Shape Parameters
Amplitude A and wavelength λ describe the visible shape of a sinusoidal wave on a y-x graph. A is vertical maximum displacement; λ is horizontal repeat distance.
Class 11 Physics notes covering amplitude, time period, frequency, angular frequency, wavelength, wave number, phase, wave equation, wave velocity, numericals and PYQs.
Amplitude A and wavelength λ describe the visible shape of a sinusoidal wave on a y-x graph. A is vertical maximum displacement; λ is horizontal repeat distance.
Time period T, frequency f and angular frequency ω describe how fast a particle oscillates at a fixed point. The key links are f = 1/T and ω = 2πf.
Wave number k, phase and wave velocity v connect the graph to motion. The key exam equation is y = A sin(ωt − kx).
Amplitude is the maximum displacement of a vibrating particle from its mean position. In y = A sin(ωt − kx), A is the amplitude.
Physical meaning: amplitude measures how far the particle moves from equilibrium, not how far the wave travels. In a rope wave, a larger hand movement produces a larger amplitude.
Real-life example: when a guitar string is plucked strongly, its amplitude is larger and the sound is louder. If it is plucked gently, amplitude is smaller.
Exam perspective: amplitude affects energy and intensity, but it does not change frequency, wavelength or wave speed in a given linear medium.
Common trap: amplitude is not the distance between crest and trough. Crest-to-trough distance is 2A.
Time period is the time taken by one particle of the medium to complete one full oscillation. It is also the time between two successive crests passing a fixed point.
Formula: T = 1/f. Unit of T is second.
Real-life example: if a water surface at one point goes up, comes down and returns to the same state in 0.5 s, the time period is 0.5 s.
Exam perspective: in a y-t graph, the horizontal distance between two consecutive crests gives T.
Common trap: T is a time interval, not a distance. Do not confuse it with wavelength.
Frequency is the number of complete oscillations performed by a particle in one second. It is also the number of complete waves crossing a fixed point per second.
Formula: f = 1/T. Unit is hertz, written Hz or s−1.
Real-life example: a 256 Hz tuning fork makes each nearby air particle complete 256 oscillations every second.
Exam perspective: frequency is decided by the source. When a wave goes from one medium to another, frequency remains unchanged.
Common trap: students often think frequency changes because speed changes. In refraction or medium change, wavelength changes, frequency remains the same.
Angular frequency is the rate of change of phase with time. It tells how many radians of phase are covered per second.
Formula: ω = 2πf = 2π/T. Unit is rad s−1.
Real-life example: if a rotating reference circle completes f rotations per second, its angular speed is 2πf rad s−1; SHM and wave equations use the same idea.
In y = A sin(ωt − kx), ω is the coefficient of t.
Common trap: angular frequency is not frequency. Frequency counts cycles per second; angular frequency counts radians per second.
Wavelength is the distance between two nearest particles vibrating in the same phase. For a transverse wave it is crest-to-crest or trough-to-trough distance; for sound it is compression-to-compression distance.
Formula: v = fλ, so λ = v/f. Unit is metre.
Real-life example: in water ripples, the distance between two neighbouring bright crest lines is the wavelength.
Exam perspective: in a y-x graph, the horizontal distance between two consecutive crests gives wavelength.
Common trap: wavelength is measured along the direction of propagation, not vertically.
Wave number is the phase change per unit distance. It tells how rapidly the wave phase changes as we move along x.
Formula: k = 2π/λ. Unit is rad m−1.
In y = A sin(ωt − kx), k is the coefficient of x.
Real-life example: closely spaced ripples have small wavelength and therefore large wave number.
Common trap: ordinary spatial frequency is 1/λ, but angular wave number is 2π/λ.
Phase describes the state of oscillation of a particle at a given position and time. It tells whether the particle is at mean position, crest, trough, moving upward, or moving downward.
For y = A sin(ωt − kx), phase is φ = ωt − kx.
Two particles are in the same phase when their phase difference is 0, 2π, 4π and so on. They are in opposite phase when phase difference is π, 3π and so on.
Real-life example: two points on a rope separated by one wavelength rise and fall together, so they are in the same phase.
Common trap: same displacement does not always mean same phase. One particle may be moving upward while the other is moving downward.
Wave velocity is the speed with which a particular phase, crest, compression, pulse or wave pattern travels through the medium.
Formula: v = fλ = ω/k. Unit is m s−1.
Real-life example: sound wave velocity in air is about 340 m s−1, while individual air molecules only vibrate locally.
Exam perspective: wave velocity depends on medium properties, not on amplitude in ordinary linear waves.
Common trap: wave velocity is not particle velocity. Wave velocity is pattern speed; particle velocity is dy/dt.
The displacement of a sinusoidal progressive wave travelling along positive x-direction can be written as y = A sin((2π/λ)(vt − x)).
Using ω = 2πf, v = fλ and k = 2π/λ, the same equation becomes y = A sin(ωt − kx).
Symbols: y is displacement of the particle, A is amplitude, ω is angular frequency, t is time, k is wave number, x is position, λ is wavelength and v is wave velocity.
For y = A sin(ωt − kx), the wave travels in positive x-direction. For y = A sin(ωt + kx), the wave travels in negative x-direction. Forms containing vt − x are equivalent to positive x-direction, while forms containing x − vt may differ only by an overall sign depending on sine convention; always reduce the phase and check whether x increases or decreases with time for constant phase.
dy/dt = Aω cos(ωt − kx)Particle velocity is the velocity of the medium particle at a fixed x. It changes with time and can be positive, negative or zero.
vp,max = AωThe maximum value of cos(ωt − kx) is 1, so maximum particle velocity is Aω.
dy/dx = −Ak cos(ωt − kx)dy/dx is the slope of the wave profile at a given instant. It is not particle velocity.
d2y/dt2 = −Aω2 sin(ωt − kx)Since y = A sin(ωt − kx), acceleration becomes a = −ω2y.
v = fλ = ω/kWave velocity is the speed of the wave pattern or phase. It is not dy/dt.
ωt − kx: +x
ωt + kx: −xKeep phase constant and see whether x increases or decreases as t increases.
| Point | Particle Velocity | Wave Velocity |
|---|---|---|
| Meaning | Velocity of an individual oscillating particle of the medium. | Velocity of propagation of the wave pattern, crest, compression or phase. |
| Formula | vp = dy/dt | v = fλ = ω/k |
| Direction | Along the direction of particle vibration. | Along the direction of wave propagation. |
| Value | Changes continuously with time; maximum is Aω. | Constant for a given wave in a uniform medium. |
| Example | A point on a rope moves up and down. | The crest on the rope moves horizontally. |
All diagrams use black graph lines and red arrows/labels so they match board-work and NCERT-style wave drawings.
If Wave Parameters or Wave Equation is not clear and you are looking for a Physics Tutor, contact Kumar Sir.
These numericals cover wave velocity, frequency, wavelength, wave number, angular frequency, particle velocity, acceleration, phase difference, direction of propagation and equation comparison.
Given: f = 50 Hz, λ = 4 m
Formula: v = fλ
Solution: v = 50 × 4 = 200 m s−1
Final Answer: 200 m s−1
Given: T = 0.02 s
Formula: f = 1/T
Solution: f = 1/0.02 = 50 Hz
Final Answer: 50 Hz
Given: v = 340 m s−1, λ = 2 m
Formula: f = v/λ
Solution: f = 340/2 = 170 Hz
Final Answer: 170 Hz
Given: f = 10 Hz
Formula: ω = 2πf
Solution: ω = 20π rad s−1
Final Answer: 20π rad s−1
Given: λ = 0.5 m
Formula: k = 2π/λ
Solution: k = 2π/0.5 = 4π rad m−1
Final Answer: 4π rad m−1
Given: Equation: y = 0.04 sin(100t − 5x)
Formula: A is coefficient before sine
Solution: A = 0.04 m
Final Answer: 0.04 m
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: Equation has coefficient of t = 20
Formula: ω is coefficient of t
Solution: ω = 20 rad s−1
Final Answer: 20 rad s−1
Given: Equation has coefficient of x = 8
Formula: k is coefficient of x
Solution: k = 8 rad m−1
Final Answer: 8 rad m−1
Given: ω = 60 rad s−1
Formula: f = ω/2π
Solution: f = 60/2π = 30/π Hz
Final Answer: 30/π Hz
Given: k = 3 rad m−1
Formula: λ = 2π/k
Solution: λ = 2π/3 m
Final Answer: 2π/3 m
Given: A = 0.02 m, ω = 100 rad s−1
Formula: vp,max = Aω
Solution: vp,max = 0.02 × 100 = 2 m s−1
Final Answer: 2 m s−1
Given: A = 0.05 m, ω = 200 rad s−1
Formula: vp,max = Aω
Solution: vp,max = 0.05 × 200 = 10 m s−1
Final Answer: 10 m s−1
Given: The phase is ωt − kx
Formula: Constant phase gives x = (ω/k)t − constant/k
Solution: x increases with t, so wave travels in positive x-direction.
Final Answer: Positive x-direction
Given: The phase is ωt + kx
Formula: Constant phase gives x = constant/k − (ω/k)t
Solution: x decreases with t, so wave travels in negative x-direction.
Final Answer: Negative x-direction
Given: T = 0.01 s, λ = 3 m
Formula: v = λ/T
Solution: v = 3/0.01 = 300 m s−1
Final Answer: 300 m s−1
Given: N = 120, t = 4 s
Formula: f = N/t, T = 1/f
Solution: f = 120/4 = 30 Hz; T = 1/30 s
Final Answer: 30 Hz, 1/30 s
Given: Separation = λ/4
Formula: Δφ = 2πΔx/λ
Solution: Δφ = 2π(λ/4)/λ = π/2
Final Answer: π/2 rad
Given: Δx = 0.25 m, λ = 1 m
Formula: Δφ = 2πΔx/λ
Solution: Δφ = 2π × 0.25 = π/2
Final Answer: π/2 rad
Given: k = 6, ω = 300
Formula: v = ω/k
Solution: v = 300/6 = 50 m s−1
Final Answer: 50 m s−1
Given: Compare with y = A sin 2π(ft − x/λ)
Formula: f is coefficient of t inside 2π
Solution: f = 50 Hz
Final Answer: 50 Hz
Given: Compare with y = A sin 2π(ft − x/λ)
Formula: x/λ = x/4
Solution: λ = 4 m
Final Answer: 4 m
Given: f = 50 Hz, λ = 4 m
Formula: v = fλ
Solution: v = 50 × 4 = 200 m s−1
Final Answer: 200 m s−1
Given: A = 0.01, ω = 100, k = 2
Formula: vp,max/v = Aω/(ω/k) = Ak
Solution: Ratio = 0.01 × 2 = 0.02
Final Answer: 0.02
Given: A = 0.04 m, ω = 50 rad s−1
Formula: amax = Aω2
Solution: amax = 0.04 × 502 = 100 m s−2
Final Answer: 100 m s−2
Given: T = 0.2 s
Formula: f = 1/T
Solution: f = 1/0.2 = 5 Hz
Final Answer: 5 Hz
Given: λ = 0.8 m
Formula: k = 2π/λ
Solution: k = 2π/0.8 = 2.5π rad m−1
Final Answer: 2.5π rad m−1
Given: Same medium means v constant; f becomes 2f
Formula: v = fλ
Solution: λ becomes λ/2
Final Answer: Wavelength becomes half
Given: Phase can be written 0.5πx − 100πt = −(100πt − 0.5πx)
Formula: Speed = ω/k = 100π/0.5π
Solution: v = 200 m s−1; form kx − ωt also travels positive x.
Final Answer: 200 m s−1, positive x-direction
Given: k = 5, ω = 100, plus sign
Formula: v = ω/k; plus sign gives negative x-direction
Solution: v = 100/5 = 20 m s−1
Final Answer: 20 m s−1, negative x-direction
Given: y = A sin(ωt − kx)
Formula: vp = dy/dt
Solution: vp = Aω cos(ωt − kx)
Final Answer: Aω cos(ωt − kx)
Given: y = A sin(ωt − kx)
Formula: a = d2y/dt2
Solution: a = −Aω2 sin(ωt − kx) = −ω2y
Final Answer: −ω2y
Given: y = A sin(ωt − kx)
Formula: dy/dx = derivative with respect to x
Solution: dy/dx = −Ak cos(ωt − kx)
Final Answer: −Ak cos(ωt − kx)
Given: A = 2 cm = 0.02 m, f = 5 Hz
Formula: vp,max = Aω = A(2πf)
Solution: vp,max = 0.02 × 10π = 0.2π m s−1
Final Answer: 0.2π m s−1
Given: λ = 0.4 m, T = 0.02 s
Formula: ω = 2π/T, k = 2π/λ, v = λ/T
Solution: ω = 100π rad s−1; k = 5π rad m−1; v = 20 m s−1
Final Answer: ω = 100π, k = 5π, v = 20 m s−1
Given: distance = 600 m, time = 2 s, f = 100 Hz
Formula: v = s/t, λ = v/f
Solution: v = 300 m s−1; λ = 300/100 = 3 m
Final Answer: 3 m
Given: λ = 1.5 m, f = 20 Hz
Formula: v = fλ
Solution: v = 20 × 1.5 = 30 m s−1
Final Answer: 30 m s−1
Given: Δx = 0.3 m, Δφ = 3π/2
Formula: Δφ = 2πΔx/λ
Solution: λ = 2π × 0.3 /(3π/2) = 0.4 m
Final Answer: 0.4 m
Given: ω = 314, k = 3.14
Formula: f = ω/2π, λ = 2π/k, v = ω/k
Solution: f = 50 Hz; λ = 2 m; v = 100 m s−1
Final Answer: 50 Hz, 2 m, 100 m s−1
Given: vp,max/v = Aω/(ω/k) = Ak = 2πA/λ
Formula: 5/100 = 2πA/λ
Solution: A/λ = 1/(40&pi)
Final Answer: A/λ = 1/(40π)
Given: A = 0.01 m, f = 100 Hz
Formula: ω = 2πf, vp,max = Aω
Solution: vp,max = 0.01 × 200π = 2π m s−1
Final Answer: 2π m s−1
This bank includes CBSE, NEET, JEE Main, JEE Advanced, IB, ICSE, IGCSE, A-Level, assertion-reason, true-false, case-study, reasoning and difficult conceptual questions.
Amplitude is maximum displacement of a particle from its mean position.
Time period is time for one oscillation; frequency is number of oscillations per second.
f = 1/T.
v = fλ.
Distance between two consecutive crests or troughs.
Distance between two consecutive compressions or rarefactions.
Angular frequency is rate of change of phase with time, ω = 2πf.
Wave number is phase change per unit length, k = 2π/λ.
A is amplitude.
ω is angular frequency.
k is wave number.
v = ω/k.
y = A sin(ωt − kx) travels in positive x-direction.
y = A sin(ωt + kx) travels in negative x-direction.
Particle velocity is dy/dt, the velocity of an oscillating medium particle.
Wave velocity is speed of propagation of phase or wave pattern, v = fλ = ω/k.
vp,max = Aω.
Slope is dy/dx at a point on the wave profile.
a = d2y/dt2 = −ω2y.
dy/dx = −Ak cos(ωt − kx).
dy/dt = Aω cos(ωt − kx).
vp,max/v = Aω/(ω/k) = Ak.
Time period T.
Wavelength λ.
Phase describes the state of oscillation of a particle at a given position and time.
When their phase difference is 0 or an integral multiple of 2π.
Hertz or s−1.
Metre.
m s−1.
rad s−1.
Wavelength decreases.
Wave speed doubles.
Louder sound, because energy/intensity is greater.
No, wave speed is decided by medium properties.
Two particles may have same displacement but opposite velocities, so their phases can differ.
x = (ω/k)t − constant/k, so x increases with t; direction is positive x.
x = constant/k − (ω/k)t, so x decreases with t; direction is negative x.
It is spatial angular frequency: phase change per metre.
Both are true and the reason correctly explains the assertion.
Both are true and the reason correctly explains the assertion.
Assertion is false; reason can be true.
Both are true and the reason correctly explains the assertion.
True.
False. k = 2π/λ.
True.
False.
T = 0.04 s, so f = 25 Hz.
k = 2π/0.5 = 4π rad m−1.
v = ω/k = 120/6 = 20 m s−1.
λ = v/f = 340/500 = 0.68 m.
The coefficient of x is k, and wavelength is 2π/k.
dy/dt measures vertical or local particle motion, while wave speed measures propagation of phase along x.
Yes, mathematically vp,max/v = Ak; depending on amplitude and wave number it can be less or greater, though small-amplitude waves usually have Ak much less than 1.
Phase increases at rate ω for y = A sin(ωt − kx).
If Wave Parameters or Wave Equation is not clear and you are looking for a Physics Tutor, contact Kumar Sir.