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双语推荐:顺磁相变

采用溶胶凝胶法制备了系列Pr0.5Sr0.5MnO3纳米晶样品,用X射线衍射仪和扫描电子显微镜观察了材料的晶体结构和微结构,并用振动样品强计对其性和热效应进行了研究.结果表明,随着烧结温度的提高,材料颗粒尺寸也相应增大.当材料颗粒尺寸大于115nm时,材料表现出反铁到铁的一级相变和铁顺磁的二级相变,而当颗粒尺寸小于115nm时,样品低温的反铁到铁磁相变消失,只剩下铁顺磁一个相变.采用Maxell关系计算了材料在1T场下的熵变,在反铁到铁磁相变附近发现了正熵变,而在铁顺磁相变附近具有负熵变.
Pr0.5Sr0.5MnO3 polycrystalline compounds were prepared by sol-gel method, and their properties were investigated by x-ray diffraction, scanning electron microscope, and vibrating sample magnetometer. It wasfound that the grain size increased with the increase of sintering temperature. When the grain size is larger than 115 nm, the material exhibits an antiferromagnetic to ferromagnetic transition and a ferromagnetic to paramagnet?ic transition. When the grain size is less than 115 nm, the low-temperature antiferromagnetic to ferromagnetic transition disappears, and only ferromagnetic to the paramagnetic transition can be observed. The magnetic entro?py changes were calculated by Maxell relation. A positive magnetic entropy change was found in the antiferro?magnetic to ferromagnetic transition, while a negative magnetic entropy change was observed in the ferromagnet?ic to the paramagnetic transition.

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由于一级相变磁制冷材料发生磁相变时有晶胞体积的突变,相变过程中有相变潜热存在,其化过程中有许多学问题有待于进一步探究.本文以LaFe13-xSix合金为研究对象,在现有对一级相变基础问题的分析基础上,对一级相变材料中系统熵变、等温熵变、绝热温变、热滞、滞、铁顺磁态两相共存的温度区间和场区间、制冷能力的计算等学基础问题进行了较为细致的探究.分析表明,在忽略完全铁态和顺磁态对热效应的贡献时,Maxwell方程和Clausius-Clapeyron方程计算熵变的值具有等效性.等温化过程中升温和降温曲线包围的面积SABCE(滞的大小),实际上是升温过程和降温过程中场做的净功,等于相变潜热之差.滞和热滞的大小与化过程数据测量的时间有关,测量时间越长则滞后越小,当相变是平衡相变则滞后为零.另外,对温度和场诱导磁相变过程进行了分析,提出了一级相变磁制冷材料制冷能力的不同计算模型.本文对一级相变磁制冷材料的学基础问题研究有一定的参考价值.
Due to the cell volume mutations and the phase transition latent heat existing during phase transition of the first-order phase transition magnetic refrigeration material, many basic problems need to further explore in the magneti-zation process. In this paper, taking LaFe13-xSixalloys as the research object, we discuss in detail some problems, such as a phase-change, entropy change, isothermal entropy change, adiabatic temperature change, thermal and magnetic hysteresis, the temperature range and magnetic field range in which the ferromagnetic and paramagnetic state coexist, and magnetic refrigeration capacity calculation, The analysis shows that the magnetic entropies calculated by Maxwell equation and Clausius-Clapeyron equation are equivalent when neglecting the contributions of ferromagnetic and param-agnetic state to magnetocaloric effect. The area surrounded by the curve in heating of isothermal magnetization process and curve in cooling of isothermal magnetization process (hyst

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采用流动氩气电弧熔炼和高温退火法,制备了Mn5Ge3-xCux(x=0.0-0.2)化合物,并用粉末X-射线衍射研究了该系列化合物的晶体结构.结果表明:这些化合物都具有Mn5Si3型六角结构,空间群为P63/mcm;Cu对Ge的替代不改变化合物的晶体结构;晶格常数a和晶胞体积V随着Cu含量的增加而增加,而晶格常数c略微减小.用Lakeshore 7407型振动样品强计对每个化合物在低场(0.05T)下进行热测量,确定了居里温度和磁相变.结果表明,随着Cu含量的增加,化合物的居里温度几乎不变,其磁相变属于铁-顺磁二级相变.
The Mn5 Ge3-xCux(x=0.0-0.2)compounds are prepared by means of flowing arc melting and high temperature quenching.The Crystal structure of the compounds has been investigated by means of X—ray diffractometer.The random power X—ray diffraction patterns show that all samples of the com—pounds crystallize in the Mn5 Ge3 type hexagonal structure with space group P63/mcm.Substitution of Cu for Ge does not lead to a change for crystal structure.The lattice parameter a and unit—cell volume monot—onously increases slightly with increasing Cu content,while the lattice parameter c decrease slightly.The magnetic measurement performed with Lakeshore 7407 type vibrating sample magnetomer.The results of the curves show that the Curie temperature TC have no change increasing with Cu content,and show that the magnetic phase transition belongs to second order transition.

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根据Nd2Fe14B的冲击加载实验,计算了3.3—7.2 GPa压力范围内冲击波阵面上压力与温度的关系.基于分子场理论,引入压力等效场,改进了双亚点阵理论模型,并分析了在不同温度和压力下Nd2Fe14B的性转变机理.计算了压力对Nd2Fe14B致伸缩系数、化率、化强度以及居里温度的影响,给出了Nd2Fe14B发生铁顺磁相变的压力和温度判据.计算结果表明:压力使Nd2Fe14B的居里温度逐渐向低温区转移,当压力从0 GPa增加到1.15 GPa时,居里温度从584 K降至292 K;随着压力的增加,Nd2Fe14B的化强度不断下降,且临界去压力随温度的升高呈下降趋势;在3.3—7.2 GPa压力范围内,Nd2Fe14B发生了铁-顺磁相变.
According to the shock wave experiment on the Nd2Fe14B ferromagnet, the relationship between pressure and temperature on the shock front is calculated in a pressure range from 3.3 GPa to 7.2 GPa. In order to analyze the magnetic transition mechanism of Nd2Fe14B under different temperatures and applied pressures, the equivalent pressure field is introduced to improve the two-sublattice model based on the molecular field theory. The pressure dependence of magnetostriction coefficient, susceptibility, magnetization, and Curie temperature of Nd2Fe14B are calculated. The criteria of the ferromagnetic-paramagnetic phase transition occurring in Nd2Fe14B at different temperatures and pressures are obtained. The results indicate that the Curie temperature of Nd2Fe14B decreases as pressure increases. The Curie temperature reduces from 584 K at 0 GPa to 298 K at 1.142 GPa. With the increasing of pressure, the magnetization of Nd2Fe14B declines. The critical demagnetization pressure of Nd2Fe14B al

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自旋s=1的海森堡反铁链材料LiVGe2 O6的化率以及核共振实验表明该材料在临界温度约为22 K时由顺磁相转变为反铁N′eel相,且低温激发谱存在能隙。本文在已有模型哈密顿量的基础上提出了一个低能场论模型--Ginzburg-Landau理论来描述这一反铁链材料,并运用这一理论讨论了LiVGe2 O6由于自发对称性破缺导致的有限温度相变及相应的化率变化情况,理论计算很好地解释了现有的实验结果。
The susceptibility and nuclear magnetic resonance measurements on quasi-one-dimensional spin-1 Heisenberg antiferromagnet LiVGe2O6 indicate that this material shows a phase transition from paramagnetic state to antiferromagnetic N′eel state at about 22 K, and there exists a gap in the low-temperature magnetic excitation spectrum. Based on the model Hamiltonian of LiVGe2O6, we propose a low-energy field theory--Ginzburg-Landau theory for this compound. From this theory, we study the finite-temperature phase transition induced by spontaneous symmetry breaking and then calculate the finite-temperature susceptibility of LiVGe2O6. All the theoretical calculations are consistent with the experimental results.

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采用溶胶-凝胶法制备不同粒径的La缺位La0.9MnO3钙钛矿氧化物.用X射线衍射、扫描电子显微镜、振动样品强计对材料的晶体结构、微结构、性和热效应进行了研究.结果表明,不同温度下退火(700oC~1100oC)的样品均具有菱形钙钛矿结构.退火温度从700oC增加到1100oC,样品的平均晶粒大小从25 nm增加到1000 nm.随着晶粒大小的增加,材料在低温的饱和化强度逐渐增强,铁顺磁相变变得陡峭,从而使材料的熵变逐渐增加.当材料的晶粒尺寸大于500 nm时,材料的熵变趋于稳定(-2.7 J/kg·K).
La-deficient La0.9MnO3 perovskite nanoparticles with different grain size were prepared by sol-gel method. The crystal structure, microstructure, magnetic properties, and magnetocaloric effect in La0.9MnO3 nanoparticles were studied using x-ray diffraction, scanning electron microscopy and vibrating sample magnetom-eter. All samples that annealed at different temperatures (700 ℃~1100 ℃) have rhombohedral structure. With the increase of annealing temperatures from 700 ℃ to 1100 ℃, the average crystal size increases gradually from 25 nm to 1000 nm. The magnetization and magnetic entropy change (ΔSM) increase with the increase of crystal size. The value of ΔSM becomes stable when the crystal size is larger than 500 nm.

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通过熔体快淬制备了 Gd59 Co41、Gd56 Co44非晶条带,并对Gd56 Co44非晶条带进行588 K、10 min的晶化处理.利用 X 射线衍射仪(XRD)分析了合金的结构,通过综合物性测量系统(PPMS)研究了合金的性及热效应.结果表明,Gd59 Co41和 Gd56 Co44非晶条带的初始晶化温度分别为523和544 K;Gd56 Co44非晶条带晶化处理后获得了 Ho4 Co3型六方单相.非晶态和晶态合金在居里温度附近都发生铁顺磁的二级相变.随着Gd/Co比例的降低,Gd59 Co41和Gd56 Co44非晶合金的居里温度(TC )从198 K 提高到217 K;晶化处理后 Gd56 Co44合金的居里温度为218 K,与非晶态合金相比变化甚微.在ΔH=5 T时, Gd59 Co41和Gd56 Co44非晶合金的最大熵变(-ΔSM)和制冷能力(RC)分别为7.7 J/kg·K、525 J/kg和6.6 J/kg·K、544 J/kg;而 Gd56 Co44晶态合金的最大熵变(-ΔSM)和制冷能力(RC)分别为5.6 J/kg·K 和528 J/kg.大的熵变和制冷能力,几乎可以忽略的矫顽力和热滞/滞效应,表明 Gd-Co 二元非晶和晶态系列合金是200 K温区附近一类具有潜在应用价值的制冷工质.
Gd59 Co41 and Gd56 Co44 amorphous ribbons were prepared by arc melt spinning,and then Gd56 Co44 amorphous ribbon was crystallized at 588 K for 10 min.By means of X-ray diffraction (XRD)and physical prop-erty measurement system (PPMS),the structure,magnetic properties and magnetocaloric effect of the alloys were investigated.The results show that the onset crystallization temperatures Tx for the Gd59 Co41 and Gd56 Co44 amorphous ribbons were found to be about 523 and 544 K,respectively.The Ho4 Co3-type hexagonal phase was obtained for crystallized Gd56 Co44 ribbons after annealing.All the amorphous and crystallized alloys undergo fer-romagnetic to paramagnetic second-order transition at their Curie temperatures.The Curie temperature (TC)of the amorphous Gd59Co41 and Gd56Co44 alloy enhances from 198 to 217 K with decreasing the Gd/Co ratio.And the TC of crystallized Gd56 Co44 alloy was 218 K,which has little change compared with that of the amorphous alloy.For a magnetic field change of

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大多数相变材料由固相转变为液相时,吸收相变潜热,相变材料体积膨胀;从液相转变为固相时放出相变潜热,体积缩小。利用相变材料的这种体积随相变而变化的特性,将一定量的相变材料封装在密闭容器中,通过环境温度引起相变材料相变,相变过程中因体积变化产生的力,为某些需要微小位移量的运动机构提供驱动动力。最后,实例说明相变材料这种特性在航天器微驱动上的应用。
Most of the phase change material when they convert from the solid phase to the liquid phase,absorb the la-tent heat of the phase change material,and the volume of the phase change material expands;when they convert from the liquid phase to the solid phase,release latent heat of the phase change material,and the volume of the phase change materi-al reduce. By use of the characteristic of the volume of the phase change material variation with the phase transition,a cer-tain amount of the phase change material closed in a sealed container,the phase transition of the phase change materials with the variation of the ambient temperature,the stress which is produced due to the volume changes during the phase transformation,provides drive force for moving mechanism requires some tiny displacement. Finally,the property of the phase change materials is applied for micro drive in spacecraft with example.

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为了充分发挥相变墙体的调温节能效果,以掺有定形相变胶囊的储能墙体及其构成的相变房间为对象,并考虑室内空气的热响应,建立相变墙体及房间的传热理论模型.采用显热容法模拟了在周期性变化的室外边界条件下,相变储能墙体内的传热过程及室内空气的温度变化.计算结果表明:储能墙体中的相变胶囊含量是影响室内空气温度衰减的重要因素之一.相变材料最佳相变中心温度宜尽量接近墙体相变层中心温度,相变温度波动幅度的大小仅影响室内空气温度的波动区间,而对振荡的平衡温度影响较弱.
In order to better improve thermoregulation and energy-saving effect of the integrated phase change building system, a heat transfer theoretical model of building envelopes with shape-sta-bilized phase change capsule ( SSPCC) and their room is presented, in which the indoor temperature response is considered.The apparent heat capacity method is used to simulate the heat transfer pro-gress of the phase change wall and variations of the indoor temperature under cyclical outdoor tem-perature variations.The calculation results show that the mass fraction of SSPCC is one of the signif-icant factors that influence the degree of decay of the indoor air temperature.It is better to make the best phase temperature as close to the core temperature of the phase change wall layer as possible. Furthermore, the phase change temperature fluctuation range only affects the fluctuation range of the indoor air temperature, its effect on the equilibrium temperature is weak.

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为了探讨相变回填材料固液相变对地埋管换热器蓄能传热性能的影响,建立了带有相变的垂直U型埋管换热器传热数学模型,并利用显热容法对相变材料的相变问题进行了处理。基于模型的数值求解,分析了夏冬季运行工况下相变材料固液相变对U型埋管换热器蓄能性能及其周围土壤温度热响应特性的影响规律,结果表明:同样条件下,相变材料固液相变会减缓埋管周围土壤温度变化趋势,缩小埋管热影响区域;夏季工况采用较低相变温度、冬季采用较高相变温度的相变材料均可以明显改善其换热效果,同时相变潜热大的相变材料可以明显增加地埋管的蓄能效果。研究结论对于缓解土壤热影响区域、改善地埋管换热器的蓄能传热性能具有重要意义。
Ground source heat pump (GSHP) has been recognized as being among the cleanest, most energy efficient and cost effective systems for residential and commercial space’s heating and cooling applications. The main advantage of using the ground as the heat source or sink of the system is that the soil temperature at tens to hundreds of meters in depth is relatively constant and is generally lower in summer and higher in winter than that of ambient air temperature. This results in an overall improvement of the system performance and thus reduces operation costs. Therefore, GSHP systems have become increasingly popular in commercial and institutional buildings. Heat transfer around vertical ground heat exchanger (GHE) is a common problem for the design and operation of GSHP. The energy storage performance of GHE and its influences on the temperature thermal response characteristics of soil around it are important for a long-term high-efficient and steady operation of GSHP systems.