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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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2

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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3

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 se
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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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5

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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6

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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7

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 estim
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8

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 t
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9

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 intrin
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10

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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11

Brown, M. R., T. E. Sheridan, and M. A. Hayes. "Reentrant cavity as a low‐power plasma source." Review of Scientific Instruments 57, no. 12 (1986): 2957–60. http://dx.doi.org/10.1063/1.1139023.

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12

Carter, R. G., Jinjun Feng, and U. Becker. "Calculation of the Properties of Reentrant Cylindrical Cavity Resonators." IEEE Transactions on Microwave Theory and Techniques 55, no. 12 (2007): 2531–38. http://dx.doi.org/10.1109/tmtt.2007.909750.

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13

Bansiwal, Ashok, Sushil Raina, K. J. Vinoy, and S. K. Datta. "A Broadband Rectangular Reentrant Cavity for Multiple-Beam Klystron." IEEE Transactions on Electron Devices 66, no. 7 (2019): 3168–70. http://dx.doi.org/10.1109/ted.2019.2916222.

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14

Huang, Pi-Ling, Chun-Jen Weng, Hung-T'sang Tuan, Shen-Chuang Pei, Yung-Hsin Chang, and Sheng-Lung Huang. "Polarization Analysis of a Nonplanar Reentrant Ring Laser Cavity." Japanese Journal of Applied Physics 42, Part 1, No. 6A (2003): 3403–8. http://dx.doi.org/10.1143/jjap.42.3403.

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15

Tuan, Hung-Tsang, and Sheng-Lung Huang. "Analysis of reentrant two-mirror nonplanar ring laser cavity." Journal of the Optical Society of America A 22, no. 11 (2005): 2476. http://dx.doi.org/10.1364/josaa.22.002476.

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16

de Paula, L. A. N., M. Goryachev, and M. E. Tobar. "Experiments match simulations in a multiple post reentrant cavity." Review of Scientific Instruments 88, no. 12 (2017): 125104. http://dx.doi.org/10.1063/1.4997626.

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17

Ishihara, Y., and N. Wadamori. "Localized heating characteristics of hyperthermia using a reentrant cavity." Journal of Medical Engineering & Technology 32, no. 5 (2008): 348–57. http://dx.doi.org/10.1080/03091900802058953.

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18

Li, XiaoJing, ShunQi Zheng, BaoRong Zhao, XiWen Zhang, and WeiZhong Tang. "Design and Numerical Simulation of Novel Reentrant Microwave Cavity." Physics Procedia 22 (2011): 101–6. http://dx.doi.org/10.1016/j.phpro.2011.11.016.

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19

Onodera, T., and T. Hoashi. "Generalized representation of beam coupling coefficient in ungridded reentrant cavity." IEEE Transactions on Electron Devices 45, no. 8 (1998): 1858–60. http://dx.doi.org/10.1109/16.704395.

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20

Lu, Fei, Yanjie Guo, Qiulin Tan, et al. "Highly Sensitive Reentrant Cavity-Microstrip Patch Antenna Integrated Wireless Passive Pressure Sensor for High Temperature Applications." Journal of Sensors 2017 (2017): 1–10. http://dx.doi.org/10.1155/2017/3417562.

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A novel reentrant cavity-microstrip patch antenna integrated wireless passive pressure sensor was proposed in this paper for high temperature applications. The reentrant cavity was analyzed from aspects of distributed model and equivalent lumped circuit model, on the basis of which an optimal sensor structure integrated with a rectangular microstrip patch antenna was proposed to better transmit/receive wireless signals. In this paper, the proposed sensor was fabricated with high temperature resistant alumina ceramic and silver metalization with weld sealing, and it was measured in a hermetic m
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21

Srinivasan, Sudharsan, and Pierre-André Duperrex. "Dielectric-Filled Reentrant Cavity Resonator as a Low-Intensity Proton Beam Diagnostic." Instruments 2, no. 4 (2018): 24. http://dx.doi.org/10.3390/instruments2040024.

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Measurement of the proton beam current (0.1–40 nA) at the medical treatment facility PROSCAN at the Paul Scherrer Institut (PSI) is performed with ionization chambers. To mitigate the scattering issues and to preserve the quality of the beam delivered to the patients, a non-interceptive monitor based on the principle of a reentrant cavity resonator has been built. The resonator with a fundamental resonance frequency of 145.7 MHz was matched to the second harmonic of the pulse repetition rate (72.85 MHz) of the beam extracted from the cyclotron. This was realized with the help of ANSYS HFSS (Hi
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22

Muzhaimey, Syarif Syahrul Syazwan, Nik Nazri Nik Ghazali, Mohd Zamri Zainon, et al. "Numerical Investigation of Heat Transfer Enhancement in a Microchannel with Conical-Shaped Reentrant Cavity." Mathematics 10, no. 22 (2022): 4330. http://dx.doi.org/10.3390/math10224330.

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The current study is focused on improving the thermal performance of the microchannel heat sink (MCHS) using the passive reentrant cavity approach. The MCHS physical model’s single channel was used in a three-dimensional numerical simulation. The basic geometrical layout of the MCHS’s computational domain was drawn from previously published research and verified using numerical and analytical correlations that were already in existence. The innovative conical-shaped microchannel heat sink’s (CMCHS) properties for heat transmission and fluid flow were examined numerically under steady-state con
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23

Wang, Minwen, Xin Zhuo, Mingtong Zhao, Mengtong Qiu, Wei Chen, and Zhongming Wang. "Design and prototype test of a high-sensitivity reentrant-cavity based Schottky pickup." Review of Scientific Instruments 94, no. 3 (2023): 033301. http://dx.doi.org/10.1063/5.0134286.

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Schottky diagnostics is an important measure for the debunched beam during the injection phase of the Xi’an Proton Application Facility (XiPAF). The existing capacitive Schottky pickup has a relatively low sensitivity and a poor signal-to-noise ratio for the low-intensity beam. A resonant Schottky pickup based on the principle of a reentrant cavity is proposed. The effects of cavity geometric parameters on cavity properties are systematically studied. A prototype was built and tested to validate the simulation results. The prototype has a resonance frequency of 24.23 MHz, a Q value of 635, and
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24

Xia, Z. X., Y. J. Cheng, and Y. Fan. "Frequency-reconfigurable TM010-mode reentrant cylindrical cavity for microwave material processing." Journal of Electromagnetic Waves and Applications 27, no. 5 (2013): 605–14. http://dx.doi.org/10.1080/09205071.2013.758224.

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25

Kedzierski, M. A., and L. Lin. "Pool boiling of HFO-1336mzz(Z) on a reentrant cavity surface." International Journal of Refrigeration 104 (August 2019): 476–83. http://dx.doi.org/10.1016/j.ijrefrig.2019.02.022.

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26

Ishihara, Y., Y. Kameyama, Y. Minegishi, and N. Wadamori. "Heating applicator based on reentrant cavity with optimized local heating characteristics." International Journal of Hyperthermia 24, no. 8 (2008): 694–704. http://dx.doi.org/10.1080/02656730802117064.

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27

Bansiwal, Ashok, Sushil Raina, K. J. Vinoy, and Subrata Kumar Datta. "A Post-Loaded Rectangular Reentrant Cavity for Broadband Multiple-Beam Klystron." IEEE Electron Device Letters 41, no. 6 (2020): 916–19. http://dx.doi.org/10.1109/led.2020.2989103.

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28

Beck, B. L., K. A. Jenkins, and J. R. Fitzsimmons. "Geometry comparisons of an 11-T coaxial reentrant cavity (ReCav) coil." Concepts in Magnetic Resonance 18B, no. 1 (2003): 24–27. http://dx.doi.org/10.1002/cmr.b.10074.

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29

Zhang, Guang Jian, and Wei Dong Shi. "Numerical Modeling of Unsteady Cloud Cavitation around a Clark-Y Hydrofoil Based on Modified SST Model." Applied Mechanics and Materials 448-453 (October 2013): 3340–43. http://dx.doi.org/10.4028/www.scientific.net/amm.448-453.3340.

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A density correction function was introduced into SST (shear stress transport) model in CFX by user defined subroutine. The unsteady cloud cavitation around a Clark-y hydrofoil was numerically simulated using the modified SST model, associated with Zwart cavitation model. The quasi-periodic evolution of cloud cavity and lift coefficient variation were analysed. The results compared with experimental data show that the modified SST model reduces turbulent viscosity in the rear part of cavity and the reentrant jet in cloud cavitation is predicted. The quasi-periodic evolution of cavity generatio
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30

Goryashko, V. A., M. Jobs, L. H. Duc, J. Ericsson, and R. Ruber. "12-Way 100 kW Reentrant Cavity-Based Power Combiner With Doorknob Couplers." IEEE Microwave and Wireless Components Letters 28, no. 2 (2018): 111–13. http://dx.doi.org/10.1109/lmwc.2017.2780619.

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31

Saimi, Motohiro, Eiji Shiohama, and Tsutomu Kobayashi. "A study of electrodeless microwave HID lamps with a reentrant-type cavity." JOURNAL OF THE ILLUMINATING ENGINEERING INSTITUTE OF JAPAN 86, Appendix (2002): 84. http://dx.doi.org/10.2150/jieij1980.86.appendix_84.

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32

Zeng, Jian, Lang Lin, Yong Tang, Yalong Sun, and Wei Yuan. "Fabrication and capillary characterization of micro-grooved wicks with reentrant cavity array." International Journal of Heat and Mass Transfer 104 (January 2017): 918–29. http://dx.doi.org/10.1016/j.ijheatmasstransfer.2016.09.007.

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33

Le, Q., J. P. Franc, and J. M. Michel. "Partial Cavities: Global Behavior and Mean Pressure Distribution." Journal of Fluids Engineering 115, no. 2 (1993): 243–48. http://dx.doi.org/10.1115/1.2910131.

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The results of an experimental work concerning the behavior of flows with partial cavities are presented. The tests were carried out using a plano-convex foil placed in the free surface channel of the I.M.G. Hydrodynamic Tunnel. The experimental conditions concerning ambient pressure, water velocity, and body size were such that various and realistic kinds of flows could be realized. The main flow regimes are described and correlated to the values of foil incidence and cavitation parameter. Attention is paid to the shedding of large vapor pockets into the cavity wake and its possible periodic
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34

Ma, Jixu, Yukang Chen, and Jie Huang. "A Microwave Displacement Sensor Based on SIW Double Reentrant Cavity with Ring Gaps." Progress In Electromagnetics Research M 113 (2022): 35–45. http://dx.doi.org/10.2528/pierm22050102.

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35

Ishihara, Yasutoshi, Yuya Gotanda, Naoki Wadamori, and Jin-ichi Matsuda. "Hyperthermia applicator based on a reentrant cavity for localized head and neck tumors." Review of Scientific Instruments 78, no. 2 (2007): 024301. http://dx.doi.org/10.1063/1.2437203.

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36

Huang, Pi-Ling, Chun-Ren Weng, Huy-Zu Cheng, and Sheng-Lung Huang. "A Passively Q-Switched Laser Constructed by a Two-Mirror Reentrant Ring Cavity." Japanese Journal of Applied Physics 40, Part 2, No. 5B (2001): L508—L510. http://dx.doi.org/10.1143/jjap.40.l508.

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37

Gu, Wei, Yousheng He, and Tianqun Hu. "Transcritical Patterns of Cavitating Flow and Trends of Acoustic Level." Journal of Fluids Engineering 123, no. 4 (2001): 850–56. http://dx.doi.org/10.1115/1.1412233.

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Hydroacoustics of the transcritical cavitating flows on a NACA16012 hydrofoil at a 2/5/8-degree angle of attack and axisymmetric bodies with hemispherical and 45-degree conical headforms were studied, and the process of cloud cavitation shedding was observed by means of high-speed cinegraphy. By expressing the cavitation noise with partial acoustic level, it is found that the development of cavitation noise varies correspondingly with cavitation patterns. The instability of cavitation is a result of cavity-flow interaction, and is mainly affected by the liquid flow rather than by the cavitatio
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38

Liao, Dong, Yinchuang Yang, and Huihe Qiu. "Droplet impact dynamics and heat transfer on nanostructured doubly reentrant cavity under freezing temperature." Physics of Fluids 33, no. 5 (2021): 052005. http://dx.doi.org/10.1063/5.0050400.

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39

Kazuma, Hiroyuki, Yoshiaki Saitoh, Michio Miyakawa, and Jun'ichi Hori. "Heating Characteristics with Reentrant Resonant-Cavity Applicator. An Experimental Study with Small Phantom Model." Thermal Medicine(Japanese Journal of Hyperthermic Oncology) 12, no. 4 (1996): 401–9. http://dx.doi.org/10.3191/thermalmedicine.12.401.

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40

Wang, Yonghui, Zhixian Ma, and Jili Zhang. "Precise determination of R134a boiling bundle effect on a column of reentrant cavity tubes." Applied Thermal Engineering 199 (November 2021): 117612. http://dx.doi.org/10.1016/j.applthermaleng.2021.117612.

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41

Yasui, Toshiaki, Hirokazu Tahara, and Takao Yoshikawa. "Plasma Generation and Beam Extraction on Reentrant-Cavity-Type Electron Cyclotron Resonance Ion Source." Japanese Journal of Applied Physics 33, Part 1, No. 8 (1994): 4787–92. http://dx.doi.org/10.1143/jjap.33.4787.

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42

Goyal, A., R. C. Jaeger, S. H. Bhavnani, et al. "Formation of silicon reentrant cavity heat sinks using anisotropic etching and direct wafer bonding." IEEE Electron Device Letters 14, no. 1 (1993): 29–32. http://dx.doi.org/10.1109/55.215090.

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43

Kedzierski, M. A., and L. Lin. "Pool boiling of R515A, R1234ze(E), and R1233zd(E) on a reentrant cavity surface." International Journal of Heat and Mass Transfer 161 (November 2020): 120252. http://dx.doi.org/10.1016/j.ijheatmasstransfer.2020.120252.

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44

Kedzierski, M. A. "Effect of concentration on R134a/Al2O3 nanolubricant mixture boiling on a reentrant cavity surface." International Journal of Refrigeration 49 (January 2015): 36–48. http://dx.doi.org/10.1016/j.ijrefrig.2014.09.012.

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45

Wang, Yonghui, Jili Zhang, and Zhixian Ma. "Experimental study of pool boiling on a novel reentrant cavity tube surface with R134a." International Journal of Heat and Mass Transfer 135 (June 2019): 124–30. http://dx.doi.org/10.1016/j.ijheatmasstransfer.2019.01.128.

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46

Ji, Wen-Tao, Chuang-Yao Zhao, Ding-Cai Zhang, et al. "Pool boiling heat transfer of R134a outside reentrant cavity tubes at higher heat flux." Applied Thermal Engineering 127 (December 2017): 1364–71. http://dx.doi.org/10.1016/j.applthermaleng.2017.08.130.

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47

Duncan, J. H., and S. Zhang. "On the interaction of a collapsing cavity and a compliant wall." Journal of Fluid Mechanics 226 (May 1991): 401–23. http://dx.doi.org/10.1017/s0022112091002446.

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The collapse of a spherical vapour cavity in the vicinity of a compliant boundary is examined numerically. The fluid is treated as a potential flow and a boundary-element method is used to solve Laplace's equation for the velocity potential. Full nonlinear boundary conditions are applied on the surface of the cavity. The compliant wall is modelled as a membrane with a spring foundation. At the interface between the fluid and the membrane, the pressure and vertical velocity in the flow are matched to the pressure and vertical velocity of the membrane using linearized conditions. The results of
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48

Bansiwal, Ashok, Sushil Raina, K. J. Vinoy, and Subrata Kumar Datta. "Equivalent Circuit Analysis of a Rectangular Double-Reentrant Cavity With Circular Cylindrical Ferrule for Klystrons." IEEE Transactions on Electron Devices 66, no. 11 (2019): 4952–56. http://dx.doi.org/10.1109/ted.2019.2942778.

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49

Zhang, Shiwei, Lang Lin, Gong Chen, et al. "Experimental study on the capillary performance of aluminum micro-grooved wicks with reentrant cavity array." International Journal of Heat and Mass Transfer 139 (August 2019): 917–27. http://dx.doi.org/10.1016/j.ijheatmasstransfer.2019.05.091.

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50

Kashiwa, T., M. Miyakawa, T. Tsukamoto, and Y. Kanai. "Resonant frequency analysis of reentrant resonant cavity applicator by using FEM and FD-TD method." IEEE Transactions on Magnetics 36, no. 4 (2000): 1750–53. http://dx.doi.org/10.1109/20.877782.

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