Seven Parameters of Sound

Period and Frequency

  • Seven sound-wave parameters (essential): ff (frequency), TT (period), cc (propagation speed), λ\lambda (wavelength), amplitude, power, intensity.

  • Five focus points to remember: definitions (and synonyms), units, symbols, formulas/relationships, and sonographer impact.

  • Period and frequency are reciprocal:

    • T=1fT = \frac{1}{f} and f=1Tf = \frac{1}{T}.

  • A cycle: one complete oscillation (rest → compress → rest → rarefaction → rest).

  • Period units: typically microseconds in ultrasound (range ~0.060.5 μs0.06-0.5\ \mu s); frequency units: typically megahertz (MHz).

  • Frequency in ultrasound: usually described as the transducer’s emitted frequency; actual frequency is largely determined by the transducer and machine bandwidth and is not freely adjustable by the sonographer.

  • Important relationship with wavelength: λ=cf\lambda = \frac{c}{f}.

  • Soft-tissue speed (average speed of sound): c1.54 mm/μsc \approx 1.54\ \text{mm/}\mu\text{s} or c1540 m/sc \approx 1540\ \text{m/s}.

  • For soft tissue, using MHz for frequency: λ1.54f(MHz) mm\lambda \approx \frac{1.54}{f\text{(MHz)}}\text{ mm}.

  • Higher frequency → shorter wavelength and better axial resolution but less penetration; lower frequency → longer wavelength with greater penetration but reduced detail.

  • Propagation speed (c) basics:

    • c is the speed at which sound travels in a medium.

    • Directly related to stiffness; inversely related to density: stiffer media speed up; denser media slow down.

    • cstiffnessdensityc \propto \sqrt{\frac{\text{stiffness}}{\text{density}}}.

  • Media speeds (conceptual): air and lungs are slowest; bone is fastest; soft tissue is the standard reference (average soft-tissue speed used by ultrasound machines).

  • Sonographer impact on period/frequency:

    • You cannot directly adjust period or the native frequency of the emitted wave.

    • Modern transducers have bandwidth; you can influence which echoes the system “listens for” by selecting a frequency range, but you are not changing the actual transducer’s innate frequency.

    • Choice of transducer frequency represents a balance: high frequency → better resolution, shallow penetration; low frequency → deeper penetration, lower resolution.

  • Audible vs ultrasound reference:

    • Audible range: 20 Hzf20 kHz20\ \text{Hz} \leq f \leq 20\ \text{kHz}.

    • Ultrasound: f > 20\ \text{kHz}; diagnostic imaging typically uses 117 MHz\approx 1-17\ \text{MHz}.

  • Quick calculation examples:

    • 2 cycles in 1 second: f=21 s=2 Hz; T=12 Hz=0.5 s.f = \frac{2}{1\text{ s}} = 2\ \text{Hz};\ T = \frac{1}{2\ \text{Hz}} = 0.5\ \text{s}.

    • 10 cycles in 1 microsecond: f=101 μs=10 MHz; T=110 MHz=0.1 μs.f = \frac{10}{1\ \mu\text{s}} = 10\ \text{MHz};\ T = \frac{1}{10\ \text{MHz}} = 0.1\ \mu\text{s}.

  • Practice reminder: use complementary units (seconds with Hz, microseconds with MHz, milliseconds with kHz) when pairing period and frequency.

Wavelength and Propagation Speed

  • Propagation speed (c): speed at which a sound wave travels through a medium.

  • Units: m/s\text{m/s} or mm/μs\text{mm}/\mu\text{s}.

  • Soft tissue average: c1.54 mm/μsc \approx 1.54\ \text{mm/}\mu\text{s} (≈ 1540 m/s).

  • Medium effects:

    • Speed increases with stiffness (more bulk modulus).

    • Speed decreases with density (more dense media slow the wave).

    • Relationship: cstiffnessdensityc \propto \sqrt{\frac{\text{stiffness}}{\text{density}}}

  • Wavelength λ\lambda: distance that one cycle occupies in space.

  • Wavelength units: typically millimeters (mm).

  • Wavelength relation:

    • λ=cf\lambda = \frac{c}{f}.

    • In soft tissue: λ=1.54 mm/μsf(MHz)\lambda = \frac{1.54\ \text{mm/}\mu\text{s}}{f\text{(MHz)}} (mm).

  • Soft-tissue wavelength ranges (example):

    • 8 MHz in soft tissue: λ0.19 mm\lambda \approx 0.19\ \text{mm}.

    • 3 MHz in soft tissue: λ0.51 mm\lambda \approx 0.51\ \text{mm}.

  • Air vs soft tissue contrast:

    • In air, c0.33 mm/μsc \approx 0.33\ \text{mm/}\mu\text{s} → much longer wavelengths at a given frequency.

  • Practical implications:

    • Shorter wavelengths improve axial resolution; wavelengths are not independently adjustable since they depend on frequency and medium.

    • The frequency choice (via transducer/bandwidth) and the medium together determine the resulting wavelength.

  • Memorized quick references (soft tissue):

    • 1 MHz: T=1 μsT = 1\ \mu\text{s}, λ1.54 mm\lambda \approx 1.54\ \text{mm}.

    • 2 MHz: T=0.5 μsT = 0.5\ \mu\text{s}, λ0.77 mm\lambda \approx 0.77\ \text{mm}.

  • Example comparison (same time frame):

    • 8 MHz → shorter cycle length than 3 MHz (in soft tissue) within the same microsecond frame.

  • Summary relation:

    • If frequency increases (within medium), wavelength decreases; if speed is higher, wavelengths are longer for the same frequency.

  • Board/workbook note reference (conceptual): with known medium, you can derive period, frequency, and wavelength from a small set of data using these relationships.