压缩区的英文

• compression area
• compression zone
• compressional zone

• "压缩"英文翻译    compress; condense; reduce; ...
• "区"英文翻译    H region; H
• "弹性压缩区" 英文翻译 :    elastic compression zone
• "可压缩区段" 英文翻译 :    squeeze section
• "压缩区域" 英文翻译 :    compressive region
• "冲击波压缩区" 英文翻译 :    compression phase of blast wave
• "冷轧弹性压缩区" 英文翻译 :    elastic compression zone
• "可压缩波导段 可压缩区段" 英文翻译 :    squeezesection
• "渐缩区" 英文翻译 :    taper
• "浓缩区" 英文翻译 :    enriching section
• "伸缩区" 英文翻译 :    breathing zone
• "收缩区" 英文翻译 :    constricted area; contracted area
• "磁收缩区" 英文翻译 :    magnetic isthmus
• "富集区, 浓缩区" 英文翻译 :    enrichment region
• "光碟微缩区" 英文翻译 :    cd microform area
• "颈缩区温度" 英文翻译 :    neck temperature
• "冒口补缩区" 英文翻译 :    feeding zone
• "异常收缩区" 英文翻译 :    abnormally contracting regions
• "浓缩区薄层板" 英文翻译 :    concentrating thin layer plate
• "压缩" 英文翻译 :    compress; condense; reduce; cut down; compression; contraction; compaction; pack; reduction; recompression; hoop (静水压的) 压缩非生产性开支 cut down non-productive expenses; 压缩国内需求 depress [lowering] domestic demand; 压缩机关团体购买力 limiting government institutions' purchase of consumer goods; 压缩不适当进口 reduce inappropriate imports; 压缩一则新闻报道 condense a news story; 压缩比 compression ratio; ratio of compression; 压缩饼干 ship biscuit; pilot bread; hardtack; 压缩成型机 compacting shape machine; 压缩冲程 [机械工程] compression stroke; 压缩处理 compressing; 压缩点火 compressed ignition; [机械工程] compression ignition; 压缩制冷 compression refrigeration; 压缩制冷机 compression refrigerating machine; 压缩作用 compression
• "压缩；压缩力" 英文翻译 :    compression
• "白压缩" 英文翻译 :    white compression
• "表压缩" 英文翻译 :    list compaction; table compression
• "冰压缩" 英文翻译 :    ice compactness
• "波压缩" 英文翻译 :    wave compression

• The interactions concentrate on two regions : the compressed region in the front and the rarefied region in the wake
  这种相互作用，集中在两个区域内：即前部压缩区和尾部稀化区。
• This paper is devoted to a detailed investigation of non - steady interaction between the moving body and plasma in compression region , whose dominating equations are obtained and whose phenomena are simulated
  文献[ 12 ]中采用双流体、双时标近似，得到了压缩区内高频调制场对带电粒子非稳态作用的控制方程。
• That is to say , high frequency modulational field radiated from the antenna system of moving bodies influents the charge distribution in plasma , while the disturbance of the charge distribution influents the field conversely
  也就是说，在压缩区内，飞行体天线辐射出的高频调制场，影响着等离子体中的电荷分布，而电荷分布的扰动又反过来影响场量。
• The equation of state ( eos ) of metals can be described commendably by the so - called trinomial eos which have " the cold part " , the thermal part contributing by crystal ( or atoms ) and the thermal part contributing by electrons
  冲击压缩区的金属通常可以由所谓的三项式物态方程描述，即将物态方程分成相对独立的“冷贡献” 、 “晶格(原子实)热贡献”和“电子热贡献”三部分。
• Robert c gauthier , mike ashman , athanasios frangioudakis , hawie mende and shanjun ma , radiation - pressure - based cylindrically shaped microactuator capable of smooth , continuous , reversible and stepped rotation , applied optics , vol . 38 , no . 22 ( 1999 ) 4850 ? 4860
  马善钧，徐学翔，空间飞行体与压缩区内等离子体非稳态相互作用的数值模拟，空间科学学报，第21卷，第4期， （ 2001 ） 305 - - 310 。
• In this paper , based on the amplitude transport equation of fast varying field and the low frequency disturbance equation of electr on density , the evolutions of the density distribution of charged particles and the collapse of electric field have been calculated numerically in two dimensions with three field components under the condition of transverse wave
  所以本文采用了ftcs有限差分格式方法，利用二维三分量轴对称，对空间飞行体与压缩区内等离子体非稳态相互作用过程进行数值模拟，得到了电荷密度扰动与电场的变化情况。
• ( 5 ) especially , a method to get p _ ( c ) has been developed based on the formerly work by hu jinbiao . many p _ ( c ) of metals have been calculated by this method and been compared with literature and experimental data . it has been proved preliminarily that though this method is very simple and very easy to use , its result is in faith reason
  对大量金属进行了计算，与文献以其它方法获得的冷压结果及实验数据的比较显示，该方法具有物理含义明确、基本不依赖于尚存在争议的热压模型、过程简便、所依赖的数据丰富以及结果稳定合理的特点，是一种适宜于高压物性日常研究的冲击压缩区半经验冷压获得方法。
• ( 1 ) the got by experiment may contain thermal contributing by electrons and this part is not can be ignored . ( 2 ) got by thermal dynamic experimental data under normal temperature and pressure can be a standard for various theoretical models , but its precision should be analysis carefully before to use . ( 3 ) the method of using the migault ' s formular associate tuning up parameter to express which often be used is not very reasonable
  本文第3章就gr neisen物态方程研究了三方面问题：第一方面，在分析了几种不同定义的gr neisen系数的区别与联系的基础上指出， ( 1 )在冲击压缩区，直接依据实验数据获得的往往包含不可忽略的电子热贡献； ( 2 )常态热力学可作为检验gr neisen系数理论模型的一个标准，但应注意该实验测量值的精度(包括由于实际材料中存在的“非三项式物态方程因素”的影响) ，而所总结的在周期表上所具有较明显的规律性，可作为对该值精确程度判断的参考； ( 3 )指出一种以调节参数的migault公式描述的常用方法的基础与实际情况并不相符。

• 压缩区的日语：そせいいき プラスチックゾーン しんとうけん