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1.
利用吸铸的方法制备了Nd60Fe20Al8Co10B2大块非晶合金。采用示差扫描量热法(DSC),X射线衍射(XRD),扫描电子显微镜(SEM)和振动样品磁强计(VSM)研究了Nd60Fe20Al8Co10B2大块非晶合金在晶化过程中的微观结构及磁性能的变化情况。Nd60Fe20Al8Co10B2大块非晶合金在低于723K退火时,富Nd相和富Fe相的析出对于合金的矫顽力影响不大。但是,富Fe相的长大使合金的饱和磁化强度和剩磁下降明显。合金完全晶化后,硬磁性迅速消失。  相似文献   

2.
利用示差扫描量热法,X射线衍射法和振动样品磁强计研究了少量B元素对Nd60Fe20All0Col0大块非晶合金的磁性和晶化行为的影响。研究表明,用B元素部分取代Nd元素后,其内禀矫顽力有所增大,饱和磁化强度降低。晶化后,Nd60Fe20All0Col0大块非晶合金退火折出的晶体相对硬磁性能无明显影响,而Nd58Fe20All0Col0B2合金退火析出非铁磁性的Nd1.lFe4B4相,使内禀矫顽力、饱和磁化强度、居里温度降低。  相似文献   

3.
采用差示扫描量热法(DSC)、X射线衍射(XRD)和透射电镜(TEM)研究了Y对Nd-Fe-Al-Ni非晶合金热稳定性和晶化行为的影响。结果表明,淬火态的Nd60Fe20Al10Ni10-xYx(x=0,2)合金基本为非晶组织同时还含有少量的淬态相,Y的加入抑制了淬态相的析出。加入Y后,非晶合金的晶化开始温度和晶化峰值温度都向高温方向移动,证明其热稳定性提高。Y的加入改变了合金的晶化方式和最终晶化产物,使非晶基体中析出的晶化相更加弥散圆整细小。并且Y具有在化学上钝化氧杂质的作用,从而抑制了氧的有害作用。利用Kissinger方程获得了Nd60Fe20Al10Ni8Y2非晶合金的晶化开始和晶化峰值激活能分别为1.21和1.16 eV。  相似文献   

4.
采用铜模吸铸制备了厚度为0.8 mm,成分为Nd9Fe81-x-yTi4C2BxNby(x=11,13,15;y=0,4)的Nd2Fe14B/Fe3B型纳米复合永磁合金块体样品,研究了添加Nb对合金铸态组织及其晶化行为的影响,并测试了其磁性能。结果表明:在合金中添加4%(原子分数)Nb元素,不仅能抑制吸铸样品表面Nd2Fe23B3软磁性相、Nd1.1Fe4B4非磁性相和未知相的形成,导致Nd2Fe14B,Fe3B和α-Fe相的相对量增加,而且促使样品内部在非晶基体上形成了少量的Nd2Fe14B和α-Fe,Fe3B纳米晶。添加了Nb的合金吸铸样品表现出一定的硬磁性,其中Nd9Fe66Ti4C2B15Nb4吸铸样品具有最高的矫顽力(Hci=116.66 k A·m-1);添加4%(原子分数)Nb使得合金在晶化过程中由原来的异相同温一步晶化转变为两步晶化,且初始晶化温度Tx均明显降低,两个放热峰的ΔTpx均增大。  相似文献   

5.
采用单辊快淬法制备了Nd12.3-xDyxFe79.7Zr0.8Nb0.8Cu0.4B6.0(x=0,0.5,1.5,2.5)合金纳米晶单相永磁薄带,研究了合金薄带晶化处理后,成分、组织结构与磁性能之间的关系.X射线衍射分析(XRD)表明,淬态合金主要由非晶相和Nd2Fe14B相组成,完全晶化后由Nd2Fe14B相和少量α-Fe组成.高分辨透射电镜(HRTEM)分析表明,经充分退火后,Nd2Fe14B晶体完整,晶粒间几乎没有边界相.随着Dy含量增加,晶粒尺寸细化,矫顽力大幅提高.x=0.5合金综合磁性能最佳,经过700℃晶化处理10min后,其磁性能为Jr=1.09 T,Hci=1048kA·m-1,(BH)max=169.5 kJ·m-3.  相似文献   

6.
铌和锆对(Nd,Pr)2Fe14B/α-Fe快淬合金晶化和磁性能的影响   总被引:1,自引:0,他引:1  
研究了Nb和Zr添加对快淬纳米双相(Nd,Pr)2Fe14B/α-Fe合金晶化行为和磁性能的影响. 结果表明 (Nd0.4Pr0.6)8.5Fe85.5B6合金非晶晶化时, 在α-Fe相初始晶化后, 出现了(Nd,Pr)3Fe62B14亚稳相, 最终亚稳相分解形成(Nd,Pr)2Fe14B和α-Fe两相组织; (Nd0.4Pr0.6)8.5Fe84.5Nb0.5Zr0.5B6非晶晶化时, 同时析出α-Fe相和(Nd,Pr)2Fe14B相. 这说明添加Nb和Zr可避免亚稳相的形成并细化晶粒, 最大磁能积(BH)max从复合添加前的107.5上升到143.6 kJ·m-3. 而且, Nb和Zr原子在非晶晶化过程中可以部分取代Nd和Pr的晶位, 使稀土原子可以参与形成更多的硬磁相, 进一步提高了内禀矫顽力iHc. 合金(Nd0.4Pr0.6)8.5Fe84.5Zr0.5Nb0.5 B6经690 ℃退火10 min后磁性能最优, Br=1.10 T, iHc=534.2 kA·m-1, (BH)max=143.6 kJ·m-3.  相似文献   

7.
采用铜模吸铸及随后的退火处理制备了厚度为0.8 mm,成分为Nd9Fe83-xTi4C4Bx(x=10~15)的Nd2Fe14B/Fe3B型纳米复相磁体,对其组织演变和磁性能进行了研究。结果表明:在铸态合金中,x=10的合金微观组织主要由Nd2Fe14B,Fe3B,α-Fe和TiC相构成。而x=11~15的合金中除含上述各相外,还出现了Nd2Fe23B3相、未知相和非晶相,且随着B含量的增加,它们在合金中的相对含量有不同程度的增加;退火过程中,随着合金中亚稳相和非晶相的转化,Nd2Fe14B,Fe3B和α-Fe相对含量增加,但不同B含量合金的相结构变化差异明显,导致退火后磁体具有不同的磁性能。其中,x=12的合金在680℃退火5 min后获得了最佳磁性能:Br=0.63 T,iHc=98.12 kA·m-1,(BH)max=22.79 kJ·m-3。  相似文献   

8.
采用熔体单辊旋淬法制备了快凝Al87Ni7Cu3Nd3合金条带,利用差热扫描热力学(DSC)分析、X射线衍射(XRD)分析等手段对比研究了快凝合金条带及其不同退火态材料的晶化行为.选择合适工艺条件,对快凝合金条带进行等温加热退火,采用高分辨透射电镜(HRTEM)观察分析了等温退火态材料显微组织特征.结果表明,快凝Al87Ni7Cu3Nd3合金薄带呈现出完全均匀的非晶态结构.随加热温度升高,非晶态薄带的晶化过程包括两个主要的相转变: α-Al晶体从非晶基体中析出的初始晶化以及有Al3Ni,Al11Nd3和Al8Cu3Nd形成的第二次晶化过程.在低于310 ℃下加热,快速凝固Al87Ni7Cu3Nd3金属玻璃中发生的主要相转变是富Al非晶的初始晶化.110 ℃等温退火态薄带主要是由α-Al加残余非晶相的两相组成,α-Al晶体纳米颗粒均匀弥散分布在残余非晶基体上.而在310 ℃热暴露后的退火试样中,在除α-Al晶体外的残留非晶相中开始出现极少量的Al3Ni金属间化合物.  相似文献   

9.
研究了Ti和C添加对Nd9.4Fe79.6-xTixB11-yCy(x=0,1,2,4,6;y=0.5,1.5,3)合金晶化方式、显微结构和磁性能的影响规律。结果表明,适量Ti和C添加改变了合金的晶化方式,使-αFe相和Nd2Fe14B相同时从Nd9.4Fe75.6Ti4B10.5C0.5非晶基体中析出,避免了先析出相晶粒的长大,利于获得细小均匀的显微结构。适量Ti和C添加的Nd-Fe-B-Ti-C非晶合金在退火过程中易析出细小弥散的TiC和TiB2相,可作为形核质点促进形核,且可抑制晶粒长大,最终形成细小均匀的显微结构。综合性能较佳的Nd9.4Fe75.6Ti4B10.5C0.5合金退磁曲线具有优异的方形度,最佳退火条件下合金薄带的剩磁Br为0.91 T,矫顽力iHc为976 kA.m-1,磁能积(BH)max达135 kJ.m-3。文章最后对Ti和C添加合金微结构的形成机制进行了探讨。  相似文献   

10.
采用单辊旋淬法首次制备了Al85Ni10ErxZr5-x(x=3,4,5)非晶合金,利用X射线衍射(XRD)证明Al85Ni10ErxZr5-x(x=4,5)结构为完全非晶态,Al85Ni10Er3Zr2合金为部分非晶。应用差示热分析法(DTA)测定该合金的热学参量,分析了其晶化过程。利用Kissinger法计算了非晶合金的晶化激活能。研究了Er的增加对于Al-Ni-Er-Zr系合金非晶形成能力和热稳定性的影响。结果表明:Er的增加提高了该合金体系非晶形成能力和热稳定性。  相似文献   

11.
It is shown that colchicine ( 4 ) can regiospecifically be transetherified at C(10) by heating in ROH in the presence of (RO)4M (M = Ti, Zr; cf. Scheme 2). (PrO)4Zr in PrOH gives better yields than (PrO)4Ti in PrOH, and also in the catalytic variant of the conversion is (PrO)4Zr more effective than (PrO)4Ti.  相似文献   

12.
13.
One-electron oxidation of two series of diaryldichalcogenides (C6F5E)2 (13a–c) and (2,6-Mes2C6H3E)2 (16a–c) was studied (E = S, Se, Te). The reaction of 13a and 13b with AsF5 and SbF5 gave rise to the formation of thermally unstable radical cations [(C6F5S)2+ (14a) and [(C6F5Se)2+ (14b) that were isolated as [Sb2F11] and [As2F11] salts, respectively. The reaction of 13c with AsF5 afforded only the product of a Te–C bond cleavage, namely the previously known dication [Te4]2+ that was isolated as [AsF6] salt. The reaction of (2,6-Mes2C6H3E)2 (16a–c) with [NO][SbF6] provided the corresponding radical cations [(2,6-Mes2C6H3E)2+ (17a–c; E = S, Se, Te) in the form of thermally stable [SbF6] salts in nearly quantitative yields. The electronic and structural properties of these radical cations were probed by X-ray diffraction analysis, EPR spectroscopy, and density functional theory calculations and other methods.  相似文献   

14.
蒽酮1和氯甲基吡啶盐酸盐2在甲苯中回流反应生成10,10-二吡啶甲基-9(10H)蒽酮(3),收率63%~68%;3用硼氢化钠还原生成10,10-二吡啶甲基-9,l0-二氢蒽-9-醇(4),收率87%~90%;蒽醇4在酸催化下发生歧化反应,得到还原产物10,10-二吡啶甲基-9,10-二氢蒽(5)和氧化产物蒽酮3.该歧化反应受催化剂、溶剂和反应温度等影响.当蒽醇4用三氟化硼为催化剂、甲苯为溶剂、回流反应,5的收率达到74%.所合成的新化合物都经1H NMR,13C NMR,MS和元素分析表征确认.  相似文献   

15.
Vanadium oxides, as highly efficiently catalysts, are widely applied in various catalytic reactions, such as the dehydrogenation of light alkanes and epoxidation of alkenes. In this paper, a series of VO x /Al 2 O 3 catalysts were fabricated by the 1-pot method for catalytic propane dehydrogenation. The results indicated that the VO x /Al 2 O 3 catalysts with loading of 10 wt.% vanadium exhibited optimized catalytic performance. The as-prepared catalysts were characterized by N 2 adsorption-desorption, XRD, TEM, H 2 -TPR, and XPS to explore the texture properties, morphology, and electronic environment of vanadium. In addition, several vanadium catalysts were also prepared by the incipient wetness impregnation (IWI) method to compare their catalytic performance with the 1-pot synthesized catalysts. The catalysts synthesized by the 1-pot method exhibited higher selectivity of propylene and longer catalyst lifetime at high propane conversion when compared to the counterpart synthesized by the IWI method.  相似文献   

16.
Ring contraction followed by an elimination reaction on anti-9-methyl-18-trans-2-(10b,10c-dimethyl-10b,10c-dihydropyrenyl)-2,11-dithia[3,3]metacyclophane gave the desired compound 10b-methyl-10c-[2-(10b,10c-dimethyl-10b,10c-dihydropyrenyl)]-10b,10c-dihydropyrene. 1H NMR spectroscopic analysis indicated a ring current effect over a considerable distance from the macro-molecular plane of each of the aromatic rings with the two pi systems freely rotating. Bathochromic shifts and peak broadening in its electronic spectrum clearly supports the presence of through-space pi-pi interactions between the two aromatic rings. This should serve as a good model to verify homo-conjugation effect in such a novel system where the two pi systems are freely revolving.  相似文献   

17.
18.
The hexanuclear gold carbonyl cluster [PPh4]2[Au6(CF3)6Br2(CO)2] (4) has been obtained by spontaneous self-assembly of the following independent units: CF3AuCO (1) and [PPh4][Br(AuCF3)2] (3). The cyclo-Au6 aggregate 4, in which the components are held together by unassisted, fairly strong aurophilic interactions (Au···Au ∼310 pm), exhibits a cyclohexane-like arrangement with chair conformation. These aurophilic interactions also result in significant ν(CO) lowering: from 2194 cm–1 in the separate component 1 to 2171 cm–1 in the mixed aggregate 4. Procedures to prepare the single-bridged dinuclear component 3 as well as the mononuclear derivative [PPh4][CF3AuBr] (2) are also reported.  相似文献   

19.
Variable‐temperature X‐ray diffraction was used to monitor the crystalline transition of Nylon 10 10. It could be found that the α‐phase of the sample transforms into a γ‐phase at about 135°C, if the sample is heated from room temperature to a high temperature, which is the so‐called Brill transition of Nylon 10 10. In addition, Nylon 10 10 was found to crystallize directly in a kind of α‐phase from the melt at high temperature, which is much different from the behavior of Nylon 66 and Nylon 10 12. Upon further cooling to room temperature, Nylon 10 10 preserved the α‐phase revealing two peaks in its XRD patterns. However, if the Nylon 10 10 sample with γ‐form was not melted, but immediately cooled from a temperature between TB and Tm, the reverse transition from γ‐form to α‐form could be observed at about 130°C, indicating reversible Brill transition of Nylon 10 10.  相似文献   

20.
Polyfurans have never been established as useful conjugated polymers, as previously they were considered to be inherently unstable and poorly conductive. Here, we show the preparation of stable and conducting polyfuran films by electropolymerization of a series of oligofurans of different chain lengths substituted with alkyl groups. The polyfuran films show good conductivity in the order of 1 S cm–1, good environmental and electrochemical stabilities, very smooth morphologies (roughness 1–5 nm), long effective conjugation lengths, well-defined spectroelectrochemistry and electro-optical switching (in the Vis-NIR region), and have optical band-gaps in the range of 2.2–2.3 eV. A low oxidation potential needed for polymerization of oligofurans (compared to furan) is a key factor in achievement of improved properties of polyfurans reported in this work. DFT calculations and experiments show that polyfurans are much more rigid than polythiophenes, and alkyl substitution does not disturb backbone planarity and conjugation. The obtained properties of polyfuran films are similar or superior to the properties of electrochemically prepared poly(oligothiophene)s under similar conditions.  相似文献   

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