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Electric Charges and Fields — NCERT Solutions

Madhya Pradesh Board · Class 12 · Physics

NCERT Solutions for Electric Charges and Fields, Madhya Pradesh Board Class 12 Physics: 23 textbook questions solved step by step. Covers Exercises.

141 questions68 flashcards7 formulas & key relations5 concepts

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Exercises

1.1What is the force between two small charged spheres having charges of 2×10−7C2 \times 10^{-7}\mathrm{C} and 3×10−7C3 \times 10^{-7}\mathrm{C} placed 30 cm30~\mathrm{cm} apart in air?Show solution

Using Coulomb’s law,

F=kq1q2r2F = k\dfrac{q_1q_2}{r^2}

Given: q1=2×10−7 Cq_1=2\times10^{-7}\,\text{C}, q2=3×10−7 Cq_2=3\times10^{-7}\,\text{C}, r=30 cm=0.30 mr=30\,\text{cm}=0.30\,\text{m}, and k=9×109 N m2/C2k=9\times10^9\,\text{N m}^2\text{/C}^2.

F=9×109×(2×10−7)(3×10−7)(0.30)2 F=9\times10^9\times\frac{(2\times10^{-7})(3\times10^{-7})}{(0.30)^2}

=(9×109)×6×10−140.09 =(9\times10^9)\times\frac{6\times10^{-14}}{0.09}

=9×109×6.67×10−13=6.0×10−3 N =9\times10^9\times6.67\times10^{-13} =6.0\times10^{-3}\,\text{N}

So the force is repulsive because both charges are positive.

1.2The electrostatic force on a small sphere of charge 0.4μC0.4\mu \mathrm{C} due to another small sphere of charge −0.8μC-0.8\mu \mathrm{C} in air is 0.2N0.2\mathrm{N}. (a) What is the distance between the two spheres? (b) What is the force on the second sphere due to the first?Show solution

By Coulomb’s law,

F=k∣q1q2∣r2 F=k\frac{|q_1q_2|}{r^2}

Given F=0.2 NF=0.2\,\text{N}, q1=0.4 μC=0.4×10−6 Cq_1=0.4\,\mu\text{C}=0.4\times10^{-6}\,\text{C}, q2=0.8 μC=0.8×10−6 Cq_2=0.8\,\mu\text{C}=0.8\times10^{-6}\,\text{C}.

So,
r2=k∣q1q2∣F=9×109×(0.4×10−6)(0.8×10−6)0.2 r^2=k\frac{|q_1q_2|}{F} =9\times10^9\times\frac{(0.4\times10^{-6})(0.8\times10^{-6})}{0.2}

=9×109×0.32×10−120.2=9×109×1.6×10−12=1.44×10−2 =9\times10^9\times\frac{0.32\times10^{-12}}{0.2} =9\times10^9\times1.6\times10^{-12} =1.44\times10^{-2}

r=1.44×10−2=0.12 m r=\sqrt{1.44\times10^{-2}}=0.12\,\text{m}

So the distance is 0.12 m.

For the force on the second sphere, by Newton’s third law, it has the same magnitude and opposite direction. Since the charges are unlike, the force is attractive.

1.3Check that the ratio ke2/Gmempke^2 /G m_e m_p is dimensionless. Look up a Table of Physical Constants and determine the value of this ratio. What does the ratio signify?Show solution

To check dimensions:

ke2Gmemp \frac{ke^2}{Gm_em_p}

  • kk has units N m2/C2\text{N m}^2\text{/C}^2
  • e2e^2 has units C2\text{C}^2
  • GG has units N m2/kg2\text{N m}^2\text{/kg}^2
  • mempm_em_p has units kg2\text{kg}^2

So the units are

(N m2/C2)(C2)(N m2/kg2)(kg2)=1 \frac{(\text{N m}^2\text{/C}^2)(\text{C}^2)}{(\text{N m}^2\text{/kg}^2)(\text{kg}^2)}=1

Hence the ratio is dimensionless.

From the chapter, the value is approximately

ke2Gmemp≈2.4×1039 \frac{ke^2}{Gm_em_p}\approx 2.4\times10^{39}

This ratio signifies the relative strength of electric force to gravitational force between a proton and an electron. The electric force is about 103910^{39} times stronger.

1.4(a) Explain the meaning of the statement 'electric charge of a body is quantised'.
(b) Why can one ignore quantisation of electric charge when dealing with macroscopic i.e., large scale charges?
Show solution

(a) Electric charge is quantised means the charge on any body is always an integral multiple of the elementary charge ee:

q=ne,n=0,±1,±2,… q=ne, \quad n=0,\pm1,\pm2,\ldots

So charge does not vary continuously at the microscopic level; it exists in discrete units of ee.

(b) For macroscopic bodies, the total charge contains an extremely large number of electrons or protons. Since e=1.6×10−19 Ce=1.6\times10^{-19}\,\text{C} is very small, the step size is negligible compared with ordinary charges like microcoulombs. Therefore charge appears continuous and quantisation can be ignored at large scale.

1.5When 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.Show solution

This is consistent with conservation of charge because when two bodies are rubbed, no new charge is created or destroyed. Charges are only transferred from one body to the other. For example, when a glass rod is rubbed with silk, some electrons move from the glass to the silk. So the glass becomes positively charged and the silk negatively charged, but the total charge of the combined system remains the same.

1.6Four point charges qA=2μC q_{\mathrm{A}} = 2\mu \mathrm{C} , qB=−5μC q_{\mathrm{B}} = -5\mu \mathrm{C} , qC=2μC q_{\mathrm{C}} = 2\mu \mathrm{C} , and qD=−5μC q_{\mathrm{D}} = -5\mu \mathrm{C} are located at the corners of a square ABCD of side 10 cm 10~\mathrm{cm} . What is the force on a charge of 1μC 1\mu \mathrm{C} placed at the centre of the square?Show solution

At the centre of the square, the charges at opposite corners are at equal distances from the centre.

  • The two +2 μC charges are at opposite corners, so their forces on the central test charge are equal and opposite.
  • The two −5 μC charges are also at opposite corners, so their forces on the central test charge are equal and opposite.

Therefore all forces cancel pairwise, and the net force is zero.

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?
Show solution

(a) A field line is drawn so that its tangent at every point gives the direction of the electric field. Since the electric field at a point has a definite direction, the field line must be a continuous curve. A sudden break would mean the field has no direction at that point, which is not possible.

(b) Two field lines can never cross because if they did, the electric field at the point of intersection would have two directions at the same time, which is impossible. The field at any point can have only one unique direction.

1.8Two point charges qA=3μC q_{\mathrm{A}} = 3\mu \mathrm{C} and qB=−3μC q_{\mathrm{B}} = -3\mu \mathrm{C} are located 20 cm 20~\mathrm{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 1.5×10−9C1.5 \times 10^{-9} \mathrm{C} is placed at this point, what is the force experienced by the test charge?
Show solution

The midpoint is 0.10 m0.10\,\text{m} from each charge.

For the positive charge +3 μC+3\,\mu\text{C}, the field at O is away from the positive charge, i.e. towards B.
For the negative charge −3 μC-3\,\mu\text{C}, the field at O is towards the negative charge, i.e. also towards B.
So the fields add.

Magnitude due to one charge:
E1=kqr2=9×109×3×10−6(0.10)2=2.7×106 N/C E_1=\frac{kq}{r^2}=\frac{9\times10^9\times3\times10^{-6}}{(0.10)^2} =2.7\times10^6\,\text{N/C}

Total field:
E=2E1=5.4×106 N/C E=2E_1=5.4\times10^6\,\text{N/C}

directed from the positive charge to the negative charge.

For the test charge q0=−1.5×10−9 Cq_0=-1.5\times10^{-9}\,\text{C},
F=q0E F=q_0E
Magnitude:
∣F∣=(1.5×10−9)(5.4×106)=8.1×10−3 N |F|=(1.5\times10^{-9})(5.4\times10^6)=8.1\times10^{-3}\,\text{N}
Since the test charge is negative, the force is opposite to the field direction, i.e. towards the positive charge.

1.9A system has two charges qA=2.5×10−7C q_{\mathrm{A}} = 2.5 \times 10^{-7} \mathrm{C} and qB=−2.5×10−7C q_{\mathrm{B}} = -2.5 \times 10^{-7} \mathrm{C} located at points A: (0, 0, -15 cm) and B: (0, 0, +15 cm), respectively. What are the total charge and electric dipole moment of the system?Show solution

Total charge:
qtotal=2.5×10−7+(−2.5×10−7)=0 q_{\text{total}}=2.5\times10^{-7}+(-2.5\times10^{-7})=0

Dipole moment is
p=q×2a p^ \mathbf{p}=q\times 2a\,\hat{p}
Here the charges are on the zz-axis at −15 cm-15\,\text{cm} and +15 cm+15\,\text{cm}, so separation is
2a=30 cm=0.30 m 2a=30\,\text{cm}=0.30\,\text{m}
Magnitude:
p=(2.5×10−7)(0.30)=7.5×10−8 C m p=(2.5\times10^{-7})(0.30)=7.5\times10^{-8}\,\text{C m}
Direction is from negative charge to positive charge, i.e. along +z-axis.

1.10An electric dipole with dipole moment 4×10−9Cm4 \times 10^{-9} \mathrm{Cm} is aligned at 30∘30^{\circ} with the direction of a uniform electric field of magnitude 5×104NC−15 \times 10^{4} \mathrm{NC}^{-1}. Calculate the magnitude of the torque acting on the dipole.Show solution

Torque on a dipole in a uniform field is

τ=pEsin⁡θ \tau=pE\sin\theta

Given p=4×10−9 C mp=4\times10^{-9}\,\text{C m}, E=5×104 N/CE=5\times10^4\,\text{N/C}, and θ=30∘\theta=30^\circ.

τ=(4×10−9)(5×104)sin⁡30∘ \tau=(4\times10^{-9})(5\times10^4)\sin30^\circ

=2×10−4×12=1×10−4 N m =2\times10^{-4}\times\frac{1}{2} =1\times10^{-4}\,\text{N m}

So the torque is 1×10−41\times10^{-4} N m.

1.11A polythene piece rubbed with wool is found to have a negative charge of 3×10−7C3 \times 10^{-7} \mathrm{C}.
(a) Estimate the number of electrons transferred (from which to which?)
(b) Is there a transfer of mass from wool to polythene?
Show solution

(a) Number of electrons transferred:

n=Qe=3×10−71.6×10−19 n=\frac{Q}{e}=\frac{3\times10^{-7}}{1.6\times10^{-19}}

=1.875×1012 =1.875\times10^{12}

Since the polythene becomes negatively charged, it must have gained electrons from the wool.

(b) Yes, there is a transfer of mass because electrons have mass. But the transferred mass is extremely small, so in practice it is negligible.

1.12(a) Two insulated charged copper spheres A and B have their centres separated by a distance of 50 cm50~\mathrm{cm}. What is the mutual force of electrostatic repulsion if the charge on each is 6.5×10−7C6.5\times 10^{-7}\mathrm{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?
Show solution

(a) Using Coulomb’s law,

F=kq2r2 F=k\frac{q^2}{r^2}

Given q=6.5×10−7 Cq=6.5\times10^{-7}\,\text{C} and r=50 cm=0.50 mr=50\,\text{cm}=0.50\,\text{m}.

F=9×109×(6.5×10−7)2(0.50)2 F=9\times10^9\times\frac{(6.5\times10^{-7})^2}{(0.50)^2}

=(9×109)×4.225×10−130.25=1.521×10−2 N =(9\times10^9)\times\frac{4.225\times10^{-13}}{0.25} =1.521\times10^{-2}\,\text{N}

So, approximately
F≈1.5×10−2 N F\approx 1.5\times10^{-2}\,\text{N}

(b) If each charge is doubled, force becomes 4 times.
If distance is halved, force becomes 4 times more.
So total increase = 4×4=164\times4=16 times.

F′=16F≈16(1.5×10−2)=2.4×10−1 N F' = 16F \approx 16(1.5\times10^{-2}) = 2.4\times10^{-1}\,\text{N}

So the new force is about 2.4×10−12.4\times10^{-1} N.

1.13Figure 1.30 shows tracks of three charged particles in a uniform electrostatic field. Give the signs of the three charges. Which particle has the highest charge to mass ratio?

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1.14Consider a uniform electric field E=3×103 hN/C\mathbf{E} = 3 \times 10^{3} \, \text{hN/C}. (a) What is the flux of this field through a square of 10 cm on a side whose plane is parallel to the yzyz plane? (b) What is the flux through the same square if the normal to its plane makes a 60∘60^{\circ} angle with the xx-axis?

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1.15What is the net flux of the uniform electric field of Exercise 1.14 through a cube of side 20 cm oriented so that its faces are parallel to the coordinate planes?

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1.16Careful 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 Nm2/C8.0 \times 10^{3} \, \text{Nm}^{2}/\text{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?

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1.17A point charge +10 μC+10 \, \mu\text{C} is a distance 5 cm directly above the centre of a square of side 10 cm, as shown in Fig. 1.31. What is the magnitude of the electric flux through the square? (Hint: Think of the square as one face of a cube with edge 10 cm.)

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1.18A point charge of 2.0 μC2.0 \, \mu\text{C} is at the centre of a cubic Gaussian surface 9.0 cm on edge. What is the net electric flux through the surface?

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1.19A point charge causes an electric flux of −1.0×103 Nm2/C-1.0 \times 10^{3} \, \text{Nm}^{2}/\text{C} to pass through a spherical Gaussian surface of 10.0 cm radius centred 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?

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1.20A conducting sphere of radius 10 cm has an unknown charge. If the electric field 20 cm from the centre of the sphere is 1.5×103 N/C1.5 \times 10^{3} \, \text{N/C} and points radially inward, what is the net charge on the sphere?

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1.21A uniformly charged conducting sphere of 2.4 m 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?

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1.22An infinite line charge produces a field of 9 × 10⁴ N/C at a distance of 2 cm. Calculate the linear charge density.

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1.23Two large, thin metal plates are parallel and close to each other. On their inner faces, the plates have surface charge densities of opposite signs and of 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?

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