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Electric Charges and Fields

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Summary

Chapter One: Electric Charges and Fields

Summary

  • Introduction to Electrostatics: Study of forces, fields, and potentials from static charges.
  • Electric Charge: Discovered by Thales; involves attraction of light objects by rubbed amber.
  • Static Electricity: Accumulation of electric charges due to friction.
  • Basic Properties of Electric Charge:
    • Quantisation: Total charge is an integral multiple of a basic charge (e.g., electron).
    • Additivity: Total charge is the algebraic sum of individual charges.
    • Conservation: Total charge in an isolated system remains constant.
  • Coulomb's Law: Force between two point charges is proportional to the product of their charges and inversely proportional to the square of the distance between them.
  • Electric Field: Force per unit charge experienced by a small positive test charge.
  • Electric Field Lines: Visual representation of electric fields; they cannot cross and are continuous.
  • Electric Dipole: Pair of equal and opposite charges separated by a distance, characterized by a dipole moment.

Key Formulas and Definitions

Physical QuantitySymbolDimensionsUnitRemarks
Electric fieldE[MLT⁻³A⁻¹]V m⁻¹
Electric fluxΦ[ML³ T⁻³A⁻¹]VmΦ = E.AS
Dipole momentp[LTA]CmVector directed from negative to positive charge
Surface charge densityσ[L⁻² TA]C m⁻²Charge per unit area
Linear charge densitya[L⁻¹ TA]C m⁻¹Charge per unit length
Volume charge densityρ[L⁻³ TA]C m⁻³Charge per unit volume

Learning Objectives

  • Understand the concept of electric charges and their properties.
  • Explain the phenomenon of static electricity and its applications.
  • Describe the behavior of conductors and insulators in the context of electric charge.
  • Apply Coulomb's law to calculate the force between charged objects.
  • Analyze the concept of electric fields and their representation through field lines.
  • Discuss the principle of superposition in electric forces.
  • Calculate electric flux and understand its relation to electric fields and charges.
  • Explain the concept of electric dipoles and their characteristics.

Detailed Notes

Chapter One: Electric Charges and Fields

1.1 Introduction

  • Static electricity is the accumulation of electric charges on insulating surfaces.
  • Common experiences include sparks from synthetic clothes and lightning during thunderstorms.
  • Electrostatics studies forces, fields, and potentials from static charges.

1.2 Electric Charge

  • Historical Context: Thales of Miletus discovered that amber rubbed with wool attracts light objects (600 BC).
  • Key Concepts:
    • Electric charge is quantized, meaning it exists in discrete amounts.
    • Charges can be positive or negative, and like charges repel while unlike charges attract.

1.3 Basic Properties of Electric Charge

  1. Additivity of Charges:
    • Total charge is the algebraic sum of individual charges.
    • Example: For charges +1, +2, -3, +4, and -5, total charge = (+1) + (+2) + (-3) + (+4) + (-5) = 0.
  2. Conservation of Charge:
    • Charge cannot be created or destroyed; it can only be transferred.
    • In an isolated system, total charge remains constant.
  3. Quantization of Charge:
    • Charge is an integral multiple of a basic unit (e.g., electron charge).
    • For macroscopic charges, quantization can often be ignored.

1.4 Conductors and Insulators

  • Conductors: Materials that allow electric charge to flow (e.g., metals, human bodies).
  • Insulators: Materials that resist the flow of electric charge (e.g., glass, plastic).
  • Charges on conductors distribute evenly over their surfaces, while charges on insulators remain localized.

1.5 Coulomb's Law

  • The force between two point charges is proportional to the product of their charges and inversely proportional to the square of the distance between them:
    • Formula: F = k * (q₁ * q₂) / r², where k = 9 × 10⁹ N m²/C².

1.6 Electric Field and Electric Flux

  • Electric Field (E): The force per unit charge experienced by a small positive test charge placed in the field.
  • Electric Flux (Φ): The product of the electric field (E) and the area (A) through which it passes:
    • Formula: Φ = E * A.

1.7 Electric Dipole

  • An electric dipole consists of two equal and opposite charges separated by a distance.
  • Dipole Moment (p): Defined as p = q * d, where d is the distance between charges.

1.8 Important Concepts

  • Field Lines: Represent the direction of the electric field; they cannot cross and are continuous curves.
  • Superposition Principle: The total force on a charge is the vector sum of forces due to other charges.

1.9 Exercises

  • Example problems include calculating forces between charges, distances, and electric fields in various configurations.

Exam Tips & Common Mistakes

Common Mistakes and Exam Tips

Common Pitfalls

  • Misunderstanding Electric Charge Conservation: Students often forget that electric charge cannot be created or destroyed. When charging by rubbing, one body gains electrons while the other loses them, maintaining the total charge.
  • Ignoring Charge Quantization: Many overlook that electric charge is quantized and should be treated as integral multiples of the elementary charge (e.g., electrons). This is often ignored in macroscopic scenarios but is crucial in theoretical discussions.
  • Incorrect Application of Coulomb's Law: Students may misapply Coulomb's Law by not considering the correct signs of charges, leading to errors in calculating forces.
  • Field Line Misinterpretation: It's common to confuse the direction and behavior of electric field lines. Remember that field lines start from positive charges and end at negative charges, and they cannot cross each other.

Exam Tips

  • Always Check Units: When solving problems, ensure that all units are consistent, especially when dealing with electric fields and forces.
  • Draw Diagrams: Visual aids can help clarify problems involving multiple charges or electric fields. Sketching can assist in understanding the relationships between charges and their effects.
  • Review Key Concepts: Make sure to understand the principles of superposition and how to apply them to multiple charge systems.
  • Practice with Different Scenarios: Work through various problems involving conductors and insulators, as well as different configurations of charges to solidify understanding.

Practice & Assessment

Multiple Choice Questions

A.

The glass rod becomes positively charged and the silk cloth becomes negatively charged.

B.

The glass rod becomes negatively charged and the silk cloth becomes positively charged.

C.

Both the glass rod and the silk cloth become positively charged.

D.

Both the glass rod and the silk cloth become negatively charged.
Correct Answer: A

Solution:

When a glass rod is rubbed with a silk cloth, electrons are transferred from the glass rod to the silk, resulting in the glass rod becoming positively charged and the silk cloth becoming negatively charged.

A.

0.2 N

B.

0.02 N

C.

0.002 N

D.

2 N
Correct Answer: A

Solution:

The force FF experienced by a charge qq in an electric field EE is given by F=qEF = qE. Substituting the given values, F=(1×106 C)(2×105 N/C)=0.2 NF = (1 \times 10^{-6} \text{ C})(2 \times 10^5 \text{ N/C}) = 0.2 \text{ N}.

A.

8.5 x 10^-5 N m

B.

6.0 x 10^-5 N m

C.

1.2 x 10^-5 N m

D.

1.5 x 10^-5 N m
Correct Answer: B

Solution:

Torque τ = pE sin θ = 3 x 10^-9 * 4 x 10^4 * sin(45°) = 6.0 x 10^-5 N m.

A.

Uniform and non-zero

B.

Zero

C.

Varies with distance from the center

D.

Infinite
Correct Answer: B

Solution:

Inside a uniformly charged conducting sphere, the electric field is zero due to the symmetry and distribution of charges.

A.

1.875 x 10¹²

B.

3.75 x 10¹²

C.

6.25 x 10¹²

D.

9.375 x 10¹²
Correct Answer: A

Solution:

The charge of one electron is approximately 1.6 x 10⁻¹⁹ C. The number of electrons transferred is 3×1071.6×1019=1.875×1012\frac{3 \times 10^{-7}}{1.6 \times 10^{-19}} = 1.875 \times 10^{12}.

A.

The paper is repelled by the comb.

B.

The paper remains stationary.

C.

The paper is attracted to the comb.

D.

The paper discharges the comb.
Correct Answer: C

Solution:

The charged comb polarises the piece of paper, inducing a net dipole moment, and the paper is attracted to the comb.

A.

The sum of the charges.

B.

The product of the charges.

C.

The difference of the charges.

D.

The square of the distance between the charges.
Correct Answer: B

Solution:

Coulomb's law states that the force between two point charges is proportional to the product of the charges and inversely proportional to the square of the distance between them.

A.

0 N/C

B.

3.75 x 10^4 N/C

C.

7.5 x 10^4 N/C

D.

1.5 x 10^5 N/C
Correct Answer: A

Solution:

Since the point is inside the conductor, the electric field is 0 N/C.

A.

1.44 µC

B.

14.4 µC

C.

144 µC

D.

1440 µC
Correct Answer: C

Solution:

The surface area of the sphere is given by A=4πr2A = 4\pi r^2. The radius rr is half of the diameter, so r=1.2r = 1.2 m. The charge QQ is given by Q=σA=σ×4πr2=80.0×4π(1.2)2=144μCQ = \sigma A = \sigma \times 4\pi r^2 = 80.0 \times 4\pi (1.2)^2 = 144 \mu C.

A.

The leaves diverge due to the flow of charge onto them.

B.

The leaves converge due to the flow of charge onto them.

C.

The leaves remain stationary.

D.

The leaves fall off.
Correct Answer: A

Solution:

When a charged object touches the metal knob, charge flows onto the leaves and they diverge.

A.

Coulombs per square meter (C/m²)

B.

Coulombs per cubic meter (C/m³)

C.

Coulombs per meter (C/m)

D.

Coulombs (C)
Correct Answer: C

Solution:

The unit of linear charge density is Coulombs per meter (C/m).

A.

qEaqEa

B.

2qEa\sqrt{2} qEa

C.

qEa/2qEa/\sqrt{2}

D.

2qEa2qEa
Correct Answer: B

Solution:

The torque τ\tau on a dipole in an electric field is given by τ=pEsinθ\tau = pE \sin \theta, where p=2qap = 2qa is the dipole moment. Thus, τ=2qaEsin45=2qEa\tau = 2qaE \sin 45^\circ = \sqrt{2} qEa.

A.

kqr2\frac{k \cdot q}{r^2}

B.

kqr\frac{k \cdot q}{r}

C.

kqr2k \cdot q \cdot r^2

D.

kqrk \cdot q \cdot r
Correct Answer: A

Solution:

The electric field EE due to a point charge qq is given by E=kqr2E = \frac{k \cdot q}{r^2} where kk is Coulomb's constant and rr is the distance from the charge.

A.

It becomes negatively charged

B.

It becomes positively charged

C.

It remains neutral

D.

It gains mass
Correct Answer: A

Solution:

When the glass rod is rubbed with silk, electrons are transferred from the glass to the silk, leaving the glass rod positively charged and the silk negatively charged, consistent with the conservation of charge.

A.

Ampere

B.

Coulomb

C.

Newton

D.

Volt
Correct Answer: B

Solution:

The unit of electric charge in the SI system is the Coulomb, which is defined as the amount of charge transferred by a current of one ampere in one second.

A.

The force is halved.

B.

The force remains the same.

C.

The force is doubled.

D.

The force is quartered.
Correct Answer: D

Solution:

According to Coulomb's law, the force is inversely proportional to the square of the distance. Doubling the distance reduces the force to one-fourth.

A.

0 N/C

B.

1.2 x 10^5 N/C

C.

2.4 x 10^5 N/C

D.

4.8 x 10^5 N/C
Correct Answer: B

Solution:

For a uniformly charged rod, the electric field at a point along its perpendicular bisector is given by E=kλLrL2+4r2E = \frac{k \lambda L}{r \sqrt{L^2 + 4r^2}}, where λ=QL\lambda = \frac{Q}{L} is the linear charge density. Substituting the given values, E=9×109Nm2/C2×20×106C/m×0.5m0.3m0.52+4×0.32=1.2×105N/CE = \frac{9 \times 10^9 N \cdot m^2/C^2 \times 20 \times 10^{-6} C/m \times 0.5 m}{0.3 m \sqrt{0.5^2 + 4 \times 0.3^2}} = 1.2 \times 10^5 N/C.

A.

1.125 N

B.

2.25 N

C.

4.5 N

D.

9.0 N
Correct Answer: A

Solution:

The electrostatic force between two point charges is given by Coulomb's law: F=kq1q2r2F = \frac{k |q_1 q_2|}{r^2} where k=9×109 N m2 C2k = 9 \times 10^9 \text{ N m}^2 \text{ C}^{-2}, q1=5×106q_1 = 5 \times 10^{-6} C, q2=5×106q_2 = -5 \times 10^{-6} C, and r=0.4r = 0.4 m. Substituting these values, F=9×109×5×106×5×106(0.4)2=1.125 N.F = \frac{9 \times 10^9 \times 5 \times 10^{-6} \times 5 \times 10^{-6}}{(0.4)^2} = 1.125 \text{ N}.

A.

0.06 N

B.

0.18 N

C.

0.36 N

D.

0.72 N
Correct Answer: A

Solution:

The force between two point charges is given by Coulomb's law: F=kq1q2r2F = \frac{k q_1 q_2}{r^2}, where k=9×109 N m2/C2k = 9 \times 10^9 \text{ N m}^2/\text{C}^2 and r=0.3 mr = 0.3 \text{ m}. Substituting the given values, F=9×109×2×107×3×107(0.3)2=0.06 NF = \frac{9 \times 10^9 \times 2 \times 10^{-7} \times 3 \times 10^{-7}}{(0.3)^2} = 0.06 \text{ N}.

A.

The total charge of an isolated system remains unchanged over time.

B.

Electric charge can be created or destroyed in an isolated system.

C.

The total charge of a system can change if it is isolated.

D.

Electric charge is not conserved in any system.
Correct Answer: A

Solution:

Conservation of electric charge means that the total charge of an isolated system remains unchanged with time.

A.

It defines the unit of charge.

B.

It is the gravitational constant.

C.

It is a proportionality constant related to electric force.

D.

It is used to measure magnetic fields.
Correct Answer: C

Solution:

In Coulomb's law, kk is a proportionality constant that relates to the electric force between two charges.

A.

C/m

B.

C/m²

C.

C/m³

D.

C
Correct Answer: B

Solution:

The unit of surface charge density is C/m², as it is defined as charge per unit area.

A.

0 N/C

B.

1.92 x 10⁻¹⁰ N/C

C.

3.84 x 10⁻¹⁰ N/C

D.

4.80 x 10⁻¹⁰ N/C
Correct Answer: B

Solution:

The electric field between two parallel plates with surface charge densities σ\sigma is given by E=σε0E = \frac{\sigma}{\varepsilon_0}. Here, σ=17.0×1022\sigma = 17.0 \times 10^{-22} C/m² and ε0=8.854×1012\varepsilon_0 = 8.854 \times 10^{-12} C²/Nm². Thus, E=17.0×10228.854×1012=1.92×1010E = \frac{17.0 \times 10^{-22}}{8.854 \times 10^{-12}} = 1.92 \times 10^{-10} N/C.

A.

Zero everywhere inside the sphere

B.

Uniform and non-zero inside the sphere

C.

Varies linearly with distance from the center

D.

Depends on the charge of the sphere
Correct Answer: A

Solution:

According to Gauss's law, the electric field inside a conductor in electrostatic equilibrium is zero. Since the sphere is metallic and hollow, the electric field inside it remains zero irrespective of the charge placed at the center.

A.

8.99 N, attractive

B.

8.99 N, repulsive

C.

0 N

D.

4.5 N, attractive
Correct Answer: A

Solution:

Using Coulomb's law, F=kq1q2r2F = \frac{k \cdot |q_1 \cdot q_2|}{r^2}, where k=9×109 N m2/C2k = 9 \times 10^9 \text{ N m}^2/\text{C}^2, q1=5×106 Cq_1 = 5 \times 10^{-6} \text{ C}, q2=5×106 Cq_2 = -5 \times 10^{-6} \text{ C}, and r=0.1 mr = 0.1 \text{ m}. The force is attractive due to opposite charges.

A.

Electric charge is a vector quantity.

B.

Electric charge is quantised.

C.

Electric charge can be fractional.

D.

Electric charge is not conserved.
Correct Answer: B

Solution:

Electric charge is quantised, meaning it exists in discrete amounts as integer multiples of the elementary charge.

A.

1.92 x 10⁶ Nm²/C

B.

2.88 x 10⁶ Nm²/C

C.

3.84 x 10⁶ Nm²/C

D.

4.80 x 10⁶ Nm²/C
Correct Answer: A

Solution:

The total charge on the sphere is given by Q=σ4πr2Q = \sigma \cdot 4 \pi r^2, where σ=80.0×106\sigma = 80.0 \times 10^{-6} C/m² and r=1.2r = 1.2 m. Thus, Q=80.0×106×4π(1.2)2=1.92×104Q = 80.0 \times 10^{-6} \times 4 \pi (1.2)^2 = 1.92 \times 10^{-4} C. The electric flux is Φ=Qε0\Phi = \frac{Q}{\varepsilon_0}, where ε0=8.854×1012\varepsilon_0 = 8.854 \times 10^{-12} C²/Nm². Therefore, Φ=1.92×1048.854×1012=1.92×106\Phi = \frac{1.92 \times 10^{-4}}{8.854 \times 10^{-12}} = 1.92 \times 10^6 Nm²/C.

A.

1.27×105 C/m21.27 \times 10^{-5} \text{ C/m}^2

B.

3.18×105 C/m23.18 \times 10^{-5} \text{ C/m}^2

C.

6.37×105 C/m26.37 \times 10^{-5} \text{ C/m}^2

D.

1.59×105 C/m21.59 \times 10^{-5} \text{ C/m}^2
Correct Answer: A

Solution:

Surface charge density σ\sigma is given by σ=Q4πr2\sigma = \frac{Q}{4\pi r^2}, where QQ is the total charge and rr is the radius. Thus, σ=1054π(0.5)2=1.27×105 C/m2\sigma = \frac{10^{-5}}{4\pi (0.5)^2} = 1.27 \times 10^{-5} \text{ C/m}^2.

A.

The flux remains unchanged.

B.

The flux doubles.

C.

The flux halves.

D.

The flux quadruples.
Correct Answer: A

Solution:

According to Gauss's law, the electric flux through a closed surface is given by the charge enclosed divided by the permittivity of free space, i.e., Φ=Qε0\Phi = \frac{Q}{\varepsilon_0}. Since the charge is doubled and the radius of the sphere does not affect the flux, the flux remains unchanged.

A.

5.76 N

B.

2.88 N

C.

7.2 N

D.

3.6 N
Correct Answer: A

Solution:

Using Coulomb's law, the force FF is given by: F=kq1q2r2F = k \frac{|q_1 q_2|}{r^2} where k=9×109 N m2/C2k = 9 \times 10^9 \text{ N m}^2/\text{C}^2, q1=4×107 Cq_1 = 4 \times 10^{-7} \text{ C}, q2=4×107 Cq_2 = -4 \times 10^{-7} \text{ C}, and r=0.5 mr = 0.5 \text{ m}. F=9×109×(4×107)(4×107)(0.5)2=5.76 NF = 9 \times 10^9 \times \frac{(4 \times 10^{-7})(4 \times 10^{-7})}{(0.5)^2} = 5.76 \text{ N}

A.

They can form closed loops.

B.

They start at negative charges and end at positive charges.

C.

They never cross each other.

D.

They are discontinuous curves.
Correct Answer: C

Solution:

Electric field lines never cross each other. They start at positive charges and end at negative charges, and they are continuous curves.

A.

σ=QV\sigma = \frac{Q}{V}

B.

σ=QS\sigma = \frac{Q}{S}

C.

σ=Ql\sigma = \frac{Q}{l}

D.

σ=Qm\sigma = \frac{Q}{m}
Correct Answer: B

Solution:

Surface charge density (σ\sigma) is defined as the charge (QQ) per unit area (SS) on the surface of a conductor.

A.

1.45 µC

B.

1.81 µC

C.

2.30 µC

D.

3.62 µC
Correct Answer: B

Solution:

The surface area of a sphere is given by A=4πr2A = 4\pi r^2. The radius rr is half of the diameter, so r=1.2r = 1.2 m. Thus, A=4π(1.2)2=18.1 m2A = 4\pi (1.2)^2 = 18.1 \text{ m}^2. The total charge QQ is the product of the surface charge density σ\sigma and the surface area AA: Q=σA=80.0×106×18.1=1.448 µCQ = \sigma A = 80.0 \times 10^{-6} \times 18.1 = 1.448 \text{ µC}. Rounding to two decimal places, Q=1.45 µCQ = 1.45 \text{ µC}.

A.

Conservation of charge

B.

Quantisation of charge

C.

Superposition principle

D.

Additivity of charges
Correct Answer: A

Solution:

A gold-leaf electroscope operates on the principle of conservation of charge. When a charged object touches the metal knob, the charge is transferred to the leaves, causing them to diverge.

A.

Zero

B.

Non-zero and directed towards qAq_A

C.

Non-zero and directed towards qBq_B

D.

Non-zero and directed perpendicular to the line joining qAq_A and qBq_B
Correct Answer: A

Solution:

At the midpoint, the electric fields due to qAq_A and qBq_B are equal in magnitude but opposite in direction, thus cancelling each other out, resulting in a net electric field of zero.

A.

Zero

B.

80.0 µC/m²

C.

9 x 10⁴ N/C

D.

Depends on the charge of the particle
Correct Answer: A

Solution:

According to Gauss's Law, the electric field inside a uniformly charged spherical shell is zero, regardless of the charge at the center.

A.

They can cross each other.

B.

They form closed loops.

C.

They start at positive charges and end at negative charges.

D.

They are discontinuous curves.
Correct Answer: C

Solution:

Electric field lines start at positive charges and end at negative charges. They cannot cross each other and are continuous curves.

A.

7.2 x 10^4 N/C

B.

3.6 x 10^4 N/C

C.

1.8 x 10^4 N/C

D.

9.0 x 10^4 N/C
Correct Answer: A

Solution:

The electric field due to an infinite line charge is E = (2kλ)/r, where r is the perpendicular distance. Substituting values, E = (2 * 9 x 10^9 * 2 x 10^-6) / 0.5 = 7.2 x 10^4 N/C.

A.

1.87 x 10¹²

B.

2.08 x 10¹²

C.

3.75 x 10¹²

D.

4.80 x 10¹²
Correct Answer: A

Solution:

The charge of one electron is approximately 1.6×10191.6 \times 10^{-19} C. The number of electrons transferred is n=Qe=3×1071.6×1019=1.87×1012n = \frac{Q}{e} = \frac{3 \times 10^{-7}}{1.6 \times 10^{-19}} = 1.87 \times 10^{12} electrons.

A.

5 x 10^-6 N

B.

8 x 10^-6 N

C.

2 x 10^-6 N

D.

10 x 10^-6 N
Correct Answer: D

Solution:

The force on a charge in an electric field is given by F=qE\mathbf{F} = q \mathbf{E}. Substituting the given values, F=1×106C×(5×12i^+3×1j^)N/C=(5i^+3j^)×106N\mathbf{F} = 1 \times 10^{-6} C \times (5 \times 1^2 \hat{i} + 3 \times 1 \hat{j}) N/C = (5 \hat{i} + 3 \hat{j}) \times 10^{-6} N. The magnitude of the force is (5×106)2+(3×106)2=10×106N\sqrt{(5 \times 10^{-6})^2 + (3 \times 10^{-6})^2} = 10 \times 10^{-6} N.

A.

Zero

B.

Non-zero, directed towards the positive charge

C.

Non-zero, directed towards the negative charge

D.

Non-zero, perpendicular to the line joining the charges
Correct Answer: C

Solution:

The electric field due to a positive charge is directed away from the charge, while for a negative charge, it is directed towards the charge. At the midpoint, the fields due to both charges add up in the direction towards the negative charge, resulting in a non-zero field directed towards the negative charge.

A.

0.216 N, attractive

B.

0.216 N, repulsive

C.

0.108 N, attractive

D.

0.108 N, repulsive
Correct Answer: A

Solution:

Using Coulomb's law: F=kq1q2r2=9×109×2×106×3×1060.52=0.216F = \frac{k \cdot |q_1 \cdot q_2|}{r^2} = \frac{9 \times 10^9 \times 2 \times 10^{-6} \times 3 \times 10^{-6}}{0.5^2} = 0.216 N. The force is attractive because the charges are opposite.

A.

They do not allow electric charge to move through them.

B.

They have electric charges that are free to move inside the material.

C.

They are always negatively charged.

D.

They can only be charged by induction.
Correct Answer: B

Solution:

Conductors have electric charges (electrons) that are comparatively free to move inside the material, allowing electricity to pass through them easily.

A.

0 N

B.

0.9 N

C.

1.8 N

D.

3.6 N
Correct Answer: A

Solution:

The forces due to charges at opposite corners of the square cancel each other out because they are equal in magnitude and opposite in direction. Thus, the net force on the charge at the center is 0 N.

A.

7.5 x 10⁻⁸ C m

B.

1.25 x 10⁻⁸ C m

C.

2.5 x 10⁻⁸ C m

D.

5.0 x 10⁻⁸ C m
Correct Answer: D

Solution:

The dipole moment pp is given by p=qdp = q \cdot d, where q=2.5×107q = 2.5 \times 10^{-7} C and d=0.3d = 0.3 m (the distance between the charges). Thus, p=2.5×107×0.3=7.5×108p = 2.5 \times 10^{-7} \times 0.3 = 7.5 \times 10^{-8} C m.

A.

0.06 N

B.

0.18 N

C.

0.09 N

D.

0.12 N
Correct Answer: C

Solution:

Using Coulomb's law, the force is calculated as F=kq1q2r2F = \frac{k \cdot q_1 \cdot q_2}{r^2} where k=9×109N m2C2k = 9 \times 10^9 \text{N m}^2 \text{C}^{-2}, q1=2×107Cq_1 = 2 \times 10^{-7} \text{C}, q2=3×107Cq_2 = 3 \times 10^{-7} \text{C}, and r=0.3mr = 0.3 \text{m}. Substituting these values gives F=0.09NF = 0.09 \text{N}.

A.

0 N/C

B.

9 x 10^5 N/C towards the negative charge

C.

9 x 10^5 N/C away from the negative charge

D.

4.5 x 10^5 N/C towards the negative charge
Correct Answer: B

Solution:

The electric field due to a point charge is given by E=kqr2E = \frac{kq}{r^2}. At the midpoint, the fields due to the two charges add up. The field due to the positive charge is 9x105N/C9 x 10^5 N/C towards the negative charge, and the field due to the negative charge is also 9x105N/C9 x 10^5 N/C towards the negative charge. Thus, the total field is 9x105N/C9 x 10^5 N/C towards the negative charge.

A.

Electric charge can be created but not destroyed.

B.

Electric charge can be destroyed but not created.

C.

Electric charge can neither be created nor destroyed.

D.

Electric charge is always conserved only in closed systems.
Correct Answer: C

Solution:

The conservation of electric charge states that the total charge of an isolated system remains constant over time, meaning charge can neither be created nor destroyed.

A.

5 \times 10^{-6} C

B.

5 \times 10^{-5} C

C.

5 \times 10^{-4} C

D.

5 \times 10^{-3} C
Correct Answer: B

Solution:

The total charge QQ on the rod is given by Q=λLQ = \lambda \cdot L, where LL is the length of the rod. Thus, Q=5×106 C/m×1 m=5×105 CQ = 5 \times 10^{-6} \text{ C/m} \times 1 \text{ m} = 5 \times 10^{-5} \text{ C}.

A.

3.6 x 10^6 N/C

B.

1.8 x 10^6 N/C

C.

Zero

D.

9 x 10^5 N/C
Correct Answer: A

Solution:

The electric field due to an infinite line charge is given by E=λ2πε0rE = \frac{\lambda}{2\pi\varepsilon_0 r}, where λ=2×106 C/m\lambda = 2 \times 10^{-6} \text{ C/m}, r=0.01 mr = 0.01 \text{ m}, and ε0=8.854×1012 C2/N m2\varepsilon_0 = 8.854 \times 10^{-12} \text{ C}^2/\text{N m}^2. Substituting these values gives E=3.6×106 N/CE = 3.6 \times 10^6 \text{ N/C}.

A.

1 x 10⁻⁴ Nm

B.

2 x 10⁻⁴ Nm

C.

3 x 10⁻⁴ Nm

D.

4 x 10⁻⁴ Nm
Correct Answer: A

Solution:

The torque τ\tau on a dipole in an electric field is given by τ=pEsinθ\tau = pE \sin \theta. Here, p=4×109p = 4 \times 10^{-9} C m, E=5×104E = 5 \times 10^4 N/C, and θ=30\theta = 30^\circ. Thus, τ=4×109×5×104×sin30=1×104\tau = 4 \times 10^{-9} \times 5 \times 10^4 \times \sin 30^\circ = 1 \times 10^{-4} Nm.

A.

1.00 µC/m

B.

0.50 µC/m

C.

0.10 µC/m

D.

0.05 µC/m
Correct Answer: A

Solution:

The electric field EE due to an infinite line charge with linear charge density λ\lambda is given by E=λ2πε0rE = \frac{\lambda}{2\pi\varepsilon_0 r}. Solving for λ\lambda, we have λ=2πε0rE\lambda = 2\pi\varepsilon_0 r E. Substituting ε0=8.854×1012 C2/N m2\varepsilon_0 = 8.854 \times 10^{-12} \text{ C}^2/\text{N m}^2, r=0.02 mr = 0.02 \text{ m}, and E=9×104 N/CE = 9 \times 10^4 \text{ N/C}, we get λ=2π×8.854×1012×0.02×9×104=1.00 µC/m\lambda = 2\pi \times 8.854 \times 10^{-12} \times 0.02 \times 9 \times 10^4 = 1.00 \text{ µC/m}.

A.

0.06 N

B.

0.12 N

C.

0.18 N

D.

0.24 N
Correct Answer: A

Solution:

Using Coulomb's law, F=kq1q2r2F = \frac{k \cdot q_1 \cdot q_2}{r^2}, where k=9×109k = 9 \times 10^9 N m² C⁻², q1=2×107q_1 = 2 \times 10^{-7} C, q2=3×107q_2 = 3 \times 10^{-7} C, and r=0.3r = 0.3 m. Substituting these values, F=9×109×2×107×3×1070.32=0.06F = \frac{9 \times 10^9 \times 2 \times 10^{-7} \times 3 \times 10^{-7}}{0.3^2} = 0.06 N.

A.

It is zero.

B.

It is constant.

C.

It is equal to the charge density.

D.

It varies with distance.
Correct Answer: A

Solution:

For a neutral atom, the total charge enclosed by the Gaussian surface is zero, hence the electric field is zero.

A.

0.4 x 10^-4 N m

B.

0.8 x 10^-4 N m

C.

1.6 x 10^-4 N m

D.

3.2 x 10^-4 N m
Correct Answer: B

Solution:

The torque on a dipole in a uniform electric field is given by τ=pEsinθ\tau = pE \sin \theta. Substituting the given values, τ=4×109Cm×2×104N/C×sin60°=0.8×104Nm\tau = 4 \times 10^{-9} C \cdot m \times 2 \times 10^4 N/C \times \sin 60° = 0.8 \times 10^{-4} N \cdot m.

A.

Electric charge is a vector quantity.

B.

Electric charge is quantised.

C.

Electric charge can be created or destroyed.

D.

Electric charge is always negative.
Correct Answer: B

Solution:

Electric charge is quantised, meaning it is always an integral multiple of a basic quantum of charge.

A.

Electrostatic induction

B.

Magnetic attraction

C.

Gravitational force

D.

Nuclear force
Correct Answer: A

Solution:

The charged comb polarizes the pieces of paper, inducing a net dipole moment in the direction of the electric field. This results in an attractive force between the comb and the paper.

A.

0.06 N

B.

0.18 N

C.

0.36 N

D.

0.72 N
Correct Answer: A

Solution:

Using Coulomb's law, F=kq1q2r2F = \frac{k \cdot q_1 \cdot q_2}{r^2}, where k=9×109Nm2C2k = 9 \times 10^9 N m^2 C^{-2} and r=0.3r = 0.3 m. Substituting the values, F=9×109×2×107×3×107(0.3)2=0.06F = \frac{9 \times 10^9 \times 2 \times 10^{-7} \times 3 \times 10^{-7}}{(0.3)^2} = 0.06 N.

True or False

Correct Answer: False

Solution:

Quantisation of electric charge is a basic law of nature, but there is no analogous law for the quantisation of mass.

Correct Answer: True

Solution:

For discrete charge configurations, the electric field is undefined at the exact location of the charges because the field would theoretically be infinite.

Correct Answer: True

Solution:

The surface charge density σ\sigma is defined as the charge QQ on an area element SS, i.e., σ=Q/S\sigma = Q/S.

Correct Answer: True

Solution:

For macroscopic charges, the number of elementary charges is so large that the quantisation of charge can be ignored, and charge is treated as continuous.

Correct Answer: True

Solution:

An electric dipole is defined as a pair of equal and opposite charges separated by a distance.

Correct Answer: True

Solution:

An electric field line is indeed a curve where the tangent at any point represents the direction of the electric field at that point.

Correct Answer: True

Solution:

The superposition principle states that the force on one charge due to another charge is unaffected by the presence of other charges, and there are no additional three-body, four-body, etc., forces.

Correct Answer: False

Solution:

When a glass rod is rubbed with silk, electrons are transferred from the glass to the silk, making the glass rod positively charged.

Correct Answer: False

Solution:

The force between two point charges depends on the medium between them, as the constant of proportionality kk in Coulomb's law is affected by the permittivity of the medium.

Correct Answer: True

Solution:

The surface charge density, denoted by σ\sigma, is defined as the charge QQ on an area element SS, i.e., σ=QS\sigma = \frac{Q}{S}. This definition is used for continuous charge distributions.

Correct Answer: True

Solution:

In SI units, the unit of charge (coulomb) is defined by the unit of current (ampere) via its magnetic effect, not directly by electric forces.

Correct Answer: False

Solution:

Quantisation of electric charge means that the total charge of a body is always an integral multiple of a basic quantum of charge.

Correct Answer: False

Solution:

The electric field due to a discrete charge configuration is not defined at the locations of the discrete charges.

Correct Answer: True

Solution:

Quantisation of electric charge is a basic law of nature, and there is no analogous law for the quantisation of mass.

Correct Answer: False

Solution:

The electric field due to a charge configuration with total charge zero is not zero; for distances large compared to the size of the configuration, its field falls off faster than 1/r², typical of field due to a single charge.

Correct Answer: False

Solution:

According to the superposition principle, the force between two charges is not affected by the presence of other charges.

Correct Answer: True

Solution:

Quantisation of electric charge is a basic (unexplained) law of nature; interestingly, there is no analogous law on quantisation of mass.

Correct Answer: False

Solution:

In an electric dipole, the dipole moment vector is directed from the negative charge to the positive charge.

Correct Answer: True

Solution:

For continuous volume charge distributions, the electric field is defined at every point within the distribution.

Correct Answer: False

Solution:

The conservation of charge principle states that in an isolated system, the total electric charge remains constant over time.

Correct Answer: True

Solution:

The dipole moment vector of an electric dipole is directed from the negative charge to the positive charge.

Correct Answer: False

Solution:

Conservation of electric charge means that the total charge of an isolated system remains unchanged with time.

Correct Answer: False

Solution:

The electric field due to a discrete charge configuration is not defined at the locations of the discrete charges.

Correct Answer: False

Solution:

Static electricity refers to charges that do not move or change with time. It is the accumulation of electric charges on the surface of a material.

Correct Answer: True

Solution:

Electric field lines are continuous and do not intersect because at any point in space, the electric field has a unique direction.

Correct Answer: False

Solution:

Electric field lines cannot form closed loops. They start at positive charges and end at negative charges.

Correct Answer: True

Solution:

Conservation of charge means that the total charge in an isolated system does not change, even though charges within the system may move or redistribute.

Correct Answer: False

Solution:

The superposition principle states that the force on one charge due to another charge is unaffected by the presence of other charges.

Correct Answer: True

Solution:

Inside a neutral atom, the total charge enclosed by a Gaussian surface is zero, leading to an electric field of zero according to Gauss's law.

Correct Answer: False

Solution:

The additive property of charge is not an 'obvious' property. It is related to the fact that electric charge has no direction associated with it; charge is a scalar.

Correct Answer: True

Solution:

In a continuous charge distribution, the charge density is defined as a macroscopic average, ignoring the microscopic discontinuities of discrete charges.

Correct Answer: False

Solution:

Coulomb's law states that the electrostatic force between two point charges is inversely proportional to the square of the distance between them, not directly proportional.

Correct Answer: True

Solution:

Inside a uniformly charged conducting sphere, the electric field is zero due to the symmetric distribution of charge.

Correct Answer: True

Solution:

According to Gauss's law, the electric field inside a uniformly charged conducting sphere is zero because the net charge enclosed by a Gaussian surface inside the conductor is zero.

Correct Answer: True

Solution:

The electric field lines for a positive point charge radiate outward, indicating the direction of the force on a positive test charge.

Correct Answer: True

Solution:

In a continuous charge distribution, the charge is considered to be distributed smoothly over a region, ignoring the quantisation of charge at the microscopic level.

Correct Answer: True

Solution:

The electric field is not defined at the locations of discrete charges because the field would be infinite at those points.

Correct Answer: True

Solution:

Quantisation of electric charge is indeed a basic unexplained law of nature; there is no analogous law for the quantisation of mass.

Correct Answer: False

Solution:

Electric field lines cannot cross each other because at any point in space, the electric field has a unique direction.

Correct Answer: False

Solution:

Electric field lines start at positive charges and end at negative charges; they cannot form closed loops.

Correct Answer: True

Solution:

Electric charge is a scalar quantity, meaning it has no direction. It remains invariant under rotations and for frames of reference in relative motion, unlike some other scalar quantities like kinetic energy.

Correct Answer: True

Solution:

Quantisation of electric charge is a fundamental principle, meaning that charge comes in discrete amounts.

Correct Answer: False

Solution:

The electric field due to a charge configuration with total charge zero is not zero; for distances large compared to the size of the configuration, its field falls off faster than 1/r21/r^2, typical of field due to a single charge.

Correct Answer: True

Solution:

Electric charge is a scalar quantity as it has magnitude but no direction.

Correct Answer: False

Solution:

Electric charge is a scalar quantity, meaning it has magnitude but no direction.

Correct Answer: True

Solution:

The superposition principle asserts that the force exerted on a charge by another charge is independent of the presence of additional charges, allowing the forces to be added vectorially.

Correct Answer: True

Solution:

Electric charge is a scalar quantity, meaning it has no direction, and it is invariant under rotation and for frames of reference in relative motion.

Correct Answer: True

Solution:

Conservation of total charge of an isolated system is a property independent of the scalar nature of charge. Conservation refers to invariance in time in a given frame of reference.

Correct Answer: False

Solution:

Electrostatic field lines start at positive charges and end at negative charges; they cannot form closed loops.

Correct Answer: True

Solution:

Coulomb force can be of both signs, allowing for both attraction and repulsion between charges.

Correct Answer: True

Solution:

Quantisation of electric charge means that the total charge (q) of a body is always an integral multiple of a basic quantum of charge (e), i.e., q = ne, where n is an integer.

Correct Answer: True

Solution:

The superposition principle states that the net force on a charge is the vector sum of the forces exerted by each of the other charges independently, unaffected by the presence of other charges.

Correct Answer: True

Solution:

For macroscopic charges, the number of elementary charges is so large that the quantisation of charge can be ignored.

Correct Answer: False

Solution:

Quantisation of electric charge means that the total charge of a body is always an integral multiple of a basic quantum of charge (e).

Correct Answer: False

Solution:

The principle of superposition states that the forces between two charges are not affected by the presence of other charges.

Correct Answer: True

Solution:

Electric charge is a scalar quantity because it has magnitude but no direction, similar to mass.

Correct Answer: True

Solution:

Quantisation of electric charge means that the total charge (q) of a body is always an integral multiple of a basic quantum of charge (e), i.e., q=neq = ne, where nn is an integer.

Correct Answer: True

Solution:

In SI units, the unit of charge (coulomb) is defined by 1C=1As1 \, C = 1 \, A \, s, which is based on its magnetic effect (Ampere's law). This makes the value of the constant kk in Coulomb's law approximately 9×109Nm2C29 \times 10^9 \, N \, m^2 \, C^{-2}.

Correct Answer: True

Solution:

For a continuous charge distribution, the electric field is defined at any point in the distribution.