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密度
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  density
     THE DENSITY OF HEAVY WATER BETWEEN 25°AND 100℃.
     重水在摄氏25°至100°间之密度(英文)
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     SIMULATION OF VERTICAL DISTRIBUTION OF SEA-WATER DENSITY (σ_t) IN SHALLOW SEA
     浅海海水密度(σ_t)垂直分布的模拟
短句来源
     MEASUREMENT OF THE NUMBER DENSITY OF HYDROGEN ATOMS WITH THE PUMPING MAGNETIC RESONANCE CURVE
     利用光泵磁共振曲线测量氢原子密度(英文)
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     Residual inhibition in density of [~3H]isradipine binding sites in rat brain membrane pretreated with amlodipine
     氨氯地平抑制大鼠脑膜与[~3H]伊拉地平结合的密度(英文)
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     Results The quantity density and area density of expression of S-100 protein and MIP-1β in lymph nodes and cancer tissue in early stage were obviously stronger than that in late stage and the differences were statistically significant respectively(P<0.01).
     结果结肠癌早期组S-100蛋白和MIP-1β在淋巴结和肿瘤组织表达的面积密度(面密度)和数量密度(数密度)明显增高,与结肠癌晚期组比较差异显著(P<0.01)。
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  “密度(”译为未确定词的双语例句
     EXPERIMENTAL INVESTIGATION ON EFFECT OF ROLLING UPON CRITICAL HEAT FLUX (CHF) FOR WATER AT ATMOSPHERIC PRESSURE
     摇摆对常压水临界热流密度(CHF)影响实验讲究
短句来源
     Experimental Comparison of Critical Heat Fluxes (CHF) for Water in Two Different Length Single Tubes
     两种管长单管中水临界热流密度(CHF)实验比较
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     Amonggastric carcinoma inour study,Survivin expression rate in middle stage of gastric carcinoma group was higher than that in early gastric carcinoma(73.6% vs66.7%,P<0.05). Expression of VEGF and MVD value in middle stage of gastric carcinoma was significantly higher than that in early gastric carcinoma(P<0.05).
     中期胃癌组Survivin阳性表达高于早期胃癌组(73.6%vs 66.7%,P<0.05),其VEGF阳性表达和微血管密度(MVD)平均值高于早期胃癌组(P<0.05)。
短句来源
     The expression of MCP-1 was correlated with that of VEGF(r = 0.233,P = 0.015) and MVD(r = 0.234,P = 0.014). MCP-1 expression in TMAs was significantly correlated with the pathological stage(P < 0.05), but not with tumor size, tumor number, blood vessel invasion, differentiation, cirrhosis and prognosis.
     HCC中MCP1与VEGF(r=0.233,P=0.015)和微血管密度(MVD,r=0.234,P=0.014)均有相关性,MCP-1的表达情况与肿瘤的病理分期亦有相关性(P<0.05),而与肿瘤的大小,数目,分化,肝硬化和预后无显著相关性。
短句来源
     Methods MVD in colorectal carcinoma was examined by immunohistochemical S-P method with anti-CD105 antibody.
     方法应用抗CD105抗体检测结直肠癌组织中微血管密度(MVD)。
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  相似匹配句对
     The line density and area density have been counted.
     区的密度
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     DENSITY OF THE EARTH
     地球的密度
短句来源
     (5)Effects of distance-dependent and density-dependent.
     ( 5 )密度和距离制约。
短句来源
     Density (calc. )
     计算密度D_(calc.)
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  density
One outcome is a simple proof that for $g_{m \alpha , n \beta}$ to span $L^2,$ the lattice $(m \alpha , n \beta )$ must have at least unit density.
      
Applications of generalized perron trees to maximal functions and density bases
      
Convergence and summability of Gabor expansions at the Nyquist density
      
It is well known that Gabor expansions generated by a lattice of Nyquist density are numerically unstable, in the sense that they do not constitute frame decompositions.
      
In 1994, Kotz, Ostrovskii and Hayfavi [10] carried out a detailed investigation of analytic and asymptotic properties of the density of the distribution for the symmetric case θ=0.
      
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The effect of pressure on photographic sensitivity is discussed on the experimental basis that the quantity E/EC, where E is the illumination actually used when the photographic emulsion is under pressure, and Ee the illumination which would be required to produce the same optical density when the emulsion is under no pressure, is a function of pressure only and that for pressures greater than a certain value, E/Ee becomes a linear function of the pressure.

当照相时,照相片子——映像纸,软片,或玻璃板——被压,则其感光性减弱,是为照相的压力效应。设E为照相片子在压力P下得光密度d所需之光照度,若片子不受压力则用光照度E_e即可得此同一之光密度d,故E_e可称在压力P下E之有效照度。吾人实验证明E/E_e为压力P之函数,当p>200kg/cm~2时,E/E_e与P成正比例。 此照相的压力效应,与照相时所用光之颜色,极有关系。黄色光较绿色光为显,绿色光较蓝色光紫色光为显至紫外光则几无此效应。 又此效应之大小,随各种照相片子而不同。就我们所研究的蔡爱斯伊康正色软片,伊司门人像软片,和矮克发等色软片而论,以第一种为最大第二种次之第三种为最小。 这个效应,在实际上,或可有些应用。

By surrounding a photo-neutron source of Ra+Ee with a thin spherical sbell of paraffin, a continuous spectrum of scattered neutrons, extending from zero energy to the energies of the primary neutrons is obtained. When a silver detector is exposed to such a spectrum, a part of the neutrons having just the energies at resonance with the silver nuclei is strongly absorbed by the detector and thereby produces the induced β-activity. By measuring the activity of silver and the apparent absorption coefficient of the...

By surrounding a photo-neutron source of Ra+Ee with a thin spherical sbell of paraffin, a continuous spectrum of scattered neutrons, extending from zero energy to the energies of the primary neutrons is obtained. When a silver detector is exposed to such a spectrum, a part of the neutrons having just the energies at resonance with the silver nuclei is strongly absorbed by the detector and thereby produces the induced β-activity. By measuring the activity of silver and the apparent absorption coefficient of the resonance neutrons in a thin silver absorber, the total width of the resonance levels effective to neutron capture and located in the above spectrum is estimated. Let τ He the average value of one half of the half-value width of the resonance levels, expressed in volts, and n be the number of resonance levels here concerned. We find nτ=260 volts for the silver nuclei of half period 22" if the energies of the primary neutrons are taken to be 2x 105 volts. Knowing nτ, we can evaluate the average spacing between adjacent resonance levels effective to neutron capture by giving a plausible value to τ. We find a spacing of the order 80-800 volts if τ be given the value 0.1-1.0 volt. This result is in good accord with the recent theoretical calculation of Bethe and also with observations of resonance groups in the low energy region.

把‘镭—铍’所产生的‘光中子’,穿过一层半厘米厚的白蜡,我们便得到一‘连续的中子谱’。他们中间有些中子,能和银的原子核起‘共振作用’,因此可以被银片吸收,而产生‘人工放射银’先测量人工放射的强度和‘共振中子’在银片中的吸收率,再应用原子核内共振能层的宽度,我们便可以求出银的原子核内‘共振能层’的密度大约共振能在零和二十万伏特中间,平均每隔一二百伏特便有一可以吸收质子的共振能层,和理论很相符合。

Equations determining the velocity and density distributions within the mixing region of two incompressible gases with different densities are set up, their temperatures being assumed to be the same. For incompressible mixing the total number of gas molecules per unit volume is constant, although the density of the gaseous mixture varies from point to point due to diffusion of matter. As an illustration we consider the plane jet and steady motion. The boundary layer method of approximation can still be applied....

Equations determining the velocity and density distributions within the mixing region of two incompressible gases with different densities are set up, their temperatures being assumed to be the same. For incompressible mixing the total number of gas molecules per unit volume is constant, although the density of the gaseous mixture varies from point to point due to diffusion of matter. As an illustration we consider the plane jet and steady motion. The boundary layer method of approximation can still be applied. The boundary of the jet is shown to be the same as that for one fluid. The solution of the problem then depends upon the numerical value of the coefticient of viscosity of the mixture which is a function of the number of molecules of each constituent gas in the unit volume. The present method of investigation is applicable to the cylindrical and half jets and also to the case where the two gases are at different temperatures.

本文求出规定二不能压缩气体的分片合流运动时,速度与质量密度分布的微分方程式。假定两种气体的密度不同但温度则相等。不能压缩的定义是每单位体积中的两种气体分子数的和不变。本文只讨论一平面守恒注中所需要的微分方程式。粘滞流体运动中之边界近似法仍可应用。同样方法亦可用到守恒圆柱体注,半注及气体中温度不同诸问题。

 
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