IEC 61788-17:2013
(Main)Superconductivity - Part 17: Electronic characteristic measurements - Local critical current density and its distribution in large-area superconducting films
Superconductivity - Part 17: Electronic characteristic measurements - Local critical current density and its distribution in large-area superconducting films
IEC 61788-17:2013 describes the measurements of the local critical current density (Jc) and its distribution in large-area high-temperature superconducting (HTS) films by an inductive method using third-harmonic voltages. The most important consideration for precise measurements is to determine Jc at liquid nitrogen temperatures by an electric-field criterion and obtain current-voltage characteristics from its frequency dependence. Although it is possible to measure Jc in applied DC magnetic fields, the scope of this standard is limited to the measurement without DC magnetic fields. This technique intrinsically measures the critical sheet current that is the product of Jc and the film thickness d. The range and measurement resolution for Jcd of HTS films are from 200 A/m to 32 kA/m, with a measurement resolution of 100 A/m.
Supraconductivité - Partie 17: Mesures de caractéristiques électroniques - Densité de courant critique local et sa distribution dans les films supraconducteurs de grande surface
La CEI 61788-17:2013 décrit les mesures de la densité de courant critique local (Jc) et sa distribution dans les films supraconducteurs à haute température (HTS) de grande surface par une méthode inductive utilisant les tensions de troisième harmonique. La considération la plus importante pour effectuer des mesures précises consiste à déterminer Jc aux températures de l'azote liquide au moyen d'un critère de champ électrique et obtenir des caractéristiques courant-tension d'après sa dépendance vis-à-vis de la fréquence. Bien qu'il soit possible de mesurer Jc dans des champs magnétiques en courant continu appliqués, le domaine d'application de la présente norme est limité à la mesure sans champ magnétique en courant continu. Cette technique mesure de façon intrinsèque le courant de feuille critique, qui est le produit de Jc par l'épaisseur d du film. La plage et la résolution de mesure pour Jcd des films HTS est de 200 A/m à 32 kA/m avec une résolution de mesure de 100 A/m.
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IEC 61788-17 ®
Edition 1.0 2013-01
INTERNATIONAL
STANDARD
NORME
INTERNATIONALE
colour
inside
Superconductivity –
Part 17: Electronic characteristic measurements – Local critical current density
and its distribution in large-area superconducting films
Supraconductivité –
Partie 17: Mesures de caractéristiques électroniques – Densité de courant
critique local et sa distribution dans les films supraconducteurs de grande
surface
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IEC 61788-17 ®
Edition 1.0 2013-01
INTERNATIONAL
STANDARD
NORME
INTERNATIONALE
colour
inside
Superconductivity –
Part 17: Electronic characteristic measurements – Local critical current density
and its distribution in large-area superconducting films
Supraconductivité –
Partie 17: Mesures de caractéristiques électroniques – Densité de courant
critique local et sa distribution dans les films supraconducteurs de grande
surface
INTERNATIONAL
ELECTROTECHNICAL
COMMISSION
COMMISSION
ELECTROTECHNIQUE
PRICE CODE
INTERNATIONALE
CODE PRIX X
ICS 17.220.20; 29.050 ISBN 978-2-83220-583-9
– 2 – 61788-17 © IEC:2013
CONTENTS
FOREWORD . 4
INTRODUCTION . 6
1 Scope . 8
2 Normative reference . 8
3 Terms and definitions . 8
4 Requirements . 9
5 Apparatus . 9
5.1 Measurement equipment . 9
5.2 Components for inductive measurements . 10
5.2.1 Coils . 10
5.2.2 Spacer film . 11
5.2.3 Mechanism for the set-up of the coil . 11
5.2.4 Calibration wafer . 11
6 Measurement procedure . 12
6.1 General . 12
6.2 Determination of the experimental coil coefficient . 12
6.2.1 Calculation of the theoretical coil coefficient k . 12
6.2.2 Transport measurements of bridges in the calibration wafer . 13
6.2.3 U measurements of the calibration wafer . 13
6.2.4 Calculation of the E-J characteristics from frequency-dependent I
th
data . 13
6.2.5 Determination of the k’ from J and J values for an appropriate E . 14
ct c0
6.3 Measurement of J in sample films . 15
c
6.4 Measurement of J with only one frequency . 15
c
6.5 Examples of the theoretical and experimental coil coefficients . 16
7 Uncertainty in the test method . 17
7.1 Major sources of systematic effects that affect the U measurement . 17
7.2 Effect of deviation from the prescribed value in the coil-to-film distance . 18
7.3 Uncertainty of the experimental coil coefficient and the obtained J . 18
c
7.4 Effects of the film edge . 19
7.5 Specimen protection . 19
8 Test report . 19
8.1 Identification of test specimen . 19
8.2 Report of J values . 19
c
8.3 Report of test conditions . 19
Annex A (informative) Additional information relating to Clauses 1 to 8 . 20
Annex B (informative) Optional measurement systems . 26
Annex C (informative) Uncertainty considerations . 32
Annex D (informative) Evaluation of the uncertainty . 37
Bibliography . 43
Figure 1 – Diagram for an electric circuit used for inductive J measurement of HTS
c
films . 10
Figure 2 – Illustration showing techniques to press the sample coil to HTS films . 11
Figure 3 – Example of a calibration wafer used to determine the coil coefficient . 12
61788-17 © IEC:2013 – 3 –
Figure 4 – Illustration for the sample coil and the magnetic field during measurement . 13
Figure 5 – E-J characteristics measured by a transport method and the U inductive
method . 14
Figure 6 –Example of the normalized third-harmonic voltages (U /fI ) measured with
3 0
various frequencies . 15
Figure 7 – Illustration for coils 1 and 3 in Table 1 . 16
Figure 8 – The coil-factor function F(r) = 2H /I calculated for the three coils . 17
0 0
Figure 9 – The coil-to-film distance Z dependence of the theoretical coil coefficient k . 18
Figure A.1 – Illustration for the sample coil and the magnetic field during measurement . 22
Figure A.2 – (a) U and (b) U /I plotted against I in a YBCO thin film measured in
3 3 0 0
applied DC magnetic fields, and the scaling observed when normalized by I (insets) . 23
th
Figure B.1 – Schematic diagram for the variable-RL-cancel circuit . 27
Figure B.2 – Diagram for an electrical circuit used for the 2-coil method . 27
Figure B.3 – Harmonic noises arising from the power source . 28
Figure B.4 – Noise reduction using a cancel coil with a superconducting film . 28
Figure B.5 – Normalized harmonic noises (U /fI ) arising from the power source . 29
3 0
Figure B.6 – Normalized noise voltages after the reduction using a cancel coil with a
superconducting film . 29
Figure B.7 – Normalized noise voltages after the reduction using a cancel coil without
a superconducting film . 30
Figure B.8 – Normalized noise voltages with the 2-coil system shown in Figure B.2 . 30
Figure D.1 – Effect of the coil position against a superconducting thin film on the
measured J values . 41
c
Table 1 – Specifications and coil coefficients of typical sample coils . 16
Table C.1 – Output signals from two nominally identical extensometers . 33
Table C.2 – Mean values of two output signals . 33
Table C.3 – Experimental standard deviations of two output signals . 33
Table C.4 – Standard uncertainties of two output signals . 34
Table C.5 – Coefficient of variations of two output signals . 34
Table D.1 – Uncertainty budget table for the experimental coil coefficient k’ . 37
Table D.2 – Examples of repeated measurements of J and n-values . 40
c
– 4 – 61788-17 © IEC:2013
INTERNATIONAL ELECTROTECHNICAL COMMISSION
____________
SUPERCONDUCTIVITY –
Part 17: Electronic characteristic measurements –
Local critical current density and its distribution
in large-area superconducting films
FOREWORD
1)
...
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