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the main body
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  空间主体
     This paper mainly studies the meaning of local architectural culture, gives prominence to the native characteristics , refers to the traditional and professional architectural expression , respects and reveals local materials and classical means , exhibits the main body of space-human beings , creates architectural works with local feature.
     研究地方建筑文化内涵,突出地方特色,借鉴传统建筑特征语汇,尊重和表现地方材料、传统手法,体现人是空间主体,走地方特色的建筑创作道路.
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     This paper mainly studies the meaning of local architectural culture,gives prominence to the native characteristics,refers to the traditional and professional architectural expression,respects and reveals local materials and classical means,exhibits the main body of space-human beings,creates architectural works with local feature.
     研究地方建筑文化内涵,突出地方特色,借鉴传统建筑特征语汇,尊重和表现地方材料、传统手法,体现人是空间主体,走地方特色的建筑创作道路。
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  “the main body”译为未确定词的双语例句
     On the System of Market Economy With the Composite Ownership as the Main Body
     论混合所有制占主体的市场经济制度
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     Comment on the Growth and Canonical Behavior of the Main Body of Information Market
     论信息市场运行主体的发育和规范性行为
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     Based on the cultivation target of the high liberal vocational education,this paper discusses on the main body position of the library of high liberal vocational college and university in the literacy education for university students,and probes into how to expand the educational function of the library to make better cultivation of the social practice ability of university students.
     根据高职教育的培养目标,论述了文科高职院校图书馆在大学生素质教育中的主体性地位,探讨了如何拓展教育职能以更好地培养大学生的社会实践能力。
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     Shaping the main body of vocational education market is to perfect both market system and laws and regulations.
     塑造职业教育市场主体,就是要完善职业教育市场主体体系和健全职业教育市场法律法规体系。
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     NH+4-N and NO-3-N were the main body of TIN,and their proportions were 52.58 and 29.99%,respectively.
     NH4+-N和NO3--N为TIN沉降主体,分别占TN沉降量的52.58和29.99%。 图4,表2,参16。
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     The main
     第一部分为导言,主要介绍本选题的依
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     Main Results:
     主要研究结果如下:
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     The main conclusions are:
     通过问卷调查及访谈,得出的主要结论是:
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     Main results:
     主要实验结果:
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     Body contact;
     身体接触;
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  the main body
The eigenvalue problem for the Laplace operator with the Neumann boundary conditions in a domain that has a thin spike of finite length is considered for the case in which the limit value is an eigenvalue both for the main body and the spike.
      
An important element of these observations is the separation of luminous fragments from the main body at the final radiation stage of the bolide as a whole.
      
The first period is probably the rotation period of the main component, while the second period may be equal to the orbital period of the satellite with one side facing the main body.
      
Another model of the asteroid is also possible: P0 = 2.h93 is the rotation period of the main body, P1 = 0.d70 is the orbital period of the synchronous satellite, and P2 = 3.d20 is the precession period.
      
The main body of the continental crust was formed 2.90-2.65 Ga ago.
      
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In this paper, the authors treated the determination of the inertia parameters (virtual mass and virtual moment of inertia) by model tests. The accuracy of the experimental method was first checked by using ellipsoids, the inertia parameters of which were known, the error being about 2%. Then. a body of revolution with a vertical stabilizing fin and rudders at tail has been tested. By conducting such tests, the inertia parameters of the whole body and its components were obtained for different states of motion...

In this paper, the authors treated the determination of the inertia parameters (virtual mass and virtual moment of inertia) by model tests. The accuracy of the experimental method was first checked by using ellipsoids, the inertia parameters of which were known, the error being about 2%. Then. a body of revolution with a vertical stabilizing fin and rudders at tail has been tested. By conducting such tests, the inertia parameters of the whole body and its components were obtained for different states of motion of the body. The authors also suggested formulas for calculating these inertia parameters. Such formulas have taken into consideration the interferences between the appendage and the main body. Except for the rudder, which needs further investigation, the agree-ment between the calculated values and experimental results is satisfactory. Finally, the effect of the free snrface on the inertia parameters has been considered and denoted by coefficients of decre-ment. Experiments show that the parameters are nearly constant when the depth of immersion of the body is greater than three times the diameter.

在本文中,作者論述了水下运动物体慣性参数(附加质量及附加轉动慣量)的实驗測定。实验方法的精确性,先用慣性参数已知的椭球体检驗之,誤差約在2%左右。然后就回轉体加上垂直鰭及尾舵的組合体进行試驗,测定了此組合体及其各部件在物体各种运动状态时的慣性参数。作者并提出了各部件慣性参数的理論計算公式,考虑了各附件与本体之間的干扰影响。理論值与实验結果之間符合程度,除牵涉到舵外,是令人滿意的。关于舵的部分,还需进一步探讨。本文最后論述了自由表面对慣性参数之影响,并用减額系数表示之。实驗証明,当物体浸水深度超过三倍直徑之后,慣性参数几乎是常值。

An automatic adiabatic calorimeter for heat capacity measurements of solids and liquids in the temperature range 80~370K has been constructed. In this apparatus the shield temperature control, the electrical energy input and the heating interval measurement are all carried out automatically. The automatic control permits one-man operation of the apparatus.The main body of the calorimeter consists of a sample container, double adiabatic shields, an upper ring for preheating lead wires and a vacum can.The sample...

An automatic adiabatic calorimeter for heat capacity measurements of solids and liquids in the temperature range 80~370K has been constructed. In this apparatus the shield temperature control, the electrical energy input and the heating interval measurement are all carried out automatically. The automatic control permits one-man operation of the apparatus.The main body of the calorimeter consists of a sample container, double adiabatic shields, an upper ring for preheating lead wires and a vacum can.The sample container is made of silver of 99.95% purity, 0.3mm thick, gold-plated and polished, and is provided with a central re-entrant well for setting a thermometer heater assembly. Eight silver radial fins of 0.2mm thick, silver-soldered to the well and to the inside wall of the container, provided good thermal contact of the sample with the container. The size of the main body of the confiner is 3.2cm in diameter and 6 cm long. The total weight of the container is about 50g and its effective capacity is ca. 40ml.The temperature of the container is measured with a standard platinum resistance thermometer and a high-precision Smith bridge. The thermometer, which is platinum encapsulated, 25Ω, 5mm in diameter and 50mm long, was made by Yunnan Instrument Manufactory of China and calibrated at the Chinese Institute for Metrology in accordance with the IPTS-68. The accuracy of the bridge is±0.005% and the temperature is measured to 0.0001K.The temperature difference between the container and the shield is detected by an eight junction copper-constantan thermocouple, the signal from which is fed into a DWT-702 type precise temperature controller for automatically adjusting the current in the shield heater so as to maintain the temperature of the shield as close as possible to that of the container. Experiments demonstrated that during the heat capacity measurements the temperature difference between the shield and the container could be kept within 0.001K. The electrical energy for heating the calorimeter is supplied by a source of power, stable to about 10 parts per million. The energy input is started and stopped automatioally by a digital electronic timer and the heating interval is measured and presented on a digital counter of the timer with an accuracy of 0.005%.The instruments used in the present measurements have been calibrated at the Chinese Institute for Metrology.The reliability of this apparatus is verified through the heat capacity measurements of α-Al_2O_3 and n-heptane which are recommended as the heat capacity standards. The purities of the α-Al_2O_3 and the n-heptane samples available in these measurements are 99.993% and 99.99%, respectively.The results obtained with the present: calorimeter are found to be in agreement with those of Furukawa et al. within±0.30%. The precision of heat capacity measurements is ±0.04% over the entire temperature range.

本文详细描述了用于80~370 K温区内精密测定固体和液体物质热容的自动绝热量热装置。其中热屏绝热控温和样品加热计时均实现了自动化,全部操作可由一人单独完成。通过测定国际量热学会议所推荐的两种标准物质α-Al_2O_3和正庚烷的热容,证实了装置的可靠性;在全部实验温区内本文结果与美国标准局数据符合在±0.30%以内,测试精密度为±0.04%。

A 3B flare and the associated phenomenon of the bright mass ejection on the disk-the spray are discribed. A gap with a width of 2 × 104 km and a length of 2.5 × 104km between the flare and the spray was observed. The intensityof the gap was about 1.6 times greater than that of the undisturbed region. The corresponding radio bursts in different wave bands were quite different. For the spray there was a corresponding type Ⅱ meter wave burst and the burst in 3 -cm wave band. On the other hand, on corresponding...

A 3B flare and the associated phenomenon of the bright mass ejection on the disk-the spray are discribed. A gap with a width of 2 × 104 km and a length of 2.5 × 104km between the flare and the spray was observed. The intensityof the gap was about 1.6 times greater than that of the undisturbed region. The corresponding radio bursts in different wave bands were quite different. For the spray there was a corresponding type Ⅱ meter wave burst and the burst in 3 -cm wave band. On the other hand, on corresponding type Ⅱ and type Ⅳ bursts were observed and the corresponding bursts 3-cm wave band was stronger than that in 10-cm wave band. The flare was also different from the spray in hard x-ray emission. The corresponding hard x-ray emission of the spray was quite weak.Some Ha optical phenomena associated with the flare such as the quiescent chromospheric brighteness of the place which was more than 10 × 105km away from the main body of the flare, the bright loop structure and the dark filament activation, etc., are also discussed.

本文描述了一个与3B级耀斑共生的、太阳视面上的明亮物质抛射现象——喷焰。观测到耀斑与喷焰间有一尺度为2×2.5万公里、强度为未扰区1.6倍的间隙。观测到耀斑和喷焰对应的射电爆发不同。喷焰对应有米波Ⅱ型和Ⅳ型爆发,10厘米爆发远大于3厘米。而耀斑无Ⅱ型和Ⅳ型爆发对应,其3厘米爆发大于10厘米。耀班和喷焰的硬x射线辐射亦不同,喷焰的硬x射线辐射极弱。 对和耀斑有关的其他H_α光学现象——远离耀斑主体十余万公里处的宁静色球增亮,环状明亮结构,暗条的突然活动等,也都作了描述(见附图12)。

 
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