天线罩使跟踪天线的极图产生了角位移。
The radome causes an angular displacement of the tracking aerial polar diagram.
天线罩使跟踪天线的极图产生了角位移。
The radome causes an angular displacement of the tracking aerial polar diagram .
定理20是极图构造更详细的研究的基础。
Theorem 20 is the basis of a rather detailed study of the structure of extremal graphs.
本文讨论了图论中的极图理论问题，给出了极图理论的几点结论。
The paper discusses the extreme picture in the theory of picture. It provides a lot ofconclusions about the theory of the extreme.
用元极图理论剖析化学领域中有关宇宙起源、原子结构、化学亲和力及催化反应等理论问题。
In the field of chemistry, the origin of universe, the structure of an atom, chemical affinity and catalytic reaction etc. are discussed and analysed by Yuanji theory.
摘要：对不同拉拔变形程度及不同温度退火后的钽丝织构，借助极图与现代ODF分析术进行了研究。
The cold drawing textures of the tantalum wires for different reductions in area and their recrystallization textures at different temperatures were investigated by pole figures and ODF.
研究表明，增加极图数目有利于缩小极图测量范围，同时极图测量范围缩小的方式也应与板材织构类型相关。
It is shown that measured area of pole figures could be reduced with increasing pole figure number, and the way how the …
本文研究与网络题有关的一些极图，得出的主要结果有：五个关于没有三角形的极大图的定理，以及它们的三个推论。
In this. paper, some extreme graphs relative to network problems are studied. The main results include five theorems on maximum graphs without triangles and their three corollaries.
研究了单圈图、双圈图的反比度，给出了它们的上下界并得到达到最大最小值的极图，还进一步给出多圈图的上下界的一个猜想。
In this paper, inverse degree of unicyclic graphs and bicyclic graphs is discussed, and the extremal graphs that reach the upper and lower bounds are given.
您应当有一种似曾相识的感觉，因为它看上去极像图2的屏幕。
You should be treated to a bit of deja vu, because it looks just like the screen in Figure 2.
德国波茨坦研究所（Potsdam Institute）的波图霍夫•弗拉基米尔（Vladimir Petoukhov）说，海上浮冰的退缩产生的影响“能够使欧洲和亚洲北部极寒气候的可能性增大两倍。”
Vladimir Petoukhov of the Potsdam Institute says that the effects of shrinking sea ice "could triple the probability of cold winter extremes in Europe and northern Asia".
图2 - 24示出静电计或皮安计的过载保护电路，其中包括一个电阻器和两个二极管(1n3595)。
Figure 2-24 shows a protection circuit for an electrometer ammeter or picoammeter, consisting of a resistor and two diodes (1n3595).
这个波形可以被看作是下列原理的叠加(图22和平台5)。全部这些波形的叠加整合结果变成图21所示的典型漏极电流。
This waveform can be presented as a superposition of the following elements (Fig. 22 and Tab. 5). The superposition of all these elements results in a typical drain current shown in Fig. 21.
图。1所示的是由两个平行解理面和二个锯出的(粗糙)侧面组成的激光二极管的管芯。
Figure I. 1 shows a basic laser diode chip which consists of two cleaved parallel facets and two sawed (roughened) sides.
把这些原理按时序整合呈现出图16所示的典型漏源极电压。
The superposition of all these elements results in a typical drain-source voltage shown in Fig. 16.
硬开关(图26所示)几乎不考虑漏源极电压的最小值。
The hard switching approach (as shown in Fig. 26) doesn't consider the minimum drain-source voltage.
文章介绍了建立在SGI图象图形工作站上的发光二极管形状识别系统的系统配置、识别原理、检测步骤、技术难点和解决方案。
The paper introduces system configuration, recognition principle, detection procedure, key technology and solutions of LED shape recognition system established on the SGI workstation.
图20描述了漏源极电压主要原理产生的电磁干扰频谱。
The spectra of the main elements of the drain-source voltage can be found in Fig. 20.
这个磁通值可以容易地从图5中永磁极的磁密和铁极磁密之间的差值和气隙面积求出。
The value of this flux can easily be deduced from the difference between flux densities at magnet poles and core poles shown in Fig. 5, and the gap area.
漏源极电压（图28）在反射过程结束后并减小到100伏特时场效应晶体管导通。
The drain-source voltage (Fig. 28) starts oscillating at the end of the flyback phase and reaching the minimum of 100V when the MOSFET turns on.
本文叙述了用信号流图来分析含有零极子的有源网络的方法。
This paper describes the method of analysis of active circuits including nullors with signal flow graph.
采用晶面的极射赤面投影方法，从理论上绘制了一套不同立方晶体的理论电子通道图。
A set of ideal ECP maps for different cubic crystals was theoretically delineated by using the sterographical projection method of crystal planes.
本文介绍了一种用于网络设计的半圆极零图法。
This article introduces the semicircle polar-zero diagram method used for the network design.
采用激光全息干涉测量技术测量了轴对称型大功率晶体三极管温度场的全息干涉图；
The holographic interferogram of the temperature field for an axisymmetrical high power semiconductor triode has been obtained by using laser holographic interferometric measurement.
运用上述模型、公式模拟了心室除极过程的心电向量图。
Finally, simulated vectorcardiogram of the ventricular depolarization is given through applying the model and expression mentioned above.
运用上述模型、公式模拟了心室除极过程的心电向量图。
Finally, simulated vectorcardiogram of the ventricular depolarization is given through applying the model and expression mentioned above.
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