# EN 62359:2011/A1:2018

(Amendment)## Ultrasonics - Field characterization - Test methods for the determination of thermal and mechanical indices related to medical diagnostic ultrasonic fields

## Ultrasonics - Field characterization - Test methods for the determination of thermal and mechanical indices related to medical diagnostic ultrasonic fields

## Ultraschall - Charakterisierung von Feldern - Prüfverfahren für die Ermittlung des thermischen und des mechanischen Indexes, bezogen auf medizinische Ultraschalldiagnostikfelder

## Ultrasons - Caractérisation du champ - Méthodes d'essai pour la détermination d'indices thermique et mécanique des champs d'ultrasons utilisés pour le diagnostic médical

## Ultrazvok - Karakterizacija polj - Preskusne metode za ugotavljanje termičnih in mehanskih znakov glede medicinskih diagnostičnih ultrazvočnih polj - Dopolnilo A1

### General Information

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### Standards Content (sample)

SLOVENSKI STANDARD

SIST EN 62359:2011/A1:2018

01-april-2018

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Ultrasonics - Field characterization - Test methods for the determination of thermal and

mechanical indices related to medical diagnostic ultrasonic fieldsUltraschall - Charakterisierung von Feldern - Prüfverfahren für die Ermittlung des

thermischen und des mechanischen Indexes bezogen auf medizinischeUltraschalldiagnostikfelder

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Ta slovenski standard je istoveten z: EN 62359:2011/A1:2018

ICS:

11.040.55 'LDJQRVWLþQDRSUHPD Diagnostic equipment

SIST EN 62359:2011/A1:2018 en

2003-01.Slovenski inštitut za standardizacijo. Razmnoževanje celote ali delov tega standarda ni dovoljeno.

---------------------- Page: 1 ----------------------SIST EN 62359:2011/A1:2018

---------------------- Page: 2 ----------------------

SIST EN 62359:2011/A1:2018

EUROPEAN STANDARD EN 62359:2011/A1

NORME EUROPÉENNE

EUROPÄISCHE NORM

January 2018

ICS 17.140.50

English Version

Ultrasonics - Field characterization - Test methods for the

determination of thermal and mechanical indices related to

medical diagnostic ultrasonic fields

(IEC 62359:2010/A1:2017)

Ultrasons - Caractérisation du champ - Méthodes d'essai Ultraschall - Charakterisierung von Feldern - Prüfverfahren

pour la détermination d'indices thermique et mécanique des für die Ermittlung des thermischen und des mechanischen

champs d'ultrasons utilisés pour le diagnostic médical Indexes bezogen auf medizinische

(IEC 62359:2010/A1:2017) Ultraschalldiagnostikfelder(IEC 62359:2010/A1:2017)

This amendment A1 modifies the European Standard EN 62359:2011; it was approved by CENELEC on 2017-11-03. CENELEC members

are bound to comply with the CEN/CENELEC Internal Regulations which stipulate the conditions for giving this amendment the status of a

national standard without any alteration.Up-to-date lists and bibliographical references concerning such national standards may be obtained on application to the CEN-CENELEC

Management Centre or to any CENELEC member.This amendment exists in three official versions (English, French, German). A version in any other language made by translation under the

responsibility of a CENELEC member into its own language and notified to the CEN-CENELEC Management Centre has the same status as

the official versions.CENELEC members are the national electrotechnical committees of Austria, Belgium, Bulgaria, Croatia, Cyprus, the Czech Republic,

Denmark, Estonia, Finland, Former Yugoslav Republic of Macedonia, France, Germany, Greece, Hungary, Iceland, Ireland, Italy, Latvia,

Lithuania, Luxembourg, Malta, the Netherlands, Norway, Poland, Portugal, Romania, Serbia, Slovakia, Slovenia, Spain, Sweden,

Switzerland, Turkey and the United Kingdom.European Committee for Electrotechnical Standardization

Comité Européen de Normalisation Electrotechnique

Europäisches Komitee für Elektrotechnische Normung

CEN-CENELEC Management Centre: Rue de la Science 23, B-1040 Brussels

© 2018 CENELEC All rights of exploitation in any form and by any means reserved worldwide for CENELEC Members.

Ref. No. EN 62359:2011/A1:2018 E---------------------- Page: 3 ----------------------

SIST EN 62359:2011/A1:2018

EN 62359:2011/A1:2018 (E)

European foreword

The text of document 87/661/FDIS, future edition 1 of IEC 62359:2010/A1:2017, prepared by IEC/TC

87 "Ultrasonics" was submitted to the IEC-CENELEC parallel vote and approved by CENELEC as

EN 62359:2011/A1:2018.The following dates are fixed:

• latest date by which this document has (dop) 2018-08-03

to be implemented at national level by

publication of an identical national

standard or by endorsement

• latest date by which the national (dow) 2020-11-03

standards conflicting with this

document have to be withdrawn

Attention is drawn to the possibility that some of the elements of this document may be the subject of

patent rights. CENELEC shall not be held responsible for identifying any or all such patent rights.

Endorsement noticeThe text of the International Standard IEC 62359:2010/A1:2017 was approved by CENELEC as a

European Standard without any modification.---------------------- Page: 4 ----------------------

SIST EN 62359:2011/A1:2018

EN 62359:2011/A1:2018 (E)

Replace the Annex ZA by the following:

Annex ZA

(normative)

Normative references to international publications

with their corresponding European publications

The following documents are referred to in the text in such a way that some or all of their content

constitutes requirements of this document. For dated references, only the edition cited applies. For

undated references, the latest edition of the referenced document (including any amendments) applies.

NOTE 1 When an International Publication has been modified by common modifications, indicated by (mod), the relevant EN/HD

applies.NOTE 2 Up-to-date information on the latest versions of the European Standards listed in this annex is available here:

www.cenelec.eu.P ublication Year Title EN/HD Year

IEC 60601-2-37 2007 Medical electrical equipment -- Part 2-37: EN 60601-2-37 2008

Particular requirements for the basic safetyand essential performance of ultrasonic

medical diagnostic and monitoring

equipment

- - + A11 2011

+ A1 2015 + A1 2015

IEC 61157 2007 Standard means for the reporting of the EN 61157 2007

acoustic output of medical diagnostic

ultrasonic equipment

+ A1 2013 + A1 2013

IEC 61161 2013 Ultrasonics - Power measurement - EN 61161 2013

Radiation force balances and performance

requirements

IEC 61828 2001 Ultrasonics - Focusing transducers - EN 61828 2001

Definitions and measurement methods for

the transmitted fields

IEC 62127-1 2007 Ultrasonics - Hydrophones -- Part 1: EN 62127-1 2007

Measurement and characterization of

medical ultrasonic fields up to 40 MHz

+ A1 2013 + A1 2013

IEC 62127-2 2007 Ultrasonics - Hydrophones -- Part 2: EN 62127-2 2007

Calibration for ultrasonic fields up to 40 MHz

IEC 62127-3 2007 Ultrasonics - Hydrophones -- Part 3: EN 62127-3 2007

Properties of hydrophones for ultrasonic

fields up to 40 MHz

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SIST EN 62359:2011/A1:2018

---------------------- Page: 6 ----------------------

SIST EN 62359:2011/A1:2018

IEC 62359

Edition 2.0 2017-09

INTERNATIONAL

STANDARD

AMENDMENT 1

Ultrasonics – Field characterization –

Test methods for the determination of thermal and mechanical indices related

to medical diagnostic ultrasonic fields

INTERNATIONAL

ELECTROTECHNICAL

COMMISSION

ICS 17.140.50 ISBN 978-2-8322-4821-8

Warning! Make sure that you obtained this publication from an authorized distributor.

® Registered trademark of the International Electrotechnical Commission---------------------- Page: 7 ----------------------

SIST EN 62359:2011/A1:2018

– 2 – IEC 62359:2010/AMD1:2017

© IEC 2017

FOREWORD

This amendment has been prepared by IEC technical committee 87: Ultrasonics.

The text of this amendment is based on the following documents:

FDIS Report on voting

87/661/FDIS 87/665/RVD

Full information on the voting for the approval of this amendment can be found in the report

on voting indicated in the above table.The committee has decided that the contents of this amendment and the base publication will

remain unchanged until the stability date indicated on the IEC website under"http://webstore.iec.ch" in the data related to the specific publication. At this date, the

publication will be• reconfirmed,

• withdrawn,

• replaced by a revised edition, or

• amended.

A bilingual version of this publication may be issued at a later date.

_____________

Introduction to Amendment

The second edition of IEC 62359 was published in 2010. Since then,

IEC 60601-2-37:2007/AMD1:2015 has been published and calls for provision of attenuated

spatial peak temporal average intensity, I , and attenuated spatial peak pulsespta,a

average intensity, I , at specific spatial maximum points in the ultrasonic field on the

sppa,abeam axis. No IEC standard describes the determination of these quantities at these specific

positions. IEC 62359 for determining the thermal indices currently uses similar values at other

positions, therefore, the determination of attenuated spatial peak temporal average

, and attenuated spatial peak pulse average intensity, I , has beenintensity, I

spta,a sppa,a

added as an annex in this amendment.

Additionally, references to newly published collateral standards have been updated.

_____________---------------------- Page: 8 ----------------------

SIST EN 62359:2011/A1:2018

IEC 62359:2010/AMD1:2017 – 3 –

© IEC 2017

2 Normative references

Replace the first reference by the following:

IEC 60601-2-37:2007, Medical electrical equipment – Part 2-37: Particular requirements for

the basic safety and essential performance of ultrasonic medical diagnostic and monitoring

equipmentIEC 60601-2-37:2007/AMD1:2015

Replace the second reference by the following:

IEC 61157:2007, Standard means for the reporting of the acoustic output of medical

diagnostic ultrasonic equipmentIEC 61157:2007/AMD1:2013

Replace, in the third reference, "IEC 61161:2006" by "IEC 61161:2013".

Replace the fifth reference by the following:

IEC 62127-1:2007, Ultrasonics – Hydrophones – Part 1: Measurement and characterization of

medical ultrasonic fields up to 40 MHzIEC 62127-1:2007/AMD1:2013

3 Terms and definitions

Replace the first existing paragraph by the following new paragraph:

For the purposes of this document, the terms and definitions given in IEC 60601-2-37,

IEC 62127-1, IEC 62127-2, IEC 62127-3, IEC 61157 and IEC 61161 apply. Several of these

are repeated below for convenience and others are listed because they have been modified

for application to this standard.3.3

acoustic repetition period

Replace the existing definition by the following new definition:

time interval between corresponding points of consecutive cycles, pulses or scans, depending

on the current operating modeAdd the following new NOTES 2 and 3:

NOTE 2 For continuous wave modes, the acoustic repetition period is the time interval between corresponding

points of consecutive cyclesNOTE 3 For combined operating modes where transmit pulsing of the constituent modes may be interrupted,

the arp determination should take into account non-pulsing time to calculate an average period.

Replace "NOTE 2" by NOTE 4".3.4

acoustic working frequency

Replace, in the existing definition, the words "at the position corresponding to the spatial-

peak temporal-peak acoustic pressure" by "on the beam axis, beyond the break-point

depth, corresponding to depth of maximum pulse-intensity integral z ."pii

Replace, in existing NOTE 2, the words "at the position of maximum pulse-pressure-squared

integral" by "at the depth for peak pulse-intensity integral".---------------------- Page: 9 ----------------------

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© IEC 2017

3.7

attenuated peak-rarefactional acoustic pressure

Replace, in the existing definition, the words "at a specified distance from" by "on a plane

perpendicular to the beam axis at a specified distance z from".Replace, in the definition list after Equation (2), the words "z is the distance from the external

transducer aperture to the point of interest" by "z is the distance from the external

transducer aperture along the beam axis to the plane containing the point of interest".

3.8attenuated pulse-intensity integral

Replace, in the definition, the words "at a specified distance from" by "on a plane

perpendicular to the beam axis at a specified distance z from".Replace, in the definition list after Equation (3), the words "z is the distance from the external

transducer aperture to the point of interest" by "z is the distance from the external

transducer aperture along the beam axis to the plane containing the point of interest".

Replace "NOTE" by "NOTE 1".Add new NOTE 2:

NOTE 2 For measurement purposes of this standard, pii is equivalent to 1/(ρc) times the attenuated pulse-

pressure-squared integral at depth z, with ρc denoting the characteristic acoustic impedance of pure water.

3.9attenuated spatial-average temporal-average intensity

Replace, in the definition, the words "at a specified distance from" by "on a plane

perpendicular to the beam axis at a specified distance z from".Replace, in the definition list after Equation (4), the words "z is the distance from the external

transducer aperture to the point of interest" by "z is the distance from the external

transducer aperture along the beam axis to the plane containing the point of interest".

3.10attenuated spatial-peak temporal-average intensity

Replace, in the definition, the words "at a specified distance from" by "on a plane

perpendicular to the beam axis at a specified distance z from".Replace, in the definition list after Equation (5), the words "z is the distance from the external

transducer aperture to the point of interest" by "z is the distance from the external

transducer aperture along the beam axis to the plane containing the point of interest".

3.11attenuated temporal-average intensity

Replace, in the definition, the words "at a specified distance from" by "on a plane

perpendicular to the beam axis at a specified distance z from".Replace, in the definition list after Equation (6), the words "z is the distance from the external

is the distance from the externaltransducer aperture to the point of interest" by "z

transducer aperture along the beam axis to the plane containing the point of interest".

3.13beam-axis

Replace the term "beam-axis" by "beam axis".

---------------------- Page: 10 ----------------------

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IEC 62359:2010/AMD1:2017 – 5 –

© IEC 2017

3.17

bone thermal index

Delete, in the definition, "or neonatal cephalic (through the fontanelle)".

3.19

break-point depth

Add, after the existing definition, the words "acoustic working frequency and intensity

parameters (such as attenuated spatial-peak temporal-average intensity)"Add, after "where D is the equivalent aperture diameter" the words "for non-scanning

modes".Replace the existing NOTE 2 by the following new note:

NOTE 2 For scanning modes, use the non-scanning mode D value calculation [Equation (8)]. Do this using

the output beam area of one ultrasonic scan line; the central scan line, corresponding to the beam axis (i.e. the

line where pii MI, and f are measured).awf

3.21

cranial-bone thermal index

Replace the existing definition by the following new definition:

thermal index for applications in which the ultrasound beam passes through bone near the

beam entrance into the body, such as paediatric and adult cranial or neonatal cephalic

applications3.22

default setting

Replace, in the definition, "ultrasonic diagnostic equipment" by "medical diagnostic

ultrasonic equipment".3.23

depth for mechanical index

Replace, in the definition, the words "to the plane of maximum attenuated pulse-intensity

integral (pii )" by "to the plane of maximum attenuated pulse-pressure-squared-integral

(ppsi )".Add new NOTE 1:

NOTE 1 Because z may occur closer to the transducer than the break-point depth z , use of ppsi rather than

MI bp αpii is technically more appropriate. If z is larger than z , then z and z are equal.

α ppsi,α bp ppsi,α pii,αReplace "NOTE" by "NOTE 2".

3.24

depth for peak pulse-intensity integral

Replace the existing term, definition and note by the following new term, definition and notes:

3.24depth for maximum pulse intensity integral

depth z on the beam axis and beyond the break-point depth z from the external

transduscer aperture to the plane of maximum pulse-intensity integral (pii) as

approximated by the pulse-pressure-squared integral (ppsi)

NOTE 1 Depth for maximum pii is expressed in metres (m).

NOTE 2 Depth for maximum pii is termed "depth for peak pulse-intensity integral" in

IEC 60601-2-37:2007/AMD1:2015.---------------------- Page: 11 ----------------------

SIST EN 62359:2011/A1:2018

– 6 – IEC 62359:2010/AMD1:2017

© IEC 2017

NOTE 3 At this depth the acoustic working frequency is determined.

3.27

Discrete-perating mode

Replace the term "Discrete-perating mode" by "discrete-operating mode".

Replace, in the definition, "ultrasonic diagnostic equipment" by "medical diagnostic

ultrasonic equipment".3.28

equivalent aperture diameter

Replace the existing definition and equation by the following new definition and equation:

diameter of a circle the area A of which is the –12 dB output beam area A for non-

scanning modes and the –12 dB scanned aperture area A for scanning modes, given by

D = A(8)

Replace the existing NOTE 1 by the following new note:

NOTE 1 Equation (8) is used in the calculation of the cranial-bone thermal index; for non-scanning modes with

A = A and for scanning modes with A = A .ob sa

Add new NOTE 2:

NOTE 2 Equation (8) with A = A is also used in calculating the break-point depth.

Replace "NOTE 2" by "NOTE 3".3.33

medical diagnostic ultrasonic equipment

Replace "NOTE" by "NOTE 1".

Add new NOTE 2:

NOTE 2 IEC 60601-2-37:2007 uses the term "ultrasonic diagnostic equipment" instead of medical diagnostic

ultrasonic equipment.3.34

non-scanning mode

Replace, in the definition, the words "ultrasonic diagnostic equipment" by "medical

diagnostic ultrasonic equipment".3.37

output power

Replace, in the source, "IEC 61161:2006" by "IEC 61161:2013".

3.40

prudent-use statements

Replace the existing definition by the following new definition:

affirmations of the principle that only necessary clinical information should be acquired and

that high exposure levels and long exposure times should be avoided---------------------- Page: 12 ----------------------

SIST EN 62359:2011/A1:2018

IEC 62359:2010/AMD1:2017 – 7 –

© IEC 2017

3.44

pulse repetition period

Add new NOTE 1:

NOTE 1 In general, for non-scanning modes the pulse repetition period needs to be adjusted to represent a

‘per-second’ average taking into account interruptions-in, or non-constant, pulsing; e.g. such as may occur in

combined operating modes.Replace "NOTE" by "NOTE 2".

3.49

scanning mode

Replace, in the definition, the words "an ultrasonic diagnostic equipment" by "a medical

diagnostic ultrasonic equipment".3.54

spatial-peak temporal-average intensity

Replace the existing NOTE 1 by the following new note:

NOTE 1 For systems in combined-operating modes, the averaging time period needs to be sufficient to include

periods in which scanning or pulsing is interrupted.3.56

thermal index

Replace, in the definition, the two occurrences of the words " attenuated acoustic power" by

"attenuated output power"Add the following new definitions:

3.61

instantaneous acoustic pressure

p(t)

pressure minus the ambient pressure at a particular instant in time and at a particular point in

an acoustic fieldNOTE Instantaneous acoustic pressure is expressed in pascals (Pa).

[SOURCE: IEC 62127-1:2007, 3.33, modified – The reference to IEV 801-01-19 has been

removed in the definition]3.62

attenuated instantaneous acoustic pressure

(z,t)

value of the instantaneous acoustic pressure at time t after attenuation on a plane

perpendicular to the beam axis at a specified distance z from the source, and given by

(−a z f 20 dB)awf

p (z,t)= p(z,t)10 (26)

where

a is the acoustic attenuation coefficient;

z is the distance from the source to the point (plane) of interest;

f is the acoustic working frequency;

awf

p(z,t) is the instantaneous acoustic pressure

NOTE Attenuated instantaneous acoustic pressure is expressed in pascals (Pa).

---------------------- Page: 13 ----------------------

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– 8 – IEC 62359:2010/AMD1:2017

© IEC 2017

3.63

attenuated pulse-pressure-squared integral

ppsi (z)

time integral of the square of the attenuated instantaneous acoustic pressure, integrated

over the acoustic pulse waveform, on a plane perpendicular to the beam axis at a specified

distance z in an acoustic field2 (−a z f 20 dB) (−a z f 10 dB)

awf awf

ppsi (z)= p (z,t)dt= [p(z,t)10 ] dt= ppsi(z)×10

a a (27)

∫ ∫

where

p(z,t) is the instantaneous acoustic pressure at depth z.

a is the acoustic attenuation coefficient;

z is the distance from the source to the point (plane) of interest;

f is the acoustic working frequency;

awf

ppsi is the pulse-pressure-squared integral

NOTE 1 Attenuated pulse-pressure-squared integral is expressed in pascal squared seconds (Pa s).

NOTE 2 See definition 3.43 for the non-attenuated version; with the addition here of the perpendicular plane at

depth z.3.64

attenuated scan intensity integral

sii (z)

sum of the attenuated pulse intensity integrals in one scan (one frame of ultrasonic scan

lines) at depth zNOTE 1 Attenuated scan intensity integral is expressed in joules per square metre (Jm ).

NOTE 2 For measurement purposes of this standard, sii (z) is equivalent to 1/(ρc) times the sum of attenuated

pulse-pressure-squared integrals at depth z, for z ≥ z , with ρc denoting the characteristic acoustic impedance of

pure water.NOTE 3 See definition 3.79 for the non-attenuated version.

3.65

attenuated spatial-peak pulse-average intensity

I (z)

sppa,α

maximum value of the spatial-peak pulse-average intensity after attenuation, on a plane

perpendicular to the beam axis at a specified distance z from the source, and given by

I (z)= pii (z)sppa,a a (28)

t (z)

where

t (z) is the pulse duration at the same depth z;

pii (z) is the attenuated pulse-intensity integral at depth z

NOTE 1 Attenuated spatial-peak pulse-average intensity is expressed in watts per square metre (Wm ).

NOTE 2 For measurement purposes of this standard, pii (z) is equivalent to 1/(ρc) times the attenuated pulse-

pressure-squared integrals at depth z, ppsi (z), for z ≥ z , with ρc denoting the characteristic acoustic impedance

α bpof pure water.

NOTE 3 See definition 3.81 for the non-attenuated version.

---------------------- Page: 14 ----------------------

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IEC 62359:2010/AMD1:2017 – 9 –

© IEC 2017

3.66

attenuated sum of pulse-pressure-squared integrals

s ppsi (z)

attenuated value of the sum of pulse-pressure-squared integrals in one scan (one frame of

ultrasonic scan lines) at depth zNOTE 1 Attenuated sum of pulse-pressure-squared integrals is expressed in pascal squared seconds (Pa s).

NOTE 2 The attenuated sum of pulse-pressure-squared integrals at depth z will be equal to the sum of

attenuated pulse-pressure-squared integrals if each ultrasonic scan line in the frame which is included in the

sum has the same acoustic working frequency.NOTE 3 See F.3.1.4.2 for additional explanation.

NOTE 4 See definition 3.83 for the non-attenuated version.

3.67

depth for maximum I

sppa

sppa,max

depth z on the beam axis and beyond the break-point depth z of maximum spatial-peak

pulse-average intensityNOTE 1 Depth for maximum I is expressed in metres (m).

sppa

NOTE 2 This depth is equivalent to the depth for maximum pii.

3.68

depth for maximum I

sppa,α

sppa,α,max

depth z on the beam axis and beyond the break-point depth z of maximum attenuated

spatial-peak pulse-average intensityNOTE 1 Depth for maximum I is expressed in metres (m).

sppa,α

NOTE 2 This depth is equivalent to the depth for maximum pii .

3.69

depth for maximum I

spta

spta,max

depth z on the beam axis and beyond the break-point depth z of maximum spatial-peak

temporal-average intensityNOTE 1 Depth for maximum I is expressed in metres (m).

spta

NOTE 2 For non-scanning modes, this depth is equivalent to the depth for maximum pii. For scanning modes,

it is equivalent to the depth for maximum sii.3.70

depth for maximum I

spta,α

spta,α,max

depth z on the beam axis and beyond the break-point depth z of maximum attenuated

spatial-peak temporal-average intensityNOTE 1 Depth for maximum I is expressed in metres (m).

spta,α

NOTE 2 For non-scanning modes, this depth is equivalent to the depth for maximum pii . For scanning modes,

it is equivalent to the depth for maximum sii .3.71

depth for maximum pii

pii,α

depth z on the beam axis and beyond the break-point depth z of maximum attenuated

pulse-intensity integral---------------------- Page: 15 ----------------------

SIST EN 62359:2011/A1:2018

– 10 – IEC 62359:2010/AMD1:2017

© IEC 2017

NOTE 1 Depth for maximum pii is expressed in metres (m).

NOTE 2 This depth is equivalent to the depth for maximum ppsi , z , when z occurs beyond the break-

α ppsi,α ppsi,αpoint depth (see 3.73).

NOTE 3 Depth for maximum pii is termed "depth for peak attenuated pulse-intensity integral" in

IEC 60601-2-37:2007+IEC 60601-2-37:2007/AMD1:2015.3.72

depth for maximum ppsi

ppsi

depth z on the beam axis of maximum pulse-pressure-squared integral

NOTE 1 Depth for maximum ppsi is expressed in metres (m).

NOTE 2 When it occurs beyond the break-point depth, this depth is equivalent to the depth for maximum pii,

(see 3.24).pii

3.73

depth for maximum ppsi

ppsi,α

depth z on the beam axis of maximum attenuated pulse-pressure-squared integral

NOTE 1 Depth for maximum ppsi is expressed in metres (m).

NOTE 2 When it occurs beyond the break-point depth, this depth is equivalent to the depth for maximum pii ,

z (i.e. depth for maximum attenuated pulse-intensity integral).pii,α

NOTE 3 This depth is the depth for mechanical index, z (see 3.23).

3.74

sii

depth for maximum

sii

depth z on the beam axis and beyond the break-point depth z of maximum scan-intensity

integralNOTE 1 Depth for maximum sii is expressed in metres (m).

NOTE 2 This depth is equivalent to the depth for maximum sppsi, z , when z occurs beyond the break-

sppsi sppsipoint depth (see 3.76).

NOTE 3 Depth for maximum sii is termed "depth for peak sum of pulse-intensity integrals" in

IEC 60601-2-37:2007+IEC 60601-2-37:2007/AMD1:2015.3.75

depth for maximum sii

sii,α

depth z on the beam axis and beyond the break-point depth z of maximum attenuated

scan-intensity integralNOTE 1 Depth for maximum sii is expressed in metres (m).

NOTE 2 This depth is equivalent to the depth for maximum sppsi , z , when z occurs beyond the

α sppsi,α sppsi,αbreak-point depth (see 3.77).

NOTE 3 Depth for maximum sii is termed "depth for peak sum of attenuated pulse-intensity integrals" in

IEC 60601-2-37:2007+IEC 60601-2-37:2007/AMD1:2015.3.76

depth for maximum sppsi

sppsi

depth z on the beam axis of maximum sum of pulse-pressure-squared integrals

NOTE 1 Depth for maximum sppsi is expressed in metres (m).

---------------------- Page: 16 ----------------------

SIST EN 62359:2011/A1:2018

IEC 62359:2010/AMD1:2017 – 11 –

© IEC 2017

NOTE 2 When it occurs beyond the break-point depth, this depth is equivalent to the depth for maximum sii, z

sii(see 3.74).

NOTE 3 Depth for maximum sppsi is termed "depth for peak sum of pulse-intensity integrals" in

IEC 60601-2-37:2007+IEC 60601-2-37:2007/AMD1:2015.3.77

depth for maximum sppsi

sppsi,α

depth z on the beam axis of maximum sum of attenuated pulse-pressure-squared

integrals

NOTE 1 Depth for maximum sppsi is expressed in metres (m).

NOTE 2 When it occurs beyond the break-point depth, this depth is equivalent to the depth for maximum sii ,

z (see 3.75).sii,α

NOTE 3 Depth for maximum sppsi is termed "depth for peak sum of attenuated pulse-intensity integrals" in

IEC 60601-2-37:2007+IEC 60601-2-37:2007/AMD1:2015.3.78

pulse-average intensity

quotient of the pulse-intensity integral to the pulse duration at a particular point in an

acoustic fieldNOTE 1 This definition applies to pulses and bursts.

NOTE 2 Pulse-average intensity is expressed in watts per square metre (Wm ).

[IEC 62127-1:2007+IEC 62127-1:2007/AMD1:2013, 3.47]

3.79

scan intensity integral

sii

sum of the pulse intensity integrals in one scan (one frame of ultrasonic scan lines) at

depth z in the acoustic fieldNOTE 1 Scan intensity integral is expressed in joules per square metre (Jm ).

NOTE 2 For measurement purposes of this standard, sii is equivalent to 1/(ρc) times the sum of pulse-pressure-

squared integral at depth z where ρc is the characteristic acoustic impedance of pure water.

3.80scan repetition rate

srr

inverse of the scan repetition period (see 3.50)

NOTE Scan repetition rate is expressed in hertz (Hz).

3.81

spatial-peak pulse-average intensity

I (z)

sppa

maximum value of the pulse-average intensity on a plane perpendicular to the beam axis at

a specified distance z from the source, and given byI (z)= pii(z)

sppa (29)

t (z)

where

t (z) is the pulse duration at the same depth z;

pii(z) is the pulse-intensity integral at depth z

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SIST EN 62359:2011/A1:2018

– 12 – IEC 62359:2010/AMD1:2017

© IEC 2017

NOTE 1 Spatial-peak pulse-average intensity is expressed in watts per squ

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