Chapter 8: Magnetism, EMI, Maxwell’s Equations & EM Waves (Set-3)

The force between two parallel currents is

A Always repulsive
B Always attractive
C Attractive if currents are in same direction
D Attractive only if currents differ

Magnetic field intensity inside a long solenoid is independent of

A Number of turns
B Current
C Length
D Radius

A current loop behaves like

A An electric dipole
B A magnetic dipole
C A capacitor
D A dielectric

Magnetic field inside a toroid is

A Zero at center
B Maximum outside
C Contained within the core
D Uniform everywhere

Gauss’s law for magnetism is written as

A ∇⋅B = ρ
B ∇⋅B = 0
C ∇×B = 0
D ∇⋅E = 0

Magnetic flux through a surface is

A Scalar
B Vector
C Always zero
D Tensor

The Hall field is produced due to

A Electric field only
B Magnetic field only
C Lorentz force on moving charges
D Thermal motion

Hall coefficient of a semiconductor can be

A Only positive
B Only negative
C Positive or negative
D Only zero

Carrier mobility can be calculated using

A RH = nq
B μ = σRH
C μ = IR
D μ = 1/σ

Diamagnetism exists due to

A Spin alignment
B Orbital motion of electrons
C Domain formation
D Magnetic dipoles

Curie’s law relates

A χ ∝ T
B χ ∝ 1/T
C χ ∝ T²
D χ independent of T

Ferromagnetic domains disappear at

A Debye temperature
B Curie temperature
C Melting temperature
D Superconducting temperature

A soft magnetic material has

A High coercivity
B Low coercivity
C Large hysteresis loop
D Very high remanence

Faraday’s law can be expressed using which Maxwell equation?

A ∇×E = −∂B/∂t
B ∇⋅E = 0
C ∇⋅B = 0
D ∇×B = μ0J

Induced EMF in a coil depends on

A Rate of change of flux
B Flux only
C Coil material
D Resistance only

Increasing the number of turns in a coil will

A Decrease EMF
B Increase EMF
C Make EMF zero
D Not affect EMF

Self-inductance of a coil is proportional to

A N
B
C 1/N
D √N

A conductor moving parallel to magnetic field lines experiences

A Maximum EMF
B Zero EMF
C Minimum EMF
D Increasing EMF

Lenz’s law is a consequence of

A Coulomb’s law
B Newton’s third law
C Conservation of energy
D Conservation of charge

The induced electric field due to changing magnetic flux is

A Conservative
B Non-conservative
C Always zero
D Infinite

In a transformer, eddy current losses are reduced by

A Thick plates
B Laminated core
C Decreasing frequency
D Increasing flux

AC current in a capacitor leads voltage by

A 90°
B 45°
C
D 180°

In a series LCR circuit at resonance

A Current is minimum
B Voltage is maximum
C Impedance is purely resistive
D Reactance is maximum

Quality factor Q is

A ω0L/R
B R/ω0L
C RC
D None

Skin effect is prominent at

A Low frequencies
B High frequencies
C DC only
D Zero frequency

Skin depth is inversely proportional to

A √frequency
B frequency
C conductivity
D both √frequency and √conductivity

Displacement current exists

A Only in dielectrics
B Only in conductors
C In vacuum or any region with changing electric field
D Only in metals

Maxwell’s equations are

A Two equations
B Three equations
C Four equations
D Five equations

Light is

A A longitudinal wave
B A transverse EM wave
C A mechanical wave
D A scalar wave

EM waves travel fastest in

A Water
B Glass
C Air
D Vacuum

In EM waves, E and B are always

A Parallel
B Perpendicular to each other
C Opposite
D Random

Energy in EM waves is carried by

A Electric field only
B Magnetic field only
C Both E and B
D Neither

Poynting vector direction indicates

A Electric flux
B Magnetic flux
C Energy flow
D Charge density

Poynting vector is given by

A E + B
B E × B / μ
C E × H
D EB

Wave impedance in free space is approximately

A 50 Ω
B 75 Ω
C 200 Ω
D 377 Ω

Attenuation of EM waves in conductors is due to

A Dielectric loss
B Electron inertia
C Ohmic loss
D None

In good conductors, phase difference between fields is

A
B 45°
C 90°
D 180°

Anomalous dispersion occurs when

A n increases with frequency
B n decreases with frequency
C n constant
D Frequency is zero

Wave equation for magnetic field is

A ∇²B = μϵ ∂²B/∂t²
B ∇⋅B = 0
C ∇×B = 0
D None

The velocity of EM waves in a medium is

A 1/μϵ
B 1/√(μϵ)
C √(μϵ)
D Infinite

The refractive index of a medium for EM waves is

A √(μϵ)
B ϵ/μ
C √(ϵr μr)
D ϵ0/μ0

A perfect conductor reflects

A All EM waves
B No EM waves
C Only low-frequency waves
D Only high-frequency waves

EM waves carry

A Momentum
B Mass
C Charge
D Spin only

A photon’s momentum is

A mc
B 0
C
D h/λ

Conductivity affects

A Attenuation
B Skin depth
C Wave propagation
D All of these

An EM wave is attenuated in conductors because

A B decreases
B E decreases
C Both decay exponentially
D None

In dispersive media

A All frequencies travel at same speed
B Group velocity ≠ phase velocity
C No dependence on ω
D EM waves vanish

For low-loss dielectrics, wave propagation is

A Strongly attenuated
B Nearly unaffected
C Increasing in amplitude
D Impossible

In a capacitor, displacement current flows due to

A Charges moving across plates
B Changing electric field between plates
C Free electrons flowing
D Zero potential

Maxwell predicted EM waves travel at

A 1/√(μ0ϵ0)
B μ0ϵ0
C c/2
D √(μ0/ε0)