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2.6 Periodic Motion, Wave Fundamentals, Superposition & Standing Waves

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2 Physics: Mechanics, Fluids & Periodic Motion

2.1 Translational Kinematics, Projectile Motion & Newton's Laws 2.2 Friction, Centripetal Force & Rotational Equilibrium in Biomechanics 2.3 Mechanical Work, Pressure-Volume Work & Forms of Energy 2.4 The Work-Energy Theorem, Power & Mechanical Advantage 2.5 Hydrostatics, Fluid Dynamics & Circulatory Hemodynamics 2.6 Periodic Motion, Wave Fundamentals, Superposition & Standing Waves 2.7 Sound Intensity, the Decibel Scale & the Doppler Effect

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13 Human Physiology: Control & Transport Systems

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18 Emotion, Stress, Motivation & Personality

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2.6 Periodic Motion, Wave Fundamentals, Superposition & Standing Waves

Key Takeaways Explain This Topic AI

Wave propagation speed is determined solely by the mechanical properties of the medium (v = √(B/ρ) in bulk fluids/tissues); upon crossing media interfaces, wave frequency remains constant while wavelength shifts in direct proportion to velocity (λ = v / f).

Standing wave boundary conditions govern acoustic resonance: conduits with identical boundary conditions (open-open pipes or fixed-end strings) support all integer harmonics (λn = 2L/n, fn = n v / [2L]), whereas closed-open pipes support only odd harmonics (λn = 4L/n, fn = n v / [4L] for odd n).

The human external auditory canal behaves acoustically as a closed-open pipe (L ≈ 2.5 cm), generating a fundamental acoustic resonance at ~3.4 kHz that matches the frequency band of maximum human auditory sensitivity.

Last updated: September 2026

2.6 Periodic Motion, Wave Fundamentals, Superposition & Standing Waves

Acoustics and mechanical wave mechanics describe how oscillatory energy propagates through compressible media. On the MCAT, wave phenomena bridge fundamental physics and clinical medicine: auditory transduction in the cochlea, acoustic resonance in the ear canal, tissue attenuation during sonography, and Doppler echocardiography of stenotic heart valves. Mastering wave fundamentals requires understanding wave speed medium-dependence, standing wave boundary conditions, decibel math, and the Doppler frequency equation.

  • Wave Fundamentals & Periodic Motion
  • Simple Harmonic Motion (SHM)

Simple harmonic motion occurs when a displaced particle experiences a restoring force directly proportional to its displacement from equilibrium, directed opposite to that displacement: F = − k x F = -k x F = − k x

Mass-spring system: Period T = 2 π m k T = 2\pi \sqrt{\frac{m}{k}} T = 2 π k m ​ ​ , angular frequency ω = k m \omega = \sqrt{\frac{k}{m}} ω = m k ​ ​

Simple pendulum: Period T = 2 π L g T = 2\pi \sqrt{\frac{L}{g}} T = 2 π g L ​ ​ , angular frequency ω = g L \omega = \sqrt{\frac{g}{L}} ω = L g ​ ​

Fundamental Wave Parameters

Wavelength ( λ \lambda λ ): Spatial distance between two consecutive in-phase points (crest to crest or compression to compression) (m).

Frequency ( f f f ): Number of complete oscillations or cycles passing a fixed point per unit time (Hertz, 1 Hz = 1 s − 1 1\text{ Hz} = 1\text{ s}^{-1} 1 Hz = 1 s − 1 ).

Period ( T T T ): Time required to complete one full cycle ( T = 1 / f T = 1/f T = 1/ f ) (s).

Amplitude ( A A A ): Maximum displacement from equilibrium. Wave energy and intensity scale with the square of amplitude ( I ∝ A 2 I \propto A^2 I ∝ A 2 ).

Wave Speed ( v v v ): The propagation speed of the wave disturbance through space: v = f λ = λ T v = f \lambda = \frac{\lambda}{T} v = f λ = T λ ​

Medium-Dependence of Wave Speed

The Cardinal Rule of Wave Mechanics: Wave speed ( v v v ) is determined strictly by the physical properties of the transmitting medium , not by the wave's frequency or amplitude. For longitudinal sound waves propagating through a bulk compressible fluid or tissue: v = B ρ v = \sqrt{\frac{B}{\rho}} v = ρ B ​ ​

where B B B is the bulk modulus (incompressible stiffness/elasticity) and ρ \rho ρ is the density of the medium.

Although solids and liquids are denser than gases, their bulk moduli are orders of magnitude greater ( B solid ≫ B liquid ≫ B gas B_{\text{solid}} \gg B_{\text{liquid}} \gg B_{\text{gas}} B solid ​ ≫ B liquid ​ ≫ B gas ​ ). Consequently, sound travels fastest in stiff solids, intermediate in liquids, and slowest in compressible gases:

  • Air ( 20 ∘ C 20^\circ\text{C} 2 0 ∘ C ): v ≈ 343 m/s v \approx 343\text{ m/s} v ≈ 343 m/s
  • Pure Water ( 20 ∘ C 20^\circ\text{C} 2 0 ∘ C ): v ≈ 1480 m/s v \approx 1480\text{ m/s} v ≈ 1480 m/s

Human Soft Tissue: v ≈ 1540 m/s v \approx 1540\text{ m/s} v ≈ 1540 m/s (universal calibration standard for diagnostic ultrasound)

  • Cortical Bone: v ≈ 3500 − 4000 m/s v \approx 3500 - 4000\text{ m/s} v ≈ 3500 − 4000 m/s
  • Boundary Transitions

When a wave crosses an interface between two different media:

Frequency ( f f f ) remains constant because oscillations are driven by the source.

Wave speed ( v v v ) changes according to the mechanical properties of the new medium.

Wavelength ( λ \lambda λ ) changes in direct proportion to speed: λ = v / f \lambda = v / f λ = v / f .

Transverse vs. Longitudinal Waves

Transverse Waves: Particle oscillations are perpendicular to the direction of wave propagation (e.g., electromagnetic radiation, surface water waves, plucking a guitar string). Transverse waves can be polarized.

Longitudinal Waves: Particle oscillations are parallel to the direction of wave propagation, creating alternating regions of compression (high density/pressure) and rarefaction (low density/pressure) (e.g., sound waves, diagnostic ultrasound pulses). Longitudinal waves cannot be polarized.

  • Superposition, Interference & Standing Waves
  • Principle of Superposition

When two or more waves travel through the same medium simultaneously, the net resultant displacement at any coordinate is the algebraic vector sum of individual displacements:

Constructive Interference: Waves arrive in phase (phase difference Δ ϕ = 0 , 2 π , 4 π \Delta\phi = 0, 2\pi, 4\pi Δ ϕ = 0 , 2 π , 4 π ; path length difference Δ d = m λ \Delta d = m \lambda Δ d = mλ , where m m m is an integer). Amplitudes add constructively ( A net = A 1 + A 2 A_{\text{net}} = A_1 + A_2 A net ​ = A 1 ​ + A 2 ​ ).

Destructive Interference: Waves arrive out of phase (phase difference Δ ϕ = π , 3 π , 5 π \Delta\phi = \pi, 3\pi, 5\pi Δ ϕ = π , 3 π , 5 π ; path length difference Δ d = [ m + 1 2 ] λ \Delta d = [m + \frac{1}{2}]\lambda Δ d = [ m + 2 1 ​ ] λ ). Amplitudes subtract ( A net = ∣ A 1 − A 2 ∣ A_{\text{net}} = |A_1 - A_2| A net ​ = ∣ A 1 ​ − A 2 ​ ∣ ).

Standing Waves

A standing wave forms when two identical harmonic waves traveling in opposite directions interfere within a bounded medium. Standing waves exhibit fixed spatial points of zero oscillation ( nodes ) and points of maximal oscillatory excursion ( antinodes ). The distance between any two adjacent nodes (or two adjacent antinodes) is exactly half a wavelength ( 1 2 λ \frac{1}{2} \lambda 2 1 ​ λ ).

1. Open Pipes & Fixed Strings (Symmetric Boundaries)

An air pipe open at both ends supports displacement antinodes at both ends. A string clamped at both ends supports displacement nodes at both ends. Both systems share identical harmonic equations: λ n = 2 L n , f n = n v 2 L = n f 1 ( n = 1 , 2 , 3 , 4 , … ) \lambda_n = \frac{2L}{n}, \quad f_n = \frac{n v}{2L} = n f_1 \quad (n = 1, 2, 3, 4, \dots) λ n ​ = n 2 L ​ , f n ​ = 2 L n v ​ = n f 1 ​ ( n = 1 , 2 , 3 , 4 , … )

where n n n is the harmonic number, L L L is conduit length, and f 1 = v 2 L f_1 = \frac{v}{2L} f 1 ​ = 2 L v ​ is the fundamental frequency. All integer harmonics exist.

2. Closed-Open Pipes (Asymmetric Boundaries)

An air column closed at one end and open at the other (such as a vocal tract or ear canal) requires a node at the closed boundary (particles cannot oscillate against a rigid wall) and an antinode at the open boundary : λ n = 4 L n , f n = n v 4 L = n f 1 ( n = 1 , 3 , 5 , 7 , … ) \lambda_n = \frac{4L}{n}, \quad f_n = \frac{n v}{4L} = n f_1 \quad (n = 1, 3, 5, 7, \dots) λ n ​ = n 4 L ​ , f n ​ = 4 L n v ​ = n f 1 ​ ( n = 1 , 3 , 5 , 7 , … )

MCAT High-Yield Rule: A closed-open pipe supports only odd harmonics ( n = 1 , 3 , 5 , … n = 1, 3, 5, \dots n = 1 , 3 , 5 , … ). Even harmonics ( n = 2 , 4 , 6 , … n = 2, 4, 6, \dots n = 2 , 4 , 6 , … ) cannot physically exist because they cannot satisfy the simultaneous node/antinode boundary conditions.

Biological Correlate: External Auditory Canal Resonance

The human external auditory canal is an air-filled tube bounded externally by the pinna (open) and internally by the tympanic membrane (closed). Average canal length is L ≈ 2.5 cm = 0.025 m L \approx 2.5\text{ cm} = 0.025\text{ m} L ≈ 2.5 cm = 0.025 m . Assuming speed of sound in air v = 343 m/s v = 343\text{ m/s} v = 343 m/s : f 1 = v 4 L = 343 m/s 4 ( 0.025 m ) = 343 0.10 = 3430 Hz ≈ 3.4 kHz f_1 = \frac{v}{4L} = \frac{343\text{ m/s}}{4(0.025\text{ m})} = \frac{343}{0.10} = 3430\text{ Hz} \approx 3.4\text{ kHz} f 1 ​ = 4 L v ​ = 4 ( 0.025 m ) 343 m/s ​ = 0.10 343 ​ = 3430 Hz ≈ 3.4 kHz

This acoustic resonance amplifies sound waves in the 2 − 4 kHz 2 - 4\text{ kHz} 2 − 4 kHz range by up to 10 − 15 dB 10 - 15\text{ dB} 10 − 15 dB , precisely corresponding to human speech frequencies and explaining peak auditory sensitivity.

Summary of Standing Wave Resonators and Harmonics

Resonator System Boundary Conditions Wavelength Formula ( λ n \lambda_n λ n ​ ) Frequency Formula ( f n f_n f n ​ ) Harmonic Values ( n n n ) Biological / Physical Analogue

String Fixed at Both Ends Node at both ends λ n = 2 L n \lambda_n = \frac{2L}{n} λ n ​ = n 2 L ​ f n = n v 2 L f_n = \frac{n v}{2L} f n ​ = 2 L n v ​ n = 1 , 2 , 3 , … n = 1, 2, 3, \dots n = 1 , 2 , 3 , … (all integers) Vocal cord vibrating segments

Open-Open Pipe Antinode at both ends λ n = 2 L n \lambda_n = \frac{2L}{n} λ n ​ = n 2 L ​ f n = n v 2 L f_n = \frac{n v}{2L} f n ​ = 2 L n v ​ n = 1 , 2 , 3 , … n = 1, 2, 3, \dots n = 1 , 2 , 3 , … (all integers) Trachea open at larynx and carina (approx.)

Closed-Open Pipe Node at closed, Antinode at open λ n = 4 L n \lambda_n = \frac{4L}{n} λ n ​ = n 4 L ​ f n = n v 4 L f_n = \frac{n v}{4L} f n ​ = 4 L n v ​ n = 1 , 3 , 5 , … n = 1, 3, 5, \dots n = 1 , 3 , 5 , … (odd integers only) External auditory canal (tympanic membrane closed, pinna open)

Closed-Closed Cavity Node at both ends λ n = 2 L n \lambda_n = \frac{2L}{n} λ n ​ = n 2 L ​ f n = n v 2 L f_n = \frac{n v}{2L} f n ​ = 2 L n v ​ n = 1 , 2 , 3 , … n = 1, 2, 3, \dots n = 1 , 2 , 3 , … (all integers) Sealed diagnostic acoustic chambers