understand how the reflection of pulses of ultrasound at boundaries between tissues can be used to obtain diagnostic information about internal structures
Cambridge A-Level Physics 9702 – Production and Use of Ultrasound
Production and Use of Ultrasound
Learning Objective
Understand how the reflection of pulses of ultrasound at boundaries between tissues can be used to obtain diagnostic information about internal structures.
1. What is Ultrasound?
Ultrasound refers to sound waves with frequencies above the upper limit of human hearing (typically >20 kHz). In medical diagnostics the frequencies used are usually between 2 MHz and 15 MHz.
2. Generation of Ultrasound Pulses
Piezoelectric transducers: A crystal (e.g., quartz or PZT) deforms when an alternating voltage is applied, producing a short burst of sound.
Pulse‑echo mode: The same transducer acts as a receiver after the pulse is emitted, allowing detection of reflected echoes.
Key parameters:
Frequency (\$f\$) – determines resolution and penetration depth.
Pulse duration – short pulses give better axial resolution.
Peak‑to‑peak voltage – controls acoustic intensity.
3. Propagation of Ultrasound in Tissue
In a homogeneous medium the speed of sound \$c\$ is given by
\$c = \sqrt{\frac{K}{\rho}}\$
where \$K\$ is the bulk modulus and \$\rho\$ is the density of the tissue.
4. Acoustic Impedance and Reflection
The acoustic impedance \$Z\$ of a medium is defined as
\$Z = \rho c\$
When an ultrasound pulse encounters a boundary between two tissues with impedances \$Z1\$ and \$Z2\$, part of the wave is reflected and part is transmitted. The intensity reflection coefficient \$R\$ is
\$R = \left(\frac{Z2 - Z1}{Z2 + Z1}\right)^2\$
The transmitted intensity coefficient \$T\$ satisfies \$R + T = 1\$ (neglecting absorption at the interface).
5. Typical Acoustic Impedances of Human Tissues
Tissue
Density \$\rho\$ (kg m⁻³)
Speed of sound \$c\$ (m s⁻¹)
Acoustic impedance \$Z\$ (MRayl)
Fat
920
1450
1.33
Muscle
1050
1580
1.66
Blood
1060
1570
1.66
Bone (cortical)
1900
4080
7.75
Soft tissue (average)
1000
1540
1.54
6. How Reflections Provide Diagnostic Information
Time‑of‑flight measurement: The interval \$\Delta t\$ between pulse emission and echo reception gives the distance \$d\$ to the reflecting interface:
\$d = \frac{c\,\Delta t}{2}\$
The factor ½ accounts for the round‑trip travel.
Amplitude of the echo: The strength of the returned signal depends on \$R\$, which varies with the difference in acoustic impedance. Large impedance mismatches (e.g., soft tissue–bone) produce strong echoes; small mismatches produce weak echoes.
Image formation: By scanning the transducer across the body and recording echo amplitudes at many depths, a two‑dimensional map (B‑mode image) is constructed, where brightness corresponds to echo strength.
Interpretation of patterns:
Bright (hyperechoic) lines often indicate interfaces such as organ capsules or calcifications.
Dark (anechoic) regions suggest fluid‑filled spaces (e.g., cysts, bladder).
Angle dependence: Accurate Doppler measurements require the ultrasound beam to be aligned within \overline{60}° of flow direction.
Operator dependence – image quality relies on correct probe placement and settings.
9. Summary Checklist
Identify the transducer type and its operating frequency.
Recall the definition of acoustic impedance \$Z = \rho c\$.
Calculate the reflection coefficient \$R\$ for a given tissue pair.
Use the time‑of‑flight formula \$d = c\Delta t/2\$ to locate structures.
Interpret echo brightness in terms of tissue composition.
Suggested diagram: Schematic of a pulse‑echo ultrasound system showing the transducer, emitted pulse, reflected echoes from successive tissue layers, and the resulting A‑mode trace.