Wave Speed
Wave speed depends on the medium. For periodic waves use v = fλ; for string waves use v = √(T/μ); for sound in fluid use v = √(B/ρ).
Class 11 Physics notes covering wave speed, wave velocity, principle of superposition, interference, resultant displacement, numericals and PYQs.
Wave speed depends on the medium. For periodic waves use v = fλ; for string waves use v = √(T/μ); for sound in fluid use v = √(B/ρ).
When waves overlap, add displacement at each point: y = y1 + y2. This is the foundation of interference, beats, standing waves and wave optics.
Same-phase waves produce constructive interference; opposite-phase waves produce destructive interference. Always check phase before adding amplitudes.
Wave speed and superposition form the bridge between simple wave description and real wave behaviour. Wave speed tells how fast the disturbance travels, while superposition tells what happens when two or more waves meet at the same place.
In coaching-class language, always keep three separate ideas in mind: the wave pattern travels with wave velocity, the medium particle vibrates with particle velocity, and when two disturbances overlap the actual displacement is the algebraic sum of individual displacements.
Real-life example: when two water ripples cross, each ripple continues after crossing, but during overlap the water level at every point is the sum of the two ripple displacements. That is superposition in front of your eyes.
Examination perspective: CBSE asks definitions and formulas, NEET checks quick use of v = fλ and interference conditions, while JEE often mixes signs, direction, phase and resultant amplitude.
Wave speed is the distance travelled by a wave disturbance per unit time. For any periodic wave, the most used formula is v = fλ. Here v is wave speed, f is frequency and λ is wavelength.
Physical meaning: in one time period T, a crest advances by one wavelength λ. Therefore v = λ/T = fλ. The source decides frequency, the medium decides speed, and wavelength adjusts according to v = fλ.
For a wave on a stretched string, v = √(T/μ). T is tension in the string and μ is mass per unit length. Greater tension makes the wave faster; greater linear density makes it slower.
For longitudinal waves in a fluid, v = √(B/ρ). B is bulk modulus and ρ is density. Greater elasticity increases speed, while greater density decreases speed.
Real-life example: a tight guitar string transmits waves faster and gives a higher pitch for a fixed length; a heavier string transmits waves more slowly.
Common mistake: saying wave speed depends on amplitude. In ordinary linear waves, amplitude changes energy, not wave speed.
Wave velocity is wave speed with direction. In one-dimensional wave motion along a string, positive wave velocity means the phase pattern moves in positive x-direction, and negative wave velocity means it moves in negative x-direction.
Mathematically, for y = A sin(ωt − kx), constant phase gives x increasing with t, so the wave travels in positive x-direction with speed v = ω/k.
Particle velocity is different. Particle velocity is dy/dt, the speed of a point of the medium. Wave velocity is the speed of the crest, compression or phase.
Real-life example: a stadium wave travels around the stadium, but each person only stands and sits locally. The wave velocity is around the stadium; the particle velocity is each person's up-down motion.
JEE conceptual trap: maximum particle velocity can be Aω, but wave velocity is ω/k. They can have different values and different directions.
The principle of superposition states that when two or more waves overlap in a medium, the resultant displacement of any particle is equal to the algebraic sum of the displacements produced by individual waves at that point.
Mathematical meaning: y = y1 + y2. If one wave displaces a particle upward by 3 mm and another displaces it downward by 1 mm, resultant displacement is 2 mm upward.
Physical meaning: each wave produces its own displacement, and the medium particle shows the combined effect. After crossing, waves continue almost unchanged in a linear medium.
Vector and algebraic addition: displacement is directional. Upward displacement may be taken positive and downward negative. For waves along the same line, add signs carefully.
Real-life example: two pulses on a rope overlap. If both are upward, the rope rises more; if one is upward and one downward, the rope may partly or completely cancel.
Interference is the sustained effect produced by superposition of two coherent waves. In basic Class 11 wave study, we focus on constructive and destructive interference.
Constructive interference occurs when waves meet in the same phase. Resultant amplitude is maximum: A = A1 + A2.
Destructive interference occurs when waves meet in opposite phase. Resultant amplitude is minimum: A = |A1 − A2|. If A1 = A2, complete cancellation occurs.
Real-life example: noise-cancelling headphones produce a sound wave nearly opposite in phase to external noise, reducing resultant sound reaching the ear.
Conceptual trap: destructive interference does not destroy energy in the universe; energy redistributes in space or transforms depending on the system.
Resultant displacement is the actual displacement of a particle when multiple waves act at the same point. It is calculated point by point and instant by instant.
If y1 = A1 sin(ωt − kx) and y2 = A2 sin(ωt − kx), then the resultant can have amplitude A1 + A2 when waves are in phase.
Amplitude changes during superposition because displacements add. Energy depends on amplitude squared, so changing amplitude changes local energy distribution.
Real-life example: in a concert hall, sound may be loud at some seats and weak at others because waves from speakers interfere differently at different points.
Common mistake: adding intensities or amplitudes without checking phase. In wave displacement questions, first add displacement functions.
Noise cancellation uses destructive interference. A microphone detects external noise and electronics generate an opposite-phase wave, reducing the resultant displacement of air near the ear.
Sound systems use superposition in speaker arrays. Correct spacing and phase make sound stronger in desired regions and weaker in unwanted regions.
Music depends on superposition of harmonics. A violin, flute and guitar may play the same fundamental frequency, but different harmonic mixtures give different quality or timbre.
Wave engineering uses interference and superposition in vibration control, bridges, buildings, ultrasound, seismology and antenna design.
Radio communication and signal transmission use superposition when multiple signals share space. Receivers select the required frequency and filter out unwanted components.
Echo and reflection problems use wave speed and time delay. If sound travels to a wall and returns, distance to wall is vt/2, not vt.
v = fλv is wave speed, f is frequency and λ is wavelength. Use this whenever frequency and wavelength are given.
v = √(T/μ)T is tension and μ is linear mass density. More tension increases speed; more mass per metre decreases speed.
v = √(B/ρ)B is bulk modulus and ρ is density. Elastic medium transmits faster; denser medium resists motion.
y = y1 + y2Add displacement functions algebraically with signs. Do not add only magnitudes.
A = A1 + A2Used when phase difference is 0, 2π, 4π and so on.
A = |A1 − A2|Used when phase difference is π, 3π, 5π and so on.
These SVG diagrams use black wave lines, red labels and red arrows in a clean board-work style.
If Wave Speed, Superposition or Interference is not clear and you are looking for a Physics Tutor, contact Kumar Sir.
This bank is intentionally curated to avoid data-only duplicate questions. It includes NEET, JEE Main and JEE Advanced style numericals across wave speed, string tension, density, elasticity, echo, sonar, graph reading, phase/path difference, constructive interference, destructive interference, resultant displacement, energy ratio and conceptual superposition.
Given: f = 5 Hz, λ = 0.12 m
Formula: v = fλ
Solution: v = 5 × 0.12 = 0.60 m s−1
Final Answer: 0.60 m s−1
Given: v = 340 m s−1, λ = 0.85 m
Formula: f = v/λ
Solution: f = 340/0.85 = 400 Hz
Final Answer: 400 Hz
Given: v = 1.8 m s−1, f = 3 Hz
Formula: λ = v/f
Solution: λ = 1.8/3 = 0.60 m
Final Answer: 0.60 m
Given: T = 0.04 s, λ = 2 m
Formula: v = λ/T
Solution: v = 2/0.04 = 50 m s−1
Final Answer: 50 m s−1
Given: t = 1.2 s, v = 340 m s−1
Formula: d = vt/2
Solution: d = 340 × 1.2/2 = 204 m
Final Answer: 204 m
Given: t = 0.08 s, v = 1500 m s−1
Formula: depth = vt/2
Solution: depth = 1500 × 0.08/2 = 60 m
Final Answer: 60 m
Given: T = 25 N, μ = 0.01 kg m−1
Formula: v = √(T/μ)
Solution: v = √(25/0.01) = 50 m s−1
Final Answer: 50 m s−1
Given: y1 = +3 mm, y2 = +5 mm
Formula: y = y1 + y2
Solution: y = 3 + 5 = 8 mm
Final Answer: 8 mm upward
Given: y1 = +6 mm, y2 = −2 mm
Formula: y = y1 + y2
Solution: y = 6 − 2 = 4 mm
Final Answer: 4 mm upward
Given: A1 = 4 cm, A2 = 4 cm, opposite phase
Formula: A = |A1 − A2|
Solution: A = |4 − 4| = 0
Final Answer: 0 cm
Given: v = 40 m s−1, T' = 4T
Formula: v ∝ √T
Solution: v' = 40 × √4 = 80 m s−1
Final Answer: 80 m s−1
Given: v = 60 m s−1, μ' = 9μ
Formula: v ∝ 1/√μ
Solution: v' = 60/3 = 20 m s−1
Final Answer: 20 m s−1
Given: B = 2.25 × 109 Pa, ρ = 1000 kg m−3
Formula: v = √(B/ρ)
Solution: v = √(2.25 × 106) = 1500 m s−1
Final Answer: 1500 m s−1
Given: vA = 300 m s−1, λB = 1.5λA
Formula: v = fλ
Solution: vB = 1.5vA = 450 m s−1
Final Answer: 450 m s−1
Given: λ = 0.75 m, f = 12/3 = 4 Hz
Formula: v = fλ
Solution: v = 4 × 0.75 = 3 m s−1
Final Answer: 3 m s−1
Given: f = 500 Hz, v = 1500 m s−1
Formula: λ = v/f
Solution: λ = 1500/500 = 3 m
Final Answer: 3 m
Given: A1 = 7 cm, A2 = 2 cm
Formula: A = A1 + A2
Solution: A = 7 + 2 = 9 cm
Final Answer: 9 cm
Given: A1 = 7 cm, A2 = 2 cm
Formula: A = |A1 − A2|
Solution: A = |7 − 2| = 5 cm
Final Answer: 5 cm
Given: Δx = 3λ
Formula: Constructive when Δx = nλ
Solution: 3λ is an integral multiple of λ, so interference is constructive.
Final Answer: Constructive interference
Given: Δx = 5λ/2
Formula: Destructive when Δx = (n + 1/2)λ
Solution: 5λ/2 = 2.5λ, a half-integral multiple; destructive.
Final Answer: Destructive interference
Given: y1 = 4 sinθ, y2 = 4 sinθ
Formula: y = y1 + y2
Solution: y = 8 sinθ
Final Answer: 8 sinθ
Given: y1 = 5 sinθ, y2 = −2 sinθ
Formula: y = y1 + y2
Solution: y = 3 sinθ
Final Answer: 3 sinθ
Given: A' = 2A
Formula: Energy ∝ A2
Solution: E'/E = (2A/A)2 = 4
Final Answer: 4 times
Given: Anoise = Acancel, phase difference = π
Formula: A = |A1 − A2|
Solution: A = 0
Final Answer: Zero resultant amplitude ideally
Given: s = 24 m, t = 0.6 s
Formula: v = s/t
Solution: v = 24/0.6 = 40 m s−1; distance in 2 s = 80 m
Final Answer: 40 m s−1, 80 m
Given: f = 10/5 = 2 Hz; distance from first to third crest = 2λ = 4 m
Formula: λ = 2 m, v = fλ
Solution: v = 2 × 2 = 4 m s−1
Final Answer: 4 m s−1
Given: v = 100 m s−1, T = 40 N
Formula: v = √(T/μ), so μ = T/v2
Solution: μ = 40/10000 = 0.004 kg m−1
Final Answer: 0.004 kg m−1
Given: v = 80 m s−1, μ = 0.02 kg m−1
Formula: T = μv2
Solution: T = 0.02 × 802 = 128 N
Final Answer: 128 N
Given: v = 1200 m s−1, ρ = 900 kg m−3
Formula: B = ρv2
Solution: B = 900 × 12002 = 1.296 × 109 Pa
Final Answer: 1.296 × 109 Pa
Given: A1 = 6 cm, A2 = 8 cm
Formula: Amax = A1 + A2, Amin = |A1 − A2|
Solution: Amax = 14 cm; Amin = 2 cm
Final Answer: 14 cm and 2 cm
Given: Equation y = A sin(ωt − kx)
Formula: v = ω/k
Solution: Wave velocity is phase speed, so v = ω/k.
Final Answer: ω/k
Given: ω = 80 rad s−1, k = 4 rad m−1
Formula: v = ω/k
Solution: v = 80/4 = 20 m s−1
Final Answer: 20 m s−1
Given: ω = 50, k = 2
Formula: f = ω/2π, λ = 2π/k
Solution: f = 25/π Hz; λ = π m
Final Answer: 25/π Hz, π m
Given: One oscillation time = T; crest advances one λ in T
Formula: distance in one T = λ
Solution: λ = 6 m
Final Answer: 6 m
Given: T' = 1.21T
Formula: v ∝ √T
Solution: v'/v = √1.21 = 1.1, so increase = 10%
Final Answer: 10%
Given: μ' = 0.64μ
Formula: v ∝ 1/√μ
Solution: v'/v = 1/√0.64 = 1/0.8 = 1.25
Final Answer: 1.25
Given: m = 0.04 kg, L = 2 m, T = 100 N
Formula: μ = m/L, v = √(T/μ)
Solution: μ = 0.02 kg m−1; v = √(100/0.02) = 70.71 m s−1
Final Answer: 70.71 m s−1
Given: μ = 0.05, v = 30
Formula: T = μv2
Solution: T = 0.05 × 900 = 45 N
Final Answer: 45 N
Given: μ1:μ2 = 1:4
Formula: v ∝ 1/√μ
Solution: v1:v2 = √4:√1 = 2:1
Final Answer: 2:1
Given: T1:T2 = 9:16
Formula: v ∝ √T
Solution: v1:v2 = 3:4
Final Answer: 3:4
Given: λ = 0.4 m, T = 0.02 s
Formula: v = λ/T
Solution: v = 0.4/0.02 = 20 m s−1
Final Answer: 20 m s−1
Given: T = 5 ms = 0.005 s, λ = 1.5 m
Formula: v = λ/T
Solution: v = 1.5/0.005 = 300 m s−1
Final Answer: 300 m s−1
Given: t = 0.03 s, v = 340 m s−1
Formula: d = vt/2
Solution: d = 340 × 0.03/2 = 5.1 m
Final Answer: 5.1 m
Given: t = 0.4 s, v = 1500 m s−1
Formula: d = vt/2
Solution: d = 1500 × 0.4/2 = 300 m
Final Answer: 300 m
Given: A1 = 10, A2 = 6
Formula: A ranges from |A1 − A2| to A1 + A2
Solution: Minimum = 4, maximum = 16
Final Answer: 4 to 16 units
Given: A1 = 5 cm, A2 = 12 cm
Formula: Allowed range: |A1 − A2| to A1 + A2
Solution: Range is 7 cm to 17 cm. 3 cm is not possible.
Final Answer: No
Given: A1 = A2 = 4 cm, Δφ = 2π
Formula: Constructive: A = A1 + A2
Solution: A = 8 cm
Final Answer: 8 cm
Given: A1 = A2 = 4 cm, Δφ = π
Formula: Destructive: A = |A1 − A2|
Solution: A = 0
Final Answer: 0
Given: Δx = 7λ/2 = 3.5λ
Formula: Half-integral multiple gives destructive interference
Solution: 3.5λ is half-integral, so destructive.
Final Answer: Destructive
Given: Δx = 6λ
Formula: Integral multiple gives constructive interference
Solution: 6λ is integral multiple, so constructive.
Final Answer: Constructive
Given: 3 cm, −4 cm, 2 cm
Formula: y = y1 + y2 + y3
Solution: y = 3 − 4 + 2 = 1 cm
Final Answer: 1 cm
Given: Equal perpendicular phase components
Formula: R = √(22 + 22)
Solution: R = 2√2
Final Answer: 2√2
Given: Components 3 and 4 in quadrature
Formula: R = √(32 + 42)
Solution: R = 5
Final Answer: 5
Given: B' = 4B, ρ unchanged
Formula: v ∝ √B
Solution: v'/v = 2
Final Answer: 2
Given: ρ' = 4ρ, B unchanged
Formula: v ∝ 1/√ρ
Solution: v'/v = 1/2
Final Answer: 1/2
Given: v = 60, f = 120
Formula: λ = v/f
Solution: λ = 60/120 = 0.5 m
Final Answer: 0.5 m
Given: λ = 0.5 m
Formula: Opposite phase separation = λ/2
Solution: distance = 0.25 m
Final Answer: 0.25 m
Given: Δx = 0.75 m, λ = 0.5 m
Formula: Δx/λ = 1.5
Solution: 1.5λ is half-integral, so destructive.
Final Answer: Destructive
Given: Δx = 1.0 m, λ = 0.5 m
Formula: Δx/λ = 2
Solution: 2λ is integral, so constructive.
Final Answer: Constructive
Given: Frequency fixed by source, speed changes due to tension
Formula: v = fλ
Solution: Since f is fixed and v changes, wavelength adjusts.
Final Answer: Wavelength
Given: Equal amplitudes, phase difference π
Formula: sin(θ + π) = −sinθ
Solution: y = A sinθ − A sinθ = 0
Final Answer: 0
Given: Phase difference 2π
Formula: Same phase
Solution: AR = A + A = 2A
Final Answer: 2A
Given: A1 = A, A2 = 2A
Formula: AR = |A1 − A2|
Solution: AR = A
Final Answer: A
Given: AR = 3A
Formula: I ∝ A2
Solution: IR/I1 = (3A/A)2 = 9
Final Answer: 9
Given: A = 3 cm each, same phase
Formula: AR = A1 + A2
Solution: AR = 6 cm
Final Answer: 6 cm
Given: +5 cm and −3 cm
Formula: y = y1 + y2
Solution: y = 5 − 3 = 2 cm
Final Answer: +2 cm
Given: A1 = 9 cm, A2 = 4 cm opposite
Formula: A = |A1 − A2|
Solution: A = 5 cm in direction of larger pulse
Final Answer: 5 cm
Given: L = 5 m, m = 0.10 kg, T = 80 N
Formula: μ = m/L, v = √(T/μ)
Solution: μ = 0.02; v = √(80/0.02) = √4000 = 63.25 m s−1
Final Answer: 63.25 m s−1
Given: T changes by factor 4
Formula: v ∝ √T
Solution: v' = 30 × 2 = 60 m s−1
Final Answer: 60 m s−1
Given: μ' = μ/4
Formula: v ∝ 1/√μ
Solution: v' = 40 × 2 = 80 m s−1
Final Answer: 80 m s−1
Given: ρ = 1.2, v = 330
Formula: B = ρv2
Solution: B = 1.2 × 3302 = 130680 Pa
Final Answer: 1.31 × 105 Pa
Given: B1:B2 = 16:25
Formula: v ∝ √B
Solution: v1:v2 = 4:5
Final Answer: 4:5
Given: ρ1:ρ2 = 9:4
Formula: v ∝ 1/√ρ
Solution: v1:v2 = 1/3 : 1/2 = 2:3
Final Answer: 2:3
Given: A, A, φ = π/3
Formula: R = 2A cos(φ/2)
Solution: R = 2A cos(π/6) = √3 A
Final Answer: √3 A
Given: A, A, φ = 2π/3
Formula: R = 2A cos(φ/2)
Solution: R = 2A cos(π/3) = A
Final Answer: A
Given: R = √2 A
Formula: R = 2A cos(φ/2)
Solution: cos(φ/2) = 1/√2, so φ/2 = π/4
Final Answer: φ = π/2
Given: A1 = 3A, A2 = 4A, φ = π/2
Formula: R = √(A12 + A22)
Solution: R = √(9A2 + 16A2) = 5A
Final Answer: 5A
Given: A = 5 cm, φ = 120°
Formula: R = 2A cos(φ/2)
Solution: R = 10 cos60° = 5 cm
Final Answer: 5 cm
Given: Δx = 1.2 m, λ = 0.8 m
Formula: Δx/λ = 1.5
Solution: Half-integral multiple, so destructive.
Final Answer: Destructive
Given: Destructive: Δx = λ/2
Formula: Δx = 0.6/2
Solution: Δx = 0.3 m
Final Answer: 0.3 m
Given: Constructive: Δx = λ
Formula: Δx = 0.6 m
Solution: smallest non-zero = 0.6 m
Final Answer: 0.6 m
Given: AR = 2A
Formula: E ∝ A2
Solution: ER/E = (2A/A)2 = 4
Final Answer: 4 times one wave
Given: Equal amplitudes, opposite phase
Formula: y = y1 + y2
Solution: They cancel at that point, so y = 0.
Final Answer: 0
Given: +2A, −3A, +5A
Formula: y = sum of displacements
Solution: y = 2A − 3A + 5A = 4A
Final Answer: 4A
Given: Linear medium
Formula: Principle of superposition
Solution: They regain their original shapes and continue moving.
Final Answer: They pass through unchanged ideally
Given: Relative speed = 10 + 15 = 25 m s−1
Formula: t = separation/relative speed
Solution: t = 5/25 = 0.2 s
Final Answer: 0.2 s
Given: Total width = 0.5 m, relative speed = 10
Formula: time = total width/relative speed
Solution: t = 0.5/10 = 0.05 s
Final Answer: 0.05 s
Given: v = 340, f = 100, Δx = 1.7 m
Formula: λ = v/f
Solution: λ = 3.4 m; Δx = λ/2, so destructive.
Final Answer: Destructive
Given: λ = 3.4 m, Δx = 3.4 m
Formula: Constructive when Δx = nλ
Solution: Path difference is one wavelength, so constructive.
Final Answer: Constructive
Given: v = 120, f = 60
Formula: λ = v/f
Solution: λ = 2 m; same phase = 2 m, opposite phase = 1 m
Final Answer: 2 m and 1 m
Given: First minimum: Δx = λ/2
Formula: λ = 2Δx
Solution: λ = 0.90 m
Final Answer: 0.90 m
Given: First non-zero constructive: Δx = λ
Formula: λ = 0.75 m
Solution: 0.75 m
Final Answer: 0.75 m
Given: Amax = 14, Amin = 2
Formula: A1 + A2 = 14; A1 − A2 = 2
Solution: Solving gives A1 = 8 cm and A2 = 6 cm
Final Answer: 8 cm and 6 cm
Questions cover CBSE, NEET, JEE Main, JEE Advanced, IB, ICSE, IGCSE, A-Level, assertion-reason, true-false, case-study, reasoning and conceptual practice.
Wave speed is distance travelled by wave per unit time. SI unit is m s−1.
v = fλ.
When waves overlap, resultant displacement is algebraic sum of individual displacements.
Actual displacement of a particle due to overlapping waves.
Interference in which waves meet in same phase and amplitude becomes maximum.
Interference in which waves meet in opposite phase and amplitude becomes minimum.
v = fλ = 200 m s−1.
Wavelength becomes half.
Zero.
7 cm.
4 cm.
No.
v = √(T/μ).
Speed becomes two times.
Speed becomes half.
v = √(B/ρ).
Particle velocity is dy/dt of medium particle; wave velocity is speed of phase propagation.
y = −3 mm.
Displacement has sign/direction, so upward and downward displacements must be added with signs.
Phase difference 2nπ or path difference nλ.
Phase difference (2n + 1)π or path difference (n + 1/2)λ.
A1 + A2.
|A1 − A2|.
Yes, in a linear medium they emerge practically unchanged.
One complete wavelength passes a point every time period, giving speed equal to frequency times wavelength.
Sound travels to the reflector and back, so total distance is twice wall distance.
It produces an opposite-phase sound wave to reduce resultant displacement.
Constructive interference and room reflections can increase resultant amplitude.
Constructive interference; amplitude increases.
Complete destructive interference.
kg m−1.
Elasticity of a medium under compression.
Faster.
Slower.
Displacements are added point by point.
No, energy is redistributed.
Δφ = 2nπ.
Δφ = (2n + 1)π.
Interference of waves with constant phase difference and same frequency.
Intensity depends on amplitude squared and phase relation.
Both are true and the reason correctly explains the assertion.
Assertion is false; reason is true.
Both are true and the reason correctly explains the assertion.
Assertion is false; reason is true.
False.
True.
True.
True.
Distance = vt/2 = 340 × 2/2 = 340 m.
Constructive interference occurs.
Destructive interference.
Wave speed increases.
Because displacement can be upward/positive or downward/negative.
In a linear medium, each wave obeys the same equation and superposes temporarily.
No, cancellation may occur at specific points or instants depending on phase and amplitudes.
It relates wave variables; v = √(T/μ) shows medium dependence for strings.
Adding magnitudes even when one displacement is negative.
Greater inertia resists rapid motion, lowering speed when elasticity is unchanged.
A student shouts near a cliff and hears the echo after 1.5 s. Take speed of sound as 340 m s−1.
Because sound travels to the cliff and returns.
d = 340 × 1.5 / 2 = 255 m.
Wave speed and reflection of sound.
A headphone detects external noise and sends an opposite-phase sound into the ear.
Destructive interference.
Displacements of pressure waves.
No, the wave field and energy distribution are changed by the device.
Two identical loudspeakers play the same tone in phase.
At points where waves arrive in phase.
Destructive interference occurs.
v = fλ.
A string instrument is tuned by changing tension.
Speed increases.
v = √(T/μ).
Mass per unit length of the string.
A signal wave travels along a stretched cable.
Linear mass density.
Wave speed decreases.
Overlapping signals can interfere depending on phase.
If Wave Speed, Superposition or Interference is not clear and you are looking for a Physics Tutor, contact Kumar Sir.