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BS PD IEC TS 62791-2015 Ultrasonics Pulse-echo scanners Low-echo sphere phantoms and method for performance testing of gray-scale medical ultrasound scanners applicable to a broad .pdf

1、BSI Standards PublicationUltrasonics Pulse-echo scanners Low-echo spherephantoms and method for performance testing of gray-scale medical ultrasoundscanners applicable to a broadrange of transducer typesPD IEC/TS 62791:2015National forewordThis Published Document is the UK implementation of IEC/TS 6

2、2791:2015.The UK participation in its preparation was entrusted to TechnicalCommittee EPL/87, Ultrasonics.A list of organizations represented on this committee can be obtained onrequest to its secretary.This publication does not purport to include all the necessary provisions ofa contract. Users are

3、 responsible for its correct application. The British Standards Institution 2015.Published by BSI Standards Limited 2015ISBN 978 0 580 80391 8ICS 11.040.50; 17.140.50Compliance with a British Standard cannot confer immunity fromlegal obligations.This Published Document was published under the author

4、ity of theStandards Policy and Strategy Committee on 30 September 2015.Amendments/corrigenda issued since publicationDate Text affectedPUBLISHED DOCUMENTPD IEC/TS 62791:2015IEC TS 62791 Edition 1.0 2015-09 TECHNICAL SPECIFICATION Ultrasonics Pulse-echo scanners Low-echo sphere phantoms and method fo

5、r performance testing of gray-scale medical ultrasound scanners applicable to a broad range of transducer types INTERNATIONAL ELECTROTECHNICAL COMMISSION ICS 11.040.50; 17.140.50 ISBN 978-2-8322-2902-6 Registered trademark of the International Electrotechnical Commission Warning! Make sure that you

6、obtained this publication from an authorized distributor. colourinsidePD IEC/TS 62791:201 2 IEC TS 62791:2015 IEC 2015 CONTENTS FOREWORD . 6 INTRODUCTION . 8 1 Scope 10 2 Normative references 10 3 Terms and definitions 10 4 Symbols 12 5 General and environmental conditions . 13 6 Equipment required

7、. 14 6.1 General . 14 6.2 Phantom geometries . 14 6.2.1 Phantoms for use in the frequency range 2 MHz to 7 MHz . 14 6.2.2 Phantoms for use in the frequency range 7 MHz to 15 MHz including “micro-convex“ arrays 14 6.2.3 Total internal-reflection surfaces 15 6.2.4 Spatially random distribution of low-

8、echo spheres 15 6.3 Ultrasonic properties of the tissue-mimicking (TM) phantoms 15 7 Data acquisition assuming a spatially random distribution of low-echo spheres . 16 7.1 Methodology . 16 7.2 Storage of digitized image data . 17 7.3 Digital image files available from the scanner itself . 18 7.4 Ima

9、ge archiving systems . 18 8 Automated data analysis for quantifying low-echo sphere detectability 18 8.1 General . 18 8.2 Computation of mean pixel values (MPVs) 18 8.3 Determination of the LSNRm-value for a given depth interval . 21 8.3.1 Preliminaries . 21 8.3.2 Computation of the LSNRn-values and

10、 LSNRm-value in a given depth interval 21 8.3.3 Standard error corresponding to each LSNRn-value 21 Annex A (informative) Example of a phantom for performance testing in the 2 MHz to 7 MHz frequency range . 22 Annex B (informative) Illustrations of the computation of LSNRm-values as a function of de

11、pth 24 Annex C (informative) Sufficient number of data images to assure reproducibility of results 29 C.1 General . 29 C.2 Phantom with low-echo sphere diameter 3,2 mm, having 2 spheres per millilitre . 29 C.3 Phantom with 2 mm-diameter, low-echo spheres and 8 spheres per millilitre 32 Annex D (info

12、rmative) Example of a phantom for performance testing in the 7 MHz to 15 MHz frequency range . 36 Annex E (informative) Determination of low-echo sphere positions to within D/8 in x, y and z Cartesian coordinates 39 E.1 Procedure . 39 E.2 Argument for the choice of seven MPV nearest-neighbour sites

13、for determining the centres of low-echo spheres 40 PD IEC/TS 62791:2015IEC TS 62791:2015 IEC 2015 3 Annex F (informative) Test of total internal reflection produced by alumina and plate-glass, plane reflectors . 41 Annex G (informative) Results of a test of reproducibility of LSNRmversus depth for a

14、 phantom with 4 mm-diameter low-echo spheres and 2 spheres per millilitre 48 Annex H (informative) Results for low-echo sphere-concentration dependence of LSNRmversus depth for phantoms with 4 mm-diameter spheres . 50 Annex I (informative) Results for low-echo sphere-concentration dependence of LSNR

15、m versus depth for phantoms with 3,2 mm-diameter spheres 53 Annex J (informative) Comparison of two different makes of scanner with similar transducers and console settings 57 Annex K (informative) Special considerations for 3-D probes 59 K.1 3-D probes operating in 2-D imaging mode . 59 K.2 2-D arr

16、ays operating in 3-D imaging mode for determining LSNRm-values as a function of depth for reconstructed images . 59 K.3 Mechanically driven 3-D probes operating in 3-D imaging mode 59 Bibliography 60 Figure 1 Flow chart 17 Figure 2 Schematic of an image plane . 20 Figure A.1 End view of the phantom

17、applicable for 2 MHz to 7 MHz showing the spatially random distribution of 4-mm diameter low-echo spheres . 22 Figure A.2 Top view of phantom with 4 mm-diameter, low-echo spheres 23 Figure B.1 Convex-array image of a prototype 4 mm-diameter low-echo sphere phantom for use in the 2 MHz to 7 MHz frequ

18、ency range 24 Figure B.2 Auxiliary figures relating to Figure B.1 25 Figure B.3 Results corresponding to Figures B.1 and B.2, demonstrating reproducibility . 25 Figure B.4 Results corresponding to Figures B.1, B.2 and B.3 . 26 Figure B.5 One of 80 parallel linear-array images of the phantom containi

19、ng 4 mm-diameter, low-echo spheres, at 4 MHz with focus at 3 cm . 26 Figure B.6 Three successive images of the set of 80, separated by D/4 equal to 1 mm 27 Figure B.7 Results for the 4 cm-wide, 3 cm-focus, linear array addressed in Figures B.5 and B.6 . 27 Figure B.8 Results for the 4 cm-wide, 3 cm-

20、focus, linear array addressed in Figures B.5, B.6 and B.7, using all 80 image frames corresponding to Figure B.7 . 28 Figure C.1 One image obtained from a phantom containing 3,2 mm-diameter, low-echo spheres by using a 4 MHz linear array focused at 3 cm 29 Figure C.2 Reproducibility result for two i

21、ndependent sets of 70 images with a mean number of low-echo sphere centres that is about 15 per 5 mm-depth interval 30 Figure C.3 Results obtained by using both sets of 70 independent images corresponding to Figure C.2 30 Figure C.4 Sector image (curved array) at 4,5 MHz with multiple foci at 4 cm,

22、8 cm and 12 cm depths; the low-echo spheres are 3,2 mm in diameter . 31 Figure C.5 Reproducibility results for a multiple-lateral-focus (4 cm, 8 cm and 12 cm) case corresponding to Figure C.4 . 31 Figure C.6 Reproducibility results for the case corresponding to Figure C.5, except that there is a sin

23、gle focus at 10 cm depth 32 Figure C.7 Reproducibility results for the case corresponding to Figure C.5, except that there is a single focus at 4 cm depth 32 PD IEC/TS 62791:2015 4 IEC TS 62791:2015 IEC 2015 Figure C.8 Image of the phantom containing 2 mm-diameter, low-echo spheres, made with a curv

24、ed array having 1,5 cm radius of curvature, with its focus at 3 cm 33 Figure C.9 Reproducibility results corresponding to Figure C.8 33 Figure C.10 Results using all 100 images in the image set that gave rise to Figure C.9 . 34 Figure C.11 Image of the phantom containing 2 mm-diameter, low-echo sphe

25、res, made with a high-frequency (15 MHz) linear array, laterally focused at 4 cm. 34 Figure C.12 Reproducibility results corresponding to Figure C.11 35 Figure C.13 Results using all 200 images in the image set that gave rise to Figure C.12 35 Figure D.1 End- and top-view diagrams of the phantom con

26、taining 2 mm-diameter, low-echo spheres for use in the 7 MHz to 15 MHz frequency range. 37 Figure D.2 Image obtained by using the phantom containing 2 mm-diameter, low-echo spheres and a pediatric transducer with a radius of curvature of about 1,5 cm . 38 Figure F.1 Average of 10 images obtained by

27、using a phased array . 42 Figure F.2 Plot of the data with blue data computed in the left rectangle in Figure F.1 and red data computed in the right rectangle 42 Figure F.3 Plot of the data when the reflector is on the right side with blue computed in the left rectangle and red computed in the right

28、 rectangle . 43 Figure F.4 The percentage by which the mean pixel values resulting from reflections differ from the mean pixel values not involving reflections . 44 Figure F.5 Wide sector (153), 1 cm-radius-of-curvature transducer with alumina reflector on the left 45 Figure F.6 Plot of the data wit

29、h blue computed in the left rectangle in Figure F.5 and red computed in the right rectangle . 45 Figure F.7 Plot of the data when the reflector is on the right side with blue computed in the left rectangle and red computed in the right rectangle . 46 Figure F.8 The percentage by which the mean pixel

30、 values resulting from reflections differ from the mean pixel values not involving reflections . 46 Figure G.1 Example image of the phantom with a 4,2 MHz curved array and two low-echo spheres per millilitre . 48 Figure G.2 Reproducibility results corresponding to the image set, one of which is show

31、n in Figure G.1 49 Figure H.1 Example of an image from the image set giving rise to the results in Figure H.2; the phantom contained an average of one 4 mm-diameter, low-echo sphere per millilitre . 50 Figure H.2 Results corresponding to an image set, one of which is shown in Figure H.1 51 Figure H.

32、3 Example of an image from the data set giving rise to the results in Figure H.4; the phantom contained an average of two 4 mm-diameter, low-echo spheres per millilitre . 51 Figure H.4 Results corresponding to an image set, one of which is shown in Figure H.3 52 Figure I.1 Example of an image from t

33、he 4 ml1data set producing the results shown in Figure I.2 53 Figure I.2 Results for the phantom containing four 3,2 mm-diameter, low-echo spheres per millilitre 54 Figure I.3 Example of an image from the 2 ml1data set producing the results shown in Figure I.4 54 Figure I.4 Results for the phantom c

34、ontaining two 3,2 mm-diameter, low-echo spheres per millilitre 55 PD IEC/TS 62791:2015IEC TS 62791:2015 IEC 2015 5 Figure I.5 Example of an image from the 1 ml1data set producing the results shown in Figure I.6 55 Figure I.6 Results for the phantom containing one 3,2 mm-diameter, low-echo sphere per

35、 millilitre . 56 Figure J.1 Results for System A scanner and 7CF2 3-D (swept convex array) transducer focused at 4 cm and operated at 4,5 MHz in 2-D mode 57 Figure J.2 Results for System B scanner with a 4DC7-3 3-D (convex array) transducer, operated at 4 MHz in 2-D mode and focused at 4 cm. The sec

36、tor angle and all other console settings mimicked those for the System A case (Figure J.1) . 57 PD IEC/TS 62791:2015 6 IEC TS 62791:2015 IEC 2015 INTERNATIONAL ELECTROTECHNICAL COMMISSION _ ULTRASONICS PULSE-ECHO SCANNERS LOW-ECHO SPHERE PHANTOMS AND METHOD FOR PERFORMANCE TESTING OF GRAY-SCALE MEDI

37、CAL ULTRASOUND SCANNERS APPLICABLE TO A BROAD RANGE OF TRANSDUCER TYPES FOREWORD 1) The International Electrotechnical Commission (IEC) is a worldwide organization for standardization comprising all national electrotechnical committees (IEC National Committees). The object of IEC is to promote inter

38、national co-operation on all questions concerning standardization in the electrical and electronic fields. To this end and in addition to other activities, IEC publishes International Standards, Technical Specifications, Technical Reports, Publicly Available Specifications (PAS) and Guides (hereafte

39、r referred to as “IEC Publication(s)”). Their preparation is entrusted to technical committees; any IEC National Committee interested in the subject dealt with may participate in this preparatory work. International, governmental and non-governmental organizations liaising with the IEC also particip

40、ate in this preparation. IEC collaborates closely with the International Organization for Standardization (ISO) in accordance with conditions determined by agreement between the two organizations. 2) The formal decisions or agreements of IEC on technical matters express, as nearly as possible, an in

41、ternational consensus of opinion on the relevant subjects since each technical committee has representation from all interested IEC National Committees. 3) IEC Publications have the form of recommendations for international use and are accepted by IEC National Committees in that sense. While all rea

42、sonable efforts are made to ensure that the technical content of IEC Publications is accurate, IEC cannot be held responsible for the way in which they are used or for any misinterpretation by any end user. 4) In order to promote international uniformity, IEC National Committees undertake to apply I

43、EC Publications transparently to the maximum extent possible in their national and regional publications. Any divergence between any IEC Publication and the corresponding national or regional publication should be clearly indicated in the latter. 5) IEC itself does not provide any attestation of con

44、formity. Independent certification bodies provide conformity assessment services and, in some areas, access to IEC marks of conformity. IEC is not responsible for any services carried out by independent certification bodies. 6) All users should ensure that they have the latest edition of this public

45、ation. 7) No liability should attach to IEC or its directors, employees, servants or agents including individual experts and members of its technical committees and IEC National Committees for any personal injury, property damage or other damage of any nature whatsoever, whether direct or indirect,

46、or for costs (including legal fees) and expenses arising out of the publication, use of, or reliance upon, this IEC Publication or any other IEC Publications. 8) Attention is drawn to the Normative references cited in this publication. Use of the referenced publications is indispensable for the corr

47、ect application of this publication. The main task of IEC technical committees is to prepare International Standards. In exceptional circumstances, a technical committee may propose the publication of a Technical Specification when the required support cannot be obtained for the publication of an In

48、ternational Standard, despite repeated efforts, or the subject is still under technical development or where, for any other reason, there is the future but no immediate possibility of an agreement on an International Standard. Technical Specifications are subject to review within three years of publ

49、ication to decide whether they can be transformed into International Standards. Technical Specification IEC TS 62791 has been prepared by IEC technical committee 87 Ultrasonics. PD IEC/TS 62791:2015IEC TS 62791:2015 IEC 2015 7 The text of this Technical Specification is based on the following documents: DTS Report on voting 87/554/DTS 87/570/RVC Full information on the voting for the approval of this Technical Specifica

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