Skip to main content

AA Alive Sdn Bhd · SSM 1204108-DEst. 2016Superbrands Malaysia 2025Batu Caves · Kota Kinabalu · Kuching

WhatsApp 010-905 2891

How Ultrasound Works: From Piezoelectric Crystal to Image

An ultrasound scanner is a very fast sonar. The probe sends a short burst of sound, times every echo that comes back, and draws each one at the depth its delay implies. Here is how the probe, the gel, the timing and the choice of frequency fit together, and how to set them for each exam.

Also called How ultrasound works, Ultrasound physics, Pulse-echo principle

Published:

The short version

Diagnostic ultrasound uses sound far above human hearing, roughly 1 to 20 MHz, and it does not use ionising radiation. Each image is built line by line, many times a second:

  • The probe converts an electrical pulse into a burst of sound a few cycles long.
  • Gel carries that sound across the skin; without it almost all of it would bounce off the air gap.
  • At every boundary between tissues, a small part of the sound reflects back as an echo.
  • The probe turns each returning echo into a voltage. The machine converts the delay into depth and the strength into brightness.
  • Repeating this along a hundred or more lines across the probe makes one frame. Repeating the frame gives a live, moving image.

Step 1: the piezoelectric effect in the probe

A piezoelectric material changes shape when a voltage is applied and produces a voltage when it is squeezed. Ultrasound probes use this both ways: the same elements transmit the pulse and receive the echoes.

Elements

Modern probes contain an array of small piezoelectric elements, usually a ceramic or a ceramic composite. Firing them with slightly different delays focuses and steers the beam electronically, with no moving parts.

Backing block

Damping material behind the elements stops them ringing after each pulse. A shorter pulse means finer detail along the beam, which is called axial resolution.

Matching layer

One or more layers on the face of the elements ease the sound from the hard ceramic into soft tissue, so less energy is reflected inside the probe.

Lens

The rubbery front face focuses the beam in the thin slice direction (elevation). It is also the part most easily damaged by the wrong wipes or by a drop.

Probe types and footprints

Step 2: pulse-echo timing turns time into depth

The machine assumes that sound travels through soft tissue at 1540 metres per second. Because each echo makes a round trip, depth equals speed multiplied by the delay, divided by two. That works out at about 13 microseconds of delay for every centimetre of depth.

A probe sends a pulse through gel, skin and fat, muscle and liver. Echoes from the boundaries at 2, 5 and 8 cm return after 26, 65 and 104 microseconds, and each is weaker than the one before.
One pulse, three echoes. The machine places each echo at depth = 1540 m/s × delay ÷ 2. Deeper echoes are weaker because the sound loses energy on the way down and back.
  • The 1540 m/s figure is an average. Fat carries sound more slowly, so structures behind thick fat can be drawn slightly out of place; this is one source of artefacts.
  • The probe cannot send the next pulse until the deepest echoes are back. Imaging to 15 cm limits the pulse rate to about 5,000 per second, and imaging to 20 cm to about 3,800.
  • Frame rate is the pulse rate divided by the number of lines in the frame. More depth, a wider sector or extra focal zones all lower the frame rate.

Step 3: why echoes happen, and why gel is needed

Echoes come from changes in acoustic impedance, which is roughly a tissue’s density multiplied by its speed of sound. The bigger the change at a boundary, the stronger the echo. The fraction reflected is ((Z2 − Z1) ÷ (Z2 + Z1))².

Approximate acoustic impedance values (MRayl) and what happens at the boundary
BoundaryApproximate impedancesShare of sound reflectedWhat you see
Fat to muscle≈1.4 and ≈1.7About 1%A thin, faint line; most sound carries on deeper
Soft tissue to bone≈1.6 and ≈7.8About 40%A bright surface with a shadow behind it
Soft tissue to air≈1.6 and ≈0.0004More than 99.9%A bright line and nothing beyond it: why bowel gas and lung block the view
Probe to skin with gelGel is close to soft tissueVery littleSound enters the body; this is the whole point of gel

Step 4: attenuation and why deep echoes need help

Sound loses energy as it travels, by absorption and scattering. In average soft tissue the loss is roughly 0.5 dB per centimetre for each megahertz of frequency, and it applies on the way down and on the way back. A 5 MHz pulse reflecting from 10 cm deep loses about 0.5 × 5 × 20 = 50 dB, a factor of about 100,000 in power.

  • Time gain compensation (TGC) amplifies later echoes more than early ones, so the image looks even from top to bottom. Set the sliders so that a uniform organ such as the liver looks uniform.
  • Fluid attenuates far less than tissue, so tissue behind a cyst or full bladder looks brighter (posterior enhancement).
  • Bone, stones and gas stop most of the sound, leaving a dark shadow behind them.

Frequency, depth and resolution: the trade-off

Higher frequencies have shorter wavelengths, so they show finer detail. They also lose energy faster, so they cannot reach as deep. Choosing a probe and frequency is choosing where on this curve to sit.

Chart of approximate useful depth against frequency: about 30 cm at 2 MHz, 17 cm at 3.5 MHz, 12 cm at 5 MHz, 8 cm at 7.5 MHz, 6 cm at 10 MHz and 4 cm at 15 MHz, with the usual frequency bands of four probe types.
A rule of thumb, not a specification: if a system can recover about 60 dB of round-trip loss, the reachable depth in average soft tissue is roughly 60 ÷ frequency in MHz. Real systems do better with harmonics and coded pulses, and worse in fatty or fibrotic tissue.
ResolutionWhat sets itHow to improve it
Axial (along the beam)Pulse length: about half the length of the pulse in tissueHigher frequency, a well-damped probe
Lateral (across the image)Beam width, narrowest at the focusPut the focal zone at the structure of interest; use a higher frequency
Elevation (slice thickness)The probe’s lens and, on some probes, a multi-row arrayChoose a probe designed for fine slices; keep the target near the lens focus
Temporal (frame rate)Depth, sector width, focal zones and line densityReduce depth and sector width; use one focal zone for moving structures

What is optimal: frequency and probe by exam

Use the highest frequency that still reaches the deepest structure you need to see, then set the depth so that structure fills most of the screen. Typical starting points:

Approximate starting points; the exact range depends on the probe’s data sheet and the patient
ExamProbeTypical frequencyOptimal set-up
Adult abdomen and kidneysCurvilinear2–5 MHzDepth 15–20 cm, harmonics on, focus at the organ
Large or deep patientsCurvilinearLowest setting, about 2 MHzHarmonics on, reduce depth to what you need, single focus
Pregnancy after the first trimesterCurvilinear2–6 MHzObstetric preset, watch the thermal index
Early pregnancy and gynaecologyEndocavity4–9 MHzEmpty bladder, probe cover, depth to the pelvis only
Adult heartPhased array1–5 MHzCardiac preset, narrow sector for a higher frame rate
Thyroid, breast, testis, skinLinear7–15 MHzDepth 3–5 cm, focus at the lesion
Carotid and leg veinsLinear5–10 MHzVascular preset, colour box small
Muscles, tendons and nerve blocksLinear7–15 MHz or higherShallow depth, needle-visualisation mode if available

Harmonics, compounding and other processing

Tissue harmonic imaging

Tissue distorts the pulse slightly as it travels, creating echoes at twice the transmitted frequency. Listening only to those reduces haze from the body wall and sharpens cyst edges. Most systems now have it on in their abdominal presets.

Spatial compounding

Combining frames steered at several angles smooths speckle and fills in edges, at some cost to frame rate.

Speckle reduction

Filters smooth the granular texture of the image. Too much makes the image look artificially soft.

What this means when you choose a system

  • Look at each probe’s frequency range on its data sheet, not just the system brochure.
  • Scan your heaviest typical patient at your deepest typical depth during the demonstration, and check the frame rate there.
  • Check that harmonics work on the probes you will use most.
  • Ask which processing features are standard and which are licensed options on the quotation.
  • MDA registration applies to the system and to every probe (Medical Device Act 2012, Act 737).

Frequently asked questions

How does ultrasound work, in one sentence?
The probe sends short pulses of high-frequency sound into the body and times the echoes that bounce back from tissue boundaries; the machine converts each delay into a depth and each echo’s strength into a brightness on the screen.
Why is gel needed for an ultrasound scan?
Almost all sound reflects at a boundary between tissue and air. Gel fills the air gap between the probe and the skin, so the sound can enter the body.
Why does a higher-frequency probe not see as deep?
Attenuation rises with frequency, roughly 0.5 dB per centimetre per megahertz in soft tissue, so high-frequency sound runs out of energy sooner. In return it gives finer detail.
Does ultrasound use radiation?
Not ionising radiation. It uses sound waves, which is why it needs no radiation licence or lead shielding, although output is still kept as low as reasonably achievable.
What is the speed of sound used by an ultrasound machine?
1540 metres per second, the average for soft tissue. The machine uses it to turn each echo’s delay into a depth, at about 13 microseconds per centimetre.

Get a written quotation

Tell us your clinic or lab type, daily workload and location. We match suitable models and send a written quotation that states who handles delivery, installation and training, and what each costs.

010-905 2891 · Mon–Sat, 9:00 am – 6:00 pm