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sections     
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  切片
     The Stability of the Streaks of Frozen Sections in Photoelastic Mechanics
     三维光测弹性力学中冻结切片条纹的稳定性
短句来源
     PLASTIC SEMITHIN SECTIONS FOR LIGHT MICROSCOPE STUDY
     用于光学显微镜研究的塑料半薄切片
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     THE METHODOLOGICAL STUDY ON RADIOLIGAND BINDING ASSAY OF β-ADRENERGIC RECEPTORS WITH RAT BRAIN SECTIONS
     用大鼠脑切片进行β—受体放射配体结合实验的方法学研究
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     THE STUDY OF IMMUNOENZYMATIC TECHNIQUE FOR THE DIAGNOSIS OF SCHISTOSOMIASIS JAPONICA USING LIVER SECTIONS OF INFECTED MICE
     感染鼠肝石蜡切片免疫酶染色法诊断血吸虫病的研究
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     Studies of in situ Hybridization in Routine Paraffin Embedded Liver Tissue Sections with Biotinylated HBV DNA Probes. Localization and Morphology of HBV DNA in Various Types of Liver Diseases
     生物素标记HBV DNA探针在肝石蜡切片上作原位杂交技术的研究——各型肝病时HBV DNA的定位及形态
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  截面
     Measurement of the Thermal Neutron Cross Sections of the Reaction of ~(126)Sn(n,γ)~(127)Sn~g, ~(127)Sn~m
     长寿命裂变产物核素~(126)Sn(n,γ)~(127)Sn~g,~(127)Sn~m反应热中子截面测量和研究
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     CALCULATION OF CRACK RESISTIVITY IN OBLIQUE SECTIONS OF PARTIALLY PRESTRESSED CONCRETE BEAMS
     部分预应力混凝土梁斜截面抗裂度计算
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     The Calculation of the Warping Coordinates of Thin-walled Mixed Sections
     开口和闭口混合薄壁截面翘曲座标的计算
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     Finite Element Analysis on the Rigid-frame with Variable Sections
     变截面刚架的有限元分析
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     DIRECT DETERMINATION OF THE COMPLETE FUSION CROSS SECTIONS FROM THE FISSION FRAGMENT ANGULAR DISTRIBUTION
     由裂变碎片角分布直接确定全熔合截面σ_(fu)
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     Formulae for Transmission Phase Shift and Cut-off Attenuation of Square and Circular Conic Waveguide Sections
     方锥、圆锥波导的传输相移和截止衰减的公式
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     A Design Method for to Realize Approximate Straight Line Sections of Link Courve by Four-bar Linkage
     铰链四杆机构实现连杆曲线近似直线的一种设计方法
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     A Study of the Speech Synthesis by MPLPC in Standard Chinese Based on Keeping the Information in the Transient Sections
     保留过渡信息的MPLPC汉语语音合成方法研究
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     EXPERIMENTAL STUDY OF WIND RESISTANT STABILITY OF PROPOSED MAYU CABLESTAYED BRIDGE FROM ITS DECK SECTIONS
     汕头妈屿跨海大桥(设计方案)节模型抗风稳定性的实验研究
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     Explosive Clad of Ta-10W Liner Tube and Steel Tubular Sections
     Ta—10W衬管与钢管的爆炸复合
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  剖面
     PARTIAL PHASE DIAGRAM OF Fe-Si (≤8wt-%)-C(≤0.1wt-%) AND PSEUDOBINARY SECTIONS OF Fe-Si AND Fe-C
     Fe-Si(≤8wt-%)-C(≤0.1wt-%)局部三元相图和等硅与等碳赝二元剖面
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     4. Analysis on its kinematics features and equilibrium profiles shows the shortening range of the profiles across four different sections of this fault zone is 8.54km, 17.5km, 11.4km&13km, 2.3km, the shortening rate is 19.1%, 34.3%, 24.8%&21.8%, 7.9%.
     4.断裂带运动学与平衡剖面分析揭示:四个区段变形后地层的变形缩短量分别为8.54Km、17.5km、11.4km-13km、2.3km,变形缩短率为19.1%、34.3%、24.8%-21.8%、7.9%;
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     PHASE DIAGRAM OF Nd-Fe-B TERNARY SYSTEM II. TWO VERTICAL SECTIONS WITH CONSTANT Nd AND B RESPECTIVELY, PASSING THROUGH Nd_2Fe_(14)B POINT
     Nd-Fe-B三元系相图的研究 Ⅱ.过Nd_2Fe_(14)B点的等硼和等Nd垂直剖面相图
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     I select several typical seismic sections(ht96180-l, ht96222, ht96568, ht96536, ht96520) to analyze seismostratigraphy.
     选择了ht96180-1,ht96222,ht96568,ht96536,ht96520几条典型的地震剖面做地震地层学研究。
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     A research of stable isotopic composition of carbonates from both standard sections of the Cambrian located at Zhangxia, Shandong Province and those of the Ordovician at Tangshan, Hebei Province, both in North China, shows that the δ18O values range from -10. 6‰ to -4. 8‰ and the δ13C values, between -5. 8‰ and + 1. 6‰ in the Cambrian;
     渤海湾地区寒武系标准剖面(山东张夏剖面)海相碳酸盐岩氧同位素δ~(18)O值分布区间为-10.6‰~-4.8‰,碳同位素的δ~(13)C值为-5.8‰~+1.6‰;
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  sections
In particular, we give a detailed description of these sets in terms of cross-sections inside maximal R-tori ofH.
      
For a classical semisimple Lie algebra, we construct equivariant line bundles whose global sections afford representations with a nilpotentp-character.
      
The main part of the work deals with abstract Higgs bundles; in the last two sections we derive the applications to Higgs bundles valued in a line bundle K and to bundles on elliptic fibrations.
      
Morse Theory and Euler Characteristic of Sections of Spherical Varieties
      
We give a representation-theoretic interpretation of this number as the exponent of growth for multiplicities of simple G-modules in the spaces of sections of homogeneous line bundles on G/H.
      
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Formulas are derived for the solution of the transient currents of dissipative low-pass T-type electric wave filters. Oscillograms taken by cathode ray oscillograph for d-c. and a-c. cases are found to agree with results calculated from these formulas. From these calculations, the following conclusions are derived. When terminating resistance is gradually increased from O, the damping constants of the sine terms begin to differ from each other, ranging in decreasing magnitude from term of the lowest frequency...

Formulas are derived for the solution of the transient currents of dissipative low-pass T-type electric wave filters. Oscillograms taken by cathode ray oscillograph for d-c. and a-c. cases are found to agree with results calculated from these formulas. From these calculations, the following conclusions are derived. When terminating resistance is gradually increased from O, the damping constants of the sine terms begin to differ from each other, ranging in decreasing magnitude from term of the lowest frequency to the last term of cut-off frequency. Hence the transient is ultimately of the cut-off frequency. At cut-off frequency, this constant is near to but greater than R/2L. For each increase of section, there is introduced an additional sine term with smaller damping constant. Therefore transients die out faster in filters of smaller number of sections. Since transient amplitudes are of the same order of magnitude before and after cut-off, filtering property only exists in the steady states.

此篇先推求收端加电阻时,低频滤波器瞬流之公式。依此公式算出之图与用阴极光示波器映出之曲线相符合。自推算之结果,可得下列结论: (一)在滤波器收端电阻渐加时,瞬流各项之挫率渐互异,其数量由低频项至隔阻频之项顺序渐减;其最小数仍比收端无电阻时之挫率(R/2L)为大。故瞬流终必变为隔阻频之电流;而较收端无电阻时易于消减。 (二)当滤波器增加一段时,瞬流之项数亦加一。所加项之挫率皆比前有者为小。故少段滤波器之瞬流易于消减。 (三)在隔阻频後瞬流之数量与在其前者相彷恒较隔阻频後之安定数量大数十倍,故滤波之特性仅能见之于安定状态。

Formulas are derived for the solution of the transient currents of resistance-terminated dissipative π-type low-pass, T- and π-type high-pass electric wave filters. Oseillograms taken by cathode ray oscillograph for d-c. and a-c. cases are found to agree with the results calculated from these formulas. From these calculations, the following conclusions are derived: (1) When the terminating resistance is gradually increased from 0, the damping constants of the damped sine terms begin to differ greatly from each...

Formulas are derived for the solution of the transient currents of resistance-terminated dissipative π-type low-pass, T- and π-type high-pass electric wave filters. Oseillograms taken by cathode ray oscillograph for d-c. and a-c. cases are found to agree with the results calculated from these formulas. From these calculations, the following conclusions are derived: (1) When the terminating resistance is gradually increased from 0, the damping constants of the damped sine terms begin to differ greatly from each other, ranging in decreasing magnitudes from the first damped sine term to the last term of cut-off frequency. Hence the transient is ultimately of the cut-off frequency. At the cut-off frequency, this constant is greater than the corresponding constant (R/2L) when the termination is absent. (2) For each increase of one section, there is introduced an additional damped sine term with smaller damping constants. Therefore transients die out faster in filters of small no. of sections. (3) With the same network constants, the damping constants of π-type filters are greater than the corresponding values of T-type filters. As a result, transients die out faster in π-type filters. (4) The amplitudes of the transient terms in the attenuation and transmission ranges are of the same order of magnitude, and the filtering property only exists in the steady states. (5) The cut-off frequency of the π-type filters varies with the no. of sections used. When only two sections of low, or, high-pass filter are used, the variation amounts to nearly 26 per cent from the theoretical value.

此篇先推求收端加电阻时,低频与高频滤波器瞬流之公式依此公式算出之图与用阴极光示波器映出之曲线相符合。自推算之结果,可得下列结论: (一)在滤波器收端电阻渐加时,瞬流各项之挫率渐渐互异其数量,由第一挫波项至最後隔阻频项,顺序渐减;其最小数仍比收端无电阻时之挫率(约等于R/2L)为大。故瞬流终必变为隔阻频之电流,而较收端无电阻时易于消灭。 (二)当滤波器增加一段时,瞬流之项数亦加一,所加项之挫率皆比前有者为小,故少段滤波器之瞬流易于消灭。 (三)在π式滤波器中,其瞬流各项之挫率恒较同一电恒数T式滤波器中之相当项之挫率为大故在π式滤波器中,瞬流消灭较易。 (四)在隔阻频后瞬流之数量与在其前者相彷,恒较隔阻频后之安定数量大数十倍,故滤波器之特性仅能见之于安定状态之下。 (五)π式滤波器之隔阻电频随所用之段数而变化在二段之滤波器中,此变化数为最高,其数与理想之数相差百分之二十六。

Formulas are derived for the solution of the transient currents of resistance-terminated dissipative T-& π-type band-pass electric wave filters of the constant X type. Oscillagrams taken hy cathode ray oscillograph for d-c. & a-c. cases are found to agree with the calculated results. From these calculations, the following conclusions are derived: (1) No matter what the impressed frequencies are, the transient is ultimately of the lower cut-off frequency. (2) The receiving-end indicial admittance consists of...

Formulas are derived for the solution of the transient currents of resistance-terminated dissipative T-& π-type band-pass electric wave filters of the constant X type. Oscillagrams taken hy cathode ray oscillograph for d-c. & a-c. cases are found to agree with the calculated results. From these calculations, the following conclusions are derived: (1) No matter what the impressed frequencies are, the transient is ultimately of the lower cut-off frequency. (2) The receiving-end indicial admittance consists of transient terms symmetrical with respect to the mid-frequency term. (3) The transients die out faster in the filters of smaller number of sections. (4) With the same network constants, the transients die out faster in the t-type filters. (5) Filtering property only exists in the steady state. (6) The band width increases with the number of sections. This increase is greater in π-type filters, but the band width is greater in T-type filters.

此篇先推求收端加电阻时,频带滤波器瞬流之公式依此公式算出之图与用阴极光示波器映出之曲线相符合自推算之秸果可得下列结论: (一)在滤波器收端加电阻时,瞬流终必变为低隔阻频之电流,而较收端无电阻时易于消滅。 (二)收端直瞬流之各项均对称於中频项。 (三)在段数较少之滤波器中瞬流易于消滅。 (四)在π式滤波器中,瞬流消滅较在T式中为易。 (五)滤波器之特性仅能见於安定状态之下。 (六)滤波器之带宽随所用之段数而增加。

 
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