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WorksheetsElectromagnetism and Materials MCQs
Total questions: 91
Worksheet time: 46mins
The interaction energy between two distant electric dipoles r goes like
r−1
r−2
r2
r−3
If the magnetization vector M in a material is equal to M(x,y,z) = axi + byj + czk, where a, b and c are constants of suitable size, the amperian currents inside the material
depend from the values of a, b and c
The question is wrong: the amperian currents don't depend on M
are zero
are different from zero
In an anisotropic dielectric material
the polarization P is parallel to the electric field E but not to the dielectric induction vector D
the polarization P is not parallel neither to the electric field E nor to the dielectric induction vector D
the polarization P is always parallel to both the electric field E and to the dielectric induction vector D
the polarization P is parallel to the dielectric induction vector D but not to the electric field E
Under what conditions is the vector magnetic solenoidal and conservative?
Only in steady state.
When rot B = 0
When there are no charges.
Always.
An electromagnetic wave having a frequency of 1.8×1012Hz propagates at the speed v=2.7×108m/s . Determine the value of the wavelength λ and of the period T .
λ = λ = 1.5 × 10^{-3} m, T = T = 5.55 × 10^{-13} s
λ = λ = 1.5 × 10^{-4} m, T = T = 5.55 × 10^{-12} s
λ = λ = 1.5 × 10^{-4} m, T = T = 5.55 × 10^{-13} s
λ = λ = 1.5 × 10^-4 m, T = T = 5.55 × 10^-35 s
The magnetic field generated at a point P by a moving (non-relativistic) charge
is inversely proportional to the distance between the charge and the point P
does not depend on the direction of motion of the charge
is inversely proportional to the square of the distance between the charge and the point P
does not depend on the distance between the charge and the point P
If the intensity of a plane electromagnetic wave is i1 at the point x1 along the direction of propagation, at the point x2 = 2x1 the intensity i2 will be
i2 = i1/2
i2 = 2i1
i2 = i1/4
i2 = i1
The ratio of the tangential components B1t and B2t of the magnetic field B measured at the interface between two materials having χ1m = 0.3 and χ2m = 0.5 respectively, magnetic susceptibility is
B1t/B2t = 0.87
B1t/B2t = 1.67
B1t/B2t = 1.15
B1t/B2t = 0.60
In a region of empty space there exists a vector A(x,y,z) = a x i + b y j + c t k and an electrical potential V(x,y,z) = − d y, (where a, b, c and d are suitably sized constants). What is the electric field E?
E = − (a t + d)i − bj - c k
E = d j − c k
E = − a i + d j
E = (a − d) x i
When an electromagnetic wave passes from one medium to another, what happens to the frequency and V the wavelength λ?
λ changes, V remains the same
λ remains the same, V remains the same
λ remains the same, V changes
λ changes, V changes
To an electric field E = a t k, where a is a constant of suitable size, is associate a displacement density of current js
js = ε0 a k
js = μ0 ε0 a k
js = a k
js = μ0 ε0 ak
If the polarization vector P(x,y,z) = a x i + b y j + 5 c k is present in a dielectric material, where a, b and c are constants of suitable size, when just surface polarization charges are present?
when a = b
when a = − b − 5 c
always
when a = − b
Kirchhoff’s second law is another way of expressing
the energy conservation
the fact that the magnetic field is solenoidal
the conservation of momentum
the conservation of charge
What is the power P dissipated in a superconductor wire crossed by a current I?
P = V
P=R2I2
P=RI2 as in a normal metal
P = 0
In a region of space there is an electric field E(x,y,z,t) = 2 a t i − 4 b y j + 3 b z k, where a and b are constants of suitable size. What is the value of the charge density ρ present in this region of space?
ρ = (2 a t + b) ε0
ρ = b ε0
ρ = 0
ρ = -b ε0
A rectilinear infinite wire, immersed in a material having magnetic permeability km = 1.2, is crossed by a current I = 5 A. Calculate the modulus of the magnetic field B generated by the wire at a distance r = 0.2 m.
B = 6.0×10−6T
B = 12.0×10−6T
B = 2.4×10−7T
B = 2.4×10−4T
In an anisotropic dielectric material the vector is P(x,y,z) = 2 a z i − 3 b y j + c x k, where a, b and c are constants of suitable size. Determine the value of the volume polarization charge density ρρ present in the dielectric material.
ρρ = (2 a − 3 b) ε0
ρρ= − 3 b ε0
ρρ = 3 b
ρρ = 3 b ε0
In an energy part of space there is a uniform electric field E linearly increasing in time. The circuitry of field B along a closed line, contained within this part of space, is
constant
zero
decreasing linearly over time
growing linearly over time
The magnetic susceptibility of a paramagnetic material
has a dependence of the type T−1 on temperature
does not depend on temperature
grows linearly with temperature
decreases linearly with temperature
In an anisotropic material the magnetization vector M is M = a x i + b y j + c z k, where a, b and c are suitably sized constants. Determine the density of magnetization current jm present within the material.
jm = a (y − z) i + b (z − x) j + c (x − y) k
jm = − a i − b j − c k
jm = a i + b j − c k
jm = 0
In an empty part of space there is a uniform electric field EEE increasing over time such as t2t^2t2 . The circuitry of the magnetic field B along a closed line totally contained within this part of space is
constant
increasing linearly over time
decreasing linearly over time
zero
The ratio of the normal electric field components E1n and E2n measured at the interface between two homogeneous and isotropic dielectrics, having electric susceptibility equal to χ1=0.5 and χ2=0.8 respectively, is
E1n/E2n=1.000
E1n/E2n=0.833
E1n/E2n=1.200
E1n/E2n=1.600
The resistivity of a metal at a temperature close to room temperature
is an increasing linear function of temperature
is a linear decreasing function of temperature
depends on the geometric characteristics of the object on which the measurement is made but it doesn’t depend on temperature
is independent of the geometric characteristics of the object on which it is measured
Calculate the drift velocity Vd of the conduction electrons inside a metal wire of cross‑section S = 3 mm2 crossed by a current I = 5 A. Assume that the density of the carriers n is equal to 3×1028m−3 .
Vd = 3.47×10−5m/s
Vd = 1.74×10−3m/s
Vd = 3.47×10−4m/s
Vd = 1.74×10−4m/s
The electrostatic field is conservative
therefore
its circulation along any closed path is zero
it has zero gradient
it has zero divergence
its flow through any closed surface is zero
Iron at temperatures above the critical behaves
in a way that depends on the particular type of magnetic field that has been applied to the material
like a paramagnet
like a diamagnet
like a ferromagnet
Kirchhoff’s first law is another way of expressing
the conservation of charge
the energy conservation
the conservation of momentum
the fact that the magnetic field is solenoidal
The phenomenon diffraction occurs only in the presence of flat electromagnetic waves.
False
True but it occurs if the waves are also harmonic electromagnetic waves
True but it occurs only if the waves are also harmonic electromagnetic waves and not in the vacuum
True
The vector E(x,y,z) = a y i + a x j + b z k, with a and b constants of appropriate size, can represent an electrostatic field?
Yes, but just when a ≠ b
Yes, because div E = 0
Yes, because rot E = 0
Yes, because div E ≠ 0
In an anisotropic dielectric material
the polarization P is parallel to the dielectric induction vector D but not to the electric field E
the polarization P is always parallel to the electric field E and to the dielectric induction vector D
the polarization P is parallel to the electric field E but not to the dielectric induction vector D
the polarization P is not parallel neither to the electric field E nor to the dielectric induction vector D
Gauss' law states that
the flow of total electric field, generated by all the charges through a closed surface, is equal to the algebraic sum of charges contained there divided by the dielectric constant of vacuum
the flow of the electric field through a closed surface is always zero
the flow of the electric field through any surface is equal to the algebraic sum of the charges contained in it divided by the dielectric constant of vacuum
the flow of the electric field through a surface is equal to the sum of the modules of the charges contained in it divided by the dielectric constant of vacuum
A rigid square coil of side a = 20 cm is crossed by a current I = 2 A and is placed in a magnetic field of modulus B = 0.03 T whose direction forms an angle θ = 30° with the normal on the plane on which the coil lies. Determine the modulus of torque M acting on the loop
1.2 × 10-2 Nm
2.4×10−4Nm
1.2 × 10-3 Nm
M = 0 Nm
Solving Maxwell's equations of electromagnetism means
to calculate the charge distributions Q and current distribution i, knowing the fields E and B
to satisfy the continuity equation ∇×j + ∂ρ/∂t = 0
to calculate the distribution of charge densities ρ and current densities j, knowing the fields E and B
to calculate the fields E and B, knowing the distributions ρ of the charge densities, j of the current densities and the boundary conditions
A monochromatic light beam (λ = 644 nm) passes through a rectangular slit a rid forms a figure of diffraction in which the first dark fringe corresponds Θ = 0.125°. What is the width of the slit?
2.95 × 10-4 m
1.66 × 10-4 m
3.8 × 10-4 m
1.25 × 10-4 m
In a dielectric material the sum of the surface polarization charges is zero when
the material is homogeneous
never
the applied electric field has a particular value
always
The bulk density of amperian currents jm, in a material with magnetization vector M, is equal to
jm = div M
jm = rot M
jm = M × n
jm = grad M
Two straight parallel wires of indefinite length, placed in the empty space and distant from each other, are crossed by two concordant currents I1 and I2. Determine the strength B of the magnetic field in the point placed in the middle of the right line joining the two wires
B = μ0 | I1 + I2 | /πd
B = μ0 | I1 + I2 | /2πd
B = μ0 | I1 - I2 | /2πd
B = μ0 | I1 − I2 | /πd
A particle with mass and charge, initially at rest, is immersed in a magnetostatic field B and electrostatic field E, vectorially parallel to each other and uniformly distributed in space. The motion assumed by the charge is
helical
uniform circular
uniformly accelerated straight line
uniform straight line
The energy dissipated by the Joule effect during the exchange of the capacitor in an RC circuit is equivalent to
RC
R/C
by generator to charge the capacitor
the electrostatic energy of the capacitor
The mutual induction coefficient M between two circuits does NOT depend on
the distance between the two circuits
the intensity of current moving in the two circuits
the medium which is interposed between the two circuits
the shape of the two circuits
What is the value of rotor of electrostatic field E(x,y) = yi(x2+y2)−xj(x2+y2) ?
rotE = 0. E is conservative everywhere
rotE ≠ 0. E is non-conservative
rotE = 0. E is conservative in R2 = [0,0]
rotE = 0. E is non-conservative in R₂ = [0,0]
Gauss's law for the magnetic necessarily provides
the flow of B is always zero if there are no currents
the flow of B across a surface is always zero
the flux of B is always zero if the magnetization of the material is negligible
there are no magnetic monopoles
The Hall effect can be used
to measure a magnetic field
to determine the intensity of an electromagnetic wave
to determine the dielectric strength of an insulator
to determine the mobility of the ions in a generic metal
Gauss's law for the electric field E necessarily provides
the charges are point-like
the surface on which to calculate the flow of E is spherical
the surface on which to calculate the flow of E is closed
field E does not depend on time
The electrostatic field is conservative therefore it
its circulation along some closed path is zero
has zero curl
has zero gradient
its flow through any closed surface is zero
Which of the following properties of the induction vector D is correct?
D = E − P
D = εr E for each type of dielectric material
∫ ∫ D ⋅ n dΣ = Q where Q is the free charge inside the unit vector n
∫ ∫ D ⋅ n dΣ = 0 where Σ is a closed surface with normal unit vector n
In a paramagnet magnetic susceptibility
depends on the applied magnetic field
does not vary with temperature
grows with temperature
decreases with temperature
An electron of charge e and velocity of module v completes a semicircle of radius R due to a magnetic field of module B placed perpendicular to v. How much is the work W done by Lorentz force worth?
W = π e v B R J
W = 2 π e v B R J
W = π e v B R / 2 J
W = 0 J
The energy associated in a given volume with the presence of an electric field is larger when
it doesn't depend on what's in the volume
the volume is filled with a dielectric material
the volume is filled with a non-homogeneous dielectric material
the volume is empty
The field B(x,y,z) = a x i + 2 b y j + 4 c z k (where a, b and c are constants of suitable size) exists in nature?
Always
Just when b = 0
Just when a = 0
Just when a = −2 b − 4 c
In an anisotropic material the magnetization vector is M=ayi^+bxj^+czk^ (where a , b , and c are constants of suitable size). When is the density of magnetization current jm present within the material is zero?
a=b
a=b+c
a=−b−c
a=−b
A dielectric material, homogeneous and isotropic, is immersed in a uniform external electrostatic field. The sum of the polarization charges on the surface of this material is
always different from zero
non-zero only if the object has a regular shape
zero only if the object has a regular shape
always zero
The intensity of a cylindrical wave at a distance r from the source
decreases as 1/r
decreases as 1/r2
doesn't change
decreases as 1/r
An electric field generated by a distribution of charges is electrostatic if and only if
the distribution of charges is spherical or point-like
the test charge is at rest
the test charge is in uniform rectilinear motion
the distribution of charges is at rest
Which of the following parameters that characterize a harmonic wave does not change when it passes between two materials with different refractive index?
speed
wavelength
wave number
frequency
At electrostatic equilibrium, the E field near the surface of a charged conductor with a uniform negative surface charge density σ is
uniform, parallel to the surface, of the direction entering the conductor
uniform, perpendicular to the surface, of the direction entering the conductor
uniform, perpendicular to the surface, facing out from the conductor
anywhere null
The charge q on the surface armatures S of an empty plane capacitor varies as a function of time with the law q(t)=at+b (where a and b are constants of suitable size). Calculate the displacement current density Jd that flows across the capacitor.
Jd=S4at3
Jd=Sa
Jd=Sε0a
Jd=Sε0at
If r is the distance from the source, the intensity of a spherical wave
varies as 1/r2
increases proportionally to r
does not depend on r
decreases proportionally to 1/r
The magnetic field B(x,y,z)=axi^−byj^+5cxk^ (where a , b and c are constants of a suitable size) is conservative
just when b=0
just when c=0
just when a=0
always
If M=χm(T)H this material is
diamagnetic and paramagnetic
paramagnetic
ferromagnetic because χm(T) doesn’t depend on H
diamagnetic
At a point of coordinates (x;y;z) in a conducting medium, the current density has the expression j(x,y,z)=3x2yux−3xy2uy+xyuz . What can be said about the charge density ρ at that point?
nothing can be said about ρ
ρ is constant
ρ decreases over time
ρ increases over time
We want to make a circuit RL using an inductance L and two resistors R1 and R2 . The resistors can be connected together in series or in parallel. Which of the following statements is right?
the rapidity of the transients RL does not depend on the connection
the transients of the RL circuit are faster if R2>R1
the transients of the RL circuit are faster if two transistors are connected in parallel
the transients of the RL circuit are faster if two transistors are connected in series
The gap between the plates of a capacitor, initially empty, is completely filled with a dielectric material. With the same charge on the plates
the capacitance decreases, the electrostatic field increases
the capacitance increases, the electrostatic field decreases
the capacitance and the electrostatic field increase
the capacitance and the electrostatic field decrease
Iron at temperatures below the critical temperature behaves
like a ferromagnet
like a paramagnet
in a way that depends on the particular type of magnetic field that has been applied to the material
like a diamagnet
In an isotropic material B=μH . This means that H is always solenoidal.
yes but just in a diamagnetic material
yes
yes but just in the paramagnetic and ferromagnetic materials
no
A parallel plane plate is entirely filled with a homogeneous and isotropic dielectric material with relative dielectric constant κr=3 placed perpendicularly to an external electric field of modulus E0=15 V/m . How much is worth the polarization module P ?
P=2.65×10−10 C/m2
P=8.85×10−11 C/m2
P=8.85×10−12 C/m2
P=3.98×10−9 C/m2
Under what conditions is the vector magnetic field B solenoidal?
in the vacuum
always
when there are no charges
only in steady state
In a region of empty space there exists potential vector A(x,y,z,t)=atxi + byj+czk (where a , b and c are constants of suitable size). How much is the associated magnetic field B ?
B=ci−atj+bk
B=ai+bj+ck
B=ati+bj+ck
B=0
The electrical potential inside a metallic material is
null only if the metallic object has a spherical shape
constant
dependent on the shape of the metallic object
null
A resistance of 8 Ω must be made but only 3 valuable resistors are possessed: R1=5 Ω , R2=4 Ω and R3=12 Ω . How can the necessary resistance be achieved?
by connecting the three resistors in parallel
by connecting the three resistors in series
by connecting R2 and R3 in parallel and R1 in series with the previous parallel
by connecting R1 and R2 in series and R3 in parallel to the series
The polarization vector P generated in an isotropic and homogeneous material with relative dielectric constant εr immersed in an external electrostatic field E0
is equal to ε0(εr−1)E0
is equal to (εr−1)E0
is equal to ε0(εr−1)E0/εr
is equal to (εr−1)E0/εr
Inside a homogeneous dielectric material without free charges
there may be volume polarization charges but only for particular materials
there can be no volume polarization charges
there can be no surface polarization charges
there may be volume polarization charges
The electrical conductivity σ in the Drude model
depends on the electric field
depends on the square of the density of carriers
doesn't depend on the sign of carriers
doesn't depend on the mean time interval between two successive collision
Considering the phenomenon of electrical polarization in a generic dielectric material, which of the following is correct
The modulus of the electric induction vector D represents a polarization charge per unit area.
The polarization P is always parallel to the electric field vector E within the material.
The polarization P is never parallel to the electric field vector E within the material.
Above the threshold value of the electric field E, the modulus of the polarization vector P tends asymptotically to a maximum saturation value.
Curie's law for a ferromagnet states that magnetic susceptibility is
Xm = Cρ(T − Tc)
Xm = Cρ/(T − Tc) for T > Tc
Xm = Cρ/(T − Tc) for T < Tc
Xm = Cρ/T
For an electric charge to move with constant speed in a region in which there is an electric field
the motion must take place on an equipotential surface
the motion must take place along a line of force of the field
the electric field must be conservative
the electric field must be uniform
The density of electric current j at each point within a conductor
is parallel to electric field E in the conductor only if the carriers are positive
is always zero
is always parallel to electric field E
is parallel to the electric field E in the conductor only if the carriers are negative
An electromagnetic wave carries quantities of motion. Consequently when it affects a surface it applies a force to it. Which of the following statements is true?
the force applied is maximum if the surface is totally absorbent
the applied force is the same whether the surface is totally reflective or totally absorbent
the force applied is maximum if the surface is totally reflective
the applied force is minimal if the surface is totally reflective
The magnetic susceptibility of a diamagnetic material
has a dependence of the type T-1 on temperature
does not depend on the temperature
grows linearly with temperature
decreases linearly with temperature
In order to observe the phenomenon of interference between the waves emitted by two coherent sources, it is necessary that
the difference of path that the two waves must travel to reach a on the screen must be much less than their length
the two waves propagate in different media
the two waves propagate in the same medium
the difference of path that the waves must travel to reach a on the screen must be much greater than their length
In the classic model of electrical conduction (Drude model)
the intensity of electric current j is independent of the applied electric field E
the drift speed of the carriers is independent of the applied electric field E
the electric current density j is independent of the applied electric field E
the electrical conductivity is independent of the applied electric field E
In a Young experiment, the maximum of order one is subtended at an angle θ = 30°. It can be deduced that
the distance the sources is half the wavelength
the distance between the sources is double the wavelength
the distance between the sources and the screen is double the wavelength
the distance between the sources and the screen is half the wavelength
The second law of Laplace provides that the force applied on a closed circuit crossed by a stationary current I on which a uniform magnetic field B acts is
non-zero if field B is parallel to the circuit
different from zero if field B is orthogonal to the circuit
only on the area enclosed by the circuit
always zero
The law of reflection of geometric optics
depends on on the characteristics of the material in which the light beam propagates
does not depend on on the characteristics of the material in which the light beam propagates
depends on the frequency of the light beam
depends on the width of the light beam
An indefinite cylinder is traversed by a current parallel to the axis of the cylinder itself with uniform and stationary current density j. The field B inside the cylinder
grows linearly as the distance r from center increases
is not known. The data of problem are not sufficient to answer
is always null
does not vary with the distance r from the cylinder axis
Given a sphere with a uniform charge density ρ, E is the field inside the sphere?
E is always constant
E is equivalent to that generated by a point charge placed in the center
E grows linearly as the distance r from the center increases
E is always null
A spherical shaped body is made of insulating material and with uniform charge density. The body has a spherical cavity inside, not concentric with respect to it. By indicating with Φz(E) the flow of the electrostatic field through a closed surface Z completely contained in the cavity, and with E(C) the electrostatic field at the center C of the cavity, which of the following statements is true?
ΦΣ(E) = 0, E(C) = 0
ΦΣ(E) ≠ 0, E(C) ≠ 0
ΦΣ(E) = 0, E(C) ≠ 0
ΦΣ(E) ≠ 0, E(C) = 0
A wavelength radiation in the vacuum λ = 600 nm propagates in a transparent dielectric medium. with a refractive index If the wavelength in the medium is reduced to λ = 400 nm, the relative constant of medium εr is
εr = 1.50
εr = 1.23
εr = 0.44
εr = 2.25
The amplitude of the magnetic field of a plane harmonic wave that propagates in vacuum is worth
B0 2 × 10-6 T. What is the maximum value of its Poynting vector S?
Smax = 478W/m2
Smax = 2.66×10−9W/m2
Smax = 5.31×10−9W/m2
Smax = 956W/m2
The vacuum capacitance of a spherical capacitor whose external armature has twice the radius of the internal one (R2 = 2R1) is
C = 4πε00R1
C = 8πε00R1
C = 8πε00R2
C = 4πε0R12
In a ferromagnet the shape of hysteresis cycle depends
from the particular ferromagnetic material and from the applied field H
just from the particular ferromagnetic material
it is equal for all ferromagnetic materials
from the applied field H
