|
Material |
Density, |
Speed of Sound, |
Acoustic Impedance, |
|
Air |
1.3 |
330 |
0.0004 |
|
Water |
1000 |
1500 |
1.5 |
|
Blood |
1060 |
1570 |
1.66 |
|
Fat |
925 |
1450 |
1.34 |
|
Soft tissue (average value) |
1060 |
1540 |
1.63 |
|
Muscle |
1075 |
1590 |
1.71 |
|
Bone (average for adult) |
1600 |
4000 |
6.4 |
When using ultrasound we are interested in the fraction of sound reflected at the boundaries between tissues since these reflections are used to make the ultrasound images. This fraction depends on the acoustic impedance
if each material. The impedance in turn depends on the density
and the speed of sound in the material![]()
We can derive an equation for the fraction of sound at the boundaries of two tissues with different acoustic impedances
and
If the sound approaches the boundary at right angles with intensity
and and the intensity of the reflected sound is
then![]()
At the interface between muscle and bone we would expect a fraction
to be reflected.
Notice that if
and
are very different then most of the ultrasound will be reflected. This happens at an air tissue boundary (to reduce this during a scan, a gel with impedance very nearly equal to that with skin is smeared over the area of contact of the transducer with the skin) and conversely, between different soft tissues very little reflection will take place, which makes soft tissues difficult to differentiate on an ultrasound scan.
Lungs and bones are difficult to see for these reasons, and to image the heart, the sound must be directed between two ribs.