Prediction of effective properties for composite superconducting strand and multi-stage cables

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Abstract

Superconducting multifilamentary Nb3Sn strand and cables have complex microstructure and macrostructure which are used in the International Thermonuclear Experimental Reactor (ITER) superconducting magnet system. In a generic form, the superconducting strand is made of copper, multifilamentary Nb3Sn and bronze which is a composite. The twisted composite strands form the superconducting cables with typical multi-stage structures. Here we propose a numerical model focusing on the problem of characterizing the effective properties of composite superconducting strand and cables at microscopic and macroscopic scales. The effective elastic constants of the composite superconducting strand can be derived by involving the combination of the representative volume element (RVE) and the Mori-Tanaka method. Subsequently, the proposed method is applied to capture the effects of temperature on the effective elastic constants of the superconducting multi-stage cables. Results show the elastic constants predicted by this model agree well with existing theoretical predictions and available experimental data. This numerical model may be utilized to optimize the mechanical properties of the composite superconducting strand by tuning the constituent fractions and to control the tensile stiffness of superconducting cables by tuning the winding laps of the cables.

Introduction

Nb3Sn strand is a kind of superconductor material used in high fields poloidal field (PF) coils and central solenoid (CS) coils which are employed in International Thermonuclear Experimental Reactor (ITER) superconducting magnet system [1]. Typical Nb3Sn strand is made of Nb3Sn filaments, bronze and copper which is regarded as a multifilament superconducting composite [2]. For the multifilament superconducting composite, there are thousands Nb3Sn filaments inlaid in the bronze matrix. In practical application, the Nb3Sn cable-in-conduit conductors (CICCs) are often subject to transverse electromagnetic forces which may lead to the damage and fracture of Nb3Sn strand [[3], [4], [5], [6], [7]]. Therefore, the prediction for the mechanical properties of Nb3Sn strand is very important issues in the design of superconducting cables which are made of twisted strands. In recent years, some models have been proposed to predict the mechanical properties of superconducting strand. For example, Zhou et al used an equivalent model which can instead of the thousands Nb3Sn filaments to give the effective moduli of the strand along axial direction [5]. A micromechanical model is adopted to characterize the mechanical behavior of the superconducting strand with twisted filaments [8]. Gao et al used the homogenization theory and Costello’s wire rope theory to determine the effective Young’s moduli of the hierarchical superconducting cable [9,10]. The equivalent Young’s modulus and Poisson’s ratio of the coil conductor are predicted by Zhou et al [11]. In addition, the axial thermal expansion coefficient of twist cable is predicted by experimental and modelling researches by Zhang et al [12]. These models focus on the single material of the superconducting strand, but the composite structures have not been considered in their studies. In this work, through considering the microscopic composite structures, a numerical model was established to model the effective properties in superconducting composite strand and multi-stage cables. As for the study of the effective properties of composite materials, there are many theoretical and numerical models have been proposed to investigate the composite elastic moduli due to the significance in predicting effective elastic constants of composite material. Prediction of the effective elastic moduli can be traced back to 1960s. Hashin and Rosen [13] developed the upper and lower bounds for composite elastic moduli based on the energy variational principles. Whitney and Riley [14] obtained closed-form analytical expressions for a composite’s elastic moduli based on the energy balance approach. Sun and Vaidya [15] developed a vigorous mechanical analysis using a representative volume element (RVE) to obtain the complete set of elastic constants for a unidirectional composite. Xia [16,17] established an explicit unified form of boundary conditions for a periodic RVE to produce all elastic moduli for unidirectional or angle-ply laminates. In the present paper, an appropriate micromechanics RVE is presented to calculate the elastic constants of superconducting composite Nb3Sn strand firstly. Then, a numerical model is addressed to predict the tensile stiffnesses of the multi-stage cables which are made of twisted strands. In addition, the Nb3Sn composite strand is brittleness which requires a special manufacturing condition [18,19]. Usually, the strand is heated up to the reaction temperature (900-950 K), then the strand is kept for several days at high temperature. Finally, it is cooled down to room temperature or to its operating conditions (about 4.2 K). Based on the above facts, a numerical model is developed to obtain the effective thermal properties due to the different thermal expansion properties of the strand material. Furthermore, the effect of the temperature on the tensile stiffnesses of multi-stage cables structures also are studied. The remainder of the paper is organized as follows. In section 2, we formally defined the problem under study and present a numerical model. Section 3 details a computational model which is used to validate the validity and applicable range of the numerical model. In section 4, the numerical results are detailed. Finally, we conclude with discuss and conclusions in section 5.

Section snippets

Micromechanical model and representative volume element

The Nb3Sn strand is a composite material which contains three components: Nb3Sn filaments, copper stabilizer and bronze matrix [20]. Generally, thousands of Nb3Sn filaments are grouped into several plies and embedded in bronze matrix. Then, by using barrier material with copper to form the Nb3Sn strand. According to the different barrier material, Nb3Sn strand can be divided into different forms. For example, bronze route strand and internal tin strand use the Tantalum and unreacted Nb and

Validate

To validate the proposed model, two examples are displayed to make a comparison with the results of literatures. The validity of the proposed scheme is demonstrated by comparisons with Sun’s theory and Boso’s results [15,19]. In Section 3.1, a unidirectional fiber composite is considered, the effective elastic moduli of the composite are determined by finite element analysis of the RVE. This is an excellent choice to study how to select the RVE of composites. In Section 3.2, a micro-macro scale

Numerical results and discussion

For the sake of predicting the effect of temperature on the effective properties of the whole FUR strand and the multi-stage cables, the elastic constants in the Nb3Sn filament phase and the whole FUR strand phase must be determined before calculating the tensile stiffness of multi-stage cables varying with temperature. Fig. 9, Fig. 10 illustrate the Young’s modulus of Nb3Sn filaments phase in the FUR strand versus temperature obtained from previous established model. Results of literature [19]

Conclusions

A numerical model was developed to investigate the effective elastic constants of the composite superconducting strand and cables at microscopic and macroscopic scales. This model is based on the RVE and Mori-Tanaka method which are typical composite approach. The effective elastic constants of the FUR strand and the effect of temperature on the effective elastic constants of multi-stage cables were predicted. The simulated results agree well with the results of existing literatures and

Declaration of Competing Interest

The authors report no declarations of interest.

Acknowledgments

The authors gratefully acknowledge the financial support provided by the Natural Science Foundation of China (NSFC 11772142, 11872196), the Fundamental Research Funds for the Central Universities (lzujbky-2015-176) and the 111 Project, B14044.

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