磁场诱导的形状恢复通过反向相位转换
1Department of Materials Science, Graduate School of Engineering, Tohoku University, 6-6-02 Aoba-yama, Sendai 980-8579, Japan. kainuma@material.tohoku.ac.jp
Nature
|February 24, 2006
概括
这项研究报告了一种NiCoMnIn合金表现出显著的磁场诱导形状恢复,产生超过100MPa的应力. 这种豪斯勒合金显示了先进磁执行器应用的潜力.
科学领域:
- 材料科学 材料科学 材料科学
- 凝聚物质物理学 凝聚物质物理学
- 磁力学 磁力学 是一种
背景情况:
- 具有身体中心立方结构的豪斯勒合金表现出巨大的磁场诱导的应变.
- 这些变化归因于马氏体结构变体在外部磁场下的重新排列.
- 这些材料是磁性执行器应用的有希望的候选材料.
研究的目的:
- 为了研究压力变形的NiCoMnIn合金中磁场诱导的形状恢复.
- 量化该合金的应力产生和变形恢复能力.
- 阐明对观察到的行为负责的潜在转换机制.
主要方法:
- 对一个Ni45Co5Mn36.7In13.3单晶体进行实验调查.
- 在预先变形的样本中应用70kOe磁场以诱导形状恢复.
- 测量产生的应力和观察到的变形恢复百分比.
主要成果:
- 在应用70kOe磁场时,NiCoMnIn合金产生了超过100MPa的应力.
- 观察到3%的变形,几乎完全恢复了原始形状.
- 产生的应力水平大约是以前铁磁形状记忆合金报告的50倍.
结论:
- 观察到的磁场诱导的形状恢复和高应力生成归因于反向转变.
- 这种转换发生在反铁磁 (或偏磁) 马氏体阶段到铁磁母阶段的298 K.
- 尼科MnIn合金显示出作为高性能磁性执行器材料的特殊潜力.
相关概念视频
¹³C NMR: Distortionless Enhancement by Polarization Transfer (DEPT)
1.3K
When proton-coupled carbon-13 spectra are simplified by a broadband proton decoupling technique, structural information about the coupled protons is lost. Distortionless enhancement by polarization transfer (DEPT) is a technique that provides information on the number of hydrogens attached to each carbon in a molecule. While the DEPT experiment utilizes complex pulse sequences, the pulse delay and flip angle are specifically manipulated. The resulting signals have different phases depending on...
1.3K
Atomic Nuclei: Magnetic Resonance
1.3K
The number of nuclear spins aligned in the lower energy state is slightly greater than those in the higher energy state. In the presence of an external magnetic field, as the spins precess at the Larmor frequency, the excess population results in a net magnetization oriented along the z axis. When a pulse or a short burst of radio waves at the Larmor frequency is applied along the x axis, the coupling of frequencies causes resonance and flips the nuclear spins of the excess population from the...
1.3K
Atomic Nuclei: Nuclear Relaxation Processes
1.1K
In the absence of an external magnetic field, nuclear spin states are degenerate and randomly oriented. When a magnetic field is applied, the spins begin to precess and orient themselves along (lower energy) or against (higher energy) the direction of the field. At equilibrium, a slight excess population of spins exists in the lower energy state. Because the direction of the magnetic field is fixed as the z-axis, the precessing magnetic moments are randomly oriented around the z-axis.
1.1K
NMR Spectrometers: Resolution and Error Correction
999
When magnetic nuclei in a sample achieve resonance and undergo relaxation, the signal detected in NMR is an approximately exponential free induction decay. Fourier transform of an exponential decay yields a Lorentzian peak in the frequency domain. Lorentzian peaks in an NMR spectrum are defined by their amplitude, full width at half maximum, and position, where the peak width is governed by the spin-spin relaxation time alone. In real experiments, however, the applied magnetic field is rendered...
999
Magnetic Fields
6.0K
A moving charge or a current creates a magnetic field in the surrounding space, in addition to its electric field. The magnetic field exerts a force on any other moving charge or current that is present in the field. Like an electric field, the magnetic field is also a vector field. At any position, the direction of the magnetic field is defined as the direction in which the north pole of a compass needle points.
A magnetic field is defined by the force that a charged particle experiences...
A magnetic field is defined by the force that a charged particle experiences...
6.0K
Magnetic Field due to Moving Charges
11.4K
A stationary charge creates and interacts with the electric field, while a moving charge creates a magnetic field.
Consider a point charge moving with a constant velocity. Like the electric field, the magnetic field at any point is directly proportional to the magnitude of the charge and inversely proportional to the square of the distance between the source point and the field point. However, unlike the electric field, the magnetic field is always perpendicular to the plane containing the line...
Consider a point charge moving with a constant velocity. Like the electric field, the magnetic field at any point is directly proportional to the magnitude of the charge and inversely proportional to the square of the distance between the source point and the field point. However, unlike the electric field, the magnetic field is always perpendicular to the plane containing the line...
11.4K


