Numerical simulation of bulk superconductor during pulsed field magnetization based on multi-field coupled analysis



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<big>'''Numerical simulation of bulk superconductor during pulsed field magnetization based on multi-field coupled analysis'''</big></div>

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<big>Yu Yang<sup>1, 2</sup>, Lingyun Jian<sup>1</sup></big></div>

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1. Fujian Key Laboratory of Intelligent Processing Technology and Equipment, School of Mechanical and Automotive Engineering, Fujian University of Technology, Fuzhou 350100</div>

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2. Fujian Provincial Research Institute of Special Equipment Inspection, Fuzhou 350100</div>

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* Corresponding author：Yu Yang，E-mail：y[mailto:angyu_mech@qq.com angyu_mech@qq.com]</div>

'''Abstract：'''High-temperature bulk superconductors are widely used in various superconducting devices due to their high critical current density, which enables them to trap high magnetic fields. However, the critical current density of bulk superconductors is influenced by magnetic field, temperature and stress, and both increase of stress and temperature can lead to a decrease in the critical current density. And the influence of magnetic field, current, stress are interactional. In this paper, the multi-field coupled analysis is employed to investigate the electromagnetic and mechanical behavior on bulk superconductor during pulsed field magnetization. The simulation results were compared with the present experimental results. The results showed a good agreement between the simulation and experimental results, further validating the reliability of the numerical simulation method. The magnetic field, current, temperature, and stress distribution and variation within the bulk sample during the pulsed magnetization process were calculated and analyzed. Additionally, the influence of the central crack and edge crack in the bulk superconductor was investigated. The results indicate that the region near the crack experiences a variation in current flow direction, resulting in local temperature rise and significant electromagnetic forces. The tip of the crack exhibits stress concentration, leading to a decrease in critical current density. Bulk supercondutor with edge crack case exhibits greater stress concentration compared to those with central crack case. The impact of crack length on maximum stress was analyzed, revealing that as the crack length increases, both the maximum hoop stress and radial stress within the bulk sample rise.

'''Keywords：'''bulk''' '''superconductor, multi-field coupled analysis, critical current density, finite element method, crack

=1 Introduction=

Due to their high critical current density and ability to trapped higher magnetic fields, high-temperature bulk superconductors have found widespread applications in various superconducting devices <span id='cite-_Ref132794187'></span>[[#_Ref132794187|[1]]]<span id='cite-_Ref132794189'></span>[[#_Ref132794189|[2]]]<span id='cite-_Ref132794191'></span>[[#_Ref132794191|[3]]]<span id='cite-_Ref132794192'></span>[[#_Ref132794192|[4]]]. There are three magnetization methods for bulk superconductor: field cooling (FC), zero-field cooling (ZFC), and pulse field magnetization (PFM). Although FC and ZFC can achieve higher trapped fields, they suffer from drawbacks such as long loading times, high energy losses, and the requirement of expensive equipment <span id='cite-_Ref132811978'></span>[[#_Ref132811978|[5]]]<span id='cite-_Ref132811980'></span>[[#_Ref132811980|[6]]]<span id='cite-_Ref132811982'></span>[[#_Ref132811982|[7]]]<span id='cite-_Ref132811983'></span>[[#_Ref132811983|[8]]]<span id='cite-_Ref132811985'></span>[[#_Ref132811985|[9]]]. In contrast, the advantages of PFM are simplicity, convenience, and cost-effectiveness. It features extremely short loading times and low energy losses, while imposing minimal requirements on the equipment. However, the limitations of PFM are the rapid loading rate leading to significant temperature rises, flux jumps and making it difficult to achieve high trapped fields <span id='cite-_Ref132814132'></span>[[#_Ref132814132|[10]]].

Due to the weak mechanical properties of bulk superconductor and the large Lorentz force in magnetization, the mechanical behavior is important in the practical application. The bulk superconductors are sometimes reinforced externally with metals to improve their mechanical performance and prevent fractures <span id='cite-_Ref132897971'></span>[[#_Ref132897971|[11]]]<span id='cite-_Ref132897972'></span>[[#_Ref132897972|[12]]]<span id='cite-_Ref144388679'></span>[[#_Ref144388679|[13]]]<span id='cite-_Ref144388911'></span>[[#_Ref144388911|[14]]]. Ainslie ''et al. ''addressed the modeling issues of magnetizing bulk superconductors and provided a finite element method to assess and predict their magnetization characteristics <span id='cite-_Ref132914481'></span>[[#_Ref132914481|[19]]]. In 2018, Wu ''et al. ''investigated the stress distribution in high-temperature superconductors under PFM magnetization process and proposed methods to mitigate stress <span id='cite-_Ref132901240'></span>[[#_Ref132901240|[15]]]. Subsequently, they studied the mechanical behavior of non-uniform high-temperature superconductors under PFM magnetization, analyzing the potential for fracture and damage due to non-uniform distributions and their impacts on performance and lifespan <span id='cite-_Ref132901719'></span>[[#_Ref132901719|[16]]]. Xia ''et al. ''studied the characteristics of thermomagnetic instability in MgB<sub>2</sub> bulk samples and provided numerical simulation methods to evaluate and predict their performance <span id='cite-_Ref132914048'></span>[[#_Ref132914048|[17]]]. Building upon this research, Zhang ''et al. ''investigated the mechanical response of cylindrical superconductors under flux jumps and analyzed the mechanical response characteristics of superconductors under different conditions <span id='cite-_Ref132914123'></span>[[#_Ref132914123|[18]]]. Wang ''et al. ''have explored the mechanical stress issues of high-temperature superconducting ring bulk samples during the PFM process <span id='cite-_Ref132916033'></span>[[#_Ref132916033|[20]]].

During the fabrication process of bulk superconductor, the occurrence of small crack and voids is inevitable, which can have a certain impact on the mechanical properties of the bulk superconductor<span id='cite-_Ref135916399'></span>[[#_Ref135916399|[30]]]. Therefore the study of crack in bulk superconductor is a wide field of scientific research and many researchers have done important work in this field <span id='cite-_Ref144388174'></span>[[#_Ref144388174|[21]]]<span id='cite-_Ref144388240'></span>[[#_Ref144388240|[22]]]<span id='cite-_Ref144388367'></span>[[#_Ref144388367|[23]]]<span id='cite-_Ref144388459'></span>[[#_Ref144388459|[24]]]. Mochizuki ''et al. ''have analyzed the trapped field characteristics and fracture behavior of REBaCuO circular bulk samples during the PFM process <span id='cite-_Ref132916814'></span>[[#_Ref132916814|[25]]]. Takahashi ''et al. ''have studied the fracture behavior of EuBaCuO superconducting circular bulk samples under different reinforcing material supports during field cooling magnetization <span id='cite-_Ref132897972'></span>[[#_Ref132897972|[12]]]. Electromagnetic forces lead to stress concentration and crack formation within the superconductor, and the rate and direction of crack propagation depend on factors such as the magnitude and direction of the electromagnetic forces, material parameters, and geometric shape <span id='cite-_Ref135916686'></span>[[#_Ref135916686|[31]]]. Ru ''et al. ''conducted numerical simulations to investigate the fracture behavior of bulk superconductor with pre-existing elliptical crack under the influence of electromagnetic forces, delving into the patterns of crack formation and propagation <span id='cite-_Ref135916990'></span>[[#_Ref135916990|[32]]].

<span id='_Hlk144060810'></span>In this paper, the performance of ring bulk superconductor during the PFM magnetization process is analyzed using finite element method based on H-formulation, heat conduction equation, and the mechanical equilibrium equation. The variation in critical current density of the bulk due to variations in magnetic field intensity, temperature, and stress are considered, and the impact of these factors on the results is examined. The analysis results are in good agreement with experimental results. Furthermore, the influence of crack at different locations on the results is analyzed, providing different simulation results for trapped fields and temperatures within the bulk affected by stress and various crack configurations.

=2 Numerical model and parameters=

The numerical model in this paper is based on the experimental sample presented by Ref. <span id='cite-_Ref132916814'></span>[[#_Ref132916814|[25]]], and the 2D axisymmetric model of the GdBCO ring bulk is adopted for simplification. <span id='cite-_Ref143373672'></span>[[#_Ref143373672|Figure 1]](a) depicts a three-dimensional schematic diagram and a 2D axisymmetric cross-section schematic (not to scale) of the ring GdBCO high-temperature bulk superconductor. The ring is installed in the holder with an aluminum alloy ring (5 mm in width). The lower part of the bulk is a layer of indium sheet (1 mm in thickness), which is connected to the cold head with an initial temperature of 65 K. A uniform critical current is assumed throughout the ring in this study, and the epoxy layer between the aluminum alloy ring and the superconducting ring is disregarded, assuming an ideal connection between them. In the experiment, a pulsed field of  <math display="inline">B_{ex}=2.53\mbox{ }T</math> was applied to the bulk, with a rise time of 13 ms and a duration of 200 ms. Hall sensors were positioned at the center of the bulk to measure the trapped field, while a Hall probe was placed 1 mm above the surface of the bulk to generate the distribution of the trapped field  <math display="inline">B_z</math> <span id='cite-_Ref132916814'></span>[[#_Ref132916814|[25]]]. High-temperature copper oxide superconductors are relatively brittle, microcrack and defects can be generated in superconductors<span id='cite-_Ref143947786'></span>[[#_Ref143947786|[36]]]. Cracking may occur in superconductors due to large electromagnetic body force<span id='cite-_Ref143947968'></span>[[#_Ref143947968|[37]]]. Furthermore, the crack and defects lead to strong local enhancement of the stress which may limit the application of the superconductor. In order to investigate the impact of crack on the superconducting and mechanical properties of the bulk superconductor, elliptical crack were introduced into the model, while both central crack case and edge crack case are considered, as shown in <span id='cite-_Ref143373672'></span>[[#_Ref143373672|Figure 1]](b) and <span id='cite-_Ref143373672'></span>[[#_Ref143373672|Figure 1]](c).

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 [[Image:Review_893267287081-image3.png|402px]] </div>

<div id="_Ref143373672" class="center" style="width: auto; margin-left: auto; margin-right: auto;">
Figure 1 (a) Sketches of the ring GdBCO bulk (left) and two-dimensional axisymmetric model (right); (b) (c) two-dimensional axisymmetric modeling of bulk superconductor containing central elliptical crack case and edge semi-elliptical crack case</div>

In this study, the magnetic field and current density were calculated using the H-formulation<span id='cite-_Ref143949294'></span>[[#_Ref143949294|[38]]]. The governing equations are given by <span id='cite-_Ref132979450'></span>[[#_Ref132979450|[26]]]

{| class="formulaSCP" style="width: 100%; text-align: center;" 
|-
| 
{| style="text-align: center; margin:auto;" 
|-
| <span id='ZEqnNum769201'></span>  <math>\nabla \times \boldsymbol{E}+\frac{\mbox{d}\boldsymbol{B}}{\mbox{d}t}=</math><math>\nabla \times \left(\rho \nabla \times \boldsymbol{H}\right)+</math><math>\frac{\mbox{d}\left({\mu }_0{\mu }_r\boldsymbol{H}\right)}{\mbox{d}t}=</math><math>0</math>
|}
| style="width: 5px;text-align: right;white-space: nowrap;" | (1)
|}


Where  <math>\boldsymbol{E}</math> ,  <math display="inline">\boldsymbol{B}</math> and  <math display="inline">\boldsymbol{H}</math> are electric field, magnetic flux density, and magnetic field intensity, respectively.

The Maxwell's equations, which are required for electromagnetic field calculations, are as follows

{| class="formulaSCP" style="width: 100%; text-align: center;" 
|-
| 
{| style="text-align: center; margin:auto;" 
|-
| <span id='ZEqnNum320282'></span>  <math>\begin{array}{c}
\nabla \times \boldsymbol{E}=-\frac{\partial \boldsymbol{B}}{\partial t}\\
\nabla \times \boldsymbol{H}=\boldsymbol{J}\\
\nabla \cdot \boldsymbol{B}=0
\end{array}</math>
|}
| style="width: 5px;text-align: right;white-space: nowrap;" | (2)
|}


Where  <math>\boldsymbol{J}</math> is the critical current density;  <math>t</math> is the time. The electromagnetic constitutive equations for superconductors are as follows

{| class="formulaSCP" style="width: 100%; text-align: center;" 
|-
| 
{| style="text-align: center; margin:auto;" 
|-
| <span id='ZEqnNum216404'></span>  <math>\begin{cases} \boldsymbol{E}=\rho \boldsymbol{J} \\ \boldsymbol{B}={\mu }_0{\mu }_r\boldsymbol{H} \end{cases}</math>
|}
| style="width: 5px;text-align: right;white-space: nowrap;" | (3)
|}


Where  <math>\rho </math> is the equivalent resistivity；the variables  <math>{\mu }_0</math> and  <math display="inline">{\mu }_r</math> are the Vacuum permeability, and the relative permeability, In this study, a value of  <math>{\mu }_r=1</math> . Furthermore, Equation <span id='cite-ZEqnNum769201'></span>[[#ZEqnNum769201|(1)]] is derived by combining Equation <span id='cite-ZEqnNum320282'></span>[[#ZEqnNum320282|(2)]] and Equation <span id='cite-ZEqnNum216404'></span>[[#ZEqnNum216404|(3)]]. To prevent the electric field from becoming excessively large when the current exceeds the critical density in the  <math display="inline">\boldsymbol{E-J}</math> model, the modified  <math display="inline">\boldsymbol{E-J}</math> model is employed, with an effective resistivity denoted as <span id='cite-_Ref142706874'></span>[[#_Ref142706874|[35]]]

{| class="formulaSCP" style="width: 100%; text-align: center;" 
|-
| 
{| style="text-align: center; margin:auto;" 
|-
| <math>f(n) = \begin{cases} \frac{{\rho }_{sc}\cdot {\rho }_{normal}}{{\rho }_{sc}+{\rho }_{normal}}, & \mbox{    }T\leq T_c \\ {\rho }_{nomal}, & \mbox{              }T>T_c \end{cases}</math>
|}
| style="width: 5px;text-align: right;white-space: nowrap;" | (4)
|}


Where  <math>{\rho }_{normal}</math> is the resistivity of the bulk superconductor in the normal state. Among them

{| class="formulaSCP" style="width: 100%; text-align: center;" 
|-
| 
{| style="text-align: center; margin:auto;" 
|-
| <math>{\rho }_{sc}=E_c{\left(\frac{J}{J_c}\right)}^{\left(n-1\right)}J_c</math>
|}
| style="width: 5px;text-align: right;white-space: nowrap;" | (5)
|}


The critical current density could be influenced by the magnetic field intensity, temperature, and stress. In this article, the modified Kim model is employed, as follows

{| class="formulaSCP" style="width: 100%; text-align: center;" 
|-
| 
{| style="text-align: center; margin:auto;" 
|-
| <math>J_c={\beta }_0{\left[1-{\left(\frac{T}{T_c}\right)}^2\right]}^{1.5}\frac{B_0}{\vert B\vert +B_0}J\left(\sigma \right)</math>
|}
| style="width: 5px;text-align: right;white-space: nowrap;" | (6)
|}


Where <math>{\beta }_0=1.32\times {10}^9\mbox{A}/\mbox{m}^2</math> <span id='cite-_Ref132985662'></span>[[#_Ref132985662|[27]]], is the critical current density at <math>B=0,T\mbox{=0}</math> is determined;  <math>T_c</math> is the critical temperature;  <math>B_0</math> is the fitted parameter.  <math>J\left(\sigma \right)</math> denotes the effect of stress on the critical current density <span id='cite-_Ref142674225'></span>[[#_Ref142674225|[34]]]. The heat transfer control equation is <span id='cite-_Ref132987311'></span>[[#_Ref132987311|[28]]]

{| class="formulaSCP" style="width: 100%; text-align: center;" 
|-
| 
{| style="text-align: center; margin:auto;" 
|-
| <math>{\rho }_mC\frac{\partial T}{\partial t}=\nabla \cdot \left(\kappa \nabla T\right)+</math><math>Q</math>
|}
| style="width: 5px;text-align: right;white-space: nowrap;" | (7)
|}

{| class="formulaSCP" style="width: 100%; text-align: center;" 
|-
| 
{| style="text-align: center; margin:auto;" 
|-
| <math>Q=\boldsymbol{E}\cdot \boldsymbol{J}</math>
|}
| style="width: 5px;text-align: right;white-space: nowrap;" | (8)
|}


Where <math>\rho </math> is the densities; <math>c</math> is the constant pressure heat capacity;  <math>k</math> is the thermal conductivity and  <math>Q</math> is the joule heat. The thermal conductivity has different values in the ab plane ( <math display="inline">{\kappa }_{ab}</math> ) and c plane ( <math display="inline">{\kappa }_c</math> ). Due to the temperature-dependent specific heat and thermal conductivity of the bulk superconductor, fitting equations obtained from the literature were utilized in our program <span id='cite-_Ref132811980'></span>[[#_Ref132811980|[6]]]. The bulk superconductor was affixed to an indium foil, and a cold head was positioned at the bottom of the indium foil, with the temperature designated as  <math display="inline">T_0</math> . Therefore, the heat transfer boundary condition is defined as the fixed temperature of  <math display="inline">T_0</math> at the lower edge, while the remaining boundaries are subjected to thermal insulation conditions.

In the experiment, the external magnetic field on the bulk sample was applied using external coils. In the simulation, the external magnetic field was imposed at the boundary of the air domain. The applied pulse magnetic field was <span id='cite-_Ref132987503'></span>[[#_Ref132987503|[29]]]

{| class="formulaSCP" style="width: 100%; text-align: center;" 
|-
| 
{| style="text-align: center; margin:auto;" 
|-
| <math>B_{ex}\left(t\right)=B_{max}t/{t_1}exp\left(1-\right. </math><math>\left. t/{t_1}\right)</math>
|}
| style="width: 5px;text-align: right;white-space: nowrap;" | (9)
|}


Where  <math>B_{max}</math> is the peak value of the applied magnetic field and  <math>t_1</math> is the rise time of the applied magnetic field.

<div id="_Ref143373393" class="center" style="width: auto; margin-left: auto; margin-right: auto;">
Table 1 Parameters in the simulation</div>

{| style="width: 100%;margin: 1em auto 0.1em auto;border-collapse: collapse;" 
|-
|  style="border-top: 2pt solid black;border-bottom: 1pt solid black;text-align: center;vertical-align: top;"|Parameter
|  style="border-top: 2pt solid black;border-bottom: 1pt solid black;text-align: center;vertical-align: top;"|Description
|  style="border-top: 2pt solid black;border-bottom: 1pt solid black;text-align: center;vertical-align: top;"|Value
|-
|  style="border-top: 1pt solid black;text-align: center;vertical-align: top;width: 14%;"|<math display="inline">c</math> 
|  style="border-top: 1pt solid black;text-align: center;vertical-align: top;"|Specific heat of the ring bulk
|  style="border-top: 1pt solid black;text-align: center;vertical-align: top;"|<span id='cite-_Ref132811980'></span>[[#_Ref132811980|[6]]]
|-
|  style="text-align: center;vertical-align: top;width: 14%;"|<math display="inline">c_{in}</math> 
|  style="text-align: center;vertical-align: top;"|Thermal conductivity of the indium
|  style="text-align: center;vertical-align: top;"|<span id='cite-_Ref132901240'></span>[[#_Ref132901240|[15]]]
|-
|  style="text-align: center;vertical-align: top;width: 14%;"|<math display="inline">c_{al}</math> 
|  style="text-align: center;vertical-align: top;"|Specific heat of the reinforced ring
|  style="text-align: center;vertical-align: top;"|<span id='cite-_Ref136003622'></span>[[#_Ref136003622|[33]]]
|-
|  style="text-align: center;vertical-align: top;width: 14%;"|<math display="inline">k_{ab}</math> 
|  style="text-align: center;vertical-align: top;"|Thermal conductivity of the bulk along the ab plane
|  style="text-align: center;vertical-align: top;"|<span id='cite-_Ref132811980'></span>[[#_Ref132811980|[6]]]
|-
|  style="text-align: center;vertical-align: top;width: 14%;"|<math display="inline">k_c</math> 
|  style="text-align: center;vertical-align: top;"|Thermal conductivity of the bulk along the c plane
|  style="text-align: center;vertical-align: top;"|<span id='cite-_Ref132811980'></span>[[#_Ref132811980|[6]]]
|-
|  style="text-align: center;vertical-align: top;width: 14%;"|<math display="inline">k_{in}</math> 
|  style="text-align: center;vertical-align: top;"|Thermal conductivity of the indium
|  style="text-align: center;vertical-align: top;"|<span id='cite-_Ref132901240'></span>[[#_Ref132901240|[15]]]
|-
|  style="text-align: center;vertical-align: top;width: 14%;"|<math display="inline">k_{al}</math> 
|  style="text-align: center;vertical-align: top;"|Thermal conductivity of the reinforced ring
|  style="text-align: center;vertical-align: top;"|<span id='cite-_Ref136003622'></span>[[#_Ref136003622|[33]]]
|-
|  style="text-align: center;vertical-align: top;width: 14%;"|<math display="inline">\rho </math> 
|  style="text-align: center;vertical-align: top;"|Density of the ring bulk
|  style="text-align: center;vertical-align: top;width: 23%;"|<math display="inline">5900\mbox{ }\mbox{}\mbox{}\mbox{}\mbox{}\mbox{}\mbox{}\mbox{kg}/\mbox{m}^3</math> 
|-
|  style="text-align: center;vertical-align: top;width: 14%;"|<math display="inline">E</math> 
|  style="text-align: center;vertical-align: top;"|Young modulus of the ring bulk
|  style="text-align: center;vertical-align: top;width: 23%;"|<math display="inline">\mbox{103 GPa}</math> 
|-
|  style="text-align: center;vertical-align: top;width: 14%;"|<math display="inline">\upsilon </math> 
|  style="text-align: center;vertical-align: top;"|Poisson ratio of the ring bulk
|  style="text-align: center;vertical-align: top;width: 23%;"|<math display="inline">0.3</math> 
|-
|  style="text-align: center;vertical-align: top;width: 14%;"|<math display="inline">\alpha </math> 
|  style="text-align: center;vertical-align: top;"|Thermal expansivity of the ring bulk
|  style="text-align: center;vertical-align: top;width: 23%;"|<math display="inline">1\times {10}^{-5}{\mbox{ K}}^{-1}</math> 
|-
|  style="text-align: center;vertical-align: top;width: 14%;"|<math display="inline">E_{al}</math> 
|  style="text-align: center;vertical-align: top;"|Young modulus of the reinforced ring
|  style="text-align: center;vertical-align: top;width: 23%;"|<math display="inline">78\mbox{ GPa}</math> 
|-
|  style="text-align: center;vertical-align: top;width: 14%;"|<math display="inline">{\upsilon }_{al}</math> 
|  style="text-align: center;vertical-align: top;"|Poisson ratio of the reinforced ring
|  style="text-align: center;vertical-align: top;width: 23%;"|<math display="inline">0.34</math> 
|-
|  style="text-align: center;vertical-align: top;width: 14%;"|<math display="inline">{\alpha }_{al}</math> 
|  style="text-align: center;vertical-align: top;"|Thermal expansivity of the reinforced ring
|  style="text-align: center;vertical-align: top;width: 23%;"|<math display="inline">1.48\times {10}^{-5}{\mbox{ K}}^{-1}</math> 
|-
|  style="border-bottom: 2pt solid black;text-align: center;vertical-align: top;width: 14%;"|<math display="inline">B_0</math> 
|  style="border-bottom: 2pt solid black;text-align: center;vertical-align: top;"|Fitting parameters
|  style="border-bottom: 2pt solid black;text-align: center;vertical-align: top;width: 23%;"|<math display="inline">1.3\mbox{ T}</math> 
|}


In the mechanical calculations, the ring bulk sample is considered as an isotropic linear elastic material. The mechanical equilibrium equation can be expressed as follows

{| class="formulaSCP" style="width: 100%; text-align: center;" 
|-
| 
{| style="text-align: center; margin:auto;" 
|-
| <math>\nabla \cdot \boldsymbol{\sigma }+\boldsymbol{F}_L=</math><math>0</math>
|}
| style="width: 5px;text-align: right;white-space: nowrap;" | (10)
|}

{| class="formulaSCP" style="width: 100%; text-align: center;" 
|-
| 
{| style="text-align: center; margin:auto;" 
|-
| <math>\boldsymbol{F}_L=\boldsymbol{J}\times \boldsymbol{B}</math>
|}
| style="width: 5px;text-align: right;white-space: nowrap;" | (11)
|}


Where  <math>\boldsymbol{F}_L</math> is the Lorentz force;  <math>\overline{\rho }</math> is the mass density. In the study, it is assumed that the transient behavior of the structure is quasi-static and that the second-order time derivative of the displacement variable  <math display="inline">u</math> - the inertia term  <math display="inline">\rho \frac{\mbox{d}^2u}{\mbox{d}t^2}</math> - are zero. Due to the occurrence of the Lorentz force during the magnetization process of the high-temperature superconducting ring bulk sample in a pulsed field, the influence of the stress distribution caused by the Lorentz force is considered in the mechanical calculations of this study. It is assumed that the bulk superconductor is fixed on a base, thus imposing a mechanical boundary condition of zero displacement at the lower edge. The stress-strain relationship in the ring bulk sample is given by

{| class="formulaSCP" style="width: 100%; text-align: center;" 
|-
| 
{| style="text-align: center; margin:auto;" 
|-
| <math>\left[\begin{array}{c}
{\epsilon }_r\\
{\epsilon }_{\varphi }\\
{\epsilon }_z\\
{\gamma }_{zr}
\end{array}\right]=\left[\begin{array}{cccc}
\frac{1}{E} & -\frac{\upsilon }{E} & -\frac{\upsilon }{E} & 0\\
-\frac{\upsilon }{E} & \frac{1}{E} & -\frac{\upsilon }{E} & 0\\
-\frac{\upsilon }{E} & -\frac{\upsilon }{E} & \frac{1}{E} & 0\\
0 & 0 & 0 & \frac{1}{G}
\end{array}\right]\left[\begin{array}{c}
{\sigma }_r\\
{\sigma }_{\varphi }\\
{\sigma }_z\\
{\tau }_{zr}
\end{array}\right]</math>
|}
| style="width: 5px;text-align: right;white-space: nowrap;" | (12)
|}


Where  <math display="inline">\upsilon </math> is the Poisson's ratio and  <math display="inline">E</math> is the Young's modulus.

The simulation and modeling of the aforementioned aspects were conducted using the finite element method. The parameter values mentioned earlier but not provided were provided in <span id='cite-_Ref143373393'></span>[[#_Ref143373393|Table 1]].

=3 Results and discussions=

''3. 1 Verification of results''

To ensure the accuracy of the simulation results, a comparative validation was conducted with experimental data <span id='cite-_Ref132916814'></span>[[#_Ref132916814|[25]]]. The validation involved a ring bulk superconductor with an inner diameter of 36 mm and an outer diameter of 30 mm, which was reinforced with a 5 mm thick aluminum alloy and affixed to a 1 mm thick indium foil. The ambient temperature during the experiment was maintained at 65 K. <span id='cite-_Ref143373643'></span>[[#_Ref143373643|Figure 2]] shows the trapped field at the center of the ring superconductor obtained from both the numerical simulation and the experimental measurements. By comparing the numerical simulation results with the experimental data, it was found that the numerical results closely approximated the experimental results, providing evidence of the accuracy of the numerical simulation.

<div class="center" style="width: auto; margin-left: auto; margin-right: auto;">
 [[Image:Review_893267287081-image72.png|294px]] </div>

<div id="_Ref143373643" class="center" style="width: auto; margin-left: auto; margin-right: auto;">
Figure 2 Comparison of numerical simulation and experimentally obtained trapped fields, where  <math display="inline">B_{ex}=2.53\mbox{ T}</math> ,  <math display="inline">t_1=13\mbox{ ms}</math> </div>

''3. 2 Calculated results for ring bulk superconductor''

To analyze the electromagnetic characteristics of the ring bulk superconductor during the PFM process, Figure 3 shows the magnetic field, and current density distributions of the bulk superconductor at different times (5 ms, 13 ms, 20 ms, 80 ms and 150 ms). As shown in the figure, the magnetic field at the ascending stage (0-13 ms), penetrates from the upper and lower ends of the bulk superconductor towards the interior. Simultaneously, a circular current is generated within the bulk, gradually flowing from the external region into the interior. Conversely, reverse currents begin to appear simultaneously from the upper and lower ends of the bulk sample at the descending stage (after 13ms).

<div class="center" style="width: auto; margin-left: auto; margin-right: auto;">
 [[Image:Review_893267287081-image75.png|600px]] </div>

<div id="_Ref143373901" class="center" style="width: auto; margin-left: auto; margin-right: auto;">
Figure 3 Magnetic field and current density distribution in the bulk under the PFM process</div>

<span id='cite-_Ref143374175'></span>[[#_Ref143374175|Figure 4]](a) and (b) depict the distribution of the trapped field and temperature at different times during the magnetization process on the z=0 plane. The observed variation in the trapped field aligns with the findings in Ref.<span id='cite-_Ref132901240'></span>[[#_Ref132901240|[15]]] for cylindrical bulk samples. However, the temperature variation differs from that of cylindrical bulk samples. In the simulation results, it could be found that the temperature gradually increases inward from the right side along the radius and then decreases gradually. This phenomenon arises due to the reinforcement of the bulk sample with an aluminum alloy ring, which affects the thermal conduction between the bulk sample and the aluminum alloy, thereby influencing the temperature distribution.

<div class="center" style="width: auto; margin-left: auto; margin-right: auto;">
 [[Image:Review_893267287081-image76.png|432px]] </div>

<div id="_Ref143374175" class="center" style="width: auto; margin-left: auto; margin-right: auto;">
Figure 4 Trapped field and temperature distribution in the z=0 plane of the bulk at different times under the PFM process</div>

<span id='_Hlk144209478'></span>For study the mechanical response in the PFM process, <span id='cite-_Ref143374303'></span>[[#_Ref143374303|Figure 5]](a) and (b) present the distribution of radial stress on the z=0 plane, corresponding to the ascending stage and descending stage of the external magnetic field, respectively. In ascending stage, compressive stress is generated within the sample when the magnetic field gradually penetrates into the bulk sample. Subsequently, during the descending stage of the external magnetic field, the radial stress undergoes a transition from compression to tension due to the variation in the direction of the current. <span id='cite-_Ref143374303'></span>[[#_Ref143374303|Figure 5]](c) and (d) show the distribution of hoop stress  <math display="inline">{\sigma }_{\varphi }</math> on the z=0 plane of the bulk sample during the magnetization process, corresponding to the ascending stage and descending stage, respectively. It can be observed that during the ascending stage, compressive stress exists at the inner edge of the ring bulk superconductor. As the external magnetic field decreases, the hoop stress at the inner edge gradually transitions to tensile stress. The hoop stress experienced by the inner edge of the ring bulk sample is higher than that of the outer edge. Therefore, it can be inferred that the inner edge of the ring bulk superconductor is more prone to crack formation than the outer edge. In the next section, we will introduce pre-existing crack and analyze their electromagnetic and mechanical characteristics separately, while both of central crack case and edge crack case are considered.

<div class="center" style="width: auto; margin-left: auto; margin-right: auto;">
 [[Image:Review_893267287081-image78.png|372px]] </div>

<div id="_Ref143374303" class="center" style="width: auto; margin-left: auto; margin-right: auto;">
Figure 5 Distribution of radial and hoop stresses at different moments in the z=0 plane of a bulk under the action of a pulsed magnetic field</div>

''3. 3 Calculated results for ring bulk superconductor with crack''

In this section, the simulation results are analyzed for the models of blocks containing elliptical center crack and blocks containing semi-elliptical edge crack, respectively The semi-major axis and semi-minor axis of the elliptical are  <math display="inline">a=1\mbox{ mm}</math> ,  <math display="inline">b=\mbox{0}\mbox{.1 mm}</math> , respectively.

<span id='cite-_Ref143374521'></span>[[#_Ref143374521|Figure 6]] depict the distributions of magnetic field and current density at 13 ms, 80 ms, and 150 ms for the ring bulk sample with a central elliptical crack and the ring bulk sample with a semi-elliptical edge crack case. It can be observed that the presence of both the central crack case and edge crack case has a minor impact on the distribution of the magnetic field. However, the presence of crack changes the geometric structure of the bulk sample, leading to variations in the current distribution. Additionally, the direction of the current density also variations in the vicinity of the crack.

The temperature of the bulk sample gradually increases as the external magnetic field rises. However, the presence of crack also introduces certain variations to the temperature rise trend. As shown in <span id='cite-_Ref143374608'></span>[[#_Ref143374608|Figure 7]], when there are without crack in the bulk sample, the temperature undergoes a sudden jump during the descending stage. The central crack case has a more gradual temperature variation than edge crack case. However, in edge crack case, the temperature experiences two jumps during the descending stage, with a larger amplitude and higher jump temperature. This phenomenon indicates that the presence of edge crack case, will change the direction of the current around the crack. The current concentrated on the region near the crack, resulting in larger electric fields. Due to the strong nonlinearity  <math display="inline">\boldsymbol{E-J}</math> relationship of the bulk superconductor, the Joule heat will rise and leads to significant local temperature increase.

<div class="center" style="width: auto; margin-left: auto; margin-right: auto;">
 [[Image:Review_893267287081-image82.png|600px]] </div>

<div id="_Ref143374521" class="center" style="width: auto; margin-left: auto; margin-right: auto;">
Figure 6 Distributions of magnetic field and current density in central crack case (left) and edge crack case (right) </div>

<div class="center" style="width: auto; margin-left: auto; margin-right: auto;">
 [[Image:Review_893267287081-image83.png|324px]] </div>

<div id="_Ref143374608" class="center" style="width: auto; margin-left: auto; margin-right: auto;">
Figure 7 Maximum temperature of the bulk as a function of time in the presence of a pulsed magnetic field</div>

<div class="center" style="width: auto; margin-left: auto; margin-right: auto;">
 [[Image:Review_893267287081-image84.png|600px]] </div>

<div id="_Ref143374695" class="center" style="width: auto; margin-left: auto; margin-right: auto;">
Figure 8 Stress distributions clouds for bulk containing central crack case (left) and edge crack case (right) </div>

<span id='cite-_Ref143374695'></span>[[#_Ref143374695|Figure 8]] show the distributions of circumferential and radial stress at 13 ms, 80 ms, and 150 ms for the ring bulk sample with a central elliptical crack and the ring bulk sample with semi-elliptical edge crack case. It can be observed that stress concentration occurs at the crack tips, resulting from the alteration of the bulk sample's geometric shape due to the presence of crack. The crack lead to the stress concentration effect.  And this stress concentration phenomenon also leads to the non-uniformity of the critical current density, thereby affecting the distribution of temperature.

<span id='cite-_Ref143374808'></span>[[#_Ref143374808|Figure 9]](a) and (b) depict the distribution of radial and hoop stress on the z=0 plane at 13 ms and 50 ms, respectively, for the bulk sample without crack, with a central crack case, and with edge crack case. As shown in Figure 9, both radial and hoop stress experience a significant increase at the crack tips, indicating stress concentration. However, the stress values at the crack tips exhibit a more pronounced increase due to the presence of crack. At 13 ms, the stress concentration caused by edge crack case is more obvious than central crack case. The maximum radial stress on the z=0 plane for the bulk sample without crack is  <math display="inline">-20.7\mbox{MPa}</math> , while for the bulk sample with a central crack case, it is  <math display="inline">-36.1\mbox{MPa}</math> , representing a 74% increase compared to the crack-free bulk sample. The bulk sample with edge crack case exhibits a maximum hoop stress on the z=0 plane of  <math display="inline">37.1\mbox{MPa}</math> , representing a 79% increase compared to the crack-free bulk sample. At 50 ms, the stress concentration caused by central crack case becomes more pronounced than that caused by edge crack case. However, overall, edge crack case can lead to larger stress concentrations than central crack case.

The size of the crack length also has a certain influence on the maximum stresses. In <span id='cite-_Ref143374903'></span>[[#_Ref143374903|Figure 10]], we analyze the variation in the maximum radial and hoop stresses among bulk samples with different edge crack lengths case. It can be observed from the figure that both radial and hoop stresses increase with the increase in crack length, with the hoop stress exhibiting a more pronounced trend. This phenomenon occurs because as the crack length increases, the stress concentration effect becomes more prominent. When the crack is shorter, the sharpness at the crack tip is lower. However, as the crack length grows, the sharpness at the crack tip increases, and the region of high stress expands accordingly, leading to higher stresses in the sample.

<div class="center" style="width: auto; margin-left: auto; margin-right: auto;">
 [[Image:Review_893267287081-image88.png|444px]] </div>

<div id="_Ref143374808" class="center" style="width: auto; margin-left: auto; margin-right: auto;">
Figure 9 Distribution of radial and hoop stresses without crack and with central case and edge crack case at different times in z=0 plane</div>

<div class="center" style="width: auto; margin-left: auto; margin-right: auto;">
 [[Image:Review_893267287081-image89.png|348px]] </div>

<div id="_Ref143374903" class="center" style="width: auto; margin-left: auto; margin-right: auto;">
Figure 10 Maximum radial and hoop stresses during magnetization of bulk containing edge crack case of different lengths</div>

=4 Conclusions=

In this study, the distribution of electromagnetic fields, temperature, and stress in ring bulk superconductor was simulated and analyzed by employing the H-formulation, heat conduction equation, and mechanical equilibrium equation. The coupled equations of force-electric-magnetic-thermal multi-field were solved to obtain the simulation results, which exhibited a good agreement with the experimental findings.

The research findings indicate that when a pulsed external magnetic field is applied, the magnetic field gradually penetrates into the bulk sample from the upper and lower ends on the right side. Induced currents are generated within the bulk sample, and the direction of these currents variations as the external magnetic field decreases. During the ascending stage of the external magnetic field, compressive stress is generated within the bulk sample. Conversely, as the external magnetic field decreases and the direction of the current variations, tensile stress is produced, leading to an influence on the critical current density of the bulk sample.

Subsequently, simulations were performed on bulk samples with central crack case and edge crack case, respectively, and the distributions of electromagnetic fields, temperature, and stress under PFM were analyzed. The results indicate the occurrence of localized stress concentration due to the presence of crack. Moreover, the crack induce variations in the direction of current and result in localized temperature elevation near the crack vicinity. The maximum radial and hoop stresses within the bulk sample also increase with the length of the crack.

==Acknowledgements==

The authors gratefully acknowledged the support from the Fujian Natural Science Foundation (2020J05180) and the Scientific Research Foundation of Fujian University of Technology (GY-Z19046). No part of this work has been published or submitted elsewhere. The authors declared that they have no conflicts of interest in this work.

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