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1

Yoo, Sangwook, Cheongho Lee, and Seongah Chin. "Physically Based Soap Bubble Synthesis for VR." Applied Sciences 11, no. 7 (March 31, 2021): 3090. http://dx.doi.org/10.3390/app11073090.

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To experience a real soap bubble show, materials and tools are required, as are skilled performers who produce the show. However, in a virtual space where spatial and temporal constraints do not exist, bubble art can be performed without real materials and tools to give a sense of immersion. For this, the realistic expression of soap bubbles is an interesting topic for virtual reality (VR). However, the current performance of VR soap bubbles is not satisfying the high expectations of users. Therefore, in this study, we propose a physically based approach for reproducing the shape of the bubble by calculating the measured parameters required for bubble modeling and the physical motion of bubbles. In addition, we applied the change in the flow of the surface of the soap bubble measured in practice to the VR rendering. To improve users’ VR experience, we propose that they should experience a bubble show in a VR HMD (Head Mounted Display) environment.
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2

Sapia, Peppino. "Soap bubble." Physics Teacher 56, no. 6 (September 2018): 416. http://dx.doi.org/10.1119/1.5051172.

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3

Morgan, Frank, Edward R. Melnick, and Ramona Nicholson. "Activities: The Soap-Bubble-Geometry Contest." Mathematics Teacher 90, no. 9 (December 1997): 746–50. http://dx.doi.org/10.5951/mt.90.9.0746.

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For many students, playing with soap bubbles is a ritual of childhood. Others observe soap bubbles in action while washing the dishes or the dog. Working with soap bubbles in mathematics class allows students to recognize that mathematics can make common experiences more fascinating. The following soap-bubble-geometry contest allows students to mesh observation and mathematical reasoning and to discover that mathematics is much more than just number crunching. Apparently simple questions expose deep geometric concepts. Students find to their amazement that some simple questions have been answered only recently, by students, and that others remain unanswered today.
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4

Hasegawa, Naoya, and Yoshihiko Takahashi. "Control of Soap Bubble Ejection Robot Using Facial Expressions." International Journal of Manufacturing, Materials, and Mechanical Engineering 11, no. 2 (April 2021): 1–16. http://dx.doi.org/10.4018/ijmmme.2021040101.

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This research has developed a soap bubble ejection robot as an amusement system that reads emotions from human facial expressions and controls the ejection of soap bubbles to improve human-robot interaction. A subject's response to soap bubble ejection is read by a built-in face recognition sensor which sends data to a control system which in turn controls the next ejection. Soap bubbles are often used to research children's emotions/emotional responses. First, evaluation experiments of the control system were performed using face photographs that show human emotions. The experimental results revealed that soap bubbles were ejected in the case of indifference, and the ejection stopped in the case of joy. Through the experimental results, it was confirmed that the control system worked properly when face photographs were used and also verified the effectiveness of the facial recognition sensor. Secondly, evaluation experiments were conducted with an actual human, and it was confirmed from the results that the control system operates as designed.
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5

Cummins, Ken. "Soap bubble respirometry." Journal of Chemical Education 68, no. 7 (July 1991): 617. http://dx.doi.org/10.1021/ed068p617.

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6

Iacono, Michael J., and Duncan C. Blanchard. "Soap Bubble Meteorology." Weatherwise 40, no. 3 (June 1987): 141–42. http://dx.doi.org/10.1080/00431672.1987.9933355.

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7

Buchholz, James, Lorenz Sigurdson, and Bill Peck. "Bursting Soap Bubble." Physics of Fluids 7, no. 9 (September 1995): S3. http://dx.doi.org/10.1063/1.4739112.

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8

Marder, M. "Soap-bubble growth." Physical Review A 36, no. 1 (July 1, 1987): 438–40. http://dx.doi.org/10.1103/physreva.36.438.

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9

Yang, Xi, and Eijiro Miyako. "Soap Bubble Pollination." iScience 23, no. 6 (June 2020): 101188. http://dx.doi.org/10.1016/j.isci.2020.101188.

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10

Morgan, Frank. "Colloquium: Soap bubble clusters." Reviews of Modern Physics 79, no. 3 (July 13, 2007): 821–27. http://dx.doi.org/10.1103/revmodphys.79.821.

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11

Cohen, Caroline, Baptiste Darbois Texier, Etienne Reyssat, Jacco H. Snoeijer, David Quéré, and Christophe Clanet. "On the shape of giant soap bubbles." Proceedings of the National Academy of Sciences 114, no. 10 (February 21, 2017): 2515–19. http://dx.doi.org/10.1073/pnas.1616904114.

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We study the effect of gravity on giant soap bubbles and show that it becomes dominant above the critical sizeℓ=a2/e0, wheree0is the mean thickness of the soap film anda=γb/ρgis the capillary length (γbstands for vapor–liquid surface tension, andρstands for the liquid density). We first show experimentally that large soap bubbles do not retain a spherical shape but flatten when increasing their size. A theoretical model is then developed to account for this effect, predicting the shape based on mechanical equilibrium. In stark contrast to liquid drops, we show that there is no mechanical limit of the height of giant bubble shapes. In practice, the physicochemical constraints imposed by surfactant molecules limit the access to this large asymptotic domain. However, by an exact analogy, it is shown how the giant bubble shapes can be realized by large inflatable structures.
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12

Almgren, Fred, and John Sullivan. "Visualization of Soap Bubble Geometries." Leonardo 25, no. 3/4 (1992): 267. http://dx.doi.org/10.2307/1575849.

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13

Kim, Namjung, SaeWoon Oh, and Kyoungju Park. "Giant soap bubble creation model." Computer Animation and Virtual Worlds 26, no. 3-4 (April 29, 2015): 445–55. http://dx.doi.org/10.1002/cav.1640.

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14

Kuna, S., and R. Gudena. ""Soap bubble" in the calcaneus." Canadian Medical Association Journal 183, no. 10 (May 16, 2011): 1171. http://dx.doi.org/10.1503/cmaj.101525.

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15

Brubaker, Nicholas D. "Shapes of large, static soap bubbles." Proceedings of the Royal Society A: Mathematical, Physical and Engineering Sciences 477, no. 2246 (February 2021): 20200851. http://dx.doi.org/10.1098/rspa.2020.0851.

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Standard predictions induced by the balance of surface tension and pressure dictate that static soap bubbles must be spherical. However, definite non-spherical shapes appear in large bubbles, where noticeable oblate or prolate deformations occur. Gravity is the principal cause of such deformations, and multiple approaches for including its influence appear in recent literature. This paper derives a general surface-theoretic model by applying asymptotic and variational methods to a fully three-dimensional set-up where the soap bubble is a finite-thickness film. The procedure illuminates implicit assumptions, clarifying the discrepancies seen in previous models. Then the model is studied in four physical situations. In three of these situations, results show that there is a maximum stable span and volume of the soap bubbles, implying that their behaviour is qualitatively more similar to liquid drops than standard soap bubbles. Also, the model presented is directly analogous to the two-dimensional version of a hanging chain, and the derived predictions give practical insights into the construction of heavy containment vessels.
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16

PELESZ, Adam. "Charging of a single soap bubble." PRZEGLĄD ELEKTROTECHNICZNY 1, no. 10 (October 5, 2018): 178–81. http://dx.doi.org/10.15199/48.2018.10.40.

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17

Grinfeld, P. "Small Oscillations of a Soap Bubble." Studies in Applied Mathematics 128, no. 1 (May 19, 2011): 30–39. http://dx.doi.org/10.1111/j.1467-9590.2011.00523.x.

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18

SULLIVAN, JOHN M., and FRANK MORGAN. "OPEN PROBLEMS IN SOAP BUBBLE GEOMETRY." International Journal of Mathematics 07, no. 06 (December 1996): 833–42. http://dx.doi.org/10.1142/s0129167x9600044x.

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The Burlington Mathfest in August 1995 included an AMS Special Session on Soap Bubble Geometry, organized by Frank Morgan. At the end of the session, participants were asked to pose open problems related to bubble geometry. We have collected those problems here, adding a few introductory comments. Participants in the special session included the following: Fred Almgren, Princeton U. Megan Barber, Williams C. Ken Brakke, Susquehanna U. John Cahn, NIST Joel Foisy, Duke U. Christopher French, U.Chicago Scott Greenleaf, SUNY Stony Brook Karsten Groeß-Brauckmann, Bonn Joel Hass, UC Davis Aladár Heppes, Budapest Michael Hutchings, Harvard U. Jenny Kelley, Rutgers U. Andy Kraynik, Sandia Rob Kusner, U.Massachusetts Rafael Lopez, Granada Joe Masters, U.Texas Helen Moore, Bowdoin C. Frank Morgan, Williams C. Ivars Peterson, Science News Robert Phelan, Dublin Joel Shore, McGill U. John Sullivan, U.Minnesota Italo Tamanini, Trento Jean Taylor, Rutgers U. Jennifer Tice, Williams C. Brian Wecht, Williams C. Henry Wente, U.Toledo Brian White, Stanford U.
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19

Bianco, Havazelet, and Abraham Marmur. "Gibbs Elasticity of a Soap Bubble." Journal of Colloid and Interface Science 158, no. 2 (July 1993): 295–302. http://dx.doi.org/10.1006/jcis.1993.1260.

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20

Jackson, David P., and Sarah Sleyman. "Analysis of a deflating soap bubble." American Journal of Physics 78, no. 10 (October 2010): 990–94. http://dx.doi.org/10.1119/1.3442800.

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21

Pinkall, U., and I. Sterling. "Computational aspects of soap bubble deformations." Proceedings of the American Mathematical Society 118, no. 2 (February 1, 1993): 571. http://dx.doi.org/10.1090/s0002-9939-1993-1164150-3.

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22

Maulik, Kaushik, Santhiya Srinivasan, Arushi Gahlot Saini, and Shiv Sajan Saini. "Soap bubble appearance: an ominous sign." BMJ Case Reports 12, no. 5 (May 2019): e229721. http://dx.doi.org/10.1136/bcr-2019-229721.

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23

Tsujimoto, Yumiko, Koji Ryoke, Nobuo Yamagami, Yuji Uchio, and Shigeko Tanaka. "DELINEATION OF EXTENSOR TENDON OF THE HAND BY MRI: USEFULNESS OF "SOAP-BUBBLE" MIP PROCESSING TECHNIQUE." Hand Surgery 20, no. 01 (January 2015): 93–98. http://dx.doi.org/10.1142/s0218810415500136.

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To evaluate the capability of the "Soap-Bubble" maximum intensity projection (MIP) processing technique in visualisation of extensor tendons of the hand, 36 intact subjects and seven patients with surgically confirmed extensor tendon rupture were examined. Three-dimensional T1-weighted turbo spin echo (3DT1TFE) MRI was performed using a sensitivity encoding flex coil, followed by Soap-Bubble MIP processing. For patients with extensor tendon ruptures, MRI findings and intraoperative findings were compared. As results, with only 3DT1TFE sequence, the entire extensor tendons that run along the arch of the hand were not shown on one image, but were visualised with addition of Soap-Bubble MIP. Although delineation of the extensor pollicis longus was poor in 27/43 subjects, it was much improved by the combination of water-suppression technique. MRI findings and intraoperative findings agreed in all patients. Soap-Bubble MIP processing with addition of water-suppression technique is considered useful for visualising the extensor tendons of the hand.
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24

Cox, S. J., F. Morgan, and F. Graner. "Are large perimeter- minimizing two-dimensional clusters of equal-area bubbles hexagonal or circular?" Proceedings of the Royal Society A: Mathematical, Physical and Engineering Sciences 469, no. 2149 (January 8, 2013): 20120392. http://dx.doi.org/10.1098/rspa.2012.0392.

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A computer study of clusters of up to N =200 000 equal-area bubbles shows for the first time that partially rounding conjectured optimal hexagonal planar soap bubble clusters reduces perimeter. Different methods of creating optimal clusters are compared, and new candidate minimizers for several N are given.
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25

Wichiramala, Wacharin. "Weak Approach to Planar Soap Bubble Clusters." Missouri Journal of Mathematical Sciences 24, no. 2 (November 2012): 167–81. http://dx.doi.org/10.35834/mjms/1352138562.

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26

Rämme, Göran. "Videotaping the lifespan of a soap bubble." Physics Teacher 33, no. 9 (December 1995): 558–61. http://dx.doi.org/10.1119/1.2344302.

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27

PV, Pradeep, and Jayashree B. "Soap Bubble Type of Calcification in Thyroid." Otolaryngology–Head and Neck Surgery 144, no. 4 (March 2011): 642–43. http://dx.doi.org/10.1177/0194599810397286.

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28

Rämme, Göran. "Surface tension from deflating a soap bubble." Physics Education 32, no. 3 (May 1997): 191–94. http://dx.doi.org/10.1088/0031-9120/32/3/022.

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29

Afanasyev, Y. D., G. T. Andrews, and C. G. Deacon. "Measuring soap bubble thickness with color matching." American Journal of Physics 79, no. 10 (October 2011): 1079–82. http://dx.doi.org/10.1119/1.3596431.

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30

Garza-Hume, C. E. "Planar soap bubble clusters with multiple cavities." Applied Mathematics Letters 23, no. 3 (March 2010): 226–29. http://dx.doi.org/10.1016/j.aml.2009.09.025.

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31

Pogorelov, A. V. "Imbedding a “soap bubble” into a tetrahedron." Mathematical Notes 56, no. 2 (August 1994): 824–26. http://dx.doi.org/10.1007/bf02110741.

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32

Ueda, Kazuhiro. "Localization of air leaks by soap bubble." Journal of Thoracic Disease 11, S9 (May 2019): S1229—S1230. http://dx.doi.org/10.21037/jtd.2019.03.14.

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33

Behroozi, F., and D. W. Olson. "Colorful demos with a long‐lasting soap bubble." American Journal of Physics 62, no. 9 (September 1994): 856–57. http://dx.doi.org/10.1119/1.17474.

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34

Takeno, Tadao. "Pressure distribution in flame propagating in soap bubble." Combustion and Flame 62, no. 1 (October 1985): 95–99. http://dx.doi.org/10.1016/0010-2180(85)90097-5.

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35

Magnanini, Rolando, and Giorgio Poggesi. "On the stability for Alexandrov’s Soap Bubble theorem." Journal d'Analyse Mathématique 139, no. 1 (October 2019): 179–205. http://dx.doi.org/10.1007/s11854-019-0058-y.

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36

Kanyanee, Tinakorn, Walter L. Borst, Jaroon Jakmunee, Kate Grudpan, Jianzhong Li, and Purnendu K. Dasgupta. "Soap Bubbles in Analytical Chemistry. Conductometric Determination of Sub-Parts Per Million Levels of Sulfur Dioxide with a Soap Bubble." Analytical Chemistry 78, no. 8 (April 2006): 2786–93. http://dx.doi.org/10.1021/ac052198h.

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37

Marković, Slobodan. "The soap bubble: Phenomenal state or perceptual system dynamics?" Behavioral and Brain Sciences 26, no. 4 (August 2003): 420–21. http://dx.doi.org/10.1017/s0140525x03340099.

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The Gestalt Bubble model describes a subjective phenomenal experience (what is seen) without taking into account the extraphenomenal constraints of perceptual experience (why it is seen as it is). If it intends to be an explanatory model, then it has to include either stimulus or neural constraints, or both.
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38

Foisy, Joel, Manuel Alfaro Garcia, Jeffrey Brock, Nickelous Hodges, and Jason Zimba. "The standard double soap bubble in R2uniquely minimizes perimeter." Pacific Journal of Mathematics 159, no. 1 (May 1, 1993): 47–59. http://dx.doi.org/10.2140/pjm.1993.159.47.

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39

Beall, Abigail. "Soap-bubble cyclone is a deadly storm in miniature." New Scientist 221, no. 2953 (January 2014): 24–25. http://dx.doi.org/10.1016/s0262-4079(14)60180-9.

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40

Sorrenti, A., O. Illa, and R. M. Ortuño. "Amphiphiles in aqueous solution: well beyond a soap bubble." Chemical Society Reviews 42, no. 21 (2013): 8200. http://dx.doi.org/10.1039/c3cs60151j.

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41

OHMAE, Takayuki. "A Soap Bubble Model for Vibrational Motionsos Spherical Fullerenes." NIPPON KAGAKU KAISHI, no. 11 (1993): 1289–91. http://dx.doi.org/10.1246/nikkashi.1993.1289.

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42

WATANABE, Kohei, Hiroyuki TORIKAI, and Akihiko ITO. "301 Filling gas flows observed in soap bubble bursting." Proceedings of Autumn Conference of Tohoku Branch 2012.48 (2012): 80–81. http://dx.doi.org/10.1299/jsmetohoku.2012.48.80.

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43

urikovic, Roman. "Animation of Soap Bubble Dynamics, Cluster Formation and Collision." Computer Graphics Forum 20, no. 3 (September 2001): 67–76. http://dx.doi.org/10.1111/1467-8659.00499.

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44

Sato, Sanae. "Invitation to chemistry through a large soap bubble chamber." Journal of Chemical Education 65, no. 7 (July 1988): 616. http://dx.doi.org/10.1021/ed065p616.

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45

MURASHITA, Takumi, Hiroyuki TORIKAI, and Akihiko ITO. "D233 Extinguishing Gas Flow Observed in Soap Bubble Extinguishment." Proceedings of the Thermal Engineering Conference 2010 (2010): 311–12. http://dx.doi.org/10.1299/jsmeted.2010.311.

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46

Salvato, Nick. "On the Bubble: The Soap Opera Diva's Ambivalent Orbit." Camera Obscura: Feminism, Culture, and Media Studies 22, no. 2 (2007): 103–23. http://dx.doi.org/10.1215/02705346-2007-005.

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47

Katsikadelis, J. T., and M. S. Nerantzaki. "A boundary element solution to the soap bubble problem." Computational Mechanics 27, no. 2 (February 26, 2001): 154–59. http://dx.doi.org/10.1007/s004660000224.

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48

Jaw, S. Y., C. J. Chen, and R. R. Hwang. "Visualization of soap bubble collapse with acoustic pressure applied." Journal of Visualization 8, no. 2 (June 2005): 88. http://dx.doi.org/10.1007/bf03181648.

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49

Correia de Melo, João Victor, Lucas Alves Ripper, José Luiz Mendes Ripper, and Walter dos Santos Teixeira Filho. "The Bubble Hall: Bamboo Reticular Geodesic Structure with the Shape of a Soap Bubble." Key Engineering Materials 600 (March 2014): 78–86. http://dx.doi.org/10.4028/www.scientific.net/kem.600.78.

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This article aims to disclose some aspects of the research and constructive methods on lightweight structures made of tied-up bamboos developed by the Laboratory for Investigation in Living Design, LILD, from PUC-Rio. In this paper, we demonstrate the way of obtaining a shape similar to the one of a soap bubble when blown and manipulated by the researcher, according to previously established parameters. The approximation of such a geometry is achieved through a variety of interactive experiments between the states of a model electronic, manufactured /miniature, and in use that follow the logics of geodesic lines, obtained by means of a grid when inflated. Finally, we present results of initial observations of the assemblage of the bamboo reticular structure in the in use state, that we call The Bubble Hall.
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50

BOTTA, Oana Daciana, István MAGOS, and Corneliu BALAN. "Experimental study on the formation and break-up of fluid bubbles." INCAS BULLETIN 12, no. 1 (March 1, 2020): 27–34. http://dx.doi.org/10.13111/2066-8201.2020.12.1.3.

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The study of fluid surfaces plays an important role in understanding the interfaces encountered in biological systems, as it allows for the investigation of the basic characteristics such as the formation, stability and permeability. Moreover, the adhesion and the fusion of biological membranes can be better understood by the experimental investigations of drops and bubbles formation in controlled dynamical processes. These studies have the potential to generate novel and value information for medical applications in the diagnosis and therapy using microfluidic-based biosensors and controlled drug-delivery micro-devices. In this paper, the dynamics of fluid interfaces have been studied experimentally and a method for determining the surface/interfacial tension is proposed. The analysis started with the investigation of the soap bubble formation and break-up. The rupture was triggered manually, by pinching the tip with a needle. The burst was recorded with high-speed cameras and the burst speed was determined. Furthermore, the thickness of the fluid membrane was approximated and the surface tension was calculated using the Culick-Taylor's law. The obtained values for the surface tension were in the same order of magnitude with that from the literature, thus, considering that the employed method can lead to adequate results. Subsequently, a set-up was created to automatically generate fluid bubbles, at different imposed flow rates. The spontaneous burst was analyzed for three different liquids: soap solution, vegetable oil and polyacrylamide. The phenomenon is characterized by the Ohnesorge number, which takes into account the influence of viscous forces in relation to the inertial and surface tension forces. For the soap bubbles, the obtained thickness of the membrane was in the range of (300-500) nm. The calculated surface tension was found to be 0.038 N/m. In the case of automatically generated fluid bubbles, the lowest Ohnesorge number was obtained for soap bubbles and the highest for oil bubbles. Moreover, soap bubbles had the highest break-up speed, while vegetable oil and polyacrylamide had lower and similar break-up speeds. The experimental study described in this paper is an alternative method for the identification of material parameters, such as density and surface tension, in a dynamical process. Numerical simulations are reported from the viewpoint of servo time constant performance.
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