Historical Background
Huygens developed a wave model before the electromagnetic theory of light. It offered a unified geometrical explanation of reflection and refraction.
Wave Optics Master Module
Understand wavefront construction, secondary wavelets, reflection, refraction and Huygens proofs for NEET, JEE Main, JEE Advanced, IB Physics, IGCSE and A-Level Physics.
In 1678, Dutch physicist Christiaan Huygens proposed a geometrical construction for wave propagation. Ray optics describes paths well, but a wave theory is needed to connect propagation with reflection, refraction, interference and diffraction.
Huygens developed a wave model before the electromagnetic theory of light. It offered a unified geometrical explanation of reflection and refraction.
Rays show direction but not how a complete constant-phase surface advances. Huygens construction evolves the entire wavefront.
Wavefront: constant phase. Wavelet: secondary disturbance. Envelope: common tangent. Normal: propagation direction.
A secondary wavelet is a small wave disturbance centered at a point of the existing wavefront. In an isotropic medium it grows spherically with radius vt.
After the same time interval, a common forward tangent to all equal-time wavelets joins points of equal phase and becomes the next wavefront.
A plane wavefront travels in air for 2 ns. Find its displacement.
Solution: d = ct = 3×10⁸ × 2×10⁻⁹ = 0.60 m.
Find the secondary-wavelet radius after 5 ns in glass of n = 1.5.
Solution: v = c/n = 2×10⁸ m s⁻¹; r = vt = 1.0 m.
A plane wavefront advances 12 cm in 0.5 ns. Find wave speed.
Solution: v = d/t = 0.12/(0.5×10⁻⁹) = 2.4×10⁸ m s⁻¹.
A wavefront speed is 2.0×10⁸ m s⁻¹. Find n.
Solution: n = c/v = 3/2 = 1.5.
Light of wavelength 600 nm enters glass of n = 1.5.
Solution: λ₂ = λ₁/n = 600/1.5 = 400 nm.
A wavefront normal strikes a mirror at 35° to the normal.
Solution: i = 35°, hence r = 35°.
An incident wavefront makes 25° with a reflecting surface.
Solution: Its normal makes 25° with the surface normal, so i = r = 25°.
Light enters n₂ = 1.5 from air at i = 30°.
Solution: sin r = sin30°/1.5 = 1/3; r ≈ 19.5°.
For i = 45° and r = 30°, find v₁/v₂.
Solution: v₁/v₂ = sin i/sin r = 0.707/0.5 = 1.414.
A 5×10¹⁴ Hz wave enters a medium of n = 1.6.
Solution: Frequency remains 5×10¹⁴ Hz; only speed and wavelength change.
Let an incident plane wavefront AB strike a plane reflecting surface. Point A touches the mirror first. During time t, point B reaches C while a secondary wavelet centered at A grows to radius AD.
In time t: BC = vt and AD = vt, hence BC = AD.
Triangles ABC and ADC are right-angled because BC ⟂ AB and AD ⟂ DC.
AC is common to both triangles.
Therefore, ΔABC ≅ ΔADC by RHS congruence.
Hence ∠BAC = ∠DCA.
The angle between wavefront and surface equals the angle between their respective normals.
Therefore, angle of incidence i = angle of reflection r.
Consider a plane wavefront AB entering medium 2 obliquely from medium 1. Point A reaches the interface first. In time t, B reaches C through medium 1 while the secondary wavelet from A advances to D in medium 2.
In time t, BC = v₁t and AD = v₂t.
From right triangle ABC: sin i = BC/AC = v₁t/AC.
From right triangle ADC: sin r = AD/AC = v₂t/AC.
Dividing: sin i / sin r = v₁/v₂.
Because n = c/v, v₁/v₂ = n₂/n₁.
Therefore sin i/sin r = n₂/n₁.
Rearranging gives n₁ sin i = n₂ sin r.
The relative refractive index of medium 2 with respect to 1 is μ₂₁ = n₂/n₁ = v₁/v₂ = sin i/sin r.
One edge of the wavefront changes speed before the other. This rotates the front; its perpendicular ray therefore changes direction.
Optically denser means larger n and smaller v. Optically rarer means smaller n and larger v. Optical density is not mass density.
Speed: changes. Wavelength: changes. Frequency: remains constant. Relation: v = fλ.
A wavefront moves through a medium at 2×10⁸ m s⁻¹ for 3 ns. Find its displacement.
Answer: 0.60 m
Detailed solution: d = vt = 2×10⁸ × 3×10⁻⁹ = 0.60 m.
A wavefront moves through a medium at 2.4×10⁸ m s⁻¹ for 5 ns. Find its displacement.
Answer: 1.20 m
Detailed solution: d = vt = 2.4×10⁸ × 5×10⁻⁹ = 1.20 m.
A wavefront moves through a medium at 1.5×10⁸ m s⁻¹ for 8 ns. Find its displacement.
Answer: 1.20 m
Detailed solution: d = vt = 1.5×10⁸ × 8×10⁻⁹ = 1.20 m.
A wavefront moves through a medium at 2.5×10⁸ m s⁻¹ for 4 ns. Find its displacement.
Answer: 1.00 m
Detailed solution: d = vt = 2.5×10⁸ × 4×10⁻⁹ = 1.00 m.
A wavefront moves through a medium at 1.8×10⁸ m s⁻¹ for 6 ns. Find its displacement.
Answer: 1.08 m
Detailed solution: d = vt = 1.8×10⁸ × 6×10⁻⁹ = 1.08 m.
Light travels at 2×10⁸ m s⁻¹ in a medium. Find its refractive index.
Answer: 1.50
Detailed solution: n = c/v = 3×10⁸/(2×10⁸) = 1.50.
Light travels at 2.4×10⁸ m s⁻¹ in a medium. Find its refractive index.
Answer: 1.25
Detailed solution: n = c/v = 3×10⁸/(2.4×10⁸) = 1.25.
Light travels at 1.875×10⁸ m s⁻¹ in a medium. Find its refractive index.
Answer: 1.60
Detailed solution: n = c/v = 3×10⁸/(1.875×10⁸) = 1.60.
Light travels at 1.5×10⁸ m s⁻¹ in a medium. Find its refractive index.
Answer: 2.00
Detailed solution: n = c/v = 3×10⁸/(1.5×10⁸) = 2.00.
Light travels at 2.5×10⁸ m s⁻¹ in a medium. Find its refractive index.
Answer: 1.20
Detailed solution: n = c/v = 3×10⁸/(2.5×10⁸) = 1.20.
Light of vacuum wavelength 600 nm enters a medium of refractive index 1.5. Find wavelength.
Answer: 400.0 nm
Detailed solution: Frequency is constant, so λ = λ₀/n = 600/1.5 = 400.0 nm.
Light of vacuum wavelength 500 nm enters a medium of refractive index 1.25. Find wavelength.
Answer: 400.0 nm
Detailed solution: Frequency is constant, so λ = λ₀/n = 500/1.25 = 400.0 nm.
Light of vacuum wavelength 650 nm enters a medium of refractive index 1.625. Find wavelength.
Answer: 400.0 nm
Detailed solution: Frequency is constant, so λ = λ₀/n = 650/1.625 = 400.0 nm.
Light of vacuum wavelength 480 nm enters a medium of refractive index 1.6. Find wavelength.
Answer: 300.0 nm
Detailed solution: Frequency is constant, so λ = λ₀/n = 480/1.6 = 300.0 nm.
Light of vacuum wavelength 700 nm enters a medium of refractive index 1.4. Find wavelength.
Answer: 500.0 nm
Detailed solution: Frequency is constant, so λ = λ₀/n = 700/1.4 = 500.0 nm.
A ray enters a medium of index 1.5 from air at 30°. Find r.
Answer: 19.5°
Detailed solution: sin r = sin 30°/1.5; therefore r = 19.5°.
A ray enters a medium of index 1.33 from air at 45°. Find r.
Answer: 32.1°
Detailed solution: sin r = sin 45°/1.33; therefore r = 32.1°.
A ray enters a medium of index 1.6 from air at 40°. Find r.
Answer: 23.7°
Detailed solution: sin r = sin 40°/1.6; therefore r = 23.7°.
A ray enters a medium of index 1.4 from air at 35°. Find r.
Answer: 24.2°
Detailed solution: sin r = sin 35°/1.4; therefore r = 24.2°.
A ray enters a medium of index 1.7 from air at 50°. Find r.
Answer: 26.8°
Detailed solution: sin r = sin 50°/1.7; therefore r = 26.8°.
For refraction angles i = 45° and r = 30°, find v₁/v₂.
Answer: 1.41
Detailed solution: v₁/v₂ = sin i/sin r = sin45°/sin30° = 1.41.
For refraction angles i = 60° and r = 35°, find v₁/v₂.
Answer: 1.51
Detailed solution: v₁/v₂ = sin i/sin r = sin60°/sin35° = 1.51.
For refraction angles i = 50° and r = 30°, find v₁/v₂.
Answer: 1.53
Detailed solution: v₁/v₂ = sin i/sin r = sin50°/sin30° = 1.53.
For refraction angles i = 40° and r = 25°, find v₁/v₂.
Answer: 1.52
Detailed solution: v₁/v₂ = sin i/sin r = sin40°/sin25° = 1.52.
For refraction angles i = 55° and r = 32°, find v₁/v₂.
Answer: 1.55
Detailed solution: v₁/v₂ = sin i/sin r = sin55°/sin32° = 1.55.
A ray is incident at 20°. Find the angle between incident and reflected rays.
Answer: 40°
Detailed solution: The two rays are symmetric about the normal, so the angle is 2i = 40°.
A ray is incident at 25°. Find the angle between incident and reflected rays.
Answer: 50°
Detailed solution: The two rays are symmetric about the normal, so the angle is 2i = 50°.
A ray is incident at 35°. Find the angle between incident and reflected rays.
Answer: 70°
Detailed solution: The two rays are symmetric about the normal, so the angle is 2i = 70°.
A ray is incident at 40°. Find the angle between incident and reflected rays.
Answer: 80°
Detailed solution: The two rays are symmetric about the normal, so the angle is 2i = 80°.
A ray is incident at 50°. Find the angle between incident and reflected rays.
Answer: 100°
Detailed solution: The two rays are symmetric about the normal, so the angle is 2i = 100°.
Case: A monochromatic beam enters water obliquely from air. Successive points of its plane wavefront reach water at different instants.
Question: Explain the wavefront behavior and identify the governing result.
Detailed solution: The part entering water first slows first, rotating the wavefront. Frequency remains constant, wavelength decreases, and the ray bends toward the normal.
Key result: Use n₁ sin i = n₂ sin r and λ₂/λ₁ = v₂/v₁.
Case: A laser wavefront strikes a plane mirror at 30° incidence and the mirror is rotated by 5°.
Question: Explain the wavefront behavior and identify the governing result.
Detailed solution: The reflected direction initially obeys r = 30°. Rotating the normal by 5° rotates the reflected ray by 10°.
Key result: The angle between incident and reflected rays is initially 60°.
Case: A plane wavefront enters and leaves a parallel-sided glass slab.
Question: Explain the wavefront behavior and identify the governing result.
Detailed solution: It bends toward the normal on entry and away on exit. The emergent ray is parallel to the incident ray but laterally displaced.
Key result: Frequency is unchanged throughout; wavelength is smaller inside glass.
Case: A straight water wave enters a shallow region where its speed decreases.
Question: Explain the wavefront behavior and identify the governing result.
Detailed solution: The wavefront spacing decreases and the propagation direction bends toward the normal.
Key result: This is the mechanical-wave analogue of optical refraction.
Case: A lamp is treated as a point source in a uniform medium.
Question: Explain the wavefront behavior and identify the governing result.
Detailed solution: Equal-time loci are spheres. Far away, a small observed patch becomes nearly plane.
Key result: Normals are radii drawn outward from the source.
Case: A long narrow slit acts approximately as a line source.
Question: Explain the wavefront behavior and identify the governing result.
Detailed solution: Equal-distance surfaces around the line are cylinders; a perpendicular cross-section shows concentric circles.
Key result: Normals point radially outward in the cross-sectional plane.
Case: A ray inside glass reaches a glass-air boundary.
Question: Explain the wavefront behavior and identify the governing result.
Detailed solution: Snell's law predicts increasing refracted angle. Beyond the critical angle, no propagating refracted ray exists and total internal reflection occurs.
Key result: At critical incidence, r = 90° and sin C = n₂/n₁.
Case: Light travels through air layers whose refractive index changes gradually.
Question: Explain the wavefront behavior and identify the governing result.
Detailed solution: The wavefront continuously changes orientation and the ray follows a curved path.
Key result: Local propagation remains normal to the evolving wavefront.
Case: An ultrasound pulse reaches a boundary between tissues.
Question: Explain the wavefront behavior and identify the governing result.
Detailed solution: Each reached boundary point produces secondary disturbances, giving reflected and transmitted fronts.
Key result: Huygens construction applies because ultrasound is a wave.
Case: A convex lens receives a plane wavefront.
Question: Explain the wavefront behavior and identify the governing result.
Detailed solution: Different lens thicknesses create phase delays that reshape it into a converging spherical wavefront.
Key result: Its normals meet at the real focus, the center of curvature.
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Academic note: These are original PYQ-pattern and exam-style questions organized by syllabus and assessment style; they are not claimed as verbatim past-paper reproductions.
A. Every point of a wavefront emits secondary wavelets; the forward envelope is the later wavefront.
B. The frequency necessarily changes whenever the propagation direction changes.
C. Wavefronts are parallel to their associated rays.
D. Secondary wavelets remain stationary at the original wavefront.
A. The frequency necessarily changes whenever the propagation direction changes.
B. Wavefronts are parallel to their associated rays.
C. Secondary wavelets remain stationary at the original wavefront.
D. A secondary wavelet travels at the wave speed in that medium.
A. Wavefronts are parallel to their associated rays.
B. Secondary wavelets remain stationary at the original wavefront.
C. The local ray direction is perpendicular to the wavefront.
D. The frequency necessarily changes whenever the propagation direction changes.
A. Secondary wavelets remain stationary at the original wavefront.
B. It is the limiting form of a spherical front with very large radius.
C. The frequency necessarily changes whenever the propagation direction changes.
D. Wavefronts are parallel to their associated rays.
A. Its normals are radii passing through the point source.
B. The frequency necessarily changes whenever the propagation direction changes.
C. Wavefronts are parallel to their associated rays.
D. Secondary wavelets remain stationary at the original wavefront.
A. The frequency necessarily changes whenever the propagation direction changes.
B. Wavefronts are parallel to their associated rays.
C. Secondary wavelets remain stationary at the original wavefront.
D. It is generated by an ideal long line source.
A. Wavefronts are parallel to their associated rays.
B. Secondary wavelets remain stationary at the original wavefront.
C. Huygens geometry gives i = r in the same medium.
D. The frequency necessarily changes whenever the propagation direction changes.
A. Secondary wavelets remain stationary at the original wavefront.
B. sin i/sin r = v₁/v₂.
C. The frequency necessarily changes whenever the propagation direction changes.
D. Wavefronts are parallel to their associated rays.
A. n₁ sin i = n₂ sin r.
B. The frequency necessarily changes whenever the propagation direction changes.
C. Wavefronts are parallel to their associated rays.
D. Secondary wavelets remain stationary at the original wavefront.
A. The frequency necessarily changes whenever the propagation direction changes.
B. Wavefronts are parallel to their associated rays.
C. Secondary wavelets remain stationary at the original wavefront.
D. Frequency remains constant because it is fixed by the source.
A. Wavefronts are parallel to their associated rays.
B. Secondary wavelets remain stationary at the original wavefront.
C. Wavelength changes in direct proportion to speed.
D. The frequency necessarily changes whenever the propagation direction changes.
A. Secondary wavelets remain stationary at the original wavefront.
B. It has larger refractive index and lower light speed.
C. The frequency necessarily changes whenever the propagation direction changes.
D. Wavefronts are parallel to their associated rays.
A. It is the common tangent in the forward propagation direction.
B. The frequency necessarily changes whenever the propagation direction changes.
C. Wavefronts are parallel to their associated rays.
D. Secondary wavelets remain stationary at the original wavefront.
A. The frequency necessarily changes whenever the propagation direction changes.
B. Wavefronts are parallel to their associated rays.
C. Secondary wavelets remain stationary at the original wavefront.
D. No directional bending occurs when i = 0.
A. Wavefronts are parallel to their associated rays.
B. Secondary wavelets remain stationary at the original wavefront.
C. For denser-to-rarer travel, r reaches 90° at the critical angle.
D. The frequency necessarily changes whenever the propagation direction changes.
A. Secondary wavelets remain stationary at the original wavefront.
B. Every point of a wavefront emits secondary wavelets; the forward envelope is the later wavefront.
C. The frequency necessarily changes whenever the propagation direction changes.
D. Wavefronts are parallel to their associated rays.
A. A secondary wavelet travels at the wave speed in that medium.
B. The frequency necessarily changes whenever the propagation direction changes.
C. Wavefronts are parallel to their associated rays.
D. Secondary wavelets remain stationary at the original wavefront.
A. The frequency necessarily changes whenever the propagation direction changes.
B. Wavefronts are parallel to their associated rays.
C. Secondary wavelets remain stationary at the original wavefront.
D. The local ray direction is perpendicular to the wavefront.
A. Wavefronts are parallel to their associated rays.
B. Secondary wavelets remain stationary at the original wavefront.
C. It is the limiting form of a spherical front with very large radius.
D. The frequency necessarily changes whenever the propagation direction changes.
A. Secondary wavelets remain stationary at the original wavefront.
B. Its normals are radii passing through the point source.
C. The frequency necessarily changes whenever the propagation direction changes.
D. Wavefronts are parallel to their associated rays.
A. It is generated by an ideal long line source.
B. The frequency necessarily changes whenever the propagation direction changes.
C. Wavefronts are parallel to their associated rays.
D. Secondary wavelets remain stationary at the original wavefront.
A. The frequency necessarily changes whenever the propagation direction changes.
B. Wavefronts are parallel to their associated rays.
C. Secondary wavelets remain stationary at the original wavefront.
D. Huygens geometry gives i = r in the same medium.
A. Wavefronts are parallel to their associated rays.
B. Secondary wavelets remain stationary at the original wavefront.
C. sin i/sin r = v₁/v₂.
D. The frequency necessarily changes whenever the propagation direction changes.
A. Secondary wavelets remain stationary at the original wavefront.
B. n₁ sin i = n₂ sin r.
C. The frequency necessarily changes whenever the propagation direction changes.
D. Wavefronts are parallel to their associated rays.
A. Frequency remains constant because it is fixed by the source.
B. The frequency necessarily changes whenever the propagation direction changes.
C. Wavefronts are parallel to their associated rays.
D. Secondary wavelets remain stationary at the original wavefront.
A. The frequency necessarily changes whenever the propagation direction changes.
B. Wavefronts are parallel to their associated rays.
C. Secondary wavelets remain stationary at the original wavefront.
D. Wavelength changes in direct proportion to speed.
A. Wavefronts are parallel to their associated rays.
B. Secondary wavelets remain stationary at the original wavefront.
C. It has larger refractive index and lower light speed.
D. The frequency necessarily changes whenever the propagation direction changes.
A. Secondary wavelets remain stationary at the original wavefront.
B. It is the common tangent in the forward propagation direction.
C. The frequency necessarily changes whenever the propagation direction changes.
D. Wavefronts are parallel to their associated rays.
A. No directional bending occurs when i = 0.
B. The frequency necessarily changes whenever the propagation direction changes.
C. Wavefronts are parallel to their associated rays.
D. Secondary wavelets remain stationary at the original wavefront.
A. The frequency necessarily changes whenever the propagation direction changes.
B. Wavefronts are parallel to their associated rays.
C. Secondary wavelets remain stationary at the original wavefront.
D. For denser-to-rarer travel, r reaches 90° at the critical angle.
A. Every point of a wavefront emits secondary wavelets; the forward envelope is the later wavefront.
B. The frequency necessarily changes whenever the propagation direction changes.
C. Wavefronts are parallel to their associated rays.
D. Secondary wavelets remain stationary at the original wavefront.
A. The frequency necessarily changes whenever the propagation direction changes.
B. Wavefronts are parallel to their associated rays.
C. Secondary wavelets remain stationary at the original wavefront.
D. A secondary wavelet travels at the wave speed in that medium.
A. Wavefronts are parallel to their associated rays.
B. Secondary wavelets remain stationary at the original wavefront.
C. The local ray direction is perpendicular to the wavefront.
D. The frequency necessarily changes whenever the propagation direction changes.
A. Secondary wavelets remain stationary at the original wavefront.
B. It is the limiting form of a spherical front with very large radius.
C. The frequency necessarily changes whenever the propagation direction changes.
D. Wavefronts are parallel to their associated rays.
A. Its normals are radii passing through the point source.
B. The frequency necessarily changes whenever the propagation direction changes.
C. Wavefronts are parallel to their associated rays.
D. Secondary wavelets remain stationary at the original wavefront.
A. The frequency necessarily changes whenever the propagation direction changes.
B. Wavefronts are parallel to their associated rays.
C. Secondary wavelets remain stationary at the original wavefront.
D. It is generated by an ideal long line source.
A. Wavefronts are parallel to their associated rays.
B. Secondary wavelets remain stationary at the original wavefront.
C. Huygens geometry gives i = r in the same medium.
D. The frequency necessarily changes whenever the propagation direction changes.
A. Secondary wavelets remain stationary at the original wavefront.
B. sin i/sin r = v₁/v₂.
C. The frequency necessarily changes whenever the propagation direction changes.
D. Wavefronts are parallel to their associated rays.
A. n₁ sin i = n₂ sin r.
B. The frequency necessarily changes whenever the propagation direction changes.
C. Wavefronts are parallel to their associated rays.
D. Secondary wavelets remain stationary at the original wavefront.
A. The frequency necessarily changes whenever the propagation direction changes.
B. Wavefronts are parallel to their associated rays.
C. Secondary wavelets remain stationary at the original wavefront.
D. Frequency remains constant because it is fixed by the source.
A. Wavefronts are parallel to their associated rays.
B. Secondary wavelets remain stationary at the original wavefront.
C. Wavelength changes in direct proportion to speed.
D. The frequency necessarily changes whenever the propagation direction changes.
A. Secondary wavelets remain stationary at the original wavefront.
B. It has larger refractive index and lower light speed.
C. The frequency necessarily changes whenever the propagation direction changes.
D. Wavefronts are parallel to their associated rays.
A. It is the common tangent in the forward propagation direction.
B. The frequency necessarily changes whenever the propagation direction changes.
C. Wavefronts are parallel to their associated rays.
D. Secondary wavelets remain stationary at the original wavefront.
A. The frequency necessarily changes whenever the propagation direction changes.
B. Wavefronts are parallel to their associated rays.
C. Secondary wavelets remain stationary at the original wavefront.
D. No directional bending occurs when i = 0.
A. Wavefronts are parallel to their associated rays.
B. Secondary wavelets remain stationary at the original wavefront.
C. For denser-to-rarer travel, r reaches 90° at the critical angle.
D. The frequency necessarily changes whenever the propagation direction changes.
A. Secondary wavelets remain stationary at the original wavefront.
B. Every point of a wavefront emits secondary wavelets; the forward envelope is the later wavefront.
C. The frequency necessarily changes whenever the propagation direction changes.
D. Wavefronts are parallel to their associated rays.
A. A secondary wavelet travels at the wave speed in that medium.
B. The frequency necessarily changes whenever the propagation direction changes.
C. Wavefronts are parallel to their associated rays.
D. Secondary wavelets remain stationary at the original wavefront.
A. The frequency necessarily changes whenever the propagation direction changes.
B. Wavefronts are parallel to their associated rays.
C. Secondary wavelets remain stationary at the original wavefront.
D. The local ray direction is perpendicular to the wavefront.
A. Wavefronts are parallel to their associated rays.
B. Secondary wavelets remain stationary at the original wavefront.
C. It is the limiting form of a spherical front with very large radius.
D. The frequency necessarily changes whenever the propagation direction changes.
A. Secondary wavelets remain stationary at the original wavefront.
B. Its normals are radii passing through the point source.
C. The frequency necessarily changes whenever the propagation direction changes.
D. Wavefronts are parallel to their associated rays.
A. It is generated by an ideal long line source.
B. The frequency necessarily changes whenever the propagation direction changes.
C. Wavefronts are parallel to their associated rays.
D. Secondary wavelets remain stationary at the original wavefront.
A. The frequency necessarily changes whenever the propagation direction changes.
B. Wavefronts are parallel to their associated rays.
C. Secondary wavelets remain stationary at the original wavefront.
D. Huygens geometry gives i = r in the same medium.
A. Wavefronts are parallel to their associated rays.
B. Secondary wavelets remain stationary at the original wavefront.
C. sin i/sin r = v₁/v₂.
D. The frequency necessarily changes whenever the propagation direction changes.
A. Secondary wavelets remain stationary at the original wavefront.
B. n₁ sin i = n₂ sin r.
C. The frequency necessarily changes whenever the propagation direction changes.
D. Wavefronts are parallel to their associated rays.
A. Frequency remains constant because it is fixed by the source.
B. The frequency necessarily changes whenever the propagation direction changes.
C. Wavefronts are parallel to their associated rays.
D. Secondary wavelets remain stationary at the original wavefront.
A. The frequency necessarily changes whenever the propagation direction changes.
B. Wavefronts are parallel to their associated rays.
C. Secondary wavelets remain stationary at the original wavefront.
D. Wavelength changes in direct proportion to speed.
A. Wavefronts are parallel to their associated rays.
B. Secondary wavelets remain stationary at the original wavefront.
C. It has larger refractive index and lower light speed.
D. The frequency necessarily changes whenever the propagation direction changes.
A. Secondary wavelets remain stationary at the original wavefront.
B. It is the common tangent in the forward propagation direction.
C. The frequency necessarily changes whenever the propagation direction changes.
D. Wavefronts are parallel to their associated rays.
A. No directional bending occurs when i = 0.
B. The frequency necessarily changes whenever the propagation direction changes.
C. Wavefronts are parallel to their associated rays.
D. Secondary wavelets remain stationary at the original wavefront.
A. The frequency necessarily changes whenever the propagation direction changes.
B. Wavefronts are parallel to their associated rays.
C. Secondary wavelets remain stationary at the original wavefront.
D. For denser-to-rarer travel, r reaches 90° at the critical angle.
A. Every point of a wavefront emits secondary wavelets; the forward envelope is the later wavefront.
B. The frequency necessarily changes whenever the propagation direction changes.
C. Wavefronts are parallel to their associated rays.
D. Secondary wavelets remain stationary at the original wavefront.
A. The frequency necessarily changes whenever the propagation direction changes.
B. Wavefronts are parallel to their associated rays.
C. Secondary wavelets remain stationary at the original wavefront.
D. A secondary wavelet travels at the wave speed in that medium.
A. Wavefronts are parallel to their associated rays.
B. Secondary wavelets remain stationary at the original wavefront.
C. The local ray direction is perpendicular to the wavefront.
D. The frequency necessarily changes whenever the propagation direction changes.
A. Secondary wavelets remain stationary at the original wavefront.
B. It is the limiting form of a spherical front with very large radius.
C. The frequency necessarily changes whenever the propagation direction changes.
D. Wavefronts are parallel to their associated rays.
A. Its normals are radii passing through the point source.
B. The frequency necessarily changes whenever the propagation direction changes.
C. Wavefronts are parallel to their associated rays.
D. Secondary wavelets remain stationary at the original wavefront.
A. The frequency necessarily changes whenever the propagation direction changes.
B. Wavefronts are parallel to their associated rays.
C. Secondary wavelets remain stationary at the original wavefront.
D. It is generated by an ideal long line source.
A. Wavefronts are parallel to their associated rays.
B. Secondary wavelets remain stationary at the original wavefront.
C. Huygens geometry gives i = r in the same medium.
D. The frequency necessarily changes whenever the propagation direction changes.
A. Secondary wavelets remain stationary at the original wavefront.
B. sin i/sin r = v₁/v₂.
C. The frequency necessarily changes whenever the propagation direction changes.
D. Wavefronts are parallel to their associated rays.
A. n₁ sin i = n₂ sin r.
B. The frequency necessarily changes whenever the propagation direction changes.
C. Wavefronts are parallel to their associated rays.
D. Secondary wavelets remain stationary at the original wavefront.
A. The frequency necessarily changes whenever the propagation direction changes.
B. Wavefronts are parallel to their associated rays.
C. Secondary wavelets remain stationary at the original wavefront.
D. Frequency remains constant because it is fixed by the source.
A. Wavefronts are parallel to their associated rays.
B. Secondary wavelets remain stationary at the original wavefront.
C. Wavelength changes in direct proportion to speed.
D. The frequency necessarily changes whenever the propagation direction changes.
A. Secondary wavelets remain stationary at the original wavefront.
B. It has larger refractive index and lower light speed.
C. The frequency necessarily changes whenever the propagation direction changes.
D. Wavefronts are parallel to their associated rays.
A. It is the common tangent in the forward propagation direction.
B. The frequency necessarily changes whenever the propagation direction changes.
C. Wavefronts are parallel to their associated rays.
D. Secondary wavelets remain stationary at the original wavefront.
A. The frequency necessarily changes whenever the propagation direction changes.
B. Wavefronts are parallel to their associated rays.
C. Secondary wavelets remain stationary at the original wavefront.
D. No directional bending occurs when i = 0.
A. Wavefronts are parallel to their associated rays.
B. Secondary wavelets remain stationary at the original wavefront.
C. For denser-to-rarer travel, r reaches 90° at the critical angle.
D. The frequency necessarily changes whenever the propagation direction changes.
A. Secondary wavelets remain stationary at the original wavefront.
B. Every point of a wavefront emits secondary wavelets; the forward envelope is the later wavefront.
C. The frequency necessarily changes whenever the propagation direction changes.
D. Wavefronts are parallel to their associated rays.
A. A secondary wavelet travels at the wave speed in that medium.
B. The frequency necessarily changes whenever the propagation direction changes.
C. Wavefronts are parallel to their associated rays.
D. Secondary wavelets remain stationary at the original wavefront.
A. The frequency necessarily changes whenever the propagation direction changes.
B. Wavefronts are parallel to their associated rays.
C. Secondary wavelets remain stationary at the original wavefront.
D. The local ray direction is perpendicular to the wavefront.
A. Wavefronts are parallel to their associated rays.
B. Secondary wavelets remain stationary at the original wavefront.
C. It is the limiting form of a spherical front with very large radius.
D. The frequency necessarily changes whenever the propagation direction changes.
A. Secondary wavelets remain stationary at the original wavefront.
B. Its normals are radii passing through the point source.
C. The frequency necessarily changes whenever the propagation direction changes.
D. Wavefronts are parallel to their associated rays.
A. It is generated by an ideal long line source.
B. The frequency necessarily changes whenever the propagation direction changes.
C. Wavefronts are parallel to their associated rays.
D. Secondary wavelets remain stationary at the original wavefront.
A. The frequency necessarily changes whenever the propagation direction changes.
B. Wavefronts are parallel to their associated rays.
C. Secondary wavelets remain stationary at the original wavefront.
D. Huygens geometry gives i = r in the same medium.
A. Wavefronts are parallel to their associated rays.
B. Secondary wavelets remain stationary at the original wavefront.
C. sin i/sin r = v₁/v₂.
D. The frequency necessarily changes whenever the propagation direction changes.
A. Secondary wavelets remain stationary at the original wavefront.
B. n₁ sin i = n₂ sin r.
C. The frequency necessarily changes whenever the propagation direction changes.
D. Wavefronts are parallel to their associated rays.
A. Frequency remains constant because it is fixed by the source.
B. The frequency necessarily changes whenever the propagation direction changes.
C. Wavefronts are parallel to their associated rays.
D. Secondary wavelets remain stationary at the original wavefront.
A. The frequency necessarily changes whenever the propagation direction changes.
B. Wavefronts are parallel to their associated rays.
C. Secondary wavelets remain stationary at the original wavefront.
D. Wavelength changes in direct proportion to speed.
A. Wavefronts are parallel to their associated rays.
B. Secondary wavelets remain stationary at the original wavefront.
C. It has larger refractive index and lower light speed.
D. The frequency necessarily changes whenever the propagation direction changes.
A. Secondary wavelets remain stationary at the original wavefront.
B. It is the common tangent in the forward propagation direction.
C. The frequency necessarily changes whenever the propagation direction changes.
D. Wavefronts are parallel to their associated rays.
A. No directional bending occurs when i = 0.
B. The frequency necessarily changes whenever the propagation direction changes.
C. Wavefronts are parallel to their associated rays.
D. Secondary wavelets remain stationary at the original wavefront.
A. The frequency necessarily changes whenever the propagation direction changes.
B. Wavefronts are parallel to their associated rays.
C. Secondary wavelets remain stationary at the original wavefront.
D. For denser-to-rarer travel, r reaches 90° at the critical angle.
A. Every point of a wavefront emits secondary wavelets; the forward envelope is the later wavefront.
B. The frequency necessarily changes whenever the propagation direction changes.
C. Wavefronts are parallel to their associated rays.
D. Secondary wavelets remain stationary at the original wavefront.
A. The frequency necessarily changes whenever the propagation direction changes.
B. Wavefronts are parallel to their associated rays.
C. Secondary wavelets remain stationary at the original wavefront.
D. A secondary wavelet travels at the wave speed in that medium.
A. Wavefronts are parallel to their associated rays.
B. Secondary wavelets remain stationary at the original wavefront.
C. The local ray direction is perpendicular to the wavefront.
D. The frequency necessarily changes whenever the propagation direction changes.
A. Secondary wavelets remain stationary at the original wavefront.
B. It is the limiting form of a spherical front with very large radius.
C. The frequency necessarily changes whenever the propagation direction changes.
D. Wavefronts are parallel to their associated rays.
A. Its normals are radii passing through the point source.
B. The frequency necessarily changes whenever the propagation direction changes.
C. Wavefronts are parallel to their associated rays.
D. Secondary wavelets remain stationary at the original wavefront.
A. The frequency necessarily changes whenever the propagation direction changes.
B. Wavefronts are parallel to their associated rays.
C. Secondary wavelets remain stationary at the original wavefront.
D. It is generated by an ideal long line source.
A. Wavefronts are parallel to their associated rays.
B. Secondary wavelets remain stationary at the original wavefront.
C. Huygens geometry gives i = r in the same medium.
D. The frequency necessarily changes whenever the propagation direction changes.
A. Secondary wavelets remain stationary at the original wavefront.
B. sin i/sin r = v₁/v₂.
C. The frequency necessarily changes whenever the propagation direction changes.
D. Wavefronts are parallel to their associated rays.
A. n₁ sin i = n₂ sin r.
B. The frequency necessarily changes whenever the propagation direction changes.
C. Wavefronts are parallel to their associated rays.
D. Secondary wavelets remain stationary at the original wavefront.
A. The frequency necessarily changes whenever the propagation direction changes.
B. Wavefronts are parallel to their associated rays.
C. Secondary wavelets remain stationary at the original wavefront.
D. Frequency remains constant because it is fixed by the source.
A. Wavefronts are parallel to their associated rays.
B. Secondary wavelets remain stationary at the original wavefront.
C. Wavelength changes in direct proportion to speed.
D. The frequency necessarily changes whenever the propagation direction changes.
A. Secondary wavelets remain stationary at the original wavefront.
B. It has larger refractive index and lower light speed.
C. The frequency necessarily changes whenever the propagation direction changes.
D. Wavefronts are parallel to their associated rays.
A. It is the common tangent in the forward propagation direction.
B. The frequency necessarily changes whenever the propagation direction changes.
C. Wavefronts are parallel to their associated rays.
D. Secondary wavelets remain stationary at the original wavefront.
A. The frequency necessarily changes whenever the propagation direction changes.
B. Wavefronts are parallel to their associated rays.
C. Secondary wavelets remain stationary at the original wavefront.
D. No directional bending occurs when i = 0.
A. Wavefronts are parallel to their associated rays.
B. Secondary wavelets remain stationary at the original wavefront.
C. For denser-to-rarer travel, r reaches 90° at the critical angle.
D. The frequency necessarily changes whenever the propagation direction changes.
A. Secondary wavelets remain stationary at the original wavefront.
B. Every point of a wavefront emits secondary wavelets; the forward envelope is the later wavefront.
C. The frequency necessarily changes whenever the propagation direction changes.
D. Wavefronts are parallel to their associated rays.
A. A secondary wavelet travels at the wave speed in that medium.
B. The frequency necessarily changes whenever the propagation direction changes.
C. Wavefronts are parallel to their associated rays.
D. Secondary wavelets remain stationary at the original wavefront.
A. The frequency necessarily changes whenever the propagation direction changes.
B. Wavefronts are parallel to their associated rays.
C. Secondary wavelets remain stationary at the original wavefront.
D. The local ray direction is perpendicular to the wavefront.
A. Wavefronts are parallel to their associated rays.
B. Secondary wavelets remain stationary at the original wavefront.
C. It is the limiting form of a spherical front with very large radius.
D. The frequency necessarily changes whenever the propagation direction changes.
A. Secondary wavelets remain stationary at the original wavefront.
B. Its normals are radii passing through the point source.
C. The frequency necessarily changes whenever the propagation direction changes.
D. Wavefronts are parallel to their associated rays.
A. It is generated by an ideal long line source.
B. The frequency necessarily changes whenever the propagation direction changes.
C. Wavefronts are parallel to their associated rays.
D. Secondary wavelets remain stationary at the original wavefront.
A. The frequency necessarily changes whenever the propagation direction changes.
B. Wavefronts are parallel to their associated rays.
C. Secondary wavelets remain stationary at the original wavefront.
D. Huygens geometry gives i = r in the same medium.
A. Wavefronts are parallel to their associated rays.
B. Secondary wavelets remain stationary at the original wavefront.
C. sin i/sin r = v₁/v₂.
D. The frequency necessarily changes whenever the propagation direction changes.
A. Secondary wavelets remain stationary at the original wavefront.
B. n₁ sin i = n₂ sin r.
C. The frequency necessarily changes whenever the propagation direction changes.
D. Wavefronts are parallel to their associated rays.
A. Frequency remains constant because it is fixed by the source.
B. The frequency necessarily changes whenever the propagation direction changes.
C. Wavefronts are parallel to their associated rays.
D. Secondary wavelets remain stationary at the original wavefront.
A. The frequency necessarily changes whenever the propagation direction changes.
B. Wavefronts are parallel to their associated rays.
C. Secondary wavelets remain stationary at the original wavefront.
D. Wavelength changes in direct proportion to speed.
A. Wavefronts are parallel to their associated rays.
B. Secondary wavelets remain stationary at the original wavefront.
C. It has larger refractive index and lower light speed.
D. The frequency necessarily changes whenever the propagation direction changes.
A. Secondary wavelets remain stationary at the original wavefront.
B. It is the common tangent in the forward propagation direction.
C. The frequency necessarily changes whenever the propagation direction changes.
D. Wavefronts are parallel to their associated rays.
A. No directional bending occurs when i = 0.
B. The frequency necessarily changes whenever the propagation direction changes.
C. Wavefronts are parallel to their associated rays.
D. Secondary wavelets remain stationary at the original wavefront.
A. The frequency necessarily changes whenever the propagation direction changes.
B. Wavefronts are parallel to their associated rays.
C. Secondary wavelets remain stationary at the original wavefront.
D. For denser-to-rarer travel, r reaches 90° at the critical angle.
A. Every point of a wavefront emits secondary wavelets; the forward envelope is the later wavefront.
B. The frequency necessarily changes whenever the propagation direction changes.
C. Wavefronts are parallel to their associated rays.
D. Secondary wavelets remain stationary at the original wavefront.
A. The frequency necessarily changes whenever the propagation direction changes.
B. Wavefronts are parallel to their associated rays.
C. Secondary wavelets remain stationary at the original wavefront.
D. A secondary wavelet travels at the wave speed in that medium.
A. Wavefronts are parallel to their associated rays.
B. Secondary wavelets remain stationary at the original wavefront.
C. The local ray direction is perpendicular to the wavefront.
D. The frequency necessarily changes whenever the propagation direction changes.
A. Secondary wavelets remain stationary at the original wavefront.
B. It is the limiting form of a spherical front with very large radius.
C. The frequency necessarily changes whenever the propagation direction changes.
D. Wavefronts are parallel to their associated rays.
A. Its normals are radii passing through the point source.
B. The frequency necessarily changes whenever the propagation direction changes.
C. Wavefronts are parallel to their associated rays.
D. Secondary wavelets remain stationary at the original wavefront.
A. The frequency necessarily changes whenever the propagation direction changes.
B. Wavefronts are parallel to their associated rays.
C. Secondary wavelets remain stationary at the original wavefront.
D. It is generated by an ideal long line source.
A. Wavefronts are parallel to their associated rays.
B. Secondary wavelets remain stationary at the original wavefront.
C. Huygens geometry gives i = r in the same medium.
D. The frequency necessarily changes whenever the propagation direction changes.
A. Secondary wavelets remain stationary at the original wavefront.
B. sin i/sin r = v₁/v₂.
C. The frequency necessarily changes whenever the propagation direction changes.
D. Wavefronts are parallel to their associated rays.
A. n₁ sin i = n₂ sin r.
B. The frequency necessarily changes whenever the propagation direction changes.
C. Wavefronts are parallel to their associated rays.
D. Secondary wavelets remain stationary at the original wavefront.
A. The frequency necessarily changes whenever the propagation direction changes.
B. Wavefronts are parallel to their associated rays.
C. Secondary wavelets remain stationary at the original wavefront.
D. Frequency remains constant because it is fixed by the source.
A. Wavefronts are parallel to their associated rays.
B. Secondary wavelets remain stationary at the original wavefront.
C. Wavelength changes in direct proportion to speed.
D. The frequency necessarily changes whenever the propagation direction changes.
A. Secondary wavelets remain stationary at the original wavefront.
B. It has larger refractive index and lower light speed.
C. The frequency necessarily changes whenever the propagation direction changes.
D. Wavefronts are parallel to their associated rays.
A. It is the common tangent in the forward propagation direction.
B. The frequency necessarily changes whenever the propagation direction changes.
C. Wavefronts are parallel to their associated rays.
D. Secondary wavelets remain stationary at the original wavefront.
A. The frequency necessarily changes whenever the propagation direction changes.
B. Wavefronts are parallel to their associated rays.
C. Secondary wavelets remain stationary at the original wavefront.
D. No directional bending occurs when i = 0.
A. Wavefronts are parallel to their associated rays.
B. Secondary wavelets remain stationary at the original wavefront.
C. For denser-to-rarer travel, r reaches 90° at the critical angle.
D. The frequency necessarily changes whenever the propagation direction changes.
A. Secondary wavelets remain stationary at the original wavefront.
B. Every point of a wavefront emits secondary wavelets; the forward envelope is the later wavefront.
C. The frequency necessarily changes whenever the propagation direction changes.
D. Wavefronts are parallel to their associated rays.
A. A secondary wavelet travels at the wave speed in that medium.
B. The frequency necessarily changes whenever the propagation direction changes.
C. Wavefronts are parallel to their associated rays.
D. Secondary wavelets remain stationary at the original wavefront.
A. The frequency necessarily changes whenever the propagation direction changes.
B. Wavefronts are parallel to their associated rays.
C. Secondary wavelets remain stationary at the original wavefront.
D. The local ray direction is perpendicular to the wavefront.
A. Wavefronts are parallel to their associated rays.
B. Secondary wavelets remain stationary at the original wavefront.
C. It is the limiting form of a spherical front with very large radius.
D. The frequency necessarily changes whenever the propagation direction changes.
A. Secondary wavelets remain stationary at the original wavefront.
B. Its normals are radii passing through the point source.
C. The frequency necessarily changes whenever the propagation direction changes.
D. Wavefronts are parallel to their associated rays.
A. It is generated by an ideal long line source.
B. The frequency necessarily changes whenever the propagation direction changes.
C. Wavefronts are parallel to their associated rays.
D. Secondary wavelets remain stationary at the original wavefront.
A. The frequency necessarily changes whenever the propagation direction changes.
B. Wavefronts are parallel to their associated rays.
C. Secondary wavelets remain stationary at the original wavefront.
D. Huygens geometry gives i = r in the same medium.
A. Wavefronts are parallel to their associated rays.
B. Secondary wavelets remain stationary at the original wavefront.
C. sin i/sin r = v₁/v₂.
D. The frequency necessarily changes whenever the propagation direction changes.
A. Secondary wavelets remain stationary at the original wavefront.
B. n₁ sin i = n₂ sin r.
C. The frequency necessarily changes whenever the propagation direction changes.
D. Wavefronts are parallel to their associated rays.
A. Frequency remains constant because it is fixed by the source.
B. The frequency necessarily changes whenever the propagation direction changes.
C. Wavefronts are parallel to their associated rays.
D. Secondary wavelets remain stationary at the original wavefront.
A. The frequency necessarily changes whenever the propagation direction changes.
B. Wavefronts are parallel to their associated rays.
C. Secondary wavelets remain stationary at the original wavefront.
D. Wavelength changes in direct proportion to speed.
A. Wavefronts are parallel to their associated rays.
B. Secondary wavelets remain stationary at the original wavefront.
C. It has larger refractive index and lower light speed.
D. The frequency necessarily changes whenever the propagation direction changes.
A. Secondary wavelets remain stationary at the original wavefront.
B. It is the common tangent in the forward propagation direction.
C. The frequency necessarily changes whenever the propagation direction changes.
D. Wavefronts are parallel to their associated rays.
A. No directional bending occurs when i = 0.
B. The frequency necessarily changes whenever the propagation direction changes.
C. Wavefronts are parallel to their associated rays.
D. Secondary wavelets remain stationary at the original wavefront.
A. The frequency necessarily changes whenever the propagation direction changes.
B. Wavefronts are parallel to their associated rays.
C. Secondary wavelets remain stationary at the original wavefront.
D. For denser-to-rarer travel, r reaches 90° at the critical angle.
A. Every point of a wavefront emits secondary wavelets; the forward envelope is the later wavefront.
B. The frequency necessarily changes whenever the propagation direction changes.
C. Wavefronts are parallel to their associated rays.
D. Secondary wavelets remain stationary at the original wavefront.
A. The frequency necessarily changes whenever the propagation direction changes.
B. Wavefronts are parallel to their associated rays.
C. Secondary wavelets remain stationary at the original wavefront.
D. A secondary wavelet travels at the wave speed in that medium.
A. Wavefronts are parallel to their associated rays.
B. Secondary wavelets remain stationary at the original wavefront.
C. The local ray direction is perpendicular to the wavefront.
D. The frequency necessarily changes whenever the propagation direction changes.
A. Secondary wavelets remain stationary at the original wavefront.
B. It is the limiting form of a spherical front with very large radius.
C. The frequency necessarily changes whenever the propagation direction changes.
D. Wavefronts are parallel to their associated rays.
A. Its normals are radii passing through the point source.
B. The frequency necessarily changes whenever the propagation direction changes.
C. Wavefronts are parallel to their associated rays.
D. Secondary wavelets remain stationary at the original wavefront.
A. The frequency necessarily changes whenever the propagation direction changes.
B. Wavefronts are parallel to their associated rays.
C. Secondary wavelets remain stationary at the original wavefront.
D. It is generated by an ideal long line source.
A. Wavefronts are parallel to their associated rays.
B. Secondary wavelets remain stationary at the original wavefront.
C. Huygens geometry gives i = r in the same medium.
D. The frequency necessarily changes whenever the propagation direction changes.
A. Secondary wavelets remain stationary at the original wavefront.
B. sin i/sin r = v₁/v₂.
C. The frequency necessarily changes whenever the propagation direction changes.
D. Wavefronts are parallel to their associated rays.
A. n₁ sin i = n₂ sin r.
B. The frequency necessarily changes whenever the propagation direction changes.
C. Wavefronts are parallel to their associated rays.
D. Secondary wavelets remain stationary at the original wavefront.
A. The frequency necessarily changes whenever the propagation direction changes.
B. Wavefronts are parallel to their associated rays.
C. Secondary wavelets remain stationary at the original wavefront.
D. Frequency remains constant because it is fixed by the source.
A. Wavefronts are parallel to their associated rays.
B. Secondary wavelets remain stationary at the original wavefront.
C. Wavelength changes in direct proportion to speed.
D. The frequency necessarily changes whenever the propagation direction changes.
A. Secondary wavelets remain stationary at the original wavefront.
B. It has larger refractive index and lower light speed.
C. The frequency necessarily changes whenever the propagation direction changes.
D. Wavefronts are parallel to their associated rays.
A. It is the common tangent in the forward propagation direction.
B. The frequency necessarily changes whenever the propagation direction changes.
C. Wavefronts are parallel to their associated rays.
D. Secondary wavelets remain stationary at the original wavefront.
A. The frequency necessarily changes whenever the propagation direction changes.
B. Wavefronts are parallel to their associated rays.
C. Secondary wavelets remain stationary at the original wavefront.
D. No directional bending occurs when i = 0.
A. Wavefronts are parallel to their associated rays.
B. Secondary wavelets remain stationary at the original wavefront.
C. For denser-to-rarer travel, r reaches 90° at the critical angle.
D. The frequency necessarily changes whenever the propagation direction changes.
A. Secondary wavelets remain stationary at the original wavefront.
B. Every point of a wavefront emits secondary wavelets; the forward envelope is the later wavefront.
C. The frequency necessarily changes whenever the propagation direction changes.
D. Wavefronts are parallel to their associated rays.
A. A secondary wavelet travels at the wave speed in that medium.
B. The frequency necessarily changes whenever the propagation direction changes.
C. Wavefronts are parallel to their associated rays.
D. Secondary wavelets remain stationary at the original wavefront.
A. The frequency necessarily changes whenever the propagation direction changes.
B. Wavefronts are parallel to their associated rays.
C. Secondary wavelets remain stationary at the original wavefront.
D. The local ray direction is perpendicular to the wavefront.
A. Wavefronts are parallel to their associated rays.
B. Secondary wavelets remain stationary at the original wavefront.
C. It is the limiting form of a spherical front with very large radius.
D. The frequency necessarily changes whenever the propagation direction changes.
A. Secondary wavelets remain stationary at the original wavefront.
B. Its normals are radii passing through the point source.
C. The frequency necessarily changes whenever the propagation direction changes.
D. Wavefronts are parallel to their associated rays.
A. It is generated by an ideal long line source.
B. The frequency necessarily changes whenever the propagation direction changes.
C. Wavefronts are parallel to their associated rays.
D. Secondary wavelets remain stationary at the original wavefront.
A. The frequency necessarily changes whenever the propagation direction changes.
B. Wavefronts are parallel to their associated rays.
C. Secondary wavelets remain stationary at the original wavefront.
D. Huygens geometry gives i = r in the same medium.
A. Wavefronts are parallel to their associated rays.
B. Secondary wavelets remain stationary at the original wavefront.
C. sin i/sin r = v₁/v₂.
D. The frequency necessarily changes whenever the propagation direction changes.
A. Secondary wavelets remain stationary at the original wavefront.
B. n₁ sin i = n₂ sin r.
C. The frequency necessarily changes whenever the propagation direction changes.
D. Wavefronts are parallel to their associated rays.
A. Frequency remains constant because it is fixed by the source.
B. The frequency necessarily changes whenever the propagation direction changes.
C. Wavefronts are parallel to their associated rays.
D. Secondary wavelets remain stationary at the original wavefront.
A. The frequency necessarily changes whenever the propagation direction changes.
B. Wavefronts are parallel to their associated rays.
C. Secondary wavelets remain stationary at the original wavefront.
D. Wavelength changes in direct proportion to speed.
A. Wavefronts are parallel to their associated rays.
B. Secondary wavelets remain stationary at the original wavefront.
C. It has larger refractive index and lower light speed.
D. The frequency necessarily changes whenever the propagation direction changes.
A. Secondary wavelets remain stationary at the original wavefront.
B. It is the common tangent in the forward propagation direction.
C. The frequency necessarily changes whenever the propagation direction changes.
D. Wavefronts are parallel to their associated rays.
A. No directional bending occurs when i = 0.
B. The frequency necessarily changes whenever the propagation direction changes.
C. Wavefronts are parallel to their associated rays.
D. Secondary wavelets remain stationary at the original wavefront.
A. The frequency necessarily changes whenever the propagation direction changes.
B. Wavefronts are parallel to their associated rays.
C. Secondary wavelets remain stationary at the original wavefront.
D. For denser-to-rarer travel, r reaches 90° at the critical angle.
A. Every point of a wavefront emits secondary wavelets; the forward envelope is the later wavefront.
B. The frequency necessarily changes whenever the propagation direction changes.
C. Wavefronts are parallel to their associated rays.
D. Secondary wavelets remain stationary at the original wavefront.
A. The frequency necessarily changes whenever the propagation direction changes.
B. Wavefronts are parallel to their associated rays.
C. Secondary wavelets remain stationary at the original wavefront.
D. A secondary wavelet travels at the wave speed in that medium.
A. Wavefronts are parallel to their associated rays.
B. Secondary wavelets remain stationary at the original wavefront.
C. The local ray direction is perpendicular to the wavefront.
D. The frequency necessarily changes whenever the propagation direction changes.
A. Secondary wavelets remain stationary at the original wavefront.
B. It is the limiting form of a spherical front with very large radius.
C. The frequency necessarily changes whenever the propagation direction changes.
D. Wavefronts are parallel to their associated rays.
A. Its normals are radii passing through the point source.
B. The frequency necessarily changes whenever the propagation direction changes.
C. Wavefronts are parallel to their associated rays.
D. Secondary wavelets remain stationary at the original wavefront.
A. The frequency necessarily changes whenever the propagation direction changes.
B. Wavefronts are parallel to their associated rays.
C. Secondary wavelets remain stationary at the original wavefront.
D. It is generated by an ideal long line source.
A. Wavefronts are parallel to their associated rays.
B. Secondary wavelets remain stationary at the original wavefront.
C. Huygens geometry gives i = r in the same medium.
D. The frequency necessarily changes whenever the propagation direction changes.
A. Secondary wavelets remain stationary at the original wavefront.
B. sin i/sin r = v₁/v₂.
C. The frequency necessarily changes whenever the propagation direction changes.
D. Wavefronts are parallel to their associated rays.
A. n₁ sin i = n₂ sin r.
B. The frequency necessarily changes whenever the propagation direction changes.
C. Wavefronts are parallel to their associated rays.
D. Secondary wavelets remain stationary at the original wavefront.
A. The frequency necessarily changes whenever the propagation direction changes.
B. Wavefronts are parallel to their associated rays.
C. Secondary wavelets remain stationary at the original wavefront.
D. Frequency remains constant because it is fixed by the source.
A. Wavefronts are parallel to their associated rays.
B. Secondary wavelets remain stationary at the original wavefront.
C. Wavelength changes in direct proportion to speed.
D. The frequency necessarily changes whenever the propagation direction changes.
A. Secondary wavelets remain stationary at the original wavefront.
B. It has larger refractive index and lower light speed.
C. The frequency necessarily changes whenever the propagation direction changes.
D. Wavefronts are parallel to their associated rays.
A. It is the common tangent in the forward propagation direction.
B. The frequency necessarily changes whenever the propagation direction changes.
C. Wavefronts are parallel to their associated rays.
D. Secondary wavelets remain stationary at the original wavefront.
A. The frequency necessarily changes whenever the propagation direction changes.
B. Wavefronts are parallel to their associated rays.
C. Secondary wavelets remain stationary at the original wavefront.
D. No directional bending occurs when i = 0.
A. Wavefronts are parallel to their associated rays.
B. Secondary wavelets remain stationary at the original wavefront.
C. For denser-to-rarer travel, r reaches 90° at the critical angle.
D. The frequency necessarily changes whenever the propagation direction changes.
A. Secondary wavelets remain stationary at the original wavefront.
B. Every point of a wavefront emits secondary wavelets; the forward envelope is the later wavefront.
C. The frequency necessarily changes whenever the propagation direction changes.
D. Wavefronts are parallel to their associated rays.
A. A secondary wavelet travels at the wave speed in that medium.
B. The frequency necessarily changes whenever the propagation direction changes.
C. Wavefronts are parallel to their associated rays.
D. Secondary wavelets remain stationary at the original wavefront.
A. The frequency necessarily changes whenever the propagation direction changes.
B. Wavefronts are parallel to their associated rays.
C. Secondary wavelets remain stationary at the original wavefront.
D. The local ray direction is perpendicular to the wavefront.
A. Wavefronts are parallel to their associated rays.
B. Secondary wavelets remain stationary at the original wavefront.
C. It is the limiting form of a spherical front with very large radius.
D. The frequency necessarily changes whenever the propagation direction changes.
A. Secondary wavelets remain stationary at the original wavefront.
B. Its normals are radii passing through the point source.
C. The frequency necessarily changes whenever the propagation direction changes.
D. Wavefronts are parallel to their associated rays.
A. It is generated by an ideal long line source.
B. The frequency necessarily changes whenever the propagation direction changes.
C. Wavefronts are parallel to their associated rays.
D. Secondary wavelets remain stationary at the original wavefront.
A. The frequency necessarily changes whenever the propagation direction changes.
B. Wavefronts are parallel to their associated rays.
C. Secondary wavelets remain stationary at the original wavefront.
D. Huygens geometry gives i = r in the same medium.
A. Wavefronts are parallel to their associated rays.
B. Secondary wavelets remain stationary at the original wavefront.
C. sin i/sin r = v₁/v₂.
D. The frequency necessarily changes whenever the propagation direction changes.
A. Secondary wavelets remain stationary at the original wavefront.
B. n₁ sin i = n₂ sin r.
C. The frequency necessarily changes whenever the propagation direction changes.
D. Wavefronts are parallel to their associated rays.
A. Frequency remains constant because it is fixed by the source.
B. The frequency necessarily changes whenever the propagation direction changes.
C. Wavefronts are parallel to their associated rays.
D. Secondary wavelets remain stationary at the original wavefront.
A. The frequency necessarily changes whenever the propagation direction changes.
B. Wavefronts are parallel to their associated rays.
C. Secondary wavelets remain stationary at the original wavefront.
D. Wavelength changes in direct proportion to speed.
A. Wavefronts are parallel to their associated rays.
B. Secondary wavelets remain stationary at the original wavefront.
C. It has larger refractive index and lower light speed.
D. The frequency necessarily changes whenever the propagation direction changes.
A. Secondary wavelets remain stationary at the original wavefront.
B. It is the common tangent in the forward propagation direction.
C. The frequency necessarily changes whenever the propagation direction changes.
D. Wavefronts are parallel to their associated rays.
A. No directional bending occurs when i = 0.
B. The frequency necessarily changes whenever the propagation direction changes.
C. Wavefronts are parallel to their associated rays.
D. Secondary wavelets remain stationary at the original wavefront.
A. The frequency necessarily changes whenever the propagation direction changes.
B. Wavefronts are parallel to their associated rays.
C. Secondary wavelets remain stationary at the original wavefront.
D. For denser-to-rarer travel, r reaches 90° at the critical angle.
Wavelet radius = vt
n = c/v
v = fλ
i = r
sin i/sin r = v₁/v₂ = n₂/n₁
n₁sin i = n₂sin r
Wavefront = constant phase. Rays are normals. New front = forward envelope. Frequency stays fixed at a boundary.
Label fronts, normals and interface. State equal-time distances. Identify right triangles. Write sine ratios. Substitute n = c/v.
Measuring angles from surface, changing frequency during refraction, reversing v and n ratios, or drawing rays parallel to wavefronts.
Distinguish optical from mass density. Track medium order in μ₂₁. Use wavefront angle carefully: angle between wavefronts equals angle between normals.
Secondary wavelets move at medium speed. Plane fronts are not tied to nearby point sources. Reflection does not change speed in the same medium.