2001
ISBN: 0-662-30974-X
Cat. No.: H46-2/01-255E
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Diagnostic ultrasound is a valuable modality and is not contraindi-cated where medical benefit is expected. Furthermore, there are no confirmed biological effects on patients caused by exposures from present diagnostic ultrasound instruments. However, the possibility exists that such biological effects may be identified in the future. Therefore, the intent of these guidelines is to help equipment manufacturers and operators ensure both the prudent use of diagnostic ultrasound and the continued excellence of its safety record. To this end, the guidance in this document should help equipment operators to identify exposures that are potentially hazardous and to ensure that the exposures they use are justified.
Manufacturers are also reminded to ensure that Health Canada has licensed any of their diagnostic ultrasound devices that are offered for sale or lease in Canada. Licensing requirements can be obtained from the Licensing Division of Health Canada's Medical Devices Bureau.
This update replaces all parts of Safety Code 23 "Guidelines for the Safe Use of Ultrasound -Part 1: Medical and Paramedical Applications (1989)"
pertaining to the safe use of diagnostic ultrasound devices. Several developments in the past decade have necessitated this update. First, methods have been developed for estimating the maximum temperature elevation in exposed tissues during clinical examinations (see Sections 3.2 and 4.1). These estimates indicated that during some Doppler blood flow examinations, temperature elevations could exceed 1 °C. Computed estimates of maximum temperature elevations have been as high as 6-10 °C. Also, biological effects studies have demonstrated capillary hemorrhaging in vivo in the lungs of several mammalian species (though not humans), as a result of pulsed ultrasound exposures in the range of those available from diagnostic devices, including B-mode imaging. This effect was purely mechanical, having been found in the absence of ultrasonic heating (see Sections 3.3 and 4.2).
In addition to these discoveries, regulatory changes in the U.S.A. have increased the potential for relatively high acoustic outputs to be available (U.S Food and Drug Administration 1997). Also, a voluntary standard was developed for diagnostic ultrasound devices to provide the equipment operator with a real-time display of Thermal and Mechanical Indices. These exposure indices are related to the potential for heating or mechanical effects, respectively, during the ultrasound examination (AIUM/NEMA 1998a, Abbott 1999).
The information presented in this update summarizes these developments and forms the basis for new recommendations for users and manufacturers. The update is also heavily based on U.S. and other national and international recommendations and guidelines for the safe use of diagnostic ultrasound (Barnett, et al., 2000, AIUM 2000).
The required new terminology is in bold in the text and is explained in the Glossary of Terms, Section 6. In this glossary, the terms used in the guidelines are explained primarily for equipment operators and other interested parties. This is done in as plain language as possible without distorting the meaning of the term. Of particular note is the extension of the ALARA principle to ultrasound exposures.
Manufacturers endeavouring to implement this document's recommendations for device performance will need to consult the referenced standards and the U.S. Food and Drug Administration 510(k) guidance document (1997).
It is recommended that equipment operators implement quality assurance measures to maintain the capability of obtaining reliable diagnostic information at acoustic exposures which are As Low As Reasonably Achievable. Guidance on quality assurance methods can be found in several documents, including Guidelines of the Canadian Society of Diagnostic Medical (CSDMS 1998), as well as publications of the American Institute for Ultrasound in Medicine (AIUM 1991, AIUM 1995a, AIUM 1995b).
As the quality of diagnostic information depends, in part, on operator training, it is also recommended that sonographers (ultrasound technologists) be appropriately qualified and registered with either the Canadian Association of Registered Diagnostic Ultrasound Professionals (CARDUP) or the American Registry of Diagnostic Medical Sonographers (ARDMS).
One of the major mechanisms for adverse biological effects from ultrasound exposure of mammalian systems is the heating of tissue via absorption of the ultrasonic beam (NCRP 1992). Therefore, guidelines have been developed in terms of exposure parameters directly related to temperature rise and the biological effects of heating.
Implementation of the recommendations in this document requires a basic knowledge of the meaning of the new primary exposure parameter, the Thermal Index (TI) (AIUM/NEMA 1998a, Lopez 1998). This index is an estimate of the maximum temperature rise which could occur in ultrasonically heated tissue during an ultrasound examination. To distinguish it from an actual temperature elevation, the TI is unitless, being normalized to a temperature elevation of 1 °C. However, in varying with changes in the user control settings, the TI is directly proportional to the potential for heating. The Thermal Index is computed from directly measurable properties of the ultrasonic field, as determined in water under standard conditions. The methods of measurement are described in the Acoustic Output Measurement Standard for Diagnostic Ultrasound Equipment (AIUM/NEMA 1998b). The methods of computation are described in the Standard for Real-Time Display of Thermal and Mechanical Acoustic Output Indices on Diagnostic Ultrasound Equipment (AIUM/NEMA 1998a). A computed index is used because it is not feasible to monitor the actual temperature elevation in a clinical examination. In addition, the complexity of the conditions also precludes calculation of the actual temperature elevation.
There are three user-selectable TI categories which can be displayed (AIUM/NEMA 1998a, Lopez 1998). The Soft Tissue Thermal Index (TIS) is meant to be displayed for examinations in which the ultrasound beam travels a path which is made up principally of homogeneous soft tissue or a soft tissue/fluid path, as in a first trimester fetal examination or an abdominal examination. The Bone Thermal Index (TIB) is applicable to examinations in which bone is exposed to ultrasound, as could occur during Doppler blood flow examinations of a second or third trimester fetus. The Cranial Bone Thermal Index (TIC) pertains to examinations in which bone is at or very near the surface of the transducer, such as during transcranial, Doppler blood flow examinations.
A number of experimental and theoretical studies provide support for the three types of Thermal Index. Earlier studies have been thoroughly documented in two major reports on the subject (NCRP 1992, AIUM 1993). Since the publication of these documents, more recent clinical (Ramnarine, et al., 1993, Siddiqi, et al., (1995)) and experimental (Bosward, et al., 1993, O'Neill, et al., (1994), Duggan, et al, . 1995, Doody, et al., 1999) research has provided further evidence to support the models used to determine the different types of Thermal Index. The Standard for Real-Time Display of Thermal and Mechanical Acoustic Output Indices on Diagnostic Ultrasound Equipment (AIUM/NEMA 1998a)also provides brief rationales for the different types of Thermal Index.
The clinical effect of an exposure depends on the nature and degree of tissue injury. This can be assessed from biological effects studies. Several extensive reviews have been published regarding the adverse biological effects of ultrasonic heating based on animal studies, particularly in mammalian species (Lele 1985, NCRP 1992, WFUMB 1992, AIUM 1993, WFUMB 1998). With regard to adult tissues, the available literature suggests that tissue temperature elevations in the range of 8-10 °C, sustained for 1 to 2 minutes will cause tissue injury (Bly, et al., 1992, Lele 1985). The reviews have also considered studies of teratogenic effects, usually on the developing brain, due to whole body heating of the embryo or fetus. The recommendations resulting from these reviews can be succinctly expressed as follows (WFUMB 1998):
In addition, it has been reported that water immersion body heating of rats yielded the development of encephalocoeles in the rat fetuses in as little as 1 minute at a temperature elevation of 5 °C above normal physiological temperature. (WFUMB 1998).
For temperature elevations greater than 1.5 °C above normal physiological levels (37 °C), this information can be approximately matched to a functional form recommended by the NCRP (NCRP 1992). This yields an equation for combinations of temperature elevation and time which should be considered potentially hazardous:
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where t is the time in minutes at the specified temperature and
is the temperature elevation above normal (37 °C).
Barnett, et al., (1997) have recently published an updated review of thermal effects, focussing on the potential for effects on the fetus. They note that there is little information on the teratogenic effects from localized heat damage by ultrasound.
To determine whether an exposure is justified, the equipment operator must assess whether reliable diagnostic information can be achieved and the severity and likelihood of an adverse health effect. To address the potential effects due to heating, estimates of the maximum exposures from various devices have been made in terms of the AIUM/NEMA Thermal Index and a method recommended by the National Council for Radiation Protection and Measurement (NCRP 1992) for estimating maximum temperature elevations.
As indicated in Sections 3.2 and 4.1.2, the dwell time is also an important parameter when considering the potential for a biological effect due to heating. One study found that the dwell time in fetal Doppler carotid artery exams was in the range of 4 to 80 seconds with a mean of 31 seconds (Duggan and McCowan 1993).
An assessment of the clinical significance of ultrasonic heating from diagnostic ultrasound devices depends upon estimates of the potential acoustic exposure. For equipment available prior to the implementation of the Output Display Standard in 1993, Patton, et al, . (1994) found no real-time B-mode devices with Thermal Indices exceeding 1, consistent with the conclusions of the World Federation for Ultrasound in Medicine and Biology (WFUMB 1998). The vast majority of M-mode devices yielded Thermal Indices less than 1, with the largest TIB being 1.4. The maximum Thermal Indices for general pulsed Doppler devices were 1.3 for soft tissue exposure (TIS) and 2.8 for exposure of bone (TIB). The majority of the Doppler console/transducer/mode/intended use combinations (samples) yielded Thermal Indices less than 1. For peripheral vascular devices, most of the samples yielded TIB values greater than 1. The maxima were 2.2 and 2.8, for soft tissue and bone respectively. For colour flow Doppler, six of the samples (19%) yielded TIS values greater than 1, with the maximum Thermal index being 2.3.
The results of one major survey of the directly measured properties of the ultrasound field, acoustic pressure and power, suggest that acoustic output may have risen since the implementation of the Output Display Standard. However, this is not clear from the information made available in the published study (Henderson, et al., 1995). It is plausible that changes to the U.S. FDA 510(k) guidance document in 1993 have led to an increase in the number of devices with acoustic output approaching the limits recommended in Section 2.4. Although two surveys have been made of Thermal Index values since that time (Shaw, et al., 1997, 1998), a comparison between devices sold before and after 1993 cannot be made from the published report.
If the path through the bladder for a 1st trimester fetal examination is more than 5 cm, computed estimates of the maximum temperature elevation according to the NCRP method (NCRP 1992) can exceed those given by the AIUM/NEMA Thermal Indices by as much as a factor of 2-3.. The evidence on propagation paths during ultrasound examinations in the study by Ramnarine, et al., (1993), suggests that the TIS might be exceeded by a factor of 2-3 for as many as 40% of 1st trimester transabdominal examinations where the path through the bladder is more than 5 cm.
However, other evidence supports the expectation that, only in more unusual circumstances, would the NCRP estimate indicate a significantly different need for exposure reduction than would be provided by the TI. For each diagnostic ultrasound device in the sample studied by Patton, et al., (1994), the TI was compared to the NCRP estimates. It was found that about 95% of the TIS values were within a factor of 2 of the corresponding NCRP estimates. In addition, Bly, et al., (1992) found that for 236 samples, the NCRP estimate of maximum temperature elevation did not exceed 1.6 °C for trans-abdominal, pulsed Doppler examination of a first trimester fetus. Other calculations made for non-autoscanning transducers with well defined focusing geometries and a derated spatial peak time average intensity, 2, (Bly, et al., 1992, AIUM 1993) also Ispta.3 , of 720 mW/cm yielded computed estimates of maximum temperature elevation which were approximately 2 °C.
There is also evidence to support the expectation that for 2nd and 3rd trimester exposures, only in relatively unusual circumstances would the NCRP estimate indicate a significantly different need for exposure reduction than would be provided by the TI. First, in the study by Ramnarine, et al., (1993), all of the propagation paths yielded ultrasound attenuation greater than or equal to 0.3 dB/cm-MHz, the value used as the basis for the tissue models in the Output Display Standard. Furthermore, the vast majority of samples in the study by Bly, et al, . (1992) yielded maximum temperature elevations of less than 4 °C for heating of second trimester fetal bone. In the study by Patton, et al, . (1994), the largest temperature elevation calculated according to the NCRP method was 5.9 °C. This occurred for a transducer with a 10.5 cm focal depth. This evidence suggests that only in highly unusual circumstances would there be a significantly different need for exposure reduction than would be provided by the TI.
Carstensen, et al., (1992) addressed the potential for ultrasonic heating during an echocardiography examination. They considered the primary heating concern to be the patient's rib(s), particularly if the patient was not able to provide an indication of discomfort or pain. It was noted that this would be the case in some pediatric examinations. Carstensen and co-workers calculated that most diagnostic ultrasound devices would not be able to ultrasonically heat the ribs by more than 1.5 °C. However, they did indicate that 1 pulsed Doppler model appeared to have the capability of heating to about 3-6 °C.
The information provided above suggests that, in most clinical examinations, exposures are not sufficient to cause adverse health effects due to ultrasonic heating. However, the maximum temperature elevations resulting from ultrasound exposure during Doppler blood flow examinations can be well above the normal diurnal variation of 1 °C. Also, in rare circumstances, the maximum potential temperature elevations appear to be near to thresholds for tissue injury for plausible clinical dwell times.
Transducer self-heating has been known to occur with diagnostic ultrasound devices and it has the potential to be a substantial source of heating (Duck, et al., 1989). Although the tissue heating should be localized to the region near the contact surface, the additional heating could be a cause for concern during transcranial, transvaginal, transrectal or transesophogeal examinations (NCRP 1992, WFUMB 1998).
Surveys of diagnostic ultrasound devices sold in Canada were last made in 1990. They indicated that, normally, devices were sold with acoustic intensities less than the limits recommended in Section 2.4 of these guidelines. These limits effectively constrain the potential for ultrasonic heating by diagnostic ultrasound devices. Therefore, having these limits on the device and using the real-time display of Thermal Indices, it should be possible to ensure that there is very little risk to the patient from ultrasonic heating.
In the absence of heating, biological effects at diagnostic exposure levels have been observed in mammalian tissues with stable gas bodies, such as lung (WFUMB 1998, AIUM 2000), and intestine. Such effects have also been observed in other tissues after injection of ultrasound gas contrast agents (microbubbles). Therefore, guidelines have been developed in terms of an exposure parameter directly related to mechanical (non-thermal) effects. At or below the recommended output limits of Section 2.4 (MI = 1.9), mechanical effects are far less likely to be important in obstetrical ultrasound because of the absence of gas bodies.
Implementation of the recommendations in this document requires a basic knowledge of the meaning of the new primary exposure parameter for mechanical effects, the Mechanical Index (MI) (AIUM/NEMA 1998a, Lopez 1998). The development of the Mechanical Index has been described in detail elsewhere (AIUM/NEMA 1998a, AIUM 1993, Apfel and Holland 1991). It is approximately the largest rarefaction pressure (in MPa) in a soft-tissue attenuated ultrasound beam, divided by the square root of the centre frequency (in MHz) of the ultrasound pulse.
The MI is related to the potential for hemorrhaging of the pulmonary alveolar capillaries due to ultrasonic exposure of the lung during a diagnostic ultrasound examination. The threshold for lung hemorrhage depends on the ultrasonic pressure at the surface of the patient's lung divided by the square root of the centre frequency of the ultrasonic pulse (AIUM 1993). Although this quantity and the MI may not always be in direct proportion, in many cases, the MI provides a relative indication of the potential for lung hemorrhage due to ultrasound exposure. It can also provide an approximate relative indication of the potential for biological effects in the presence of contrast agents (AIUM 2000).
Hemorrhaging of lung capillaries is the first and most thoroughly studied mechanical biological effect which has been observed in mammals at diagnostically relevant exposures. Beginning with the study by Child, et al., (1990), this effect has also been observed in several laboratories and in several mammalian species when the lung was directly exposed by pulsed ultrasound (Dalecki, et al., 1997, Baggs, et al, . 1996, Holland, et al., 1996, Zachary and O'Brien 1995, Tarantal and Canfield 1994, Frizzell, et al., 1994). The acoustic pressures, centre frequencies, pulse durations and pulse repetition rates were at diagnostically relevant values in the studies. The species included swine, rat, rabbit, monkey and mouse. The species with lungs most similar to humans were monkey and swine. Studies prior to 1993 have been summarized elsewhere (AIUM 1993). Some of the studies published after 1993 are summarized below in chronological order. More detailed reviews have also either been recently published or are in preparation (WFUMB 1998, AIUM 2000, NCRP in preparation).
Tarantal and Canfield (1994) reported findings of multiple, circular hemorrhagic foci of 1 - 10 mm diameter in the lungs of monkeys directly exposed by ultrasound. The lesions were usually near the pleural surface and appeared to originate from alveolar capillaries. A clinical scanner operating in "triple mode"(B-mode imaging + colour Doppler + pulsed Doppler)at maximum output was used to provide the exposure. The monkeys ranged in age from 3 months to 5 years (infant to young adult). The frequency was 4 MHz, with a pulse duration of 0.65 microseconds and a PRF of 1515 Hz. The rarefaction pressure was maximal at 1.2 cm depth where the MI was 1.8. The exposure duration was 5 minutes. The chest wall thickness in the monkeys was 0.3 to 1.2 cm and the transducer was held directly to the chest.
O'Brien and Zachary (1997) found evidence for lung hemorrhaging in adult rabbits and mice after exposure to pulsed wave ultrasound for 5 minutes with a commercial diagnostic ultrasound imaging system operating at 3 and 6 MHz, with MI values between 0.8 and 2.2. All exposures were above threshold. However, in adult pigs(10-12 weeks old, weighing about 30 kg), no hemorrhaging was observed.
Dalecki and co-workers (Dalecki, et al., 1997, Baggs, et al., 1996) reported lung hemorrhaging in neonatal and 10 day old swine after exposure by a stationary 2.3 MHz ultrasound beam with a pulse length of 10 microseconds and a 100 Hz pulse repetition frequency. The exposure duration at a single location was between 10 s and 2 minutes. In water, at the surface of the animal, the maximum negative pressure at threshold was about 1.1-1.4 Mpa. The threshold pressure at the surface of the lung was reported as 0.7-1.0 MPa. This quantity divided by the square root of the centre frequency has a value between 0.5 and 0.7. Exposures at a pressure 1.5x the threshold value showed 1 - 1.5 mm focal hemorrhages. At a factor of 2 - 3 above threshold pressure, clearly defined hemorrhagic areas were observed with linear dimensions up to 6 mm. Damage was restricted to single lobules and all hemorrhages were subcapsular, with no rupture of the parietal pleura.
Dalecki, et al., (1997) summarized the results of studies about the way in which the pressure threshold for lung hemorrhage depended on other parameters of the ultrasound exposure. These parameters included centre frequency, pulse duration and exposure duration (Holland, et al., 1996, Child, et al., 1990). The studies indicated that the pressure threshold increases as the square root of the centre frequency and that reducing the pulse duration by a factor of 10 increases the pressure threshold by a factor of 2. The threshold of lung hemorrhaging was found to be a weak function of exposure duration.
Meltzer, et al.,(1998) found no evidence of hemorrhaging after intraoperative transesophageal echocardiography in adults where the MI was 1.3.
There was also evidence of hemorrhaging in murine intestine (Dalecki, et al., 1995) after 5 minutes of exposure to ultrasound exposure at diagnostically relevant frequencies, pulse durations (10 µs) and pulse repetition frequencies (100 Hz). The effect occurred in the absence of significant heating. At 2.4 and 3.6 MHz, the threshold pressure divided by the square root of the frequency was approximately 1.9.
A preliminary report has also been published by Skyba, et al, . (1998) of microbubble destruction of rat muscle capillaries in vivo using 2.3 MHz ultrasound at reported MI values ranging from 0.4 to 1. In another study, Miller and Gies (1998) injected mice with gas contrast agents and demonstrated significant enhancements in the generation of petechiae in the mouse intestine due to pulsed ultrasound exposure at 1 MHz with a 10 microsecond pulse duration and exposure levels as low as 1 MPa.
Recently, a study has been published (Dalecki, et al., 1999) that describes hemorrhaging in murine fetuses exposed to pulsed ultrasound with 10 microsecond pulses delivered with a pulse repetition frequency of 100 Hz. In this case, the hemorrhaging appeared near developing bone. Gas bodies did not appear to be a relevant factor. At 1.2 MHz, the negative pressure threshold for hemorrhage to the fetal head was about 2.5 MPa. No statistically significant hemorrhage was found at frequencies of 2.4 and 3.6 MHz at the highest negative pressure of 5 MPa.
To determine whether an exposure is justified, the equipment operator must assess whether reliable diagnostic information can be achieved as well as the severity and likelihood of an adverse health effect.
Carstensen and co-workers (Carstensen, et al., 1992, Baggs, et al, . 1996) discussed the likelihood of finding clinical ultrasound exposures above the thresholds for capillary lung hemorrhage found in the experimental studies noted in Section 4.2.2. Their conclusion was that the largest outputs available from equipment in 1992 were very near the thresholds of macroscopic hemorrhage of lung tissue, if exposure was directly over the lung in an echocardiographic exam. This was considered the most common way in which the lung would be exposed.
It is plausible that more recent devices have higher output levels and may exceed the thresholds for lung hemorrhaging for the type of exposure described above. The output levels for the devices considered by Carstensen and co-workers are expected to have been similar to those in the survey of Patton, et al., (1994). In that study, it was found that 14 of 266 samples yielded MI values greater than 1, the largest being 1.3. However, current equipment has MI values as high as 1.9. This is the current limit for diagnostic ultrasound devices in the U.S. FDA 510(k) guidance document. Therefore, commercial devices with these values of MI appear to be able to generate suprathreshold levels.
The potential for lung hemorrhaging was found to be greater for less typical diagnostic procedures, where the focus of the sound beam could strike the surface of lung tissue. Baggs, et al., (1996) stated that this could occur if a standoff is used and the lung tissue is near the surface of the chest. They noted that the focus of the beam could also strike the surface of lung tissue at the far side of the heart, particularly in pediatric or transesophageal applications. In these circumstances, it is estimated that devices with MI values of 1.9 could lead to exposures above the thresholds for lung hemorrhaging; by about factors of 1.5 and 3 for 1 microsecond and 10 microsecond pulse lengths, respectively. The 1 microsecond pulse length is typical for Doppler and B-mode imaging exams, although pulse durations up to 10 microseconds are available in some pulsed Doppler modes. This indicates that, for such exposures, there is a risk of some pulmonary alveolar hemorrhaging of the capillaries for neonatal or infant examinations.
The evidence concerning the biological effects studies and the acoustic outputs of diagnostic ultrasound devices, suggests that a cautious but reasonable approach is to assume that, if MI exceeds 1, there is some risk of capillary hemorrhaging on the lung surface in diagnostic ultrasound examinations of neonates and infants in which the lung is exposed. However, the long term implications of the injury may not be serious (Baggs, et al., 1996). For example, Tarantal and Canfield (1994) described the hemorrhage observed in their study as anatomically mild. In both monkey and swine studies, the pathology did not indicate any disruption of the alveolar architecture. Therefore, clinically, recovery of the lesions would be expected upon the resorption of blood and reconstitution of existing architecture. No symptoms suggestive of any respiratory distress would be expected because of the lung's ability to compensate and the focal nature of the hemorrhages. Although there are no published results on whether the outcome would differ in the presence of other disease, hemorrhaging could be more extensive in the presence of coagulation disorders.
It is unlikely that there would be any significant intestinal hemorrhaging, even at the highest MI values available. However, pathologic conditions inhibiting intestinal peristalsis or promoting submucosal gas collections may increase the likelihood of such an effect.
Although studies are preliminary and the clinical significance has not been demonstrated, it is important that equipment operators be aware of the increased potential for capillary damage during a diagnostic ultrasound examination when GCAs are used, particularly in applications where malignant tumours may be exposed.
A maximum attainable value of 1.9 for the MI greatly reduces the potential for clinically significant damage from mechanical effects during diagnostic ultrasound examinations. If thresholds for biological effects must be exceeded to obtain useful diagnostic information, an examination technique that uses the real-time display of the Mechanical Index should make it relatively easy to ensure that the risk to the patient from mechanical effects is clinically justified. Above biological effects thresholds, the ALARA principle can be implemented by lowering the MI and/or reducing the dwell time to help minimize the severity of any potential injury, if required.
Section 6 (Glossary) provides more information about the extension of the ALARA principle to diagnostic ultrasound.