Large Bulk (RE)BCO superconducting magnets for desktop NMR/MRI

Lead Research Organisation: University of Cambridge
Department Name: Engineering

Abstract

NMR and MRI are techniques that use the interactions of atoms with external magnetic fields to look inside materials, objects and organisms to study their composition (NMR) and provide images (MRI). They are used very widely in scientific research, medical research and in industry and medicine. Put simply, the stronger the magnetic field available the better these techniques work. Unfortunately, obtaining large magnetic fields (typically 20 -30 times strong than a fridge magnet) generally requires expensive magnets, which are usually wound from long lengths of superconducting wire. It would be ideal to be able to produce these very large magnetic fields in a much simpler fashion to provide convenient and cheap desktop systems. Making these systems widely available and cheaper would allow more scientists, engineers and medical researchers to have access to this equipment, and to use it more often. The importance of this proposed project is underlined by the active participation and practical help offered by our three industrial partners.

We are proposing to use ceramic bulk (in disc- or ring-form) superconductors, rather than complex solenoidal coils made from superconducting wire. The three main challenges that must be overcome to do achieve this are (i) making bulk superconductors of sufficient size and uniformity, (ii) making the magnetic field they produce highly uniform, and (iii) developing a practical way of charging bulks samples with magnetic field. To address the first two challenges the Cambridge group, with extensive experience of the fabrication and manufacture of these bulk superconductors, is going to partner with the Oxford group, who have experience of using advanced microscopy to look carefully at the fine details of the manufacturing process. To magnetise the bulk superconductors, we propose to discharge, over a period of several milliseconds, the energy stored in a bank of capacitors into a conventional coil magnet made of copper. Such a copper coil would overheat and melt if were to generate a large magnetic field continuously. However, using this pulsed field magnetisation technique, we can achieve the required field over a short period of time, but long enough to allow the bulk superconductor to "capture" the magnetic field.

We will consider the project successful if we can replace the conventional, permanent magnet of an existing NMR system, provided by our industrial partner, with our prototype bulk superconductor based system and demonstrate that it operates effectively at the proton resonance frequency of 200 MHz, rather than at 90 MHz, which is typical of existing permanent magnet systems and a limiting feature of this technology.

Planned Impact

The aim of this project is to lay the foundation to open up a whole new market segment for desktop MRI and NMR systems utilising magnetic fields of up to 5 T. Existing systems either use large and bulky room size superconducting solenoids and are expensive (>£1m) or sacrifice performance by employing much cheaper permanent magnets [1]. Our project would therefore make a direct and positive economic contribution in a field where UK companies, including Oxford Instruments and Siemens Healthineers, both of which are partners in this project, are sector leaders [2]. The NMR market has been predicted to reach over $2.5 billion by the mid 2020s [3] and that of the MRI market $5 billion [4].
Reducing the cost and size of these instruments will have a broader societal impact, making the technology, as well as the analysis, more affordable for end-users. In addition, the increased field offered by bulk superconducting magnets will allow improvements in performance, from 40-90 MHz typical of permanent magnet systems [5] to 200 MHz, increasing throughput and widening the range of applications for these cheaper systems.

Our proposal has been developed with companies that make systems using these technologies. This means they will be able to advise us at every stage of the project to make sure that our focus is relevant to the ultimate exploitation of the technology. This also means that, if successful, there will be a clear route from laboratory to factory for the progress we demonstrate.
This project targets a bore size suitable for research, rather than medical diagnostic work. Nonetheless, if we successfully overcome the limitations of sample size, solenoids based on bulk superconductors could find a role in Extremity MRI [6]. These are compact systems that reduce the load on expensive full size systems by providing imaging of limbs. This is of increasing importance as MRI becomes a more heavily used technique, in the NHS there has been an over 200% increase in demand over a 10-year period [7].

The availability of larger, high quality, bulk superconductors that we propose to develop would benefit the wide range of potential applications for bulk superconductors. Those identified, besides NMR and MRI , in our recently published roadmap for the application of bulk superconductors[8] include compact high power density motors for electric aircraft and road transport, large magnetic fields for drug targeting and magnetic shielding systems.



[1] https://lbnmedical.com/how-much-does-an-mri-machine-cost/
[2] Melhem Z 2011 Materials UK Prelim. Review, Superconducting Materials and Applications: A UK Challenge and an Opportunity
[3] https://www.reuters.com/brandfeatures/venture-capital/article?id=78610
[4] https://www.reuters.com/brandfeatures/venture-capital/article?id=104390
[5] http://www.magritek.com/products/spinsolve/
[6] https://www.gehealthcare.com/news-center/optima-mr430s-scanner
[7] https://www.england.nhs.uk/statistics/
[8] Durrell et al., Superconductor Science and Technology, Volume 31, Number 1

Publications

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Huang K (2019) Composite stacks for reliable > 17 T trapped fields in bulk superconductor magnets in Superconductor Science and Technology

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Namburi D (2021) Improved mechanical properties through recycling of Y-Ba-Cu-O bulk superconductors in Journal of the European Ceramic Society

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Tsui Y (2022) Trapped Fields >1 T in a Bulk Superconducting Ring by Pulsed Field Magnetization in IEEE Transactions on Applied Superconductivity

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Tsui Y (2022) Waveform Control Pulsed Field Magnetization of RE-Ba-Cu-O Bulk Superconducting Rings in IEEE Transactions on Applied Superconductivity

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Tutt N (2023) Fabrication of high-quality joints between Gd-Ba-Cu-O bulk superconductors in Superconductor Science and Technology

 
Description Due to the Covid-2019, there has been limited access to the lab in 2020-21, which means only 60% of the work has been completed.

1. A study on the stacking of two single grains exhibiting different trapped fields at their top and bottom surfaces has been performed and completed. The results show that the best high and most uniform trapped field of the stack of two samples is achieved by placing the two bottom surfaces (which are usually those with lower and non-uniform trapped fields) in intimate contact in the middle of the stack.

2. A further improved and stabilised the melt process has been developed. This process involves wet-ball mixing to increase the uniformity of the mixed precursor powder to improve the reliability of the crystal growth and uniformity of the superconductivity within the bulk single grains.

3. A method that allows the growth of ring-shaped single grains directly has been developed to improve the uniformity of the superconducting properties.

4. The superconducting properties of single grains containing different rare-earth elements (Gd and Eu), different sources of supply and the effects of the Ag addition has been investigated. The results show that adding Ag improves the superconducting properties of the single grain, including the trapped field, despite the fact that Ag is not superconducting. Research in this area is continuing.

5. Multi pulse-magnetisation of a relatively large numbers of bulk and ring samples has been used to demonstrate there is no clear correlation between the trapped field obtained by field-cooling by pulse-magnetisation. The thermal conductivity of the assembled composite single grain, however, is most likely a dominating factor in determining the final trapped field.

6. The intrinsic uniformity of the superconducting properties of single grain (RE)BCO materials has been further studied. For the first time, the distribution of the Jc-B at a facet line has been measured and compared with the distribution of Jc-B in the a/b direction. In general, and significantly, the facet lines exhibit higher Jc-B.

7. A variety of shapes of bulk, single grain material, such as cylinders, rings 41OD16ID (8 of 10), square and triangular geometries have been fabricated successfully. The work for assembling the samples for designs A and B in the proposal is in progress.

8. GdBCOAg single grains up to 60 mm in diameter have been grown for the first time.

9. EuBCOAg single grains up to 60 mm in diameter have been grown for the first time. The Eu/Ba substitution issue in the EuBCO system has been resolved and the BaO2 content optimised for suppressing the Eu/Ba substitution to improve the trapped field.

10. Detailed research on the distribution of the critical supercurrent density (Jc) of single grains has been performed. A comparison of Jc at the facet line and along the a/b direction over the entire ac-plane has been made and the effect of the observed difference in the trapped field contour map examined.

11. It has been confirmed that the distributions of Jc do not correlate directly with volume fraction of Gd-211 phase content, suggesting for the first time that Gd-211 may not be the main factor determining Jc.

12. An arrangement has been proposed to reduce the effect of the changing Jc distribution along the facet lines to provide a more uniform trapped field, which may inspire future research directions.

13. The microstructure and superconducting properties of EuBaCuO and GdBaCuO single grain samples have been compared and a paper has been published.

14. Systematic PFM measurements on a Gd-Ba-Cu-O ring bulk sample have been carried out and a trapped field of 1.3 T at 55 K has been achieved using a multi-pulse, step-wise cooling (MPSC) technique (a paper has been published). The MPSC technique is repeatable and helps to avoid catastrophic flux jumps that can occur during the PFM of bulk ring that reduce significantly the trapped field and/or interrupt the circulating supercurrent.

15. 6 GdBCOAg and EuBCOAg single grains of diameter 60 mm have been fabricated successfully as required for the field pulse tests (one sample was broken during the mounting process).
16. After confirming that RE-211 sometimes may not be the main factor determining Jc, the effect of porosity on Jc has also been investigated by examining statistically 25 YBCO single grains of different sizes, suggesting for the first time that there is a strong correlation between the average Jc and porosity.
17. The effect of differences in Jc along the facet lines and the a/b direction has been studied mainly in terms of the shape of trapped field. Published results confirmed that the top surface of single grains tend to produce non-uniform square-shaped trapped field contour maps. However, circular contour maps can be achieved by stacking single grains with their facet lines off-set by 45 degrees. This research also suggests that a more uniform trapped field can be achieved by assembling samples in an appropriate arrangement, which has led, in turn, to the concept of "housing".
18. A multi-pulse step-wise-cooling (MPSC) sequence that includes a longer first-pulse rise time and multiple pulses of the same magnitude for some steps has been developed to achieve a trapped field of 1.3 T at 55 K. This is about four times that of the highest trapped field reported for any single ring bulk single grain sampel magnetised using PFM to date and represents a promising step forward in magnetising bulk, single-grain superconducting rings for use in practical engineering applications.

19. The magnitisation processes of single grains rings are better understood both analytically and experimentally as a result of this research. Magnetic flux is found to penetrate finite-thickness HTS rings from both the inner and outer surfaces, inducing a negative field at the inner face of the ring. As the applied field increases past the point of full penetration, the field at the inner surface is reversed, causing significant heating of the sample around this location. This makes HTS rings significantly more susceptible to localised heating and thermomagnetic instabilities that limit severely their ability to trap a useful magnetic field. In some cases, this can result in breaking the supercurrent flowing around the ring related to the HTS ring magnetisation, and a negative trapped field in the ring bore. Consequently, thermomagnetic stability of HTS rings during typical single-pulse PFM can only be ensured by applying a magnetising field that does not fully penetrate the sample, or by using more advanced PFM techniques like waveform control or multi-pulse stepwise-cooling to increase the trapped field.
Exploitation Route The results of the study on the stacking of two single grains will help the scientific community understand the use of one type of an assembly of single grains. The improved trapped field obtained and uniformity in the resultant composite bulk compared to a monolithic bulk superconductor of the same diameter will help design the assemblies for bespoke, high field applications.

The processing technique developed to allow the growth of ring-shape single grains directly what the potential to save materials and improve superconducting properties (more analysis is being performed).

An arrangement has been proposed to reduce the effect of changing Jc distribution and provide a more uniform trapped field, which has direct implications for practical applications and may inspire future research directions.

Further understanding on achieving uniform trapped field has triggered a "housing" idea, e.g. placing the object that is needed to provide uniform filed in applications in a "house" like assembly of smaller single grains to obtaining higher and more uniform magnetic field. The idea may attract interest from industry.
Sectors Energy,Healthcare,Transport

 
Description Detailed research on 20 specimens of half cross-section of a GdBCO single grain have shown that Jc-B at 77 K of these samples measured along facet line is about 10% higher than that in a/b direction (intrinsic compositional and structural differences along a facet line and the a/b direction is the reason for different Jc behaviour). As a result, trapped fields measured at the top layers of fully grown, high quality single grains exhibit squarer cross-sections, which is not generally desirable in practical applications. A sample arrangement has been proposed that reduces the effect of the variation in Jc distribution to provide a more uniform trapped field across the entire sample cross-section. This has been achieved by stacking two single grain slices with square-shaped trapped field contour maps in different orientations resulting in a uniform circular trapped field, demonstrating that it is possible to achieve a uniform trapped field from non-uniform material with non-uniform Jc. This observation may be used ultimately to achieve higher and more uniform fields in applications, such as MRI/NMR, levitation and undulators by the careful arrangement of individual single grains in an assembly. Further understanding on achieving uniform trapped field triggered a "housing" idea, e.g. placing the object that is needed to provide uniform magnetic field in applications in a "house-like" assembly of smaller single grains to obtain a higher and more uniform magnetic field. The idea is innovative and may attract interest from industry and initiate new research activity. After confirming that RE-211 may not always be the main factor determining Jc, the effect of porosity on Jc was also performed by examining statistically 25 YBCO single grains of different sizes, suggesting for the first time that there is a strong correlation between the average measured Jc and porosity. This observation suggests that any method that reduces porosity would improve the average Jc and hence trapped field. Although reducing porosity is limited to some extent, the relevant methods and processing techniques should be explored further and improved. The magnitisation processes of single grain rings are better understood both analytically and experimentally as a direct result of this research. Magnetic flux is found to penetrate finite-thickness HTS rings from both the inner and outer surfaces, inducing a negative field at the inner face of the ring. As the applied field increases past the point of full penetration, the field at the inner surface is reversed, causing significant heating of the sample around this location. This makes single grain HTS rings significantly more susceptible to localised heating and thermomagnetic instability that limit severely their ability to trap a useful magnetic field. This observation aids significantly the understanding of the pulse magnitisation of ring-shaped single grains, which is particularly important for NMR/MRI applications.
First Year Of Impact 2020
Sector Energy,Transport
Impact Types Societal

 
Title Research Data supporting "Understanding the porosity and its effects on the superconducting properties of YBCO single grains" 
Description This dataset contains the raw data for the journal article "Understanding the porosity and its effects on the superconducting properties of YBCO single grains". The file "README.txt" contains detailed information about the measurement of the raw data and the determination of the data shown in the paper. The .tif files contain tracking microscope images (OLYMPUS BX51M) of all 22 investigated YBCO bulk superconductors (5x 13.6 mm, 5x 16.0 mm, 5x 20.8 mm, 4x 24.8 mm, 2x 30.7 mm, and 1x 41.8 mm diameter). The file "Raw_data.xlsx" contains the sample number, diameter, height, area, pore count, average pore size and porosity of each of the 22 samples investigated. Furthermore, the file contains the maximum/minimum trapped field measured at the top and bottom of each sample. The average critical current density at the top/bottom of each sample was calculated with the formula shown in Equation 4 in the paper. Furthermore, "Raw_data.xlsx" contains the pore sizes measured for each sample set (Figure 6 in publication). The file "Raw_data_trapped_field.xlsx" contains the raw data for the trapped field profiles measured with 18 rotating hall probes 1.5 mm above the sample surface at 77 K (Figure 3 in publication). 
Type Of Material Database/Collection of data 
Year Produced 2022 
Provided To Others? Yes  
URL https://www.repository.cam.ac.uk/handle/1810/343120
 
Title Research data supporting "Dynamics of Magnetic Flux Propagation in Bulk, Single Grain Superconducting Rings during Pulsed Field Magnetisation" 
Description A summary of the research data supporting "Dynamics of Magnetic Flux Propagation in Bulk, Single Grain Superconducting Rings during Pulsed Field Magnetisation" The corresponding files contain the supplementary data for the paper DOI: - Modelling_Data.xlsx - Experimental_Data.xlsx - Fig17_Bz_J-Q-T-export-15-17-19ms.txt - Fig17-J-Q-higherdensity-export-15-17-19ms.txt - Fig17-J-Q-export-17p5ms.txt Detailed information about each file can be found in the READ_ME.txt file. 
Type Of Material Database/Collection of data 
Year Produced 2022 
Provided To Others? Yes  
URL https://www.repository.cam.ac.uk/handle/1810/341253
 
Title Research data supporting "Trapped Fields > 1 T in a Bulk Superconducting Ring by Pulsed Field Magnetization" 
Description Research data supporting [Trapped Fields > 1 T in a Bulk Superconducting Ring by Pulsed Field Magnetization]. The Microsoft Excel file contains all data plotted in figures 1 to 5 in the main manuscript. For all pulsed field magnetization data, the sample was first cooled down from the normal state to the superconducting state then a pulsed field or a sequence of pulsed field was applied to it. The values of trapped field shown in the data file are the values recorded at 15 seconds after applying each pulsed field. For a multi-pulse, stepwise cooling sequence, the wait time between two successive pulses was from ~5 min (at 77 K) to ~15 min (at 55 K) to allow sufficient time for the sample to return to its operating temperature before applying the next pulse. Unless stated otherwise, the applied field and the trapped field were the peak value of the magnetizing pulse and the trapped field at the centre of the sample bore, respectively. See the main manuscript for more details. 
Type Of Material Database/Collection of data 
Year Produced 2022 
Provided To Others? Yes  
URL https://www.repository.cam.ac.uk/handle/1810/335834
 
Title Research data supporting ''The effect of facet lines on critical current density and trapped field in bulk RE-Ba-Cu-O single grains'' 
Description Detailed current density measurements and the trapped fields measurements which show the effects of Jc distribution. Figure3 & Figure 4(a,c) (Tc and Jc along a faceline of sample 20181123 F7-1).xlsx are the results of critical transition temperature Tc and M-H loops measured using MPMS in the Maxwell centre. The critical current density Jc is calculated from the M-H loops for each cuboid at 77 K for an applied field cycle of 0 to 7 T to 0 T using the Bean model. All the data of 20 pieces of superconductor bulk samples in figure 1 is in this .xlsx file. The results are shown in figure 3 and 4. All .opj Origin 8.5 files are showing the measurements of trapped fields which are the indicators of samples' quality. We show the readers the shapes and magnitudes of trapped field for discussing ''The effect of facet lines on critical current density and trapped field in bulk RE-Ba-Cu-O single grains''. Each sample to be measured was field cooled at 77 K in an applied magnetic field of 1.0 T prior to 2D trapped field mapping using a rotating Hall sensor array. Origin was used to record the original data. These files here in .opj recorded the original data and their generated figures. 
Type Of Material Database/Collection of data 
Year Produced 2022 
Provided To Others? Yes  
URL https://www.repository.cam.ac.uk/handle/1810/339788
 
Description Can Superconductors 
Organisation Can Superconductors
Country Czech Republic 
Sector Private 
PI Contribution The investigation of parallel processing techniques for bulk single grain superconductors.
Collaborator Contribution Play the fundamental role in understanding the properties of performance of bulk superconductors fabricated from a variety of rare earth elements.
Impact The development of an improved melt process for bulk superconductors that yields better trapped field and greater potential for engineering applications.
Start Year 2006
 
Description Siemens 
Organisation Siemens AG
Department Siemens plc, Keele
Country United Kingdom 
Sector Private 
PI Contribution We provide samples for Siemens to do some measurements using their equipment.
Collaborator Contribution Siemens is interested in the applications of bulk materials in motors. Our research results will provide better understanding.
Impact multi-disciplinary
Start Year 2016