- Nano Express
- Open Access
DC bias immune nanocrystalline magnetic cores made of Fe73Nb3Cu1B7Si16 ribbon with induced transverse magnetic anisotropy
© Nosenko et al. 2016
- Received: 28 November 2015
- Accepted: 26 January 2016
- Published: 5 February 2016
The comparative analysis of magnetic properties of cut cores made of nanocrystalline Fe73Nb3Cu1B7Si16 alloy ribbon and cores made of the same ribbon with preliminary tension-induced transverse magnetic anisotropy was carried out. The possibility of improving magnetic properties of cut cores, decreasing loss, and increasing DC bias immunity of reversible magnetic permeability is presented. The influence of induced magnetic anisotropy on DC bias immunity of reversible magnetic permeability was investigated. The advantages and disadvantages of new cores (made of ribbon heated under tensile stress) over cut ones were determined.
- Nanocrystalline magnetic core
- Induced magnetic anisotropy
- Tensile stress
- DC bias immunity
Soft magnetic alloys are used in magnetic cores of various inductive components (of transformers and chokes) [1, 2]. Magnetic cores made of nanocrystalline Fe–Nb–Cu–B–Si system alloys occupy the leading position due to their high initial magnetic permeability and low remagnetization loss . Volume fraction of α-Fe(Si) nanocrystals in them is 75–80 %; their size is about 10–12 nm [3–6]. Excellent soft magnetic properties of these alloys are explained by strong magnetic exchange interaction between α-Fe(Si) nanocrystals through remaining amorphous matrix .
Cut cores made of nanocrystalline Fe–Nb–Cu–B–Si alloy with linear loop are widely used in power electronics for the manufacture of linear and storage chokes as well as power reactors because these cores have lower remagnetization loss compared to crystalline ferrite cores and cut cores made of iron-based amorphous alloy . It is known that the increase in nonmagnetic gap length of cut cores made of Fe–Nb–Cu–B–Si alloy leads to effective magnetic permeability decrease and, unfortunately, to core loss increase . Another disadvantage of cut cores is fringing effect (effective area of generated magnetic lines flux in nonmagnetic gap is noticeably larger than core cross section area) which in electric circuit can negatively influence neighboring elements of electronic board.
It is known that for uncut cores made of Fe–Nb–Cu–B–Si alloy, high remagnetization loop linearity can be obtained by inducing uniaxial transverse magnetic anisotropy in them using magnetic field annealing [8, 9] and/or annealing under tensile stress [10–12]. Ribbon annealed under tensile stress has higher induced transverse magnetic anisotropy than the one annealed in transverse magnetic field . The main contribution to the induced magnetic anisotropy originates from the residual deformation of lattice of nanosized crystals of α-Fe(Si) solid solution ordered by DO3 type  and the magnetoelastic anisotropy of Fe-enriched grains due to tensile back stresses exerted by inelastically deformed amorphous matrix . It is known that such ribbon can be annealed under very high tensile stress up to 800 MPa .
Cores (made of Fe–Nb–Cu–B–Si alloy with tension-induced transverse magnetic anisotropy) have a number of advantages compared to cores made of other alloys, which are characterized by the same magnetic permeability. The main advantages are the following: high-frequency stability of magnetic permeability [12, 15–18] and low core loss in frequency range of widest use (1–100 kHz) [12, 15–19]. These cores are characterized by significantly higher remagnetization loop linearity compared to cut cores made of the same alloy and consequently by magnetic permeability independence on field strength .
DC bias on transformer primary winding presents in the most simple and widespread single-step converters; therefore, magnetic properties of cores used in them should be immune to such influence. It is known from literature that new cores have high immunity of magnetic permeability and core loss to DC bias field [16, 17]; however, the influence of induced magnetic anisotropy on DC bias immunity remains insufficiently investigated.
The aim of this work is to compare the main magnetic characteristics of cut cores made of nanocrystalline Fe73Nb3Cu1B7Si16 alloy ribbon with new cores made of the same ribbon subjected to electric current heating under tensile stress (up to 180 MPa) and to determine the main advantages of new uncut cores with induced transverse magnetic anisotropy.
Obtaining of amorphous ribbon and manufacture of nanocrystalline magnetic cores
The initial alloy was prepared in an experimental facility for induction melting in pure argon atmosphere. The alloy components (iron recovered in hydrogen (99.96 mass %), single-crystal silicon (99.999 mass %), niobium (≥99.7 mass %), Fe2B master alloy preliminary melted using amorphous boron (99.8 mass %), and electrical copper (99.9 mass %) were melted in a ceramic crucible and held 6–7 min at temperature 1500 °С; then, the melt was cast into a graphite mold. Thus, the ingot weighed about 1 kg was obtained, which was portioned for the following manufacture of amorphous ribbon in a facility for rapid quenching of the melt (RQM).
The amorphous ribbon was obtained in the available RQM open-type facility. Melting of the initial alloy was performed in a ceramic ampoule in a heat-resistant holder of precise motion system. After overheating of melt 150 °С above liquidus temperature Т L, it was ejected by an excess argon pressure of 20 kPa through a narrow nozzle of 0.4 × 10 mm from the distance of 0.2 mm maintained constant during the whole casting cycle.
The special designed chromium copper quenching disc of diameter about 580 mm was used in the facility. The linear rotary disc speed was 25 m/s. Formed ribbon was separated from the disc surface by special pneumatic “knife-remover” after 1/4 disc revolution, i.e., after 500 mm.
Core size with ferrite plates was the same as cut cores—30 × 42 mm, segments were equal to ferrite plates size—16 mm, and nonmagnetic gap length 4 mm were cut from the core (Fig. 1).
Amorphous ribbon crystallized under fast heating at simultaneous application of tensile stresses from 0 to 180 MPa along ribbon axis . Fast heating was realized by conducting of electric current with density j h = 42 A/mm2 and frequency 50 Hz through straight piece of the ribbon for t h = 3.7 s that ensured its heating above 600 °С. We determined  that these heating modes (j h = 42 А/mm2, t h = 3.7 s) of amorphous ribbon allow to reach the maximum improvement of magnetic characteristics of cores made of the heated ribbon: initial magnetic permeability increase and core loss decrease. The reason of improving the magnetic characteristics is the formation (the time 3.7 s) of optimal volume fraction of α-Fe(Si) nanocrystals with minimal size in the amorphous matrix phase. Increasing time of heating by electric current leads to noticeable increase in the ribbon brittleness and deterioration of magnetic properties which is likely due to the formation of larger nanocrystals and possible negative influence of surface oxidation.
After heating, the ribbon was wound to form cores with inner/outer diameter ratio—30/42. Relatively large core diameter was selected to decrease the tension that appears in the ribbon after winding. It is known [16, 17] that core loss increases considerably when the inner diameter of the core is less than critical diameter (D in ≤ D c).
Initial magnetic permeability μ i1 of magnetic cores (at remagnetization frequency f = 1 kHz) was calculated by values of inductance of a few-turn coil in AC field 0.2 А/m measured by LCR Measurement Bridge HM8118 (HAMEG Instruments, Mainhausen, Germany).
Сore loss at different frequencies was measured using the measuring complex MS-02 B-H ANALYZER (MSTATOR, Novgorodskaya oblast, Russia) whose detailed description is presented in ref. .
- 3.Reversible magnetic permeability μ rev1 immunity to DC bias in magnetic field 2 A/m was measured using the measuring complex MS-02 Universal LZQ Meter (MSTATOR, Novgorodskaya oblast, Russia), whose functional scheme is presented in Fig. 2. AC current of frequency 1 kHz proportional to voltage on the instrument shunt of 1 Ohm is applied to the magnetizing coil from the broadband power amplifier. Regulated DC current is supplied to secondary winding of studied magnetic core. Measuring device has two precise differential amplifiers no.1 and no.2 which, correspondingly, amplify voltage signal from measuring-magnetizing coil and voltage signal from the instrument shunt connected to magnetization circuit. Signals from different amplifiers are registered at inputs B and A, respectively, of virtual digital two-channel storage oscilloscope ASK-3105 integrated in PC system unit.
where l с is the core midline length, A c is the effective cross section area of magnetic core, N is the number of winding turns, and μ 0 is the magnetic constant.
It is also possible to decrease magnetic permeability μ i1 of the core made of the same alloy without cuts by the increase of tensile stresses applied to the ribbon during heating (Fig. 3b)  that is explained by inducing uniaxial transverse magnetic anisotropy in the ribbon .
One of the disadvantages of obtaining new cores by this method is the impossibility of decreasing magnetic permeability below 300 because brittle nanocrystalline ribbon breaks at the increase of tensile stresses.
It can be seen in Fig. 7b that magnetic permeability is constant at DC bias 1 kA/m in cores with four and eight gaps. So the conclusion can be drawn that it is not reasonable to increase the gap number over four.
Taking into account that DC bias does not exceed 1 kA/m under commonly used conditions of core exploitation, we can state that new core (made of the ribbon crystallized under application of tensile stress 180 MPa) have significant advantage by loss level over cut cores made of the same Fe73Nb3Cu1B7Si16 alloy.
Reversible magnetic permeability can be controllably decreased for cut cores and nanocrystalline cores by the increase of nonmagnetic gap length and/or tensile stress during heating (nanocrystallization) of as-cast amorphous ribbon before manufacture (winding) of new toroidal cores. Permeability decrease is accompanied by core loss increase for cut core and core loss decrease for new nanocrystalline core.
Distribution of 4 mm total gap over the core leads to higher DC bias immunity of magnetic permeability.
Increase of tensile stress (from 80 to 180 MPa) applied to the ribbon during its heating leads to linear increase of DC bias immunity of reversible magnetic permeability of new nanocrystalline cores.
New nanocrystalline cores (made of the ribbon heated under tensile stress up to 180 MPa) and cut cores (with four cuts 1 mm each) made of the same Fe73Nb3Cu1B7Si16 alloy have constant magnetic permeability up to 1 kA/m DC bias field. Wherein, new cores are characterized by very low loss: two to four times less than cut core loss.
The obtained characteristics are advantageous for application of new magnetic cores made of Fe73Nb3Cu1B7Si16 alloy in power reactors and line chokes of filters of switch mode power supplies.
The authors are very much obliged to MELTA Ltd. scientific production company for the provided quenching facility  and devices for measurement of magnetic properties.
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- Herzer G (2013) Modern soft magnets: amorphous and nanocrystalline materials. Acta Mater 61:718–734View ArticleGoogle Scholar
- Hasegawa R (2001) Applications of amorphous magnetic alloys in electronic devices. J of Non-Crystalline Solids 287:405–412View ArticleGoogle Scholar
- Yoshizawa Y, Oguma S, Yamauchi K (1988) New Fe-based soft magnetic alloys composed of ultrafine grain structure. J Appl Phys 64:6044–6046View ArticleGoogle Scholar
- Nemoshkalenko V, Vlasnko L, Romanova A, Brovko A, Maslov V, Nosenko V, Petrov Y (1998) Nanocrystal structure at the stages prior to crystallization of amorphous Fe73.5Si13.5B9Cu1Nb3. Metallofizika i Noveishie Tekhnologii 20:22–34Google Scholar
- Maslov V, Nosenko V, Tapanenko L, Brovko A (2001) Nanocrystallization in alloys of Finemet type. Phys Metals Metal Sci 91:47–55Google Scholar
- Herzer G (1989) Grain structure and magnetism of nanocrystalline ferromagnets. IEEE Trans Magn 25:3327–3329View ArticleGoogle Scholar
- Fukunaga H, Eguchi T, Koga K, Ohta Y, Kakehashi H (1990) High performance cut cores prepared from crystallized Fe-based amorphous ribbon. IEEE Trans Magn 26:2008–2010View ArticleGoogle Scholar
- Herzer G (2005) Anisotropies in soft magnetic nanocrystalline alloys. J Magn Magn Mater 294:99–106View ArticleGoogle Scholar
- Flohrer S, Schafer R, McCord J, Roth S, Schultz L, Fiorillo F, Gunther W, Herzer G (2006) Dynamic magnetization process of nanocrystalline tape wound cores with transverse field-induced anisotropy. Acta Mater 54:4693–4698View ArticleGoogle Scholar
- Kraus L, Záveta K, Heczko O, Duhaj P, Vlasák G, Schneider J (1992) Magnetic anisotropy in as-quenched and stress-annealed amorphous and nanocrystalline Fe73.5Cu1Nb3Si13.5B9 alloys. J Magn Magn Mater 112:275–277View ArticleGoogle Scholar
- Herzer G (1994) Creep induced magnetic anisotropy in nanocrystalline Fe-Cu-Nb-Si-B alloys. IEEE Trans Magn 30:4800–4802View ArticleGoogle Scholar
- Fukunaga H, Furukawa N, Tanaka H, Nakano M (2000) Nanostructured soft magnetic material with low loss and low permeability. J Appl Phys 87:7103–7105View ArticleGoogle Scholar
- Herzer G, Budinsky V, Polak C (2011) Magnetic properties of nanocrystalline FeCuNbSiB with huge creep induced anisotropy. J Phys Conf Ser 266:012010View ArticleGoogle Scholar
- Ohnuma M, Yanai T, Hono K, Nakano M, Fukunaga H, Yoshizawa Y, Herzer G (2010) Stress-induced magnetic and structural anisotropy of nanocrystalline Fe-based alloys. J Appl Phys 108:093927View ArticleGoogle Scholar
- Yanai T, Takagi K, Takahashi K, Nakano M, Yoshizawa Y, Fukunaga H (2008) Fabrication of Fe-based ribbon with controlled permeability by Joule heating under tensile stress. J Magn Magn Mater 320:e833–e836View ArticleGoogle Scholar
- Fukunaga H, Yanai T, Tanaka H, Nakano M, Takahashi K, Yoshizawa Y, Ishiyama K, Arai K (2002) Nanostructured metallic cores with extremely low loss and controlled permeability. IEEE Trans Magn 38:3138–3140View ArticleGoogle Scholar
- Fukunaga H, Tanaka H, Yanai T, Nakano M, Takahashi K, Yoshizawa Y (2002) High performance nanostructured cores for chock coils prepared by using creep-induced anisotropy. J Magn Magn Mater 242–245:279–281View ArticleGoogle Scholar
- Nosenko A, Mika T, Rudenko O, Yarmoshchuk Y, Nosenko V (2015) Soft magnetic properties of nanocrystalline Fe73B7Si16Nb3Cu1 alloy after rapid heating under tensile stress. Nanoscale Res Lett 10:136View ArticleGoogle Scholar
- Alves F (2001) Flash stress annealings in nanocrystalline alloys for new inductive components. J Magn Magn Mater 226–230:1490–1492View ArticleGoogle Scholar
- Equipment for rapid melt quenching: http://melta.com.ua/?page_id=34.