The specific acoustic impedance of a medium is defined as \$Z = \rho c\$, where \$\rho\$ is the density of the medium and \$c\$ is the speed of sound in that medium. It tells us how much resistance the medium offers to the propagation of sound waves.
Think of it like a traffic jam on a highway: the denser the traffic (higher \$\rho\$) and the slower the cars move (lower \$c\$), the harder it is for a new car (sound wave) to get through.
In ultrasound, we often use materials with high impedance to reflect sound back to the transducer, creating an image.
Suppose we have water with density \$\rho = 1000 \,\text{kg/m}^3\$ and speed of sound \$c = 1500 \,\text{m/s}\$. Then:
\$Z = \rho c = 1000 \times 1500 = 1.5 \times 10^6 \,\text{kg/(m}^2\text{s)}\$
That’s the impedance of water.
🔍 Remember: When you’re given \$\rho\$ and \$c\$, just multiply to find \$Z\$. If you’re asked why a boundary reflects sound, think about the impedance mismatch.
📝 Practice: Calculate the impedance of bone (density ~ 1900 kg/m³, \$c\$ ~ 3000 m/s) and compare it to soft tissue.
Answers: 1) \$Z = \rho c\$; 2) \$Z = 9.6 \times 10^5\$; 3) c) Both a and b.
| Medium | Density (kg/m³) | Speed of Sound (m/s) | \$Z\$ (kg/m²s) |
|---|---|---|---|
| Water | 1000 | 1500 | 1.5 × 10⁶ |
| Soft Tissue | 1040 | 1540 | 1.60 × 10⁶ |
| Bone | 1900 | 3000 | 5.70 × 10⁶ |