Abstract

Magnetic field can generate interface instability when some liquids are put close to magnetic field. A well-known interface instability is called Rosensweig instability or normal field instability. Here we report that pure liquid Co can be highly undercooled close to its Curie temperature in strong magnetic field with very high magnetization and exhibiting unique morphology instability called the normal field instability. To obtain such unique instability pattern, the sample size, undercooling and magnetic field intensity need fulfill certain condition. In the present study, we have studied the required condition for obtaining normal field instability. The magnetization of the undercooled liquid Co is measured in a wide temperature range with different magnetic field intensities and calculated as a function of undercooling and field intensity. The critical size and critical magnetization for the normal field instability are calculated with the changing temperature and field intensity. Then the required conditions including the critical size, the minimum undercooling and field intensity for the existence of the instability pattern formation are determined.

Highlights

  • Ferromagnetism has been known exist only in solid state since no substance is known whose Curie temperature (TC) exceeds its melting point (Tm)[6]

  • Except for the ferrofluids, the existence of Rosensweig instability in pure liquid system is only observed in liquid oxygen[10]

  • A new idea considering undercooling technique was adopted for some special alloy system and ferromagnetism or strongly magnetized liquid was achieved by directly undercool the alloy below or approach the transition temperature of the magnetic state (TC(L))[6, 8, 12,13,14,15]

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Summary

Introduction

Ferromagnetism has been known exist only in solid state since no substance is known whose Curie temperature (TC) exceeds its melting point (Tm)[6]. By inserting the determined parameters into equation (2), the magnetization of Co above Curie temperature are calculated for solid during heating and liquid during cooling, respectively.

Results
Conclusion

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