Unit I: Concepts Leading to Quantum Mechanics

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Comprehensive practice flashcards covering Unit I: Concepts Leading to Quantum Mechanics from PES University, including review of electrodynamics, Maxwell's equations, EM waves, black-body radiation, atomic spectra, wave-particle duality, wave packets, uncertainty principle, wave functions, operators, and qubits.

Last updated 7:16 PM on 10/18/26
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390 Terms

1
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What causes an electric field to exist?

The presence of electric charges.

2
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Can electric charges be isolated?

Yes, electric charges can be isolated.

3
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What are the two fundamental kinds of electric charges?

Positive and negative.

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What is the fundamental unit of electric charge and what is its magnitude?

The charge of the electron, which has a magnitude of 1.602×10−19 C1.602 \times 10^{-19}\,\text{C}.

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What is the net electrical state of an undisturbed atom?

An undisturbed atom is electrically neutral.

6
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How can an electron be removed from the influence of the nucleus according to the text?

By providing enough energy in the form of thermal energy.

7
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What remains when an electron is removed from an atom?

An ion with a unit positive charge, while the liberated electron carries a unit negative charge.

8
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Through what phenomenon is the presence of positive or negative charges felt?

Through the electric field.

9
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What determines the strength of the electric field at any point?

The quantity of charge at that point.

10
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How is electric potential defined?

The work done in bringing a unit positive charge from infinity to the point at a distance xx.

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What is the mathematical expression for the electric potential VxV_x at a distance xx from a point charge QQ?

Vx=Q4πε0×1xV_x = \frac{Q}{4\pi\varepsilon_0} \times \frac{1}{x}

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How does electric potential depend on the distance xx from a point charge?

It is inversely proportional to the distance xx.

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What must be done to move a positive test charge towards a positive point charge?

External work has to be done.

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What does the work when moving a positive test charge towards a negative point charge?

The electric field does the work.

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What is the mathematical expression for the electric field ExE_x due to a point charge QQ at distance xx?

Ex=Q4πε0×1x2E_x = \frac{Q}{4\pi\varepsilon_0} \times \frac{1}{x^2}

16
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How does the electric field of a point charge depend on distance?

It is inversely proportional to the square of the distance from the point charge.

17
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How is the electric field expressed in differential form in terms of electric potential VxV_x?

Ex=−dVxdxE_x = -\frac{dV_x}{dx}

18
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How can the presence of an electric field be visualized?

In terms of flux lines.

19
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What do electric flux lines indicate?

The direction of the force felt by a unit positive charge placed along the line.

20
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What is the direction of electric lines of force in the presence of a positive charge?

Radially outwards, which is the direction of repulsion of the test charge.

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What is the direction of electric lines of force in the presence of a negative charge?

Radially inwards, which is the direction of attraction of the test charge.

22
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What is the flux of electric field lines a measure of?

It is a measure of the electric field at a point, and hence a measure of the amount of charge present at that point.

23
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What are magnetic fields generally produced by?

A magnetic dipole, consisting of a north and a south pole.

24
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Can the north and south poles of a magnetic dipole be isolated from each other?

No, they cannot be isolated from each other.

25
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Have magnetic monopoles been experimentally confirmed?

No experimental results are available to confirm the existence of magnetic monopoles as of date.

26
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How does the magnetic field vary with distance from a magnetic dipole?

It is inversely proportional to the square of the distance from the magnetic dipole.

27
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How does the magnetic potential vary with distance from a magnetic dipole?

It is inversely proportional to the distance of the reference point from the given dipole.

28
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What is the geometric path of magnetic field lines external to a magnet?

Continuous closed loops directed from the north pole to the south pole.

29
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Are magnetic field lines continuous inside the magnetic material?

Yes, the field lines are continuous in the material as well.

30
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What does the flux of magnetic field lines indicate?

The strength of the magnetic field at any point.

31
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What defines which end of a current-carrying solenoid behaves as a north or south pole?

The direction of the current flowing through the solenoid.

32
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Under what condition is there a strong interplay between electric and magnetic fields?

When the fields are time dependent.

33
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What does Ampère's law state regarding a current through a straight conductor?

The current through a straight conductor creates a magnetic field around the wire.

34
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What does Faraday's law of electromagnetic induction state?

An induced current appears in a closed coil placed in a time-varying magnetic field.

35
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What two classical laws serve as strong evidence for the interplay between electric and magnetic forces?

Ampère's law and Faraday's law of electromagnetic induction.

36
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What determines whether work in moving a test charge is done by an external agent or by the field?

The sign of the point charge: external work is done if it is positive, and the field does work if it is negative.

37
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Why can an electron be easily separated from an atom via thermal energy?

Because providing enough thermal energy overcomes the electrostatic influence of the nucleus.

38
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What is the net charge of an atom after one electron is liberated?

A unit positive charge (+1+1).

39
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What is the primary difference in isolation between electric and magnetic sources?

Electric charges can be isolated as single positive or negative charges, whereas magnetic poles exist in inseparable dipole pairs.

40
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What is the relationship between the direction of electric flux lines and the force on a positive test charge?

The flux lines indicate the exact direction of the force experienced by a unit positive charge.

41
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How does the electric field depend on the electric potential gradient?

The electric field is the negative gradient (negative spatial derivative) of the electric potential.

42
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What is the reference point for calculating electric potential?

Infinity, where the potential is taken to be zero.

43
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How do magnetic field lines differ fundamentally from electrostatic field lines regarding loops?

Magnetic field lines always form continuous closed loops, whereas electrostatic lines originate and terminate on discrete charges.

44
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Does a static electric charge produce a magnetic field?

No, a magnetic field is created by moving charges (currents) or time-varying electric fields.

45
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What property of magnetic field lines guarantees that as much flux enters a closed surface as leaves it?

The fact that they are continuous closed loops.

46
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In what year were Maxwell's equations published?

1860.

47
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What major unification did Maxwell achieve with his four equations?

He summarized existing ideas of electric and magnetic fields and their interrelated phenomena, describing radiation as an electromagnetic wave.

48
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What is the definition of the partial differential operator ∇\nabla (del)?

∇=i^∂∂x+j^∂∂y+k^∂∂z\nabla = \hat{i}\frac{\partial}{\partial x} + \hat{j}\frac{\partial}{\partial y} + \hat{k}\frac{\partial}{\partial z}

49
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What are i^\hat{i}, j^\hat{j}, and k^\hat{k} in the del operator?

Unit vectors in the three orthogonal directions.

50
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What mathematical object results when the ∇\nabla operator acts on a scalar quantity?

A vector quantity.

51
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What is the gradient of a scalar field AA?

The simple multiplication of ∇\nabla with the scalar field AA, giving the direction and magnitude of the highest rate of change of the field.

52
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What is the result of the ∇\nabla operator acting on the electric potential VV?

∇V=i^∂Vx∂x+j^∂Vy∂y+k^∂Vz∂z=i^Ex+j^Ey+k^Ez=E⃗\nabla V = \hat{i}\frac{\partial V_x}{\partial x} + \hat{j}\frac{\partial V_y}{\partial y} + \hat{k}\frac{\partial V_z}{\partial z} = \hat{i}E_x + \hat{j}E_y + \hat{k}E_z = \vec{E}

53
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What mathematical operation gives the divergence of a vector field A⃗\vec{A}?

The dot product of the ∇\nabla operator with the vector field, ∇⋅A⃗\nabla \cdot \vec{A}.

54
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What is the algebraic expression for ∇⋅A⃗\nabla \cdot \vec{A}?

∇⋅A⃗=∂Ax∂x+∂Ay∂y+∂Az∂z\nabla \cdot \vec{A} = \frac{\partial A_x}{\partial x} + \frac{\partial A_y}{\partial y} + \frac{\partial A_z}{\partial z}

55
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Is the divergence of a vector field a scalar or a vector quantity?

A scalar quantity.

56
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What does the divergence of a vector field represent physically?

The rate of change of the field in the three orthogonal directions (outflow per unit volume).

57
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What operation gives the curl of a vector field A⃗\vec{A}?

The cross product of the ∇\nabla operator with the vector field, ∇×A⃗\nabla \times \vec{A}.

58
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What is the orientation of the vector resulting from the curl of a field?

It is perpendicular to both ∇\nabla and the given vector field.

59
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What is the determinant representation of ∇×A⃗\nabla \times \vec{A}?

∇×A⃗=∣i^j^k^∂∂x∂∂y∂∂zAxAyAz∣\nabla \times \vec{A} = \begin{vmatrix} \hat{i} & \hat{j} & \hat{k} \\ \frac{\partial}{\partial x} & \frac{\partial}{\partial y} & \frac{\partial}{\partial z} \\ A_x & A_y & A_z \end{vmatrix}

60
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What is the expanded component form of ∇×A⃗\nabla \times \vec{A}?

i^(∂Az∂y−∂Ay∂z)−j^(∂Az∂x−∂Ax∂z)+k^(∂Ay∂x−∂Ax∂y)\hat{i}\left(\frac{\partial A_z}{\partial y} - \frac{\partial A_y}{\partial z}\right) - \hat{j}\left(\frac{\partial A_z}{\partial x} - \frac{\partial A_x}{\partial z}\right) + \hat{k}\left(\frac{\partial A_y}{\partial x} - \frac{\partial A_x}{\partial y}\right)

61
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<p>What physical independence between divergence and curl is demonstrated in this diagram?</p>

What physical independence between divergence and curl is demonstrated in this diagram?

A field can possess divergence without curl (source: ∇⋅F>0\nabla \cdot \mathbf{F} > 0), curl without divergence (pure circulation: ∇⋅F=0,∇×F≠0\nabla \cdot \mathbf{F} = 0, \nabla \times \mathbf{F} \neq 0 where a paddle wheel spins), or neither (uniform flow: paddle wheel does not spin).

62
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What vector identity relates the curl of the curl of a vector E⃗\vec{E} to its divergence and Laplacian?

∇×(∇×E⃗)=∇(∇⋅E⃗)−∇2E⃗\nabla \times (\nabla \times \vec{E}) = \nabla(\nabla \cdot \vec{E}) - \nabla^2 \vec{E}

63
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How is the scalar Laplacian operator ∇2\nabla^2 defined in Cartesian coordinates?

∇2=∇⋅∇=∂2∂x2+∂2∂y2+∂2∂z2\nabla^2 = \nabla \cdot \nabla = \frac{\partial^2}{\partial x^2} + \frac{\partial^2}{\partial y^2} + \frac{\partial^2}{\partial z^2}

64
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What is the differential form of Gauss's law for electric fields?

∇⋅E⃗=ρε0\nabla \cdot \vec{E} = \frac{\rho}{\varepsilon_0}

65
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What does ρ\rho represent in Gauss's law for electric fields?

The charge density.

66
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What does ε0\varepsilon_0 represent in electromagnetic theory?

The permittivity of free space.

67
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What is the differential form of Gauss's law for magnetic fields?

∇⋅B⃗=0\nabla \cdot \vec{B} = 0

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What physical fact is implied by ∇⋅B⃗=0\nabla \cdot \vec{B} = 0?

The absence of magnetic monopoles: magnetic field lines always form closed loops so that as much flux enters any closed surface as leaves it.

69
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What is the differential form of Faraday's law of electromagnetic induction?

∇×E⃗=−∂B⃗∂t\nabla \times \vec{E} = -\frac{\partial \vec{B}}{\partial t}

70
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What does the differential Faraday's law state in words?

The curl of the electric field is equal to the negative rate of change of the magnetic field.

71
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What is the differential form of the Ampère–Maxwell circuital law?

∇×B⃗=μ0j⃗+μ0ε0∂E⃗∂t\nabla \times \vec{B} = \mu_0 \vec{j} + \mu_0\varepsilon_0 \frac{\partial \vec{E}}{\partial t}

72
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What does μ0\mu_0 represent in electromagnetic equations?

The permeability of free space.

73
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What does j⃗\vec{j} represent in the Ampère–Maxwell law?

The conduction current density.

74
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What does the second term μ0ε0∂E⃗∂t\mu_0\varepsilon_0 \frac{\partial \vec{E}}{\partial t} in the Ampère–Maxwell law represent?

The displacement current associated with time-varying electric fields, which was Maxwell's contribution.

75
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<p>What paradox in capacitor circuits is illustrated in this diagram and how is it resolved?</p>

What paradox in capacitor circuits is illustrated in this diagram and how is it resolved?

The capacitor paradox: for Surface 1 pierced by the wire, enclosed current is II, but for Surface 2 between the plates, enclosed conduction current is 00. Maxwell's displacement current between the plates resolves this discrepancy.

76
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Why was the introduction of displacement current necessary for consistency in Ampère's law?

Without it, Ampère's law gave contradictory magnetic field circulations depending on which open surface bounded by a closed loop was chosen across capacitor plates.

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What are the source conditions defining free space?

There are no sources of charges (ρ=0\rho = 0) and no conduction currents (j⃗=0\vec{j} = 0).

78
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<p>What summary of electromagnetic fundamentals is depicted in this four-panel overview?</p>

What summary of electromagnetic fundamentals is depicted in this four-panel overview?

Maxwell's four equations: 01 Gauss-Electricity (∇⋅E=ρε0\nabla \cdot \mathbf{E} = \frac{\rho}{\varepsilon_0}, charge is source of E), 02 Gauss-Magnetism (∇⋅B=0\nabla \cdot \mathbf{B} = 0, no magnetic sources), 03 Faraday (∇×E=−∂B∂t\nabla \times \mathbf{E} = -\frac{\partial \mathbf{B}}{\partial t}, changing B circulates E), 04 Ampère-Maxwell (∇×B=μ0J+μ0ε0∂E∂t\nabla \times \mathbf{B} = \mu_0\mathbf{J} + \mu_0\varepsilon_0\frac{\partial \mathbf{E}}{\partial t}, current and changing E circulate B).

79
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What is Gauss's law for electric fields in free space?

∇⋅E⃗=0\nabla \cdot \vec{E} = 0

80
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What is Gauss's law for magnetic fields in free space?

∇⋅B⃗=0\nabla \cdot \vec{B} = 0

81
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What is Faraday's law in free space?

∇×E⃗=−∂B⃗∂t\nabla \times \vec{E} = -\frac{\partial \vec{B}}{\partial t}

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What is the Ampère–Maxwell circuital law in free space?

∇×B⃗=+μ0ε0∂E⃗∂t\nabla \times \vec{B} = +\mu_0\varepsilon_0 \frac{\partial \vec{E}}{\partial t}

83
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In vector calculus, what is the divergence of the curl of any arbitrary vector field?

It is identically zero: ∇⋅(∇×A⃗)=0\nabla \cdot (\nabla \times \vec{A}) = 0.

84
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Taking the divergence of both sides of Faraday's law yields which other Maxwell equation?

Gauss's law for magnetism: ∂∂t(∇⋅B⃗)=0\frac{\partial}{\partial t}(\nabla \cdot \vec{B}) = 0, showing ∇⋅B⃗=0\nabla \cdot \vec{B} = 0.

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What does a non-zero curl of an electric field imply about the field's electrostatic nature?

It implies the field is non-conservative and induced by a time-varying magnetic field, unlike electrostatic fields whose curl is zero.

86
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How does the curl of a vector field behave under coordinate rotation?

It transforms as an axial (or pseudo) vector perpendicular to the plane of circulation.

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What physical system demonstrates that a field can possess zero divergence and non-zero curl?

Pure circular flow around a vortex, where a paddle wheel placed in the fluid rotates.

88
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What physical situation exhibits positive divergence but zero curl?

A static point charge acting as a source with field lines radiating outward symmetrically.

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What physical flow shows both zero divergence and zero curl?

Uniform laminar flow with constant velocity everywhere.

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How does Maxwell's modification of Ampère's law satisfy the continuity equation for charge?

Taking the divergence of ∇×B⃗=μ0j⃗+μ0ε0∂E⃗∂t\nabla \times \vec{B} = \mu_0 \vec{j} + \mu_0\varepsilon_0 \frac{\partial \vec{E}}{\partial t} gives 0=μ0(∇⋅j⃗+∂ρ∂t)0 = \mu_0\left(\nabla \cdot \vec{j} + \frac{\partial \rho}{\partial t}\right), perfectly matching ∇⋅j⃗+∂ρ∂t=0\nabla \cdot \vec{j} + \frac{\partial \rho}{\partial t} = 0.

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In the capacitor paradox, why is the conduction current zero between the capacitor plates?

Because there is vacuum or a dielectric between the plates and no physical wire crosses the gap.

92
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What replaces the conduction current between charging capacitor plates?

The displacement current, Id=ε0dΦEdtI_d = \varepsilon_0 \frac{d\Phi_E}{dt}.

93
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What is the initial step in deriving the electromagnetic wave equation for the electric field?

Taking the curl of the curl of the electric field: ∇×(∇×E⃗)\nabla \times (\nabla \times \vec{E}).

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What is obtained when Faraday's law is substituted into the right side of ∇×(∇×E⃗)\nabla \times (\nabla \times \vec{E})?

∇×(−∂B⃗∂t)=−∂∂t(∇×B⃗)\nabla \times \left(-\frac{\partial \vec{B}}{\partial t}\right) = -\frac{\partial}{\partial t}(\nabla \times \vec{B}).

95
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How does the identity ∇(∇⋅E⃗)−∇2E⃗\nabla(\nabla \cdot \vec{E}) - \nabla^2 \vec{E} simplify in free space?

Because ∇⋅E⃗=0\nabla \cdot \vec{E} = 0 in free space, the first term vanishes, leaving −∇2E⃗-\nabla^2 \vec{E}.

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What is substituted for ∇×B⃗\nabla \times \vec{B} in the derivation of the electric wave equation in free space?

μ0ε0∂E⃗∂t\mu_0\varepsilon_0 \frac{\partial \vec{E}}{\partial t}.

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What is the final differential wave equation for the electric field in free space?

∇2E⃗=μ0ε0∂2E⃗∂t2\nabla^2 \vec{E} = \mu_0\varepsilon_0 \frac{\partial^2 \vec{E}}{\partial t^2}

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What expression gives the speed of propagation cc of an electromagnetic wave in free space?

c=1μ0ε0c = \frac{1}{\sqrt{\mu_0\varepsilon_0}}

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What constants determine the speed of light in free space alone?

The permeability of free space μ0\mu_0 and the permittivity of free space ε0\varepsilon_0.

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What is the wave equation for the magnetic field in free space obtained by starting from ∇×(∇×B⃗)\nabla \times (\nabla \times \vec{B})?

∇2B⃗=1c2∂2B⃗∂t2\nabla^2 \vec{B} = \frac{1}{c^2}\frac{\partial^2 \vec{B}}{\partial t^2}