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orthorhombic相关的网络例句

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与 orthorhombic 相关的网络例句 [注:此内容来源于网络,仅供参考]

The results show that LSCF and LSM precursors can be transformed to the pure orthorhombic perovskite structure having been calcined at 900℃ and 1200℃ for 5 h, respectively, and LSCF cathode has a smaller particle size and a bigger specific surface area compared with LSM cathode.

采用氨水沉淀法分别制备La0.6Sr0.4Co0.2Fe0.8O(下标 3-δ)与La0.8Sr0.2MnO(下标 3-δ)两种阴极材料,并用X射线衍射、场发射扫描电子显微镜和比表面积对所制备材料的结构、晶粒大小、形貌及比表面积进行表征。

Molybdenum trioxides( MoO3) usually have three forms: orthorhombic,hexagonal and monoclinic.

三氧化钼(MoO3)以三种常见的物相存在:正交相、六方相和单斜相,前者为热力学稳定相,后两者为热力学介稳相。

The results indicated that BaCe0.8Ho0.2O(subscript 3-α) sinters are of single-phase structures of orthorhombic perovskite. In the temperature range of 600~1000℃, the nonstoichiometric materials (x=1.03 and 0.97) have higher conductivities in wet hydrogen and wet air and better performances of hydrogen-air fuel cells than the stoichiometric one (x=1). In this series, BaCe0.8Ho0.2O(subscript 3-α) has the highest conductivities 2.10×10^(-2Scm^(-1) in wet hydrogen, 3.46×10^(-2) Scm^(-1) in wet air, at 1000℃ and the maximum power output density 122 mWcm^(-2 at 1000℃.

结果表明,在600~1000℃温度范围内、湿润氢气和湿润空气气氛中,该系列材料的电导率随温度和钡离子含量的变化均与以该系列材料为固体电解质的氢-空气燃料电池性能随温度和钡离子含量变化的次序一致,即:非化学计量组成材料BaCe0.8Ho0.2O(下标 3-α)(x=1.03, 0.97)具有较化学计量组成材料BaCe0.8Ho0.2O(下标 3-α)(x=1)高的电导率和氢-空气燃料电池输出功率密度,其中BaCe0.8Ho0.2O(下标 3-α)有最高的电导率(1000℃时、在湿润的氢气气氛中:2.10×10^(-2)Scm^(-1);在湿润的空气气氛中:3.46×l0^(-2)Scm^(-1))和最大的氢-空气燃料电池输出功率密度(1000℃时:122mWcm^(-2))。

X-ray diffraction Rietveld refinement results indicate that La2Ni1- y Co y O4+δ compositions have an orthorhombic structure with Fmmm space group. The substitution of partial La3+ with Co at the B-site caused an increase in the length of Ni/Co—O1 bond in the ab plane and La/Sr—O2 bond along c axis.

研究结果表明, La2Ni1- y Co y O4+δ具有正交结构, Co离子取代增加了钙钛矿层中 ab 平面上Ni/Co—O键的键长、岩盐层中沿 c 轴方向上La—O键的键长和非化学计量氧含量,并有利于改善材料的烧结性能。

Significantly shortening of 〓C T〓s for orthorhombic crystals indicates that the thicknesses of crystals decrease during the course of stretching.

通过对不同拉伸比样品〓C T〓弛豫行为的研究发现,拉伸导致正交晶晶片厚度明显变薄,拉伸对于无定形相的高频分子运动几乎无影响。

The molecular motion of amorphous region at high-frequency was found to be hardly affected during the stretching processes. In summary, elongation has created major but different influences on the morphology and molecular motion of the aforementioned four series of polymeric elastomers. For those elastomers like natural rubber and poly , elongation has induced crystallization of the noncrystalline or the soft segments. The crytallinitiy and the crystal thicknesses increase monotonously during the course of the stretching; On the other hand, the stretching processes for those semicrytalline copolymers like EMA and POE are rather complex, including the formation of crystal at relatively low λand the destruction of the crystal at the utmost λ. It revealed that stretching process has resulted in a decreasing of the thicknesses and a shortening of 〓C T〓s for the orthorhombic crystalline components.

拉伸对上述四个弹性体体系的聚集态结构都产生了很大影响,但是影响的程度和内容因体系而不同,对于本身存在着化学交联或者是物理交联的体系而言,拉伸导致了其中本来难以结晶组分的结晶,且结晶度随着拉伸比增加而增加,与此同时,体系结晶的晶片厚度也会逐渐增加;而对于结晶性共聚物体系,如EMA和POE,结晶区本来起到了物理交联的作用,在这种情况下拉伸的影响变得比较复杂,拉伸对于不同晶型的影响有所不同,在拉伸比较低的情况下体系总体的结晶度会有所增加,说明有新的结晶产生,当接近或达到断裂伸长比时,体系的结晶度会突然降低,含量占优的结晶会被拉伸所破坏,含量较低的结晶在整个拉伸过程中受的影响较小。

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