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Artykuły w czasopismach na temat "Reentrant Cavity"

1

Migliuolo, M., and T. G. Castner. "Novel tunable reentrant microwave cavity." Review of Scientific Instruments 59, no. 2 (1988): 388–90. http://dx.doi.org/10.1063/1.1140216.

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Paoloni, Claudio. "Periodically Allocated Reentrant Cavity Klystron." IEEE Transactions on Electron Devices 61, no. 6 (2014): 1687–91. http://dx.doi.org/10.1109/ted.2014.2301813.

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Uhlman, James S. "A Note on the Development of a Nonlinear Axisymmetric Reentrant Jet Cavitation Model." Journal of Ship Research 50, no. 03 (2006): 259–67. http://dx.doi.org/10.5957/jsr.2006.50.3.259.

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The boundary integral method is formulated for the problem of the fully nonlinear, axisymmetric potential flow past a body of revolution. A model is devised for the exact formulation of the reentrant jet cavity closure condition. It is demonstrated that the solution obtained is essentially independent of the length selected for the jet. Results obtained using the reentrant jet cavity closure model are compared with those obtained using the Riabouchinsky-type cavity closure model used by Uhlman (1987, 1989) and with experimental results. The agreement between the two cavity closure models is seen to be excellent, with the Riabouchinsky wall results deviating only slightly at short cavity lengths. The agreement of the reentrant jet model with the experimental data is also excellent, although the addition of the viscous component of drag is seen to be required for cavitating cones of sufficiently small half-angle.
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4

Sheng-Lung Huang, Ying-Hui Chen, Pi-Ling Huang, Jui-Yun Yi, and Huy-Zu Cheng. "Multi-reentrant nonplanar ring laser cavity." IEEE Journal of Quantum Electronics 38, no. 10 (2002): 1301–8. http://dx.doi.org/10.1109/jqe.2002.802955.

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Carvalho, N. C., Y. Fan, J.-M. Le Floch, and M. E. Tobar. "Piezoelectric voltage coupled reentrant cavity resonator." Review of Scientific Instruments 85, no. 10 (2014): 104705. http://dx.doi.org/10.1063/1.4897482.

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Tiwari, Ashish Kumar, and P. R. Hannurkar. "Electromagnetic Analysis of Reentrant Klystron Cavity." Journal of Infrared, Millimeter, and Terahertz Waves 31, no. 10 (2010): 1221–24. http://dx.doi.org/10.1007/s10762-010-9701-5.

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Bansiwal, Ashok, Sushil Raina, K. J. Vinoy, and Subrata Kumar Datta. "Effect of Beam tunnels on Resonant Frequency of Cylindrical Reentrant Cavity." Defence Science Journal 71, no. 03 (2021): 332–36. http://dx.doi.org/10.14429/dsj.71.16814.

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Analytical formulations for the resonant frequency of a reentrant cavity for klystron are available in the literature only for such cavities having a single beam-tunnel. An improved analytical formulation has been proposed in this paper for the calculation of cavity gap-capacitance of reentrant cavities having single and multiple beam-tunnels and its effects on the resonant frequency are studied. The results obtained through analysis have been validated against those obtained from the 3D electromagnetic field simulations and measurements. The proposed analytical formulation provides good estimation of resonant frequency of cavity with single and multiple beam-tunnels.
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Nouroozi, M., M. Pasandidehfard, and M. H. Djavareshkian. "Simulation of Partial and Supercavitating Flows around Axisymmetric and Quasi-3D Bodies by Boundary Element Method Using Simple and Reentrant Jet Models at the Closure Zone of Cavity." Mathematical Problems in Engineering 2016 (2016): 1–13. http://dx.doi.org/10.1155/2016/1593849.

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A fixed-length Boundary Element Method (BEM) is used to investigate the super- and partial cavitating flows around various axisymmetric bodies using simple and reentrant jet models at the closure zone of cavity. Also, a simple algorithm is proposed to model the quasi-3D cavitating flows over elliptical-head bodies using the axisymmetric method. Cavity and reentrant jet lengths are the inputs of the problem and the cavity shape and cavitation number are some of the outputs of this simulation. A numerical modeling based on Navier-Stokes equations using commercial CFD code (Fluent) is performed to evaluate the BEM results (in 2D and 3D cases). The cavitation properties approximated by the present research study (especially with the reentrant jet model) are very close to the results of other experimental and numerical solutions. The need for a very short time (only a few minutes) to reach the desirable convergence and relatively good accuracy are the main advantages of this method.
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Seo, Dongjin, Alex M. Schrader, Szu-Ying Chen, et al. "Rates of cavity filling by liquids." Proceedings of the National Academy of Sciences 115, no. 32 (2018): 8070–75. http://dx.doi.org/10.1073/pnas.1804437115.

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Understanding the fundamental wetting behavior of liquids on surfaces with pores or cavities provides insights into the wetting phenomena associated with rough or patterned surfaces, such as skin and fabrics, as well as the development of everyday products such as ointments and paints, and industrial applications such as enhanced oil recovery and pitting during chemical mechanical polishing. We have studied, both experimentally and theoretically, the dynamics of the transitions from the unfilled/partially filled (Cassie–Baxter) wetting state to the fully filled (Wenzel) wetting state on intrinsically hydrophilic surfaces (intrinsic water contact angle <90°, where the Wenzel state is always the thermodynamically favorable state, while a temporary metastable Cassie–Baxter state can also exist) to determine the variables that control the rates of such transitions. We prepared silicon wafers with cylindrical cavities of different geometries and immersed them in bulk water. With bright-field and confocal fluorescence microscopy, we observed the details of, and the rates associated with, water penetration into the cavities from the bulk. We find that unconnected, reentrant cavities (i.e., cavities that open up below the surface) have the slowest cavity-filling rates, while connected or non-reentrant cavities undergo very rapid transitions. Using these unconnected, reentrant cavities, we identified the variables that affect cavity-filling rates: (i) the intrinsic contact angle, (ii) the concentration of dissolved air in the bulk water phase (i.e., aeration), (iii) the liquid volatility that determines the rate of capillary condensation inside the cavities, and (iv) the presence of surfactants.
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Fan, Yaohui, Zhengyu Zhang, Natalia C. Carvalho, Jean-Michel Le Floch, Qingxiao Shan, and Michael E. Tobar. "Investigation of Higher Order Reentrant Modes of a Cylindrical Reentrant-Ring Cavity Resonator." IEEE Transactions on Microwave Theory and Techniques 62, no. 8 (2014): 1657–62. http://dx.doi.org/10.1109/tmtt.2014.2331625.

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