2010
DOI: 10.1088/0022-3727/43/19/195003
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Magnetic anisotropy of plastically deformed low-carbon steel

Abstract: Abstract. Macroscopic hysteresis and local Barkhausen noise techniques were used for the comprehensive magnetic investigation of structural low-carbon steel subjected to uniaxial plastic tension. Scattering of the measured magnetic parameters was substantial within the Lüders band region with stabilization at higher strains. Compressive residual stresses in the deformation direction formed a hard magnetization axis with intriguing two-phase remagnetization. The magnetic parameters had highest sensitivity to st… Show more

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Cited by 34 publications
(19 citation statements)
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References 28 publications
(107 reference statements)
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“…The dramatic drop of the remanent polarization value, already occurring with deformation values as low as ε p = 0.5%, is driven by the compressive residual stress, easily engendering, in the demagnetized state, the transition of the magnetization inside the domains towards the easy axes far-off the stress (i.e., field) direction. It is remarked in Figure 5b, in agreement with previous findings of the literature [24,25], that all the plastically strained loops tend to cross at the same point in the second and fourth quadrants. It has been suggested that the additional field H 1 required to achieve the same polarization value attained in the unstrained material can be expressed as the product H 1 (σ, J) = h(σ) g(J) [24].…”
Section: Introductionsupporting
confidence: 92%
See 2 more Smart Citations
“…The dramatic drop of the remanent polarization value, already occurring with deformation values as low as ε p = 0.5%, is driven by the compressive residual stress, easily engendering, in the demagnetized state, the transition of the magnetization inside the domains towards the easy axes far-off the stress (i.e., field) direction. It is remarked in Figure 5b, in agreement with previous findings of the literature [24,25], that all the plastically strained loops tend to cross at the same point in the second and fourth quadrants. It has been suggested that the additional field H 1 required to achieve the same polarization value attained in the unstrained material can be expressed as the product H 1 (σ, J) = h(σ) g(J) [24].…”
Section: Introductionsupporting
confidence: 92%
“…If we then recognize a proportional relationship between ∆H c (ε p ) and an equivalent internal demagnetizing factor N d~1 /µ a , we arrive at justifying Equation (1). Figure 5b, in agreement with previous findings of the literature [24,25], that all the plastically strained loops tend to cross at the same point in the second and fourth quadrants. It has been suggested that the additional field H1 required to achieve the same polarization value attained in the unstrained material can be expressed as the product H1(σ, J) = h(σ) g(J) [24].…”
Section: Introductionsupporting
confidence: 88%
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“…4a the local coercivity (h c ) can be found from the BN loops for each carbon steel sample. Local coercivity (h c ), also known as BN coercivity [28], has been shown to have strong correlations with bulk coercive force [28,29], energy loss [29], residual stress [30] and decarburization depth [27]. However, the correlation between h c and carbon content has not been investigated previously.…”
Section: Bn Loops and Local Coercivitymentioning
confidence: 99%
“…These approaches can also be used in nondestructive tests; However, the test areas of the samples under study should have larger dimensions. For the techniques based on the Barkhausen noise signal that have been applied for the same purpose, sample sizes from 50.4 to 100 cm 2 have been used [17,21,23,[26][27][28][29]33]. …”
Section: Introductionmentioning
confidence: 99%