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61.
This paper describes a method for analysing inviscid transonic flow. This method is based on the fact that the angle made
by the streamline of the transonic flow and of the corresponding incompressible flow is usually small. By using curvilinear
coordinates, the differential equation of the stream function of an inviscid compressible flow is simplified and a general
solution of the equation obtained.
As examples of the method, transonic solutions are given for flow through twodimensional and axisymmetric Laval nozzles of
different throat wall radii together with sonic lines and iso-Mach lines. To determine the discharge coefficients of Laval
nozzles, an integral relation is developed. The general behaviour of the transonic flow in the throat region is presented,
and the effect of the mass discharge on the Mach number distribution in the nozzle analysed. The effects of the ratio of the
specific heats on the characteristics of the flow in the throat region are discussed. For transonic flow around a circular
cylinder and a sphere, sonic lines and iso-Mach lines are presented for free-stream Mach number varying from the subcritical
to the supercritical, including a free-stream Mach number of one.
Part of the results obtained are compared with those available in current literature. For the two-dimensional hyperbolic Laval
nozzles, the iso-Mach lines are compared with those given by Cherry (1959) and Serra (1972). For, axisymmetric Laval nozzles,
the discharge coefficient and the Mach number at the throatsection for various throat wall radii are compared with those given
by Sauer (1944), Hall (1962), Kliegel & Levine (1969), and Klopfer & Holt (1975). The theoretical discharge coefficients are
compared with the experimental results by Backet al (1975), Durham (1955), Norton & Shelton (1969) etc. For the transonic flow around a circular cylinder, the iso-Mach lines
are compared with Cherry’s exact solution for the quasi-circular cylinder for.M∞ equal to 0.51. The. Mach number distributions on the surface of the circular cylinder are compared with those given by Imai
(1941) forM∞ equal to 0.4, by Cherry (1947) forM∞ equal to 0.51, by Dorodnicyn (1956) forM∞ equal to 1, and by Hafez, South & Murman (1979) forM∞ equal to 0.51.
The present method has a much wider scope of application, requires simpler computation and gives results with good accuracy.
It is being used to analyse supercritical wings and cascades, and we expect to extend its application to the field of transonic
unsteady flow. 相似文献
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Aidan Leach Rana Sabouni Franco Berruti Cedric Briens 《American Institute of Chemical Engineers》2013,59(3):719-728
Gas‐atomized liquid injections into fluidized beds are commonly used in industrial processes such as fluid coking, fluid catalytic cracking (FCC), and pharmaceutical granulation, where it is important to optimize the distribution of the injected liquid to prevent the formation of unwanted liquid–solid agglomerates and maximize product yields. This injection is typically a two‐phase, gas‐atomized liquid injection. One issue with such a liquid injection is that most of the liquid is deposited at the end of the jet tip within the reactor. This study proposes introducing artificial fluctuations into the injection flow, which causes the jet penetration to vary, allowing for a more even spread of liquid throughout a fluidized bed reactor. The effect of artificial pulsations in the atomized injection, of various frequency and amplitude, was investigated in this study. Using pulsations, greatly enhanced the liquid distribution on the bed particles. © 2012 American Institute of Chemical Engineers AIChE J, 59: 719–728, 2013 相似文献
64.
液体雾化在工业生产过程中应用非常普遍,雾化质量的好坏,直接影响燃油的燃烧过程.本文介绍了雾化的机理,分析了影响雾化油滴粒径的主要因素,给出了影响雾化质量的评价指标. 相似文献
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湛江发电厂3号汽轮机汽流激振分析及处理 总被引:1,自引:0,他引:1
对湛江发电厂3号汽轮机汽流激振的机理进行简要分析,并根据3号机组汽流激振的特点提出了消除与预防对策。 相似文献
69.
“田”字型双级双向热底冷盖熔铝炉 总被引:1,自引:1,他引:0
介绍一种与地方铝厂技术水平,生产规模,产品结构相适应原新型铝炉。该炉是将中,小型企业无法操作使用的巨型熔铝炉分解成两组双级,双向炉,采用冷炉盖,热底连体结构,与普通单炉相比可减少16个散热面;采用炉料预热罩强制烟气循环预热炉可节省40%以上。 相似文献
70.