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     An in situ analysis was performed in Pan Gang: the volume ratio of water to ore powder in the ore slurry is between 2/5 and 2/1,under the condition of(L×W×H=8×2×20 cm),static measurement(60 s) after 9-minutes natural sediment;
     铁精矿矿浆品位原位EDXRF(能量色散X射线荧光)分析试验在攀钢选矿厂进行,矿浆中水与矿粉体积比在2/5~2/1之间,在(L×W×H=8×2×20cm)的沉淀条件下,经过9 min自然沉淀,静态测量(60 s);
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     Methods Twenty one eyes of PACG were treated by laser peripheral iridoplasty(160~240 mW,500 μm,0.4 s) and laser iridectomy(energy 2.1~7.8 mJ)one day later.
     方法21眼原发性闭角型青光眼第1次急性发作时行激光周边虹膜成形术(160~240mW,500μm,0.4s)和激光周边虹膜切除术(能量:2.0~7.8mJ)治疗。
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     Compared with the stiffness of SHRP, the index of force ductility determined is as flow. (1)Unmodified asphalt: useful compliance D1 /F0 (energy W1 or Inclined rate ratio∣K0/K1∣);
     通过与SHRP低温劲度的相关性分析,确定的测力延度评价指标如下:(1)基质沥青:有效拉伸柔量D1/F0(能量W1或斜率比∣ K0/K1∣);
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     For the test of 241 Am αsource, the position resolution for X and Y of Padova PPAC is 1.0mm and 0.8mm, and 1.8mm and 1.0mm for Argonne PPAC, respectively. The detection efficiency is 49% and 85% for Padova PPAC and 12.75% and 4.5% for Argonne PPAC, respectively. The position resolution, especially the detection efficiency, for any detectors when the heavy ions are detected are certainly improved.
     对α源 (能量为 5 .5 Me V) ,Padova型 PPAC的 X、Y位置分辨分别为 1.0和 0 .8mm,对应的探测效率分别为 4 9%和 85 % ,Argonne型 PPAC的 X、Y位置分辨分别为 1.8和 1.0 mm,对应的探测效率分别为 12 .7%和 4 .5 %。
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     Military middle and low power CO_2 laser technology
     军用中小功率(能量)CO_2激光技术
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     Tracking down the energy
     能量追踪
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     The energy is full.
     能量充足;
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     (2) high single-pulse energy;
     (2)高的单脉冲能量;
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  (energy
Finite energy band-limited functions are reconstructed iteratively
      
When, in addition, the Tolimieri-Orr condition A is satisfied, the minimum energy dual windowoγ ε L2(?) can be sampled as well, and the two sampled windows continue to be related by duality and minimality.
      
Finite-energy high frequency signals, band-pass frequency signals, and band-stop frequency signals are characterized.
      
We use the analytic tools such as the energy, and the Laplacians defined by Kigami
      
On Global Finite Energy Solutions of the Camassa-Holm Equation
      
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In the statistical theory of superlattices in binary alloys, the dependence of the interaction energy upon atomic arrangements is taken into account by regarding the interaction energy in Bethe's theory as an average quantity depending on the degree of order and the composition of the alloy. Two simple assumptions concerning the functional relationship of the interaction energy with order and composition are made. The first is a linear function of order and composition. The second is a linear function of the...

In the statistical theory of superlattices in binary alloys, the dependence of the interaction energy upon atomic arrangements is taken into account by regarding the interaction energy in Bethe's theory as an average quantity depending on the degree of order and the composition of the alloy. Two simple assumptions concerning the functional relationship of the interaction energy with order and composition are made. The first is a linear function of order and composition. The second is a linear function of the average numbers of pairs of atoms. The result of applying these assumptions to superlattices of the type AB is that the critical temperature as a function of the composition is a maximum for equal sumber of A and B atoms only when a certain relation between the coefficients in the assumed function is satisfied. In the cass of superlattices of type AB3 the theory of Bragg and Williams is used for simplicity. It is shown that when the composition varies, the maximum of the critical temperature may occur at any desired composition by a suitables adjustment of the coefficients in the assumed functions. There is thus a hope of removing the discrepancy between theory and experiment on this line. The anomalous specific heat at the critical temperature is also calculated for different compositions. In the case of the AB type of superlattices, Bethe's formula for the energy is no longer valid, and in order to calculate the specific heat, an approximate formula for the energy is obtained by analogy with the theory of Bragg and Williams. Finally, the problem of separation into more than one phase is briefly discussed.

在二元合金超格之统计力学理论中,原子间互作用能量,因原子之排列不同而异,其所生之影响,吾人擬於此篇中讨论之。吾人认为有Bethe氏理论中之相互作用能量,实为一平均值,其值因合金之秩序程度及其成分而异。吾人作二简单假设:一设相互作用能量为秩序及成分之线性函数,另一设其与原子对偶之数成线性函数。将此等假设应用於AB类之合金,则必须在所设函数中之系数间,有适当关系,合金之临界温度,始在成分为1:1时,有极大值。在AB_3类之合金,吾人乃应用Bragg及Williams二氏之理论以求简便。於此可证明若所设函数中之系数,可任意调整则所计算出之临界温度之极大值可在任何成分发生。故关於此点理论与实验不合之处,可望解决。又合金之反常比热,亦经算出。在AB类之合金,Bethe氏原来之能量公式不復可用,故另用与Bragg及Williams理论比较而得之公式计算。又关於合金可分为二相或多相之问题,此篇亦大略论及。

Wang's theory for determining the approximate configurational partition function of the adsorbed layer is modified in two different ways. One is to assume that the configurational energy should be corrected: the other to advocate that the deficiency due to a wrong expression for the a priori probability of the. central site is more significant.The configurational partition function is evaluated is both methods and the adsorptipn isotherin and the beat of adsorption computed for the case of quadratic lattice...

Wang's theory for determining the approximate configurational partition function of the adsorbed layer is modified in two different ways. One is to assume that the configurational energy should be corrected: the other to advocate that the deficiency due to a wrong expression for the a priori probability of the. central site is more significant.The configurational partition function is evaluated is both methods and the adsorptipn isotherin and the beat of adsorption computed for the case of quadratic lattice With dipole interaction. values for the last two quantities when a uniform continuous distribution of the distant adsorbed particles is assumed are further given for comparison. The second method, which surpasses the first, is compared with Kirkwood's method. in the case of hexagonal lattice with neighbour interaction. Numerical work is also carried out in this case.

本文就王竹溪先生之理论用两种不同方法加以改良。一种为改变能量公式,另一种为改变中心格点之或然率。用此二法皆可求得近似配分函数。所得关於方格在偶极作用情形下之粘附等温曲线及粘附热之数值用图比较之,并与旧日平均连续分布之理论比较。本文所用之第二法实较第一法为佳,故应用之以讨论一三角格在相邻作用情形下之粘附现象,且应用Kirkwood理论以为比较。数值结果亦有图表之。

The single-electron wave function of the ground state of the helium atom is obtained from Hylleraas' well-known wave function by integrating the latter over the coordinates of one electron. The energy of the ground state calculated with this one-eleetron wave function is -5.717Rh. compared with the value -5.755 given by the seif-consistant field solution.

将Hylleraas 氏之著名波动函数对一个电子之各座标积分之,吾人求得正常状态氦单一电子之波动函子。由此单一电子波动函数所求得之正常状态能量为-5.717h较自身一致场的解法所求得之值-5.755Rh为大。

 
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