磁化水的检测及评价

近几年来 ,随着磁化用品越来越多的出现 ,对磁化理论的研究越来越深入。实践证明 ,磁化水对植物的生长、对人体高血压、糖尿病、血稠、肾结石等都有一定的刺激和疗效。要真正揭示磁疗机理 ,必须首先研究水经过磁化器后产生的变化。本文通过水经过磁化器后的物理试验数据 ,对磁化机理进行了初步探索。1　水的密度试验(1)自来水与磁化水密度差试验　水经过磁化器后产生物理变化而不是化学变化 ,磁场改变了水分子的氢键角 ,所以首先进行密度测量 ,见表 1。表 1　不同时间自来水和磁化水的密度差 (2 5℃ )时间 (ｔ/ｈ) 密度差 (ρ/ ｇ·ｃｍ-3 )…     

磁化作用对汽油动态挥发性影响的研究

用热重（TG）分析和自行设计的原位动态挥发实验，研究了在不同条件下汽油的挥发性，结果表明，磁化空气或磁化汽油都可提高汽油的挥发性，而汽油和空气共同磁化，可更大幅度地提高汽油的挥发性。     

宁镇山脉古生代与三叠纪沉积岩的重磁化研究

本文通过岩石磁学结合有效的古地磁检验方法,对宁镇山脉古生代与三叠纪岩石进行了专门的岩石重磁化研究,发现了该区岩石多期重磁化的证据,并将重磁化分为:(1)古生代重磁化;(2)印支期重磁化;(3)燕山期重磁化;探讨了各期重磁化与相关时代构造运动的相互关系。     

Nd—Fe—B烧结磁体的磁化行为

研究了热退磁态和磁场退磁态Nd-Fe-B和Nd-Dy-Fe-B烧结磁体室温至150℃不同磁化场的磁化曲线、退磁曲线和磁滞回线。室温下磁场退磁态磁化曲线和内禀矫顽力_MH_C随磁化场H_M的变化曲线在磁化场接近样品最大内禀矫顽力绝对值时出现台阶,当温度升至100～150℃或样品在居里温发以上热退磁后,磁化曲线的形状由阶梯型变成陡峭型,而且_MH_C—H_M曲线的台阶移到低磁化场。膝点矫顽力H_K随H_M的快速升高出现在_MH_C随H_M的快速升高之后。表明Nd-Fe-B烧结磁体的磁硬化主要被畴壁钉扎所控制。     

Tm2Fe14B中的晶场作用和交换作用

本文基于单离子模型,定量地解释了Tm_2Fe_(14)B的自发磁化随温度的变化,自旋重取向转变,以及不同温度下(T=4.2、100、150和200K)沿(100)、(110)和(001)轴的磁化曲线。详细分析了不同温度下Fe和Tm次晶格磁矩的磁化过程。磁化过程中Fe磁矩和Tm磁矩之间存在明显的非共线性。     

Fe3O4-PEI磁化破乳剂的制备及性能研究

针对乳化原油破乳难度较大的问题,提出了在磁化破乳剂上枝接聚乙烯亚胺（PEI）,增加磁性粒子表面官能团的解决方案,并对其结构进行了表征。研究了破乳剂加量、沉降时间和pH对其破乳效果的影响,磁性粒子的循环利用率,并对其破乳机理进行了探讨。结果表明：磁化破乳剂最优加量为600 mg/L;沉降2 h后,乳化原油透光率仍可达到98.3%;磁化破乳剂Fe₃O₄-PEI在酸性环境中的破乳效果优于碱性环境;磁性粒子重复利用10次后,透光率仍超过90%。      

工业应用中钕铁硼磁体不可逆磁通损失的影响因素研究

由于Nd-Fe-B磁体热稳定性较差,在服役过程中会产生不可逆磁通损失,限制了磁体的应用范围。通过探究钕铁硼磁体不可逆磁通损失与矫顽力、导磁系数(Pc值)、服役温度、服役时间之间的关系,并阐述了磁体不可逆磁通损失的产生机制。研究发现磁体随服役温度和服役时间的增加不可逆磁通损失大幅度增加,热稳定性变差,提高磁体矫顽力和Pc值可以降低磁体的不可逆磁通损失。不可逆磁通损失的产生主要是磁体磁矩发生偏转,与原磁化方向不同,反向畴增多,形成了反磁化场,造成磁体磁性能下降。     

磁场对氢氧化铁胶体ζ电位的影响

本文研究了磁场对氢氧化铁胶体ζ电位的影响。实验表明在磁场作用下,胶体的ζ电位、电导率和聚沉值都发生变化,其值与磁场强度、磁化时间及胶体浓度有关。同时用电镜观察了磁作用前后的胶体颗粒,并对实验结果进行了讨论。     

R_(15)Fe_(78)B_7的磁晶各向异性

用磁测量和X-射线衍射方法研究了R_(15)Fe_(78)B_7(R=Pr,Nd,Sm,Gd,Y)的磁晶各向异性。发现R=Pr,Gd和Y时,无论室温或低温,c轴都是易磁化方向;R=Sm时,易磁化方向都是在与c轴垂直的基面内;而R=Nd时,易磁化方向随温度变化。在室温时,c轴是易磁化方向,但当温度低于140K时,易磁化方向相对c轴形成一个θ角度。利用Sucksmith-Thompson方法估算了R_(15)Fe_(78)B_7的磁晶各向异性常数K_1和K_2的数值和符号;测量了θ与温度的依赖关系。并通过测定Nd_(15)Fe_(78)B_7和Y_(15)Fe_(78)B_7的磁晶各向异性及其随温度的变化,进一步分析了Nd_(15)Fe_(78)B_7中Nd和Fe不同次点阵对磁晶各向异性的贡献。     

气基磁化焙烧回收包头稀土尾矿中铁的研究

试验采用磁化焙烧-磁选的方法来回收包头稀土尾矿中的Fe。考察了还原球团的粒径、焙烧温度、还原气体的成分、还原气气体流量、焙烧时间对于磁化焙烧回收Fe的影响。在焙烧温度为580℃,CO与CO2的浓度比为40∶60,还原气体气流量为1.2 L·min-1,焙烧时间为60 min的条件下对球团进行磁化焙烧,并将焙烧后的球团进行磨矿,使得-200目的物料占物料总重量的95%。将磨矿后的物料置于磁场强度为233 k A·m-1的磁选管中进行磁选,可以得到品位为60%左右的铁精矿,其铁回收率达到70%左右。     

Magnetization Switching in the GdFeCo Films with In-Plane Anisotropy via Femtosecond Laser Pulses

Ferrimagnetic rare-earth substituted metal alloys GdFeCo were shown to exhibit the phenomenon of all-optical magnetization switching via femtosecond laser pulses. All-optical magnetization switching has been comprehensively investigated in out-of-plane magnetized GdFeCo films; however, the films with the in-plane magnetic anisotropy have not yet been studied in detail. We report experimental observations of the magnetization switching of in-plane magnetized GdFeCo films by means of the femtosecond laser pulses in the presence of a small magnetic field of about 40 µT. The switching effect has a threshold both in the applied magnetic field and in the light intensity.     

Magnetization of Bi0:9-xGdxLa0:1FeO3 System

Magnetization of Bi0:9-xGdxLa0:1FeO3 (x=0.3, 0.5, 0.6 and 0.7) is reported. An abnormal negative magnetization appears in the temperature-dependent magnetization curves, and the temperature-dependent coercive field shows a maximum in the vicinity of the compensation temperature where the total magnetization is zero. These results suggest that in the ferrimagnetic-like Bi0:9-xGdxLa0:1FeO3 system the Gd and Fe magnetic sublattices are coupled antiferromagnetically.     

Sm0.88Dy0.12Fe2合金的易磁化方向研究

运用穆斯堡尔效应，对Ｓｍ０．８８Ｄｙ０．１２Ｆｅ２合金的易磁化方向的变化进行了研究。结果表明；随着温度的升高，其易磁化方向从「１１０」渐变地转向「１１１」，在１５３至２１３Ｋ温度范围内，「１１０」和「１１１」两者共存，而并非由「１１０」其一温度突变至「１１１」。     

含砷金矿的磁场强化生物预氧化

生物氧化;浸金工艺;含砷金矿的磁场强化生物预氧化     

Six‐Coordinate Lanthanide Complexes: Slow Relaxation of Magnetization in the Dysprosium(III) Complex

A series of six‐coordinate lanthanide complexes {(H₃O)[Ln(NA)₂]?H₂O}_n (H₂NA=5‐hydroxynicotinic acid; Ln=Gd^III ( 1?Gd ); Tb^III ( 2?Tb ); Dy^III ( 3?Dy ); Ho^III ( 4?Ho )) have been synthesized from aqueous solution and fully characterized. Slow relaxation of the magnetization was observed in 3?Dy . To suppress the quantum tunneling of the magnetization, 3?Dy diluted by diamagnetic Y^III ions was also synthesized and magnetically studied. Interesting butterfly‐like hysteresis loops and an enhanced energy barrier for the slow relaxation of magnetization were observed in diluted 3?Dy . The energy barrier (Δ_τ) and pre‐exponential factor (τ₀) of the diluted 3?Dy are 75 K and 4.21×10^?5 s, respectively. This work illustrates a successful way to obtain low‐coordination‐number lanthanide complexes by a framework approach to show single‐ion‐magnet‐like behavior.     

磁场作用下乳化重油稳定性的实验研究

燃油磁化燃烧技术是一种新的燃烧技术 ,目前以日本发展较快[1,2 ] ,其节能效果也已为实践所证实[3～ 5] 。我们知道 ,掺水乳化重油稳定性好 ,燃烧状况就稳定 ;稳定性差 ,油水在进入炉膛燃烧前就已分层 ,不但起不到“微爆”效果 ,而且严重时导致熄火。作者曾对未磁化乳化重油的粘度、稳定性和分散度进行了实验研究[6～ 8] ,丘纪华等学者[9～ 11] 对磁化技术在石油、化工、燃料等方面的作用机理及应用进行了一定的研究 ,但是重油掺水乳化后再经磁化处理后其稳定性发生怎样的变化 ,尚未见实验报道。因此 ,为了更好地发挥这一技术的节油和环保效…     

Room‐Temperature,Strain‐Tunable Orientation of Magnetization in a Hybrid Ferromagnetic Co Nanorod–Liquid Crystalline Elastomer Nanocomposite

Hybrid nanocomposites based on magnetic nanoparticles dispersed in liquid crystalline elastomers are fascinating emerging materials. Their expected strong magneto‐elastic coupling may open new applications as actuators, magnetic switches, and for reversible storage of magnetic information. We report here the synthesis of a novel hybrid ferromagnetic liquid crystalline elastomer. In this material, highly anisotropic Co nanorods are aligned through a cross‐linking process performed in the presence of an external magnetic field. We obtain a highly anisotropic magnetic material which exhibits remarkable magneto‐elastic coupling. The nanorod alignment can be switched at will at room temperature by weak mechanical stress, leading to a change of more than 50 % of the remnant magnetization ratio and of the coercive field.     

Magnetization dynamics in arrays of strongly interacting magnetic nanocrystals

Arrays of 6.6 nm iron oxide nanocrystals coated with fatty acid molecules were produced using the Langmuir-Blodgett technique. The arrays had a varying number of layers stacked together, going from two dimensional to three dimensional and two different in-plane interparticle separations. While temperature-dependent ac susceptibility measurements of the isolated nanocrystals obeyed the Neel-Brown relaxation law, the array relaxation deviated significantly from this simple law. This deviation together with the observed dc field influence on the susceptibility-temperature curves, the large shifts in blocking temperatures and reduction in susceptibility-temperature curve widths on going from isolated particles to the arrays indicated collective magnetization dynamics during magnetization freezing. A scaling law analysis of this freezing dynamics yielded different powers for the two different interparticle separations with no dependence on dimensionality. In spite of the spin-glass-like behavior, it is possible that small, magnetically ordered domains of nanocrystals form at low temperature.     

A pH‐Responsive MRI Agent that Can Be Activated Beyond the Tissue Magnetization Transfer Window

A terbium‐based complex that displays a water exchange CEST resonance well outside the normal magnetization transfer (MT) frequency range of tissues provides a direct readout of pH values by MRI. Deprotonation of the phenolic proton in this complex results in a frequency shift of 56 ppm in a bound water molecule exchange peak between pH 5 and 8. This allows direct imaging of pH without prior knowledge of the agent concentration and with essentially no interference from the tissue MT signal.     

磁化后掺水乳化重油分散度的实验研究

乳化重油的分散相（水）微粒大小对重油掺水乳化燃烧技术的应用效果有很大影响,本人在过去实验的基础上,用光学反射显微镜法对磁场作用下掺水乳化重油中分散相（水）的分散度进行了测定,研究了乳化重油的分散度与磁场强度、温度以及流速之间的关系,实验结果表明：磁化后有利于乳化重油的微细化,且效果比较显著;温度的升高有利于分散相（水）的微细化,兼顾能耗和燃油的发泡、沸腾现象,以及磁化后温度的升高对分散度的影响减少,有一个合理的温度范围;磁化后分散度与流速的关系呈峰值关系,本实验中流速较佳值为8m/s;磁场强度的增大也有利于微细化,磁场强度太高或太低均不会取得太好的处理效果,在1000GS－1400GS范围内为宜。