Beats
Beats are loud-soft variations caused by superposition of two nearby frequencies. Beat frequency is |f1 - f2|.
Class 11 Physics notes covering beats, beat frequency, Doppler effect, moving source, moving observer, applications, numericals and PYQs.
Important Note: Doppler Effect is not part of the NEET 2026 syllabus. The status of NEET 2027 and future syllabi may change depending on NMC updates. However, Doppler Effect remains important for JEE Main, JEE Advanced, Olympiads, IB, IGCSE and A-Level Physics.
Beats are loud-soft variations caused by superposition of two nearby frequencies. Beat frequency is |f1 - f2|.
Apparent frequency changes because source and observer motion changes wavefront spacing or receiving rate.
Draw source and observer arrows first. Approach increases frequency; separation decreases frequency.
Beats and Doppler Effect are two beautiful applications of superposition and relative motion in sound. Beats explain waxing and waning loudness when two nearby frequencies combine. Doppler Effect explains why apparent frequency changes when source, observer or both move.
Important Note: Doppler Effect is not part of the NEET 2026 syllabus. The status of NEET 2027 and future syllabi may change depending on NMC updates. However, Doppler Effect remains important for JEE Main, JEE Advanced, Olympiads, IB, IGCSE and A-Level Physics.
Real-life examples include tuning a guitar using beats, ambulance siren pitch changing as it passes, train horn pitch shift, police radar, aircraft motion and astronomical red shift.
Exam perspective: beats questions are usually short and formula-based, while Doppler questions test sign convention, relative approach, source motion versus observer motion and apparent frequency.
Beats are periodic variations in loudness heard when two sound waves of nearly equal frequencies and comparable amplitudes superpose. The sound alternately becomes loud and soft.
Suppose two waves are y1 = A sin(2πf1t) and y2 = A sin(2πf2t). On adding them, the resultant can be written as a fast oscillation multiplied by a slowly varying amplitude factor.
Using sin C + sin D = 2 sin((C+D)/2) cos((C-D)/2), resultant displacement becomes y = 2A cos[π(f1-f2)t] sin[2π((f1+f2)/2)t].
The amplitude factor changes slowly, so intensity and loudness rise and fall. Maximum loudness occurs when waves are in phase; minimum loudness occurs when they are nearly opposite in phase.
Beat frequency is fb = |f1 - f2|. It tells the number of loud beats heard per second.
Real-life example: when a tuning fork of 256 Hz and another of 258 Hz are sounded together, 2 beats per second are heard.
Beats are used to tune musical instruments. A musician compares an instrument note with a standard tuning fork. If beats are heard, frequencies are not equal. As tuning improves, beat frequency decreases to zero.
In laboratories, beats help detect small frequency differences that are difficult to measure directly. Counting beats per second gives the difference between two frequencies.
Sound engineering uses beating to identify unwanted frequency mismatch, phase issues and modulation-like effects in audio systems.
Real-life example: two guitar strings meant to produce the same note create a wavering sound if one is slightly out of tune. Tightening or loosening one string reduces the beat frequency.
Common mistake: if beat frequency is 4 Hz and one source is 256 Hz, the other source may be 252 Hz or 260 Hz unless extra information is given.
Doppler Effect is the apparent change in frequency heard by an observer due to relative motion between source and observer along the line joining them.
The actual frequency emitted by the source does not change. What changes is the rate at which wavefronts reach the observer.
When source and observer move towards each other, wavefronts are received more frequently and apparent frequency increases. When they move away from each other, apparent frequency decreases.
The compact formula is f' = f[(v ± v0)/(v ∓ vs)], but signs must be selected from physical approach or separation, not blindly.
Real-life example: an ambulance siren sounds higher pitched when approaching and lower pitched after passing.
When the source moves, it changes spacing of wavefronts in front and behind. In front of an approaching source, wavefronts are compressed and wavelength decreases. Behind a receding source, wavefronts are stretched.
Source moving towards stationary observer: f' = fv/(v - vs). Source moving away: f' = fv/(v + vs).
Physical meaning: the source emits each next crest from a new position. If it moves toward the observer, crests are closer together; if it moves away, crests are farther apart.
Common trap: source velocity appears in denominator because source motion changes effective wavelength.
Example: a train horn moving toward a platform observer is heard at higher pitch.
When the observer moves, the emitted wavelength in the medium is unchanged if source is stationary, but the observer cuts wavefronts at a different rate.
Observer moving towards stationary source: f' = f(v + v0)/v. Observer moving away: f' = f(v - v0)/v.
Physical meaning: moving towards wavefronts increases the number of crests received per second. Moving with the wavefronts decreases the receiving rate.
Common trap: observer velocity appears in numerator because observer motion changes the rate of receiving waves.
Example: a cyclist moving towards a stationary siren hears a higher pitch.
General one-dimensional Doppler formula can be remembered as f' = f(v ± v0)/(v ∓ vs). Choose signs so approach increases f' and separation decreases f'.
Source and observer moving towards each other: use larger numerator and smaller denominator, so apparent frequency increases strongly.
Source and observer moving away from each other: use smaller numerator and larger denominator, so apparent frequency decreases strongly.
Source chasing observer: if source is behind and faster than observer, separation decreases, apparent frequency increases; if observer is faster, separation increases, apparent frequency decreases.
Observer chasing source: if observer gains on source, separation decreases; if not, separation increases. Always draw arrows before formula.
Ambulance and police sirens show Doppler pitch shift as they approach and recede. The sudden change after passing is a classic real-life observation.
Radar speed guns use Doppler shift in reflected electromagnetic waves to measure vehicle speed. Similar ideas are used in aircraft tracking and weather radar.
Astronomy uses Doppler shift of light to detect motion of stars and galaxies. Red shift indicates recession; blue shift indicates approach.
Medical Doppler ultrasound measures blood flow by detecting frequency shift of reflected ultrasound from moving blood cells.
In aircraft and train motion, Doppler shift helps estimate relative speeds and explain observed changes in pitch.
| Situation | Use | Reason | Common Mistake |
|---|---|---|---|
| Observer moving towards source | +v0 in numerator | Observer meets more wavefronts per second. | Putting observer speed in denominator. |
| Observer moving away from source | -v0 in numerator | Observer meets fewer wavefronts per second. | Using plus just because observer is moving. |
| Source moving towards observer | -vs in denominator | Wavelength ahead decreases. | Adding vs for approach. |
| Source moving away from observer | +vs in denominator | Wavelength reaching observer increases. | Confusing source and observer formulas. |
fb = |f1 - f2|Number of loud beats heard per second.
f' = f[(v ± v0)/(v ∓ vs)]Choose signs from approach or separation.
f' = f(v + v0)/vStationary source, moving observer.
f' = f(v - v0)/vReceiving rate decreases.
f' = fv/(v - vs)Wavelength in front becomes smaller.
f' = fv/(v + vs)Wavelength reaching observer becomes larger.
Diagrams use black wavefronts and red arrows/labels for clear sign-convention reading.
If Beats or Doppler Effect is not clear and you are looking for a Physics Tutor, contact Kumar Sir.
Each numerical tests a different idea: beats, ambiguity, tuning, moving source, moving observer, combined motion, chasing cases, reflected Doppler, radar and graph-based beat reading.
Given: f1=256 Hz, f2=260 Hz
Formula: fb=|f1-f2|
Solution: fb=|256-260|=4 Hz
Final Answer: 4 Hz
Given: f=512 Hz, fb=3 Hz
Formula: unknown = f ± fb
Solution: possible frequencies = 512±3 = 509 Hz or 515 Hz
Final Answer: 509 Hz or 515 Hz
Given: standard=300 Hz, beats=5, filing increases f and beats decrease
Formula: original was below standard
Solution: f = 300 - 5 = 295 Hz
Final Answer: 295 Hz
Given: f1=250 Hz, f2=254 Hz
Formula: fb=|f1-f2|
Solution: fb=4 Hz
Final Answer: 4 Hz
Given: f=440 Hz, beat=6 Hz, other lower
Formula: unknown=440-6
Solution: unknown=434 Hz
Final Answer: 434 Hz
Given: (f1+f2)/2=500, |f1-f2|=8
Formula: frequencies = average ± beat/2
Solution: f = 500 ± 4 = 496 Hz, 504 Hz
Final Answer: 496 Hz and 504 Hz
Given: f=500, v=340, vs=34
Formula: f'=fv/(v-vs)
Solution: f'=500×340/(340-34)=555.6 Hz
Final Answer: 555.6 Hz
Given: f=500, v=340, vs=34
Formula: f'=fv/(v+vs)
Solution: f'=500×340/374=454.5 Hz
Final Answer: 454.5 Hz
Given: f=600, v=340, v0=20
Formula: f'=f(v+v0)/v
Solution: f'=600×360/340=635.3 Hz
Final Answer: 635.3 Hz
Given: f=600, v=340, v0=20
Formula: f'=f(v-v0)/v
Solution: f'=600×320/340=564.7 Hz
Final Answer: 564.7 Hz
Given: f=800, v=340, vs=30, v0=20
Formula: f'=f(v+v0)/(v-vs)
Solution: f'=800×360/310=929.0 Hz
Final Answer: 929 Hz
Given: f=800, v=340, vs=30, v0=20
Formula: f'=f(v-v0)/(v+vs)
Solution: f'=800×320/370=691.9 Hz
Final Answer: 691.9 Hz
Given: source behind, both same direction, source faster; source approaches observer
Formula: f'=f(v-v0)/(v-vs)
Solution: f'=700×(340-20)/(340-40)=746.7 Hz
Final Answer: 746.7 Hz
Given: observer behind, observer faster; separation decreases
Formula: f'=f(v+v0)/(v+vs)
Solution: f'=700×(340+40)/(340+20)=738.9 Hz
Final Answer: 738.9 Hz
Given: separation increases
Formula: f'=f(v+v0)/(v+vs)
Solution: f'=700×350/370=662.2 Hz
Final Answer: 662.2 Hz
Given: moving source receives echo from stationary wall; apparent reflected frequency has double Doppler
Formula: fecho=f(v+vs)/(v-vs)
Solution: fecho=500×360/320=562.5 Hz; beats=62.5 Hz
Final Answer: 62.5 Hz
Given: f=1010 Hz, u=30, c=3×108
Formula: Δf=2uf/c
Solution: Δf=2×30×1010/(3×108)=2000 Hz
Final Answer: 2000 Hz
Given: fa=fv/(v-u), fr=fv/(v+u)
Formula: ratio=550/450=(v+u)/(v-u)
Solution: 11/9=(340+u)/(340-u); u=34 m/s
Final Answer: 34 m/s
Given: f'=fv/(v-vs)
Formula: f=f'(v-vs)/v
Solution: f=550×306/340=495 Hz
Final Answer: 495 Hz
Given: f'=f(v±v0)/v, f'>f so towards
Formula: v0=v(f'/f-1)
Solution: v0=340(408/400-1)=6.8 m/s
Final Answer: 6.8 m/s towards source
Given: f1=440, f2=442
Formula: beat frequency=|f1-f2|
Solution: 2 beats/s
Final Answer: 2
Given: f=1000, v=350, vs=25
Formula: f'=fv/(v-vs)
Solution: f'=1000×350/325=1076.9 Hz
Final Answer: 1076.9 Hz
Given: source receding
Formula: separation increases, frequency decreases
Solution: pitch decreases
Final Answer: decreases
Given: f=256, beat=3
Formula: unknown=f±beat
Solution: 253 Hz or 259 Hz
Final Answer: 253 Hz or 259 Hz
Given: vs=0.1v
Formula: f'=fv/(v-vs)=f/(0.9)
Solution: f'=1111.1 Hz
Final Answer: 1111.1 Hz
Given: v0=0.05v
Formula: f'=f(1+0.05)
Solution: f'=840 Hz
Final Answer: 840 Hz
Given: radial relative velocity zero
Formula: Doppler depends on radial component
Solution: First-order shift is zero
Final Answer: zero
Given: T=0.01 s, vs=0.1v
Formula: f'=f/(1-0.1), so T'=T(1-0.1)
Solution: T'=0.009 s
Final Answer: 0.009 s
Given: standard=300, original beat=8, wax lowers and beat decreases
Formula: original above standard
Solution: f=308 Hz
Final Answer: 308 Hz
Given: 550=500×340/(340-u)
Formula: 340-u=309.09, u=30.91
Solution: receding f'=500×340/(340+30.91)=458.3 Hz
Final Answer: 458.3 Hz
Given: source behind, observer in front, same speed
Formula: f'=f(v-v0)/(v-vs)
Solution: v0=vs, so ratio=1
Final Answer: 600 Hz
Given: same velocity, separation constant
Formula: Doppler ratio becomes 1 for same line velocity
Solution: f'=f
Final Answer: same as source frequency
Given: 10 beats in 5 s
Formula: fb=N/t
Solution: fb=2 Hz; difference=2 Hz
Final Answer: 2 Hz
Given: Tbeat=0.25 s
Formula: fb=1/Tbeat
Solution: fb=4 Hz
Final Answer: 4 Hz
Given: beat=4 with 500 Hz
Formula: f'=500±4
Solution: 496 or 504 Hz; but siren source actual 480 context may need motion details
Final Answer: 496 Hz or 504 Hz
Given: f'/f=v/(v+vs)=0.9
Formula: v+vs=v/0.9
Solution: vs=(1/0.9-1)v=v/9
Final Answer: v/9
Given: f'/f=(v-v0)/v=0.9
Formula: v0=0.1v
Solution: 0.1v
Final Answer: undefined
Given: f'/f=v/(v-vs)=1.25
Formula: v-vs=0.8v
Solution: vs=0.2v
Final Answer: 0.2v
Given: f'/f=(v+v0)/v=1.25
Formula: v0=0.25v
Solution: 0.25v
Final Answer: 0.25v
Given: fb=0
Formula: fb=|f1-f2|
Solution: |f1-f2|=0, so f1=f2
Final Answer: equal frequencies
Given: v0=v away
Formula: f'=f(v-v0)/v
Solution: f'=0
Final Answer: zero
Given: vs approaches v
Formula: f'=fv/(v-vs)
Solution: denominator approaches zero, f' becomes very large
Final Answer: tends to infinity classically
Given: f1=301, f2=299
Formula: average=(f1+f2)/2, beat=|f1-f2|
Solution: average=300 Hz, beat=2 Hz
Final Answer: 300 Hz, 2 Hz
Periodic waxing and waning of sound intensity due to superposition of two nearly equal frequencies.
fb = |f1 - f2|.
If difference is large, loudness variations are too rapid to perceive as beats.
252 Hz or 260 Hz.
It becomes zero.
Apparent change in observed frequency due to relative motion of source and observer.
Increases.
Decreases.
f' = f(v+v0)/v.
f' = fv/(v-vs).
Moving source changes wavelength in the medium.
Moving observer changes rate of encountering wavefronts.
Component along line joining source and observer.
Zero in classical sound Doppler if radial component is zero.
No, apparent frequency changes for observer.
Ambulance siren pitch changes as it passes.
Wavefronts reach observer more frequently.
Tuning instruments.
Equal frequencies.
Frequency received or measured by observer.
2.
Lower.
Higher.
Two sound waves of nearly equal frequencies.
Time interval between successive loud sounds; Tb=1/fb.
It decreases.
No first-order shift for sound if radial relative velocity is zero.
Doppler shift.
Doppler ultrasound.
Classically zero frequency.
f' = f(v ± v0)/(v ∓ vs) with signs chosen by approach/separation.
The slowly varying amplitude envelope has frequency equal to difference of component frequencies.
Waves are in phase.
Waves are out of phase.
Yes, but relativistic treatment is needed for high speeds.
Shock waves and Mach cone form; simple subsonic formula fails.
Supersonic motion and overlapping wavefronts.
Wave is shifted during incidence and again during reflection from moving target.
Red shift.
Blue shift.
Both true and reason explains assertion.
Both true and reason explains assertion.
Both false as stated; observer velocity appears in numerator and changes encounter rate.
Assertion false; apparent frequency changes.
False.
True.
True.
False.
True.
High pitch while approaching, sudden change near passing, lower pitch while receding.
Adjust tension until beats disappear.
Vehicle speed.
It increases while approaching.
It is receding from observer.
Because |f1-f2| gives a difference, not whether unknown is above or below.
To decide approach/separation and signs correctly.
Putting source and observer velocities in wrong numerator/denominator or wrong sign.
They arise from superposition of nearby frequency waves.
Doppler changes received frequency; source frequency remains same.
Observer meets more wavefronts per second.
Wavefront spacing reaching observer is larger.
Relative phase between two nearby frequencies changes periodically.
Amplitude changes too rapidly for ear to perceive separate beats.
An ambulance siren approaches and then moves away from a stationary observer.
Doppler Effect.
During approach.
During recession.
A train horn of fixed frequency moves towards a platform.
No.
Apparent frequency.
f'=fv/(v-vs).
Two strings of nearly equal frequencies produce 3 beats/s.
3 Hz.
Beat frequency becomes zero.
Small frequency differences become audible.
Radar wave reflects from a moving vehicle.
Doppler shift.
Shift occurs in going and returning wave.
Vehicle speed.
An aircraft approaches a listener and then passes overhead.
Higher than emitted.
Lower than emitted.
Radial component of relative velocity.
If Beats or Doppler Effect is not clear and you are looking for a Physics Tutor, contact Kumar Sir.