Submitted:
01 October 2024
Posted:
03 October 2024
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Abstract
Keywords:
1. Introduction
1.1. Background
1.2. Problem Statement
1.2.1. Energy Requirements:
1.2.2. Cost
1.2.3. Material Durability
1.3. Research Objectives
- How can the high energy demand of MHD propulsion be met efficiently using available or emerging technologies?
- What technological advancements or economic strategies can reduce the overall cost of MHD system implementation?
- What new materials or design improvements are necessary to enhance the durability of system components exposed to corrosive marine environments?
1.4. Significance
2. Literature Review
- (a)
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The text Marine Propellers and Propulsion [1] provides a comprehensive overview of the advancements and key findings in the development of propulsion systems. Several notable insights regarding these systems are highlighted below:
- “The thrust of an MHD drive is proportional to σB2, where σ is the conductivity of the liquid being pumped; in the case of a ship this being sea water. The necessary magnetic fields can be large even by modern standards. For torpedoes with a high-top speed it may be necessary to create fields in the range 15–20 T; however, for ships and submarines at typical speeds the magnetic field can be lower, around 5–10 T.”
- “In theory, the electrical field can be generated either internally or externally, in the latter case by positioning a system of electrodes in the bottom of the ship. This, however, is a relatively inefficient method for ship propulsion and the environmental impact of the internal system is considerably reduced due to the containment of the electromagnetic fields. Most work, therefore, has concentrated on systems using internal magnetic fields and the principle of this type of system is shown in Figure 1 in which a duct, through which sea water flows, is surrounded by superconducting magnetic coils, which are immersed in a cryostat. Two electrodes are placed inside the duct, which create the electric field necessary to interact with the magnetic field to create the Lorentz forces for propulsion. Nevertheless, the efficiency of a unit is low. The efficiency, however, is proportional to the square of the magnetic flux intensity and to the flow speed, which is a function of ship speed. Consequently, to arrive at a reasonable efficiency, it is necessary to create a strong magnetic flux intensity through the use of powerful magnets.”
- “Magnetohydrodynamic propulsion does have certain potential advantages in terms of providing a basis for noise and vibration-free hydrodynamic propulsion. However, a major obstacle to the development of this form of propulsion until relatively recently was that of the design of the superconducting coil and its attendant refrigeration equipment to maintain its zero-resistance property. However, developments in superconductivity have in the last few years shown potential to produce marine propulsion motors using the high-temperature superconductors.”
- (b)
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The Yamato-1 [2], recognized as the world's first superconducting magnetohydrodynamic (MHD) propulsion ship, was developed after six years of research and development, culminating in 1991. This pioneering work led to significant practical advancements, demonstrating the feasibility of MHD propulsion in real-world applications. Several key findings from this research are highlighted below as citations:
- “The most important result was gaining the manufacturing technology for a lightweight but large-size superconducting magnet with a stable and strong magnetic field of 4 Tesla with 23 megajoules (MJ).”
- “According to the results reached by our group, it seems that ships with such propulsion systems would be justified for commercial operation, if we could raise the magnetic field magnitude of the MHD thruster to 20 to 30 Tesla.”
- “Although we used the superconducting coils to create such a magnetic field, it may be possible eventually to use a magnetic field in the form of a permanent magnet if science and technology make progress in this area. Then the hoop stress problem we had to deal with painstakingly in the case of the Yamato-I would be solved more easily.”
- “Displacement” is the weight of a ship. A 185-ton displacement in the case of a passenger ship generally means a size large enough to carry 500 passengers comfortably. However, in the case of the Yamato-I, due to its extremely heavy propulsion system and overall related systems, the complement was only 10 people in spite of her 185-ton displacement.

- (c)
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Additionally, another study [3] explored the benefits of utilizing an efficient magnetic field. The research highlights the advantage of employing a strong magnetic field generated through a disk-shaped generator, as detailed below:
- “Another advantage of this design is that the application of the magnetic field is more efficient, has a parallel field configuration, and the working fluid is processed in the magnetic disk closer so that the magnetic strength increases.”

- (d)
-
The principle of superposition, as discussed in the website [4], explains how the magnetic field generated by an iron core within a solenoid significantly exceeds the magnetic field initially produced by the solenoid itself. This amplification effect is central to understanding the enhanced magnetic field strength in such systems.
-
“It comes down to superposition. The magnetic field generated by the coil is augmented by the magnetic field generated by the core (that itself is caused by the magnetic field from the coil). As the ferromagnetic atoms with their unpaired outer electrons are aligned by the coil’s magnetic field, their own now aligned magnetic fields are added to the field that caused them. In fact, the magnetic field contributed by the core is much stronger than the coil’s magnetic field that ‘triggered’ it.”Furthermore, in Wikipedia [6], an idea of how powerful a magnetic field can be created by an iron core is obtainable. It is cited as below:
- “Soft (annealed) iron is used in magnetic assemblies, direct current (DC) electromagnets and in some electric motors; and it can create a concentrated field that is as much as 50,000 times more intense than an air core.”
-
- (e)
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The study [6] also highlights that the realization of such ships remaining unfeasible due to the insufficient magnetic field generated:
- “For magnets based MHD ships, the strength of the magnets currently available actually limits the efficiency at this order of magnitude. To obtain the same efficiency than conventional propellers, MHD thrusters require compact and light generators of approximately 10 Tesla magnetic fields, which still remains challenging nowadays.”
- (f)
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Further exploration led to the identification of healthcare devices utilizing strong magnetic fields, as highlighted in [7]. One such device, developed for magnetic field therapy, employs pulsating electromagnetic fields capable of reaching 4 Tesla in magnitude. This technology is primarily used for pain relief and the treatment of musculoskeletal disorders. The following citation was obtained in support of this finding.
- “Magnetic field therapy is a treatment method that uses magnetic fields to relieve pain and promote healing. It is based on the fact that magnetic fields can influence the flow of energy in the body. The device we use has a field strength of 4 Tesla.”
- (g)
-
Subsequent investigations focused on low-field MRI technology, which emerged as a relevant area of interest due to its emphasis on achieving high magnetic field uniformity over large volumes through cost-effective methods, while maintaining minimal weight and size. These objectives aligned closely with our own research goals. To make MRI technology more accessible, particularly given the prohibitive costs associated with traditional high-field MRI systems, numerous studies have been conducted on low-cost MRI solutions. Notably, [8] documents significant efforts toward the development of affordable low-field MRI systems, with relevant citations provided below.
- “The basic concept of the new magnet design (Fig. 1d) involves two identical rectangular pole structures, comprising a backing yoke of low-carbon steel on which are mounted magnetized blocks of Neodymium-Boron-Iron (Nd-B-Fe) permanent magnets. The north and the south poles on the two halves of the assembly are arranged to oppose each other symmetrically, thus generating the net magnetic field B0 in the central region between the poles is parallel to the x-axis.”
- “The designed field of 0.15 Tesla at an accessible gap of 220 mm was chosen as a realistically achievable target using Nd-B-Fe permanent magnets while having a proven record of providing clinically useful MRI images.

- (h)
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Next was a research article [9] on the design of an efficient electromagnet for homogeneous low field MRI which turned out to be an eye opener. Here the efficiency was improved because of the use of a ferromagnetic housing of 10mm thickness. Maximum achievable field strength was 80mT. Citations offered several insights as below:
- “Effective implementation succeeded through the unique use of steel plates as a housing system. This setup increased the effectiveness of the B0 field and eliminated adjacent stray fields. The steel housing serves as a magnetic return circuit, amplifies the generated B0 field, and simultaneously provides several opportunities for shimming (e.g., by using permanent magnets on the outer and inner sides of the housing). In addition, the housing effectively shields interferences and comprises a stable mounting suspension of the magnet coils and gradient system. Another special feature is the compact design of the gradient coil system, which is embedded within the magnet coils and therefore does not require additional space. The system operates at a B0 field strength of 23mT (965 kHz) generated by a 500 W amplifier.”
- “At a similar B0 field strength, less power is needed in the presence of such high magnetic susceptibility housing; thus, at a constant total weight, magnetic efficiency increases. For instance, the B0 field decreases from 23 to 6 mT when calculated for the same coil geometry but in the absence of the steel housing.”
- “In this paper, we present a low-cost and compact electromagnet that consists of a steel housing with copper coils. The housing was used for field enhancement, homogenization, and shielding. This concept ensures a compromise between large sample volumes, high homogeneity, high B0 field, low power consumption, light weight, simple fabrication, and conserved mobility, without the necessity of a dedicated water-cooling system.”

3. Objectives
4. Research Gaps
5. Opportunities and Constraints
5.1. Technological Opportunities
5.1.1. Environmental Impact:
5.1.2. Innovation in Marine Propulsion:
5.1.3. Research and Development:
5.2. Economic and Industrial Constraints
5.2.1. High Initial Costs:
5.2.2. Energy Supply and Infrastructure:
5.2.3. Limited Scalability for Smaller Vessels:
5.3. Material and Durability Constraints
5.3.1. Material Limitations:
5.3.2. Advancements in Material Science:
5.4. Regulatory and Market Constraints
5.4.1. Regulatory Challenges:
5.4.2. Market Demand:
5.5. Future Prospects
6. Conclusions
6.1. Summary of Key Findings
6.2. Implications for the Future
6.3. Recommendations for Further Research
6.3.1. Energy Efficiency:
6.3.2. Cost Reduction Strategies:
6.3.3. Material Durability:
6.3.4. Regulatory Frameworks:
6.4. Concluding Remarks
References
- J.S. Carlton FREng, Marine Propellers and Propulsion (Fourth Edition): Elsevier Ltd., 2019. [CrossRef]
- Under editorial Supervision of Yohei Sasakawa n.d. “Yamato-1”. 21 September. https://www.spf.org/en/_opri_media/publication/docs/yamato-1.pdf# (accessed on 21 September 2024).
- Wiwik Purwati W (1), Slamet Priyo Atmojo (2), Margana (3), Suwarti (4), Budhi Prasetiyo (5), Ikhwatinah Khoiroh (6), Performance of Magneto Hydro Dynamic (MHD) as a Power Generation Support Tool: Eksergi, Vol. 18, No. 2. May 2022. [CrossRef]
- Robin Bornoff, “Demystifying Electromagnetics, Part 5 – Ferromagnetic Cores”, blogs.sw.siemens.com, June 14, 2021. [Online]. Available: https://blogs.sw.siemens.com/simulating-the-real-world/2021/06/14/demystifying-electromagnetics-part-5-ferromagnetic-cores/ (accessed on 22 September 2024).
- “Magnetic core”, en.wikipedia.org/, Last edited on 4 July 2024. [Online]. Available: https://en.wikipedia.org/wiki/Magnetic_core (accessed on 10 September 2024).
- David Cébron, Sylvain Viroulet, Jérémie Vidal, Jean-Paul Masson, Philippe Viroulet, “Experimental and Theoretical Study of Magnetohydrodynamic Ship Models”: HAL, 5 Jul 2017. [CrossRef]
- “4T-Magnetic field therapy”, https://tom-mallorca.com/en/. [Online]. Available: https://tom-mallorca.com/en/treatments/4t-therapy/ (accessed on 20 September 2024).
- John V.M. McGinley, Mihailo Ristic ⇑, Ian R. Young, A permanent MRI magnet for magic angle imaging having its field parallel to the poles, Journal of Magnetic Resonance 271 (2016) 60–67: Elsevier Ltd. [CrossRef]
- Steffen Lother, Steven J. Schiff, Thomas Neuberger, Peter M. Jakob, Florian Fidler, Design of a mobile, homogeneous, and efficient electromagnet with a large field of view for neonatal low field MRI, Magnetic Resonance Materials in Physics: ESMRMB 2016. [CrossRef]

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