1) cubic TaN
立方相TaN
1.
The influence of N2 pressure on the as-synthesized cubic TaN samples was studied.
结果表明:所制备的纳米粉为单一的立方相TaN,纳米颗粒的平均粒度为5-10nm。
2) cubic
[英]['kju:bɪk] [美]['kjubɪk]
立方相
1.
2～2∶1) were used to prepare the cubic nano-sized zinc titanante powders.
2~2∶1的条件下,通过煅烧,得到粒径小于100 nm的立方相钛酸锌粉体。
2.
The results showed that: the CdS film realized the transition from hexagonal phase to cubic phase and the band-gap of CdS increased with the increasing of the cadmium ion concentration and the bath temperature,.
L-1)和提高沉积温度(80~90℃)来加快沉积速率,CdS薄膜晶相由六方相(H)向立方相(C)转变,且禁带宽度随Cd2+离子浓度增大逐渐变大;当Cd2+离子浓度从0。
3.
High quality cubic GaN (c GaN) is grown by metalorganic vapor deposition (MOCVD) at an increased growth temperature of 900℃,with the growth rate of 1 6μm/h.
利用 MOCVD技术在提高生长温度 (90 0℃ )下生长出了高质量的立方相 Ga N ,生长速度提高到 1。
3) cubic laves phase
立方Laves相
1.
95 substantially retained the MgCu 2 type C 15 cubic Laves phase structure and the lattice constant increases with increasing x.
95完全保持MgCl2立方Laves相结构 ,晶格常量a随Al含量x的增加而增大 。
4) cubic structure ZrO_2
立方相ZrO_2
5) new cubic phase
新立方相
6) cubic phase
立方相
1.
Precipitation of new cubic phase in Al-Li alloys and its mechanism
铝锂合金新型立方相的析出规律及机理
2.
The result showed that the crystal was cubic phase structure by XRD analysis and the first grade grain size was about 50 nm by SEM;the crystal form was stable using TG;the amount of impurity was about the percent of 0.
XRD分析表明晶体为立方相B aT iO3,SEM显示B aT iO3颗粒形貌主要为立方相,一次粒子的粒径约为50 nm,TG分析表明所制得的B aT iO3粉体晶形稳定,原子吸收分析表明所制得的B aT iO3粉体杂质总含量为0。
3.
Fired at l600℃ for 2h,the relative bulk density of the samples made from the powder is up to 95%and the phase of the samples is all of cubic phase.
粉末的煅烧温度为８００℃，成型后试样经１６００℃，２ｈ烧成，相对体积密度达到了９５％以上，且全部为立方相。
补充资料：loss factor tan δ
分子式：
CAS号：
性质：损耗模量与弹性模量之比，又称阻尼因子(damping factor)或内耗(internal dissipation)或损耗角正切(loss tangent)，是每周期耗散能量与在一周期内的最大贮能之比。对剪切应力而言，损耗因子tan δ=G″/Gˊ；对法向应力而言，损耗因子tan δ=E″/E′。如果δ=0，作用力完全有效地用于橡胶变形，没有内耗；如果作用力完全用于克服橡胶的黏性阻力(内摩擦)，损耗角的大小代表了动态变形下能量损耗的大小。
CAS号：
性质：损耗模量与弹性模量之比，又称阻尼因子(damping factor)或内耗(internal dissipation)或损耗角正切(loss tangent)，是每周期耗散能量与在一周期内的最大贮能之比。对剪切应力而言，损耗因子tan δ=G″/Gˊ；对法向应力而言，损耗因子tan δ=E″/E′。如果δ=0，作用力完全有效地用于橡胶变形，没有内耗；如果作用力完全用于克服橡胶的黏性阻力(内摩擦)，损耗角的大小代表了动态变形下能量损耗的大小。
说明：补充资料仅用于学习参考，请勿用于其它任何用途。
参考词条