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Diagnostic ultrasound ( PDFDrive )

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CHAPTER 2 Biologic Effects and Safety 35

to the operator regarding the relative potential for bioefects.

herefore informed decision making is important concerning

the possible adverse efects of ultrasound in relation to the desired

diagnostic information. Current FDA regulations that limit the

maximum output are still in place, but in the future, systems

might allow sonographers and physicians the discretion to increase

acoustic output beyond a level that might induce a biologic

response.

Although the choices made during sonographic examinations

may not be equivalent to the risk-versus-beneit decisions associated

with imaging modalities using ionizing radiation, the operator

will be increasingly responsible for determining the diagnostically

required amount of ultrasound exposure. hus the operator

should know the potential bioefects associated with ultrasound

exposure. Patients also need to be reassured about the safety of

a diagnostic ultrasound scan. he scientiic community has

identiied some potential bioefects from sonography, and although

no causal relation has been established, it does not mean that

no efects exist. herefore it is important to understand the

interaction of ultrasound with biologic systems.

PHYSICAL EFFECTS OF SOUND

he physical efects of sound can be divided into two principal

groups: thermal and nonthermal. Most medical professionals

recognize the thermal efects of elevated temperature on tissue,

and the efects caused by ultrasound are similar to those of any

localized heat source. With ultrasound, the heating mainly results

from the absorption of the sound ield as it propagates through

tissue. However, “nonthermal” sources can generate heat as well.

Many nonthermal mechanisms for bioefects exist. Acoustic

ields can apply radiation forces (not ionizing radiation) on the

structures within the body at both the macroscopic and the

microscopic levels, resulting in exerted pressure and torque. he

temporal average pressure in an acoustic ield is diferent from

the hydrostatic pressure of the luid, and any object in the ield

is subject to this change in pressure. he efect is typically

considered smaller than other efects because it relies on less

signiicant factors in the formulation of the acoustic ield. Acoustic

ields can also cause motion of luids. Such acoustically induced

low is called streaming.

Acoustic cavitation is the action of acoustic ields within a

luid to generate bubbles and cause volume pulsation or even

collapse in response to the acoustic ield. he result can be heat

generation and associated free radical formation, microstreaming

of luid around the bubble, radiation forces generated by the

scattered acoustic ield from the bubble, and mechanical actions

from bubble collapse. he interaction of acoustic ields with

bubbles or “gas bodies” (as they are generally called) has been

a signiicant area of bioefects research for many years.

THERMAL EFFECTS

Ultrasound Produces Heat

As ultrasound propagates through the body, energy is lost through

attenuation. Attenuation causes loss of penetration and the

inability to image deeper tissues. Attenuation is the result of two

processes, scattering and absorption. Scattering of the ultrasound

results from the redirection of the acoustic energy by tissue

encountered during propagation. With diagnostic ultrasound,

some of the acoustic energy transmitted into the tissue is scattered

back in the direction of the transducer, termed backscatter, which

allows a signal to be detected and images to be made. Energy

also is lost along the propagation path of the ultrasound by

absorption. Absorption loss occurs substantially through the

conversion of the ultrasound energy into heat. his heating

provides a mechanism for ultrasound-induced bioefects.

Factors Controlling Tissue Heating

he rate of temperature increase in tissues exposed to ultrasound

depends on several factors, including spatial focusing, ultrasound

frequency, exposure duration, and tissue type.

Spatial Focusing

Ultrasound systems use multiple techniques to concentrate or

focus ultrasound energy and improve the quality of measured

signals. he analogy for light is that of a magnifying glass. he

glass collects all the light striking its surface and concentrates it

into a small region. In sonography and acoustics in general, the

term intensity is used to describe the spatial distribution of

ultrasonic power (energy per unit time), where intensity = power/

area and the area refers to the cross-sectional area of the ultrasound

beam. Another common beam dimension is the beam

width at a speciied location of the ield. If the same ultrasonic

power is concentrated into a smaller area, the intensity will

increase. Focusing occurs on both transmission of the ultrasound

and when receiving the backscattered signals used to form the

image. he transmit focusing is of importance in terms of potential

biologic efects because this phenomenon controls the applied

energy to the tissue. here are ultrasound imaging systems that

use plane wave transmission or limited transmit focusing, which

may reduce the local intensity, but all ultrasound systems must

still operate under the FDA limits.

Focusing in an ultrasound system can be used to improve

the spatial resolution of the images. he side efect is an increased

potential for bioefects caused by heating and cavitation. In

general, the greatest heating potential is between the scanhead

and the focus, but the exact position depends on the focal distance,

tissue properties, and heat generated within the scanhead itself.

Returning to the magnifying glass analogy, most children

learn that the secret to incineration is a steady hand. Movement

distributes the power of the light beam over a larger area, thereby

reducing its intensity. he same is true in ultrasound imaging.

hus imaging systems that scan a beam through tissue reduce

the spatial average intensity. Spectral Doppler and M-mode

ultrasound imaging maintain the ultrasound beam in a stationary

position (both considered unscanned modes) and therefore

provide no opportunity to distribute the ultrasonic power

spatially, whereas color low Doppler, power mode Doppler,

and B-mode (also called gray-scale) ultrasound imaging require

that the beam be moved to new locations (scanned modes)

at a rate suicient to produce the real-time nature of these

imaging modes.

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