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991.
992.
Highly birefringent dual-core photonic crystal fibers (PCFs) can be used as a polarization splitter because the orthogonal polarization modes with dissimilar coupling lengths are easily separated from each other. Different from the traditional methods achieving high birefringence, a new highly birefringent hybrid PCF that guides light by both index guiding and bandgap guiding is proposed. Firstly, a novel polarization splitter based on this kind of dual-core hybrid PCF is designed. The transmission modes, coupling lengths for the two orthogonal polarizations and performance of the proposed polarization splitter are investigated and numerically analyzed. The results demonstrate that it is possible to obtain a 4.72-mm-long polarization splitter. The splitting ratio is better than −20 dB in a large wavelength range of 1.53-1.72 μm. Its bandwidth is about 190 nm. 相似文献
993.
A multi-mode opto-thermo-mechanical stretching system was modified to study the changes in the 3D of optical and structural properties of stretched fibre along its axis. The structural deformation of isotactic Polypropylene, (iPP), fibres was studied at different draw ratios. The modified system coupled with Pluta polarising interference microscope was used to determine the variation of the birefringence in three dimensions during stretching process. Using this modified system, the multi-necking was detected. Subfringe analysis technique was used to determine the phase distribution of the obtained microinterferograms, which were given for illustration. 相似文献
994.
In the problems of large deflection of clamped circular plates under uniformly distributed loads, various perturbation parameters
relating to load, deflection, slope of deflection, membrane force, etc, are studied. For a general perturbation parameter,
the variational principle is used for the solution of such a problem. The applicable range of these perturbation parameters
are studied in detail. In the case of uniformly loaded plate, perturbation parameter relating to central deflection seems
to be the best among all others. The method of determination of perturbation solution by means of variational principle can
be used to treat a variety of problems, including the large deflection problems under combine loads.
This paper is completed under the guidance of Prof. Chien Wei-zang. 相似文献
995.
Constitutive theories for nonlocal micropolar continua with implicity and with multiple interactions
戴天民 《应用数学和力学(英文版)》1981,2(4):375-382
In this paper the constitutive theory for nonlocal micropolar continua which was proposed by A. C. Eringen is extended to the cases for nonlocal micropolar continua with implicity and with multiple interactions. Here nonlocal micropolar thermoelastic solids with implicity and with multiple interactions are cited as instances to illustrate the procedure for the establishment of their constitutive theories as well as two relevant theorems concerning the constitutive theories for those solids are given. 相似文献
996.
Summary Compared to the similar pressure-distribution cone-and-plate apparatus of Adams and Lodge (4), the new apparatus' improvements include: temperature control of the cone (as well as the plate); increased stiffening of the frame; four (not three) pressuremeasuring holes in the cone/plate region; inclusion of a pressure-measuring hole on the axis under the cone truncation; exclusive use of a vertical free liquid boundary at the cone rim (without a sea of liquid). Temperature control of the rotating cone and of the fixed plate leads to acceptable temperature uniformity in the test liquid for working temperatures within 10°C or 20°C of ambient; the corresponding interval is about 1°C if the cone temperature control is abandoned. Pressure gradients measured using a Newtonian liquid agree with those calculated using Walters' eq. (3). For a viscoelastic liquid, after subtracting inertial contributions, pressure distributions measured at a given shear rate in the cone/plate region do not change when the gap angle is changed from 2° to 3°, showing that the effects of secondary flow are negligible. Values ofN
3 =N
1 + 2N
2 obtained from the gradients of these distributions are believed to be in error by not more than ±1 Pa, in favorable cases. The present most useful ranges are: 10 to 5000 Pa forN
3; 0.1 to 200 sec–1 for shear rate; up to 5 Pa s for viscosity; and 5 to 40°C for temperature. As an application, it is shown that adding 0.1% of a high molecular weight polyisobutylene to a 2% polyisobutylene solution doublesN
3 and has no detectable effect on the viscosity measured at low shear rates with a Ferranti-Shirley viscometer.
udsf unidirectional shear flow - TCP truncated-cone and plate - N 1,N 2 1st and 2nd normal stress differences in udsf - N 3 N 1 + 2N 2 - : = A is defined by the equationA := B - P * hole pressurePw – Pm; Pw, Pm = pressures measured by flush transducer and by hole-mounted transducer - t time - , strain rate, shear rate - (P,t) covariant body metric tensor at particleP and timet - i , i covariant and contravariant udsf body base vectors (i = 1, 2, 3) - –1 inverse of - R, plate radius, cone/plate gap angle - r 0,h 0 radius and height of cone truncation - r,, spherical polar coordinates; cone axis = 0; plate surface = /2 - physical components of stress; for a tensile component - cone angular velocity - p on the plate = /2 - ,T, density, absolute temperature, viscosity - P 0.15 2(r 2 –R 2) (inertial contribution) [2.7] - P ve contribution [2.8] from flow perturbations of viscoelastic origin - r i i = 1,2,3,4; values ofr at centers of holes in cone/plate region - P i () pressure change recorded by transducerTi when cone angular velocity goes from zero to - 1/2 {P i ()+ P i (–)} (average for 2 senses of rotation) - rim pressure, from least-squares line through four points - Re Reynolds' number:R 2/ - (P,t)/t With 11 figures and 2 tables 相似文献
Zusammenfassung Im Vergleich zu dem ähnlichen Kegel-Platte-Gerät von Adams und Lodge (4) zur Messung der Druckverteilung wurden an dem neuen Gerät die folgenden Verbesserungen vorgenommen: Temperaturregelung an Kegel und Platte, Versteifung des Rahmens, vier (anstatt drei) Druckmeßlöcher im Kegel-Platte-Bereich, ein zusätzliches Druckmeßloch auf der Achse unter der Kegelstumpf-Deckfläche, ausschließliche Verwendung einer vertikalen freien Grenzfläche der Flüssigkeit am Kegelrand (ohne umgebenden Flüssigkeitssee). Die Temperaturregelung des rotierenden Kegels und der festen Platte führt zu einer ausreichenden Temperaturgleichförmigkeit in der Testflüssigkeit für Betriebstemperaturen, die höchstens um 10–20°C von der Umgebungstemperatur abweichen. Dieses Intervall beträgt dagegen nur etwa 1°C, wenn auf die Temperaturregelung am Kegel verzichtet wird. Für newtonsche Flüssigkeiten entsprechen die gemessenen Druckgradienten den mittels der Gleichung von Walters (3) berechneten. Für viskoelastische Flüssigkeiten zeigen sich bei der Änderung des Spaltwinkels von 2° auf 3° nach Abzug der Trägheitsbeiträge keine Änderungen der bei einer bestimmten Schergeschwindigkeit gemessenen Druckverteilung. Dies zeigt, daß Sekundärströmungseffekte vernachlässigbar sind. Es darf angenommen werden, daß die Werte vonN 3 =N 1 + 2N 2, die man aus den Gradienten dieser Verteilungen erhält, unter günstigen Umständen mit einem Fehler von nicht mehr als ±1 Pa behaftet sind. Gegenwärtig liegen die günstigsten Bereiche bei 10 bis 5000 Pa fürN 3, 0,1 bis 200 s–1 für die Schergeschwindigkeit, unterhalb von 5 Pa s für die Viskosität und 5 bis 40°C für die Temperatur. Als Anwendung wird gezeigt, daß ein Zusatz von 0,1% hochmolekularen Polyisobutylens zu einer 2%igen Polyisobutylenlösung den Wert vonN 3 verdoppelt, aber keinen erkennbaren Einfluß auf die (bei geringen Schergeschwindigkeiten mit einem Ferranti-Shirley-Viskosimeter gemessen) Viskosität hat.
udsf unidirectional shear flow - TCP truncated-cone and plate - N 1,N 2 1st and 2nd normal stress differences in udsf - N 3 N 1 + 2N 2 - : = A is defined by the equationA := B - P * hole pressurePw – Pm; Pw, Pm = pressures measured by flush transducer and by hole-mounted transducer - t time - , strain rate, shear rate - (P,t) covariant body metric tensor at particleP and timet - i , i covariant and contravariant udsf body base vectors (i = 1, 2, 3) - –1 inverse of - R, plate radius, cone/plate gap angle - r 0,h 0 radius and height of cone truncation - r,, spherical polar coordinates; cone axis = 0; plate surface = /2 - physical components of stress; for a tensile component - cone angular velocity - p on the plate = /2 - ,T, density, absolute temperature, viscosity - P 0.15 2(r 2 –R 2) (inertial contribution) [2.7] - P ve contribution [2.8] from flow perturbations of viscoelastic origin - r i i = 1,2,3,4; values ofr at centers of holes in cone/plate region - P i () pressure change recorded by transducerTi when cone angular velocity goes from zero to - 1/2 {P i ()+ P i (–)} (average for 2 senses of rotation) - rim pressure, from least-squares line through four points - Re Reynolds' number:R 2/ - (P,t)/t With 11 figures and 2 tables 相似文献
997.
钱伟长 《应用数学和力学(英文版)》1985,6(1):25-39
In this paper, the generalizd variational principles of plate bending, froblems are established from their minimum potential energy principle and minimum complementary energy principle through the elimination of their constraints by means of the method of Lagrange multipliers. The involutory transformations are also introduced in order to reduce the order of differentiations for the variables in the variation. Funhermore, these involutory transformations become infacl the additional constraints in the varialion. and additional Lagrange multipliers may be used in order to remove these additional constraints. Thus, various multi-variable variational principles are obtained for the plate bending problems. However, it is observed that. nol all the constrainls ofva’iaticn can be removed simply by the ordinary method of linear Lagrange multipliers. In such cases, the method of high-order Lagrange multipliers are usedto remove iliose constrainls left over by ordinary linear multiplier method. And consequently. some funct ionals of more general forms are oblained for the generaleed variational principles of plate bending problems. 相似文献
998.
999.
本文在SAND迭代法的基础上,采取带有周期性光滑化的限幅迭代方法,求解激光核聚变中的X光能谱取得了较好的结果。这个方法适用于根据亚千X射线谱仪、多道k边滤波谱仪和多道滤波-荧光谱仪的测量结果回推靶等离子体的X射线能谱。计算结果表明,该方法完全抑制了数值不稳定性,消除了非物理的“负能谱”现象和解谱结果中的数值结构。特别是该方法对初始试探谱有很强的适应性,解谱计算结果与初始试探谱无关。 相似文献
1000.