphere, d = 2.4TradiusThe radius
Radius of the sphere, r = 1.2 m
Surface charge density, σ = 80.0 μC/m2 = 80 × 10−6 C/m2
The total charge on the surface of the sphere,
Q = Charge density × Surface area
= 80 × 10−6 × 4 × 3.14 × (1.2)2
= 1.447 × 10−3 C
Therefore, the charge on the sphere is 1.447 × 10−3 C.
(b) Total electric flux leaving out the surface of a sphere containing net charge Q is given by the relation,
Where,
∈0 = Permittivity of free space
= 8.854 × 10−12 N−1C2 m−2
Q = 1.447 × 10−3 C
= 1.63 × 108 N C−1 m2
Therefore, the total electric flux leaving the surface of the sphere is 1.63 × 108 N C−1 m2.
Question 1.23:
An infinite line charge produces a field of 9 × 104 N/C at a distance of 2 cm. Calculate the linear charge density.
Solution:
The electric field produced by the infinite line charges at a distance d having linear charge density λ is given by the relation,
Where,
d = 2 cm = 0.02 m
E = 9 × 104 N/C
∈0 = Permittivity of free space
= 9 × 109 N m2 C−2
=10 μC/m
Therefore, the linear charge density is 10 μC/m.
Question 1.24:
Two large, thin metal plates are parallel and close to each other. On their inner faces, the plates have surface charge densities of opposite si and magnitude 17.0 × 10−22 C/m2. What is E: (a) in the outer region of the first plate, (b) in the outer region of the second plate, and (c) between the plates?
Solution:
The situation is represented in the following figure.
A and B are two parallel plates close to each other. The outer region of plate A is labeled as I, the outer region of plate B is labeled as III, and the region between the plates, A and B, is labeled as II.
The charge density of plate A, σ = 17.0 × 10−22 C/m2
The charge density of plate B, σ = −17.0 × 10−22 C/m2
In the regions, I and III, electric field E is zero. This is because the use charge is not enclosed by the respective plates.
Electric field E in region II is given by the relation,
Where,
∈0 = Permittivity of free space = 8.854 × 10−12 N−1C2 m−2
= 1.92 × 10−10 N/C
Therefore, the electric field between the plates is 1.92 × 10−10 N/C.
Question 1.25:
An oil drop of 12 excess electrons is held stationary under a constant electric field of 2.55 × 104 N C−1 in Millikan’s oil drop experiment. The density of the oil is 1.26 g cm−3. Estimate the radius of the drop. (g = 9.81 m s−2; e = 1.60 × 10−19 C).
Solution:
Excess electrons on an oil drop, n = 12
Electric field intensity, E = 2.55 × 104 N C−1
Density of oil, ρ = 1.26 gm/cm3 = 1.26 × 103 kg/m3
Acceleration due to gravity, g = 9.81 m s−2
Charge on an electron, e = 1.6 × 10−19 C
The radius of the oil drop = r
Force (F) due to electric field E is equal to the weight of the oil drop (W)
F = W
Eq = mg
Where,
q = Net charge on the oil drop = ne
m = Mass of the oil drop
= Volume of the oil drop × Density of oil
= 9.82 × 10−4 mm
Therefore, the radius of the oil drop is 9.82 × 10−4 mm.
Question 1.26:
Which among the curves shown in Fig. 1.35 cannot possibly represent electrostatic field lines?
(a)
(b)
(c)
(d)
(e)
Solution:
(a) The field lines showed in (a) do not represent electrostatic field lines because field lines must be normal to the surface of the conductor.
(b) The field lines showed in (b) do not represent electrostatic field lines because the field lines cannot emerge from a negative charge and cannot terminate at a positive charge.
(c) The field lines shown in (c) represent electrostatic field lines. This is because the field lines emerge from the positive charges and repel each other.
(d) The field dishonored in (d) does not represent electrostatic field lines because the field lines should not intersect each other.
(e) The field lines showed in (e) do not represent electrostatic field lines because closed loops are not formed in the area between the field lines.
Question 1.27:
In a certain region of space, the electric field is along the z-direction throughout. The magnitude of the electric field is, however, not constant but increases uniformly along the positive z-direction, at the rate of 105 NC−1 per meter. What are the force and torque experienced by a system having a total dipole moment equal to 10−7 Cm in the negative z-direction?
Solution:
The dipole moment of the system, p = q × dl = −10−7 C m
Rate of increase of electric field per unit length,
Force (F) experienced by the system is given by the relation,
F = qE
= −10−7 × 10−5
= −10−2 N
The force is −10−2 N in the negative z-direction i.e., opposite to the direction of the electric field. Hence, the angle between the electric field and the dipole moment is 180°.
Torque (τ) is given by the relation,
τ = pE sin180°
= 0
Therefore, the torque experienced by the system is zero.
Question 1.28:
(a) A conductor A with a cavity as shown in Fig. 1.36(a) is given a charge Q. Show that the entire charge must appear on the outer surface of the conductor. (b) Another conductor B with charge q is inserted into the cavity keeping B insulated from A. Show that the total charge on the outside surface of A is Q + q [Fig. 1.36(b)]. (c) A sensitive instrument is to be shielded from the strong electrostatic fields in its environment. Suggest a possible way.
Solution:
(a) Let us consider a Gaussian surface that is lying wholly within a conductor and enclosing the cavity. The electric field intensity E inside the charged conductor is zero.
Let q is the charge inside the conductor and ∈∘ is the permittivity of free space.
According to Gauss’s law,
Flux, 
Here, E = 0
Therefore, the charge inside the conductor is zero.
The entire charge Q appears on the outer surface of the conductor.
(b) The outer surface of conductor A has a charge of amount Q. Another conductor B having charge +q is kept inside conductor A and it is insulated from A. Hence, a charge of amount −q will be induced on the inner surface of conductor A and +q is induced on the outer surface of conductor A. Therefore, the total charge on the outer surface of conductor A is Q + q.
(c) A sensitive instrument can be shielded from the strong electrostatic field in its environment by enclosing it fully inside a metallic surface. A closed metallic body acts as an electrostatic shield.
Question 1.29:
A hollow charged conductor has a tiny hole cut into its surface. Show that the electric field in the hole is
, where is the unit vector in the outward normal direction, and σ is the surface charge density near the hole.
Solution:
Let us consider a conductor with a cavity or a hole. The electric field inside the cavity is zero.
Let E is the electric field just outside the conductor, q is the electric charge, σ is the charge density, and ∈∘ is the permittivity of free space.
Charge
According to Gauss’s law,
Therefore, the electric field just outside the conductor is
. This field is a superposition of field due to the cavity and the field due to the rest of the charged conductor These fields are equal and opposite inside the conductor, and equal in magnitude and direction outside the conductor.
Therefore, the field due to the rest of the conductor is 
Hence, proved.
Question 1.30:
Obtain the formula for the electric field due to a long thin wire of uniform linear charge density λ without using Gauss’s law. [Hint: Use Coulomb’s law directly and evaluate the necessary integral.
Solution:
Take a long thin wire XY (as shown in the figure) of uniform linear charge density 
Consider a point A at a perpendicular distance l from the mid-point O of the wire, as shown in the following figure.
Let E be the electric field at point A due to the wire, XY.
Consider a small length element dx on the wire section with OZ = x
Let q be the charge on this piece.
Electric field due to the piece,
The electric field is resolved into two rectangular components.
is the perpendicular component and
is the parallel component.
When the whole wire is considered, the component is canceled.
Only the perpendicular component affects point A.
Hence, the effective electric field at point A due to the element dx is dE1.
By differentiating equation (2), we obtain
dxdθ = lsec2θdx = lsec2θ dθ
From equation (2),
Putting equations (3) and (4) in equation (1), we obtain
The wire is so long that 
tends from
By integrating equation (5), we obtain the value of field E1 as,
Therefore, the electric field due to the long wire is 
.
Question 1.31:
It is now believed that protons and neutrons (which constitute nuclei of ordinary matter) are themselves built out of more elementary units called quarks. A proton and a neutron consist of three quarks each. Two types of quarks, the so-called ‘up’ quark (denoted by u) of charge (+2/3) e, and the ‘down’ quark (denoted by d) of charge (−1/3) e, together with electrons build up ordinary matter. (Quarks of other types have also been found which give rise to different unusual varieties of matter.) Suggest a possible quark composition of a proton and neutron.
Solution:
A proton has three quarks. Let there be n up quarks in a proton, each having a charge of 
.
Charge due to n up quarks 
Number of down quarks in a proton = 3 − n
Each down quark has a charge oThe number
The number of down quarks is 3 − n, each having a charge of 
Charge on a neutron due to 
down quarks = 
Total charge on a neutron = 0
Number of up quarks in a neutron, n = 1
Number of down quarks in a neutron = 3 − n = 2
Therefore, a neutron can be represented with the number resented as ‘udd’.
Question 1.32:
(a) Consider an arbitrary electrostatic field configuration. A small test charge is placed at a null point (i.e., where E = 0) of the configuration. Show that the equilibrium of the test charge is necessarily unstable.
(b) Verify this result for the simple configuration of two charges of the same magnitude and sign placed a certain distance apart.
Solution:
(a) Let the equilibrium of the test charge be stable. If a test charge is in equilibrium and displaced from its position in any direction, then it experiences a restoring force towards a null point, where the electric field is zero. All the field lines near the null point are directed inwards towards the null point. There is a net inward flux of electric field through a closed surface around the null point. According to Gauss’s law, the flux of electric field through a surface, which is not enclosing any charge, is zero. Hence, the equilibrium of the test charge can be stable.
(b) Two charges of the same magnitude and same sign are placed at a certain distance. The mid-point of the joining line of the charges is the null point. When a test charged is displaced along the line, it experiences a restoring force. If it is displaced normal to the joining line, then the net force takes it away from the null point. Hence, the charge is unstable because the stability of equilibrium requires restoring force in all directions.
Question 1.33:
A particle of mass m and charge (−q) enters the region between the two charged plates initially moving along the x-axis with speed vx (like particle 1 in Fig. 1.33). The length of the plate is L and a uniform electric field E is maintained between the plates. Show that the vertical deflection of the particle at the far edge of the plate is qEL2/ (2m
)
Compare this motion with the motion of a projectile the in gravitational field discussed in Section 4.10 of Class XI Textbook of Physics.
Solution:
Charge on a particle of mass m = − q
The velocity of the particle = vx
Length of the plates = L
The magnitude of the uniform electric field between the plates = E
Mechanical force, F = Mass (m) × Acceleration (a)
Therefore, acceleration, 
The Time taken by the particle to cross the field of length L is given by,
t
In the vertical direction, initial velocity, u = 0
According to the third equation of motion, vertical deflection s of the particle can be obtained as,
Hence, the vertical deflection of the particle at the far edge of the plate is
.This is similar to the motion of horizontal projectiles under gravity.
Question 1.34:
Suppose that the particle in Exercise 1.33 is an electron projected with velocity vx= 2.0 × 106 m s−1. If E between the plates separated by 0.5 cm is 9.1 × 102 N/C, where will the electron strike the upper plate? (| e | =1.6 × 10−19 C, me = 9.1 × 10−31 kg.)
Solution:
Velocity of the particle, vx = 2.0 × 106 m/s
Separation of the two plates, d = 0.5 cm = 0.005 m
The electric field between the two plates, E = 9.1 × 102 N/C
Charge on an electron, q = 1.6 × 10−19 C
Mass of an electron, me = 9.1 × 10−31 kg
Let the electron strike the upper plate at the end of plate L when deflection is s.
Therefore,
Therefore, the electron will strike the upper plate after traveling 1.6 cm.