Basic theory of ultrasound

James Lai / Chris Nixon

 

High frequency sound of 2-50 MHz is used in medical ultrasound systems. This is well above the human hearing range of 20-20 kHz. Sound is propagated through a medium as the molecules are vibrated creating pressure waves with areas of compression and rarefaction. The waves have the characteristic features of wavelength, frequency and amplitude.

Wavelength (λ) is the distance between two areas of maximal compression (or rarefaction). The importance of wavelength is that the penetration of the ultrasound wave is proportional to wavelength and image resolution is no more than 1-2 wavelengths.

Frequency (f) is the number of wavelengths that pass per unit time. It is measured as cycles (or wavelengths) per second and the unit is hertz (Hz). It is a specific feature of the crystal used in the ultrasound transducer.  It can be varied by the operator within set limits – the higher the frequency, the better the resolution but the lower the penetration.

The magnitude of pressure change is given by the amplitude. It is expressed in decibels on a logarithmic scale.


       
Figure 1.  Sound wave characteristics


The sound waves travel at a Propagation Velocity (v) dependent on the density and compressibility of the medium.

The relationship between these variables is expressed by the Wave Equation -

v =λf

In soft tissue propagation velocity is relatively constant at 1540 m/sec and this is the value assumed by ultrasound machines for all human tissue. Hence wavelength is inversely proportional to frequency.

Acoustic Power is the amount of acoustic energy generated per unit time. Energy is measured in joules (J) with joules being the amount of heat generated by the energy in question. The unit is the Watt (W) with 1W = 1J/sec. The biological effects of ultrasound in terms of power are in the milliwatt range.

Intensity is the power density or concentration of power within an area expressed as Watts/m2 or mW/cm2. Intensity varies spacially within the beam and is greatest in the centre. In a pulsed beam it varies temporally as well as spatially


How is Ultrasound produced?

Pierre Curie discovered that when an electrical current is applied to a quartz crystal its shape changes with polarity.  This causes expansion and contraction that in turn leads to the production of compression and rarefaction sound waves. This was termed the piezo-electric effect. He later discovered the reverse also occured, an electrical current being generated on exposure to the pressure waves of returning echoes. Ultrasound transducers contain and array of piezoelectric crystals functioning as transmitter and responder. The frequency of the generated wave is a function of the crystal used.

Modern transducers use multiple small elements to generate the ultrasound wave. If a single small element transducer is used the waves radiate from it in a circular fashion as do ripples in a pool. If multiple small elements fire simultaneously however the individual curved wave fronts combine to form a linear wave front moving perpendicularly away from the transducer face. This system, that is multiple small elements fired individually, is termed phased array.  The transducer contains a backing block and acoustic insulator to prevent reverberation within the probe.  Quarter wave matching and electronic focusing allows the sound profile produced to be controlled.  Some machines allow the focus point to be used defined whilst in others it is set automatically according to scan depth


Near field and focusing

In a standard disc shaped transducer the beam shape is cylindrical. Initially the beam is of comparable diameter to the transducer as the series of ultrasound waves that make up the beam travel parallel to each other. This is the near-field or Fresnel zone. At some point distal to the transducer however the beam begins to diverge which will reduce the ability to distinguish two objects close together (resolution). Beyond the point at which the beam begins to diverge is the far-field or Fraunhofer zone. It is possible to focus the ultrasound beam to cause convergence and narrowing of the beam thus improving (lateral) resolution. Focusing can be achieved by either mechanical or, in a phased array element, by electronic means. If the transducer face is concave or a concave acoustic lens is placed on the surface of the transducer, the beam can be narrowed at a predetermined distance from the transducer. The point at which the beam is at its narrowest is the focal point or focal zone and is the point of greatest intensity and best lateral resolution.

Figure 2. Schematic of beam characteristics. Multiple side lobes may be present.

 

 

Resolution

The ability of ultrasound to distinguish between two objects is the resolution. The resolution may be spatial, discrimating distance between objects or temporal, discrimation movement in time. Spatial resolution can be further divided into axial resolution and lateral resolution.
Axial Resolution is the ability to recognise two different objects at slightly different depths from the transducer along the axis of the ultrasound beam.

Axial resolution = spatial pulse length (SPL)
                             2
where  SPL = λ * no. of cycles

It is improved by higher frequency (shorter wavelength) transducers but at the expense of penetration. Higher frequencies therefore are used to image structures close to the transducer.
Lateral Resolution is the ability to distinguish objects that are side by side. It is generally poorer than axial resolution and is dependent on beam width.  As the ultrasound machine assumes that any echo originates from the centre of the beam then two objects side by side cannot be distinguished if they are separated by less than the beam width.

Beam width  is determined by:-
     • Transducer frequency (beam width increases with lower frequency transducers)
     • Focusing of the beam
     • Gain (increased gain will increase the beam width and reduce resolution)

To optimise lateral resolution therefore:
     • Use the highest frequency (but note that this occurs at the expense of penetration).
     • Optimise the focal zone.
     • Use the minimum necessary gain (see the knobology section).

Temporal Resolution is dependent on frame rate.  It is improved by:
     • Minimising Depth – Ultrasound is sent in a pulse of 2-3 cycles in length, the spatial pulse length and then the transducer assumes a receive mode listening for echoes.  The depth of scan alters the time required for sound wave to travel to and from the  transducer.  Thus a shallow scan reduces the distance and time taken and allows more pulses per second. This is known as the pulse repetition frequency (PRF).
     • Narrowing the Sector to the area of interest - narrowing the sector angle.
     • Minimise Line density (but at the expense of lateral resolution).


Image production

For 2D or B mode ultrasound, the US probe sends pulses of sound waves from piezoelectric crystal arrays. Returning echoes are received by the crystals, each echo having an energy level which is displayed as brightness, and a depth under the probe calculated by the time delay between send and receive.  The depth calculation

 


  Acoustic impedance         Z  =  V  (kg-2s-1)

                                   

Acoustic characteristics of materials
Material

Density

(kg.m3)

Velocity

(m.sec-1)

Acoustic impedance

(kg-2s-1)

Air 1.2 343 429
Water 1.1 1525 1.43
Fat 0.92 1450 1.33
Muscle 1.04 1580 1.64
Bone 1.9 4040

7.68

 

                                    

As sound waves strike a surface between two tissues of differing acoustic impedance some of the sound is reflected. The strength of the returning echo is dependent on the difference in acoustic impedance between two tissues,.   Two principal types of reflector are described, a specular reflector where the sound beam is reflected in a single direction and a scattering reflector where the energy is reflected in multiple directions.  The former usually has a surface width of more than 1 wavelength while the latter has a surface width less than one wavelength.  The image created in this way is dependent on the direction from which the sound encounters a barrier, and is directionally dependent; a phenomenon known as Anisotropy.


Figure 3  Specular and scattering reflectors.  Incidence sound wave (i) with single reflection (R) from a specular reflector, and multiple reflections (r) from a scattering reflector.  The acoustic impedance difference between tissues determines the relative amount of reflected to transmitted sound (T)

As sound passes through tissues the energy losses or attenuation occurs due to absorption and reflection.  Attenuation is defined as the decrease in amplitude or intensity of a sound wave as it passes through a medium. The magnitude of this loss varies between tissues, and is defined by the attenuation coefficient () according to the formula:-
Attenuation (dB) =  (dB) x 2 x  depth of reflector(cm) x Frequency (MHz)
It therefore increases with depth and higher frequencies. 

Attenuation coefficients
Material Attenuation coefficient
(dB/cm)
Water 0.002
Soft tissue 0.3-0.8
Fat 0.5-1.8
Bone 13-26
Air 12

CONTACT

Administrative contact

Please contact Karen Patching -
Desk phone: +64 (0)9 375 7085
Email: karenp@adhb.govt.nz

c/- Department of Anaesthesia & Perioperative Medicine
Level 8 - Support Building, Auckland City Hospital
PO Box 92024, Auckland, New Zealand