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971.
Let K m,nbe a complete bipartite graph with two partite sets having m and n vertices, respectively. A K p,q-factorization of K m,n is a set of edge-disjoint K p,q-factors of K m,n which partition the set of edges of K m,n. When p = 1 and q is a prime number, Wang, in his paper “On K 1,k -factorizations of a complete bipartite graph” (Discrete Math, 1994, 126: 359—364), investigated the K 1,q -factorization of K m,nand gave a sufficient condition for such a factorization to exist. In the paper “K 1,k -factorizations of complete bipartite graphs” (Discrete Math, 2002, 259: 301—306), Du and Wang extended Wang’s result to the case that q is any positive integer. In this paper, we give a sufficient condition for K m,n to have a K p,q-factorization. As a special case, it is shown that the Martin’s BAC conjecture is true when p : q = k : (k+ 1) for any positive integer k.  相似文献   
972.
In this paper a theory of modal analysis for the dynamic response of fluid-structure systems is presented. A pair of generalized eigenvalue equations with three real symmetric matrices and their relationships are derived from the finite element equations in the form of structural displacements and fluid velocity potential. Generalized orthogonality relations of modal vectors are then developed. The response of the system to external excitation is derived in closed form by modal expansion. Two examples of the solution are given for illustration.  相似文献   
973.
When a focused Gaussian ultrasonic beam in soft tissue normally impinges on the boundary of a contiguous bone, reflection and transmission occur. Taking account of the reflection, the steady-state temperature elevation along the beam axis for this case was calculated. The effect of perfusion is also included.  相似文献   
974.
975.
The single 110 K phase Bi(Pb)–Sr–Ca–Cu–O superconductor was made by sintering in air. Its zero-resistance temperature is 106 K, and it is an orthorhombic cell witha=5.403 Å,b=5.412 Å andc=37.062 Å. It formed around the low-T c phase. The forming period of the 110 K phase can be shortened by multiple sintering and grinding. If PbO is mixed into the samples after the 85 K phase has formed, the forming rate of the 110 K phase can be increased significantly. EDAX analysis of grain composition confirms that the Pb atoms enter the unit cell, and probably Pb cations replace some Ca cations.  相似文献   
976.
二元光学反/衍混合Schmidt望远系统光学设计   总被引:4,自引:2,他引:2  
针对空间光学系统轻型的特点,采用衍射光学元件取代Schmidt校正板来校正系统像差,设计了一个二元光学反/衍混合Schmidt望远系统。光学系统的通光孔径为=200mm,相对孔径F/#=1.9,波长λ=4.3μm,视场2ω=10°。光学设计采用OSLOsix软件。光学设计结果:空间频率ν≤60cycles/mm时,调制传递函数MTF≥0.4。  相似文献   
977.
978.
电镜样品的激光镀膜技术   总被引:1,自引:0,他引:1  
非导电的样品用扫描电镜进行观测时需要对样品进行镀膜处理以获得清晰的图像, 本文介绍应用脉冲激光沉积(PLD)技术对非导电样品的表面进行镀膜处理的方法和实验装置及实验结果.  相似文献   
979.
A novel method, based on the coupling of ionic liquid-based headspace single-drop microextraction (SDME) with gas chromatography (GC), is developed for the determination of chlorobenzene derivatives. For the SDME of five chlorobenzene derivatives, a 1.0 μL 1-octyl-3-methylimidazolium hexafluorophosphate microdrop is exposed for 20 min to the headspace of a 15 ml aqueous sample containing 20% (w/v) NaCl placed in 25 ml vial at 40 °C. Then, the extractant is directly injected into the injector block of the GC instrument. To avoid ionic liquid leaking into the chromatographic column, a small glass tube is placed in the injection block. Under optimized operation conditions, linear relation between peak areas and analyte concentrations up to 1.5 mg L?1 has been obtained The detection limits range from 0.1 to 0.5 μg L?1 for the various analytes. The relative standard deviations at 1.0 μg L?1 range from 7.7 to 12.4%, and the enrichment factors from 41 to 127. The method is simple and sensitive, and does not suffer from the influence of a solvent peak. Its applicability is demonstrated by the determination of chlorobenzenes in wastewater samples.  相似文献   
980.
Radiance coming from the interior of an uncooled infrared camera has a significant effect on the measured value of the temperature of the object. This paper presents a three-phase compensation scheme for coping with this effect. The first phase acquires the calibration data and forms the calibration function by least square fitting. Likewise, the second phase obtains the compensation data and builds the compensation function by fitting. With the aid of these functions, the third phase determines the temperature of the object in concern from any given ambient temperature. It is known that acquiring the compensation data of a camera is very time-consuming. For the purpose of getting the compensation data at a reasonable time cost, we propose a transplantable scheme. The idea of this scheme is to calculate the ratio between the central pixel’s responsivity of the child camera to the radiance from the interior and that of the mother camera, followed by determining the compensation data of the child camera using this ratio and the compensation data of the mother camera Experimental results show that either of the child camera and the mother camera can measure the temperature of the object with an error of no more than 2°C.  相似文献   
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