1) reconstituted
空心圆柱扭剪仪
1.
And then, a new compacting tool for HCA was developed to do reconstituted samples.
动态空心圆柱扭剪仪(HCA)可以模拟地震荷载和波浪荷载等不同的循环荷载，在同一台仪器上可以探讨不同动应力路径下土的动力特性，以往这方面的研究大多针对砂土，而易于液化的粉土却一直被忽视。
2) hollow
空心
1.
Bone Transplantation for Fracture of Lumbar and Thoracic Vertebrae Through Hollow Bone-planting Appliance;
经椎弓根空心椎体植骨器的设计与临床应用
2.
Construction technology of hollow and high pier of railway bridge;
铁路桥梁空心高墩施工技术
3.
The preparation and application of hollow core-shell structured nanomaterials were introduced in this article.
本文对空心核壳结构纳米粒子的制备研究及应用进行了综述。
3) hollow square pile
空心方桩
1.
The article introduces the main characteristics and application prospect of prestresses reinforced concrete hollow square pile.
文章介绍预应力钢筋混凝土空心方桩的主要特点及应用前
2.
Prefabricate hollow square pile is a kind of new pile,of which performance is between the solid square pile and prestressed pipe pile.
预制空心方桩兼备预制桩和预应力管桩的一些特性。
4) fly ash cenospheres
空心微珠
1.
Electroless plating Co-P alloy on the surface of fly ash cenospheres;
空心微珠表面化学沉积Co-P合金研究
2.
Nanocomposite microwave absorbing coatings were prepared by using prepared Ni-Co-P/CNT and Ni-Co-P/fly ash cenospheres composite powders as absorbers,choosing epoxy resin as film forming resin and adding some proper solvent,curing agent and auxiliary agents.
以Ni-Co-P/CNT复合粉体和Ni-Co-P/空心微珠复合粉体作为吸收剂,选用高分子聚合物环氧树脂作为成膜树脂,同时加入适当的溶剂、固化剂和助剂制备出纳米复合微波吸收涂料,并将涂料涂刷于塑料薄板上制备出涂层样品。
5) hollow microsphere
空心微球
1.
NiS2 hollow microspheres were prepared by hydrothermal reaction between NiCl2·6H2O and Na2S2O3·5H2O at the low temperature of 150°C.
5H2O为原料,在150℃较低温度的水热条件下制备了NiS2空心微球,用XRD和SEM对产物进行了表征,NiS2粉体的X射线衍射的衍射峰均与标准衍射图一致(JCPDS:653 325,立方晶系,a=0。
2.
Subsequently, the similar microstructured NiO hollow microspheres were obtained by calcining the above precursor at 400 ℃ for 2 h.
报道一种非常简单的制备NiO和Ni(OH)2空心微球的无模板水热法,即通过NiCl2与氨水在140℃水热反应12h,制备了Ni(OH)2纳米片自组装的空心微球,经400℃热处理2h得到了NiO空心微球。
3.
NiS hollow microspheres were synthesized by the reaction of nickel acetate and thioacetamide inethanol at 150 ℃.
以醋酸镍和硫代乙酰胺为原料,乙醇为溶剂,在150℃的溶剂热条件下制备了硫化镍空心微球,并用XRD,TEM,SAED和SEM对产物进行了表征。
6) hollow ingot
空心钢锭
1.
Effect of Mould Structure on Hollow Ingot Solidification;
空心钢锭锭型结构对空心钢锭凝固过程的影响
2.
Study on the Heat Transfer Boundary Conditions of Core in Hollow Ingot;
空心钢锭芯部换热条件的确定
参考词条
补充资料：横向磁场中的空心超导圆柱体（hollowsuperconductingcylinderinatransversalmagneticfield）
横向磁场中的空心超导圆柱体（hollowsuperconductingcylinderinatransversalmagneticfield）
垂直于柱轴（横向）磁场H0中的空心超导长圆柱体就其磁性质讲是单连通超导体。徐龙道和Zharkov由GL理论给出中空部分的磁场强度H1和样品单位长度磁矩M的完整解式，而在`\zeta_1\gt\gt1`和$\Delta\gt\gt1$条件下为：
$H_1=\frac{4H_0}{\zeta_1}sqrt{\frac{\zeta_2}{\zeta_1}}e^{-Delta}$
$M=-\frac{H_0}{2}r_2^2(1-\frac{2}{\zeta_2})$
这里r1和r2分别为空心柱体的内、外半径，d=r2-r1为柱壁厚度，ζ=r/δ(r1≤r≤r2)，Δ=d/δ，δ=δ0/ψ，δ0为大样品弱磁场穿透深度，ψ是有序参量。显然此时H1→0，M→-H0r22/2，样品可用作磁屏蔽体。当$\zeta_1\gt\gt1$，$\Delta\lt\lt1$时，则
H1=H0/(1 ζ1Δ/2)，
M=-H0r23[1-(1 ζ1Δ/2)-1]。
若$\zeta_1\Delta\gt\gt1$，则$H_1\lt\ltH_0$或H1≈0。所以，虽然$d\lt\lt\delta$，但磁场几乎为薄壁所屏蔽而难于透入空心，称ζ1Δ/2为横向磁场中空心长圆柱体的屏蔽因子。当$\zeta_1\Delta\lt\lt1$时，则H1≈H0，磁场穿透薄壁而均进入空腔，失去屏蔽作用，此时M≈0。类似于实心小样品，由GL理论可求出薄壁样品的临界磁场HK1，HK，HK2和临界尺寸等。
说明：补充资料仅用于学习参考，请勿用于其它任何用途。