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  • 1
    Online Resource
    Online Resource
    Walter de Gruyter GmbH ; 2002
    In:  International Journal of Nonlinear Sciences and Numerical Simulation Vol. 3, No. 3-4 ( 2002-01)
    In: International Journal of Nonlinear Sciences and Numerical Simulation, Walter de Gruyter GmbH, Vol. 3, No. 3-4 ( 2002-01)
    Type of Medium: Online Resource
    ISSN: 2191-0294 , 1565-1339
    Language: Unknown
    Publisher: Walter de Gruyter GmbH
    Publication Date: 2002
    detail.hit.zdb_id: 2602467-6
    SSG: 11
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  • 2
    Online Resource
    Online Resource
    IOP Publishing ; 2006
    In:  Chinese Physics Letters Vol. 23, No. 5 ( 2006-05), p. 1230-1233
    In: Chinese Physics Letters, IOP Publishing, Vol. 23, No. 5 ( 2006-05), p. 1230-1233
    Type of Medium: Online Resource
    ISSN: 0256-307X , 1741-3540
    Language: Unknown
    Publisher: IOP Publishing
    Publication Date: 2006
    detail.hit.zdb_id: 2040565-0
    SSG: 6,25
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  • 3
    Online Resource
    Online Resource
    Royal Society of Chemistry (RSC) ; 2009
    In:  Lab on a Chip Vol. 9, No. 16 ( 2009), p. 2306-
    In: Lab on a Chip, Royal Society of Chemistry (RSC), Vol. 9, No. 16 ( 2009), p. 2306-
    Type of Medium: Online Resource
    ISSN: 1473-0197 , 1473-0189
    Language: English
    Publisher: Royal Society of Chemistry (RSC)
    Publication Date: 2009
    detail.hit.zdb_id: 2056646-3
    SSG: 12
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  • 4
    In: Acta Physica Sinica, Acta Physica Sinica, Chinese Physical Society and Institute of Physics, Chinese Academy of Sciences, Vol. 72, No. 16 ( 2023), p. 164703-
    Abstract: 〈sec〉Self-propelled micromotor serves as a bridge between the microfluidic environment and macroscopic control. It has broad application prospects in targeted drug delivery, biosensors, and other fields. The high driving speed of bubble micromotor is an irreplaceable advantage in practical applications. Bubble micromotor converts chemical energy in ambient solutions into mechanical energy through asymmetric surface catalytic reactions to drive its own motion. The energy conversion rate of bubble driving is used as an indicator to evaluate the driving force. The Pt catalytic layer of a tubular micromotor is located on the inner wall of the microtube. Bubbles form inside the tube. They are released from one end of the microtubule into the solution and self driven by bubble rebound, with an energy conversion rate of 〈inline-formula〉〈tex-math id="M1"〉\begin{document}$ \sim {10^{ - 10}}$\end{document}〈/tex-math〉〈alternatives〉〈graphic xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="16-20230608_M1.jpg"/〉〈graphic xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="16-20230608_M1.png"/〉〈/alternatives〉〈/inline-formula〉. The Janus microsphere motor near the gas-liquid interface utilizes the energy of the bubble coalesced with the interface to drive the microsphere, with an energy conversion rate of 〈inline-formula〉〈tex-math id="M2"〉\begin{document}$ \sim {10^{ - 7}}$\end{document}〈/tex-math〉〈alternatives〉〈graphic xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="16-20230608_M2.jpg"/〉〈graphic xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="16-20230608_M2.png"/〉〈/alternatives〉〈/inline-formula〉. In sum, the tubular bubble motor is suitable for complex scenarios but has a low energy conversion rate. The Janus microsphere motor driven by bubbles has a high efficiency but is only suitable near the gas-liquid interface. This paper combines the advantages of driving tubular micromotors in bulk solution and Janus microsphere motors which can be driven efficiently by interface energy, proposes a new method of driving Janus microsphere motors by dual bubble coalescence.〈/sec〉〈sec〉In the experiment, a high-speed camera is used to record the ~100 μs of dual bubble coalescence and the process of driving micromotor. Then we investigate the initial kinetic energy conversion rate of micro motor driven by bubble coalescence. Three sets of different bubble/particle size ratios of 〈inline-formula〉〈tex-math id="M3"〉\begin{document}${R_{\rm{b}}}/{R_{\rm{p}}} 〈 1$\end{document}〈/tex-math〉〈alternatives〉〈graphic xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="16-20230608_M3.jpg"/〉〈graphic xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="16-20230608_M3.png"/〉〈/alternatives〉〈/inline-formula〉, 〈inline-formula〉〈tex-math id="M4"〉\begin{document}${R_{\rm{b}}}/{R_{\rm{p}}} \approx 1$\end{document}〈/tex-math〉〈alternatives〉〈graphic xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="16-20230608_M4.jpg"/〉〈graphic xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="16-20230608_M4.png"/〉〈/alternatives〉〈/inline-formula〉, 〈inline-formula〉〈tex-math id="M5"〉\begin{document}${R_{\rm{b}}}/{R_{\rm{p}}} 〉 1$\end{document}〈/tex-math〉〈alternatives〉〈graphic xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="16-20230608_M5.jpg"/〉〈graphic xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="16-20230608_M5.png"/〉〈/alternatives〉〈/inline-formula〉 are adopted for their propulsion effects on microspheres. The initial kinetic energy conversion rate is defined to characterize the contribution of bubble coalescence process to microsphere driving.〈/sec〉〈sec〉After simulations with the pseudo potential lattice Boltzmann method, the mechanism of bubble coalescence driving the motion of microspheres is revealed. It is clarified that the interface oscillation caused by bubble coalescence is the main reason of driving the micromotor, and its energy conversion rate is between the rebound driving of the tubular micromotor and the one-bubble coalescence driving with the free surface. The research results reveal the details of bubble coalescence at different time periods, and provide the effects of factors such as bubble particle size ratio on microsphere displacement and initial kinetic energy conversion rate. Thus the efficient driving mechanism of dual bubble coalescence and release of surface energy are confirmed.〈/sec〉
    Type of Medium: Online Resource
    ISSN: 1000-3290 , 1000-3290
    Language: Unknown
    Publisher: Acta Physica Sinica, Chinese Physical Society and Institute of Physics, Chinese Academy of Sciences
    Publication Date: 2023
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  • 5
    In: Acta Physica Sinica, Acta Physica Sinica, Chinese Physical Society and Institute of Physics, Chinese Academy of Sciences, Vol. 69, No. 6 ( 2020), p. 064701-
    Abstract: Adding nanoparticles with high light response characteristics to a light-transmitting fluid medium can form a light-driven nanofluid and achieve efficient use of light energy. This paper conducts the experimental observation and theoretical analysis of the light driven nanofluid flow behavior, which is the theoretical basis for achieving the precise control of optical drive nanofluid. To realize the efficient conversion of light energy into kinetic energy, here, the motion of Fe〈sub〉3〈/sub〉O〈sub〉4〈/sub〉 particles with a diameter of 300 nm in droplets induced by the Marangoni effect is studied under different light sources by using the particle image velocimetry (PIV). The experimental results show that when the number density of particles is higher than the critical value, the vertical vortices with symmetrical structure can be induced. At the bottom of the droplet, the particles move from the periphery to the center of droplet, and at the top of the droplet, the particles move from the center to the periphery of droplet. In addition, the frequency of light source and the number density of particles are the dominant factors in this process. Subsequently, for the light driven nanofluid experiment in this paper, the analytical solution of the flow field distribution is achieved by using the Stokes equation and the surface tension gradient boundary condition. The analytical solution of the flow field distribution obtained here is consistent with the experimental results, confirming the validity of the quantitative theory. Finally, the correlation between various driving modes, including surface tension at the top surface, surface pressure at the bottom surface or concentrated light radiation force in bulk phase, is discussed. This research provides theoretical support for the precise regulation of flow behavior and efficient conversion of light energy in the optical microfluidic system.
    Type of Medium: Online Resource
    ISSN: 1000-3290 , 1000-3290
    Language: Unknown
    Publisher: Acta Physica Sinica, Chinese Physical Society and Institute of Physics, Chinese Academy of Sciences
    Publication Date: 2020
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  • 6
    Online Resource
    Online Resource
    American Chemical Society (ACS) ; 2009
    In:  Langmuir Vol. 25, No. 6 ( 2009-03-17), p. 3336-3339
    In: Langmuir, American Chemical Society (ACS), Vol. 25, No. 6 ( 2009-03-17), p. 3336-3339
    Type of Medium: Online Resource
    ISSN: 0743-7463 , 1520-5827
    RVK:
    Language: English
    Publisher: American Chemical Society (ACS)
    Publication Date: 2009
    detail.hit.zdb_id: 2005937-1
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  • 7
    Online Resource
    Online Resource
    AIP Publishing ; 2004
    In:  Physics of Fluids Vol. 16, No. 5 ( 2004-05-01), p. 1803-1810
    In: Physics of Fluids, AIP Publishing, Vol. 16, No. 5 ( 2004-05-01), p. 1803-1810
    Abstract: The flow characteristics of liquids in microtubes driven by a high pressure ranging from 1 MPa to 30 MPa are studied in this paper. The diameter of the microtube is from 3 μm to 10 μm and liquids composed of simple small molecules are chosen as the working fluids. The Reynolds number ranges from 0.1 to 24. The behavior of isopropanol and carbon tetrachloride under high pressure is found different from the prediction from conventional Hagen–Poiseuille (HP) equation. The normalized friction coefficient C* increases significantly with the pressure. From an analysis of the microtube deformation, liquid compressibility, viscous heating and wall slip, it may be seen that the viscosity at high pressure plays an important role here. An exponential function of viscosity vs pressure is introduced into the HP equation to counteract the difference between experimental and theoretical values. However, this difference is not so marked for di-water.
    Type of Medium: Online Resource
    ISSN: 1070-6631 , 1089-7666
    Language: English
    Publisher: AIP Publishing
    Publication Date: 2004
    detail.hit.zdb_id: 1472743-2
    detail.hit.zdb_id: 241528-8
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  • 8
    Online Resource
    Online Resource
    Acta Physica Sinica, Chinese Physical Society and Institute of Physics, Chinese Academy of Sciences ; 2015
    In:  Acta Physica Sinica Vol. 64, No. 13 ( 2015), p. 134705-
    In: Acta Physica Sinica, Acta Physica Sinica, Chinese Physical Society and Institute of Physics, Chinese Academy of Sciences, Vol. 64, No. 13 ( 2015), p. 134705-
    Abstract: Self-propellant Janus microsphere is a special class of active particles with a regular shape and irregular surface characteristic. With the self-propulsion of 2 μm diameter Pt-SiO2 Janus microsphere near the wall, we have measured the relationship of self-propellant velocity VJanus versus the observed time Δtobs. A diffusiophoretic force-dominated motion, which can be deemed as a quasi-1 D motion with the characteristics of both force free and torque free, is distinguished from the entire motion process. At the same time, it is also observed that the Janus microsphere is deflected about the vertical direction with an angle ψ. The deflection angle ψ is found to decrease with the increase of H2O2 concentration in the solution. For the 2.5%-10% H2O2 solution in this experiment, the angle ψ ranges from 20° to 7° approximately. A numerical model, involving viscous force, diffusiophoretic force and the effective gravity, is created with a reference frame, this quasi-1 D self-propellant motion can be solved to satisfy the conditions of the force and torque balance simultaneously. We have studied the changes of angle ψ and separation distance δ of the microsphere from the substrate under different conditions, including the concentrations of H2O2 solution, the material density, and the diameter of the microsphere. For the self-propulsion velocity VJanus and the deflection angle ψ, numerical results show good agreement with the published experimental observation results. Moreover, it is found that the lower density or the smaller diameter of the microsphere will generate the smaller distance δ, while the higher concentration of H2O2 in the solution will result in a larger distance δ. The predicted δ is 2-8 μm. With the obtained data, we further discuss the effect of near wall on the characteristic time τR of rotational diffusion of the Janus microsphere. Because the predicted values of δ are relative high, the near wall effect can be neglected, indicating that this effect should not be a significant factor to cause a big discrepancy of τR in different references. The present work will be beneficial to the understanding of the mechanism of self-propulsion and the development in its potential applications.
    Type of Medium: Online Resource
    ISSN: 1000-3290 , 1000-3290
    Language: Unknown
    Publisher: Acta Physica Sinica, Chinese Physical Society and Institute of Physics, Chinese Academy of Sciences
    Publication Date: 2015
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  • 9
    Online Resource
    Online Resource
    American Chemical Society (ACS) ; 2018
    In:  Langmuir Vol. 34, No. 35 ( 2018-09-04), p. 10426-10433
    In: Langmuir, American Chemical Society (ACS), Vol. 34, No. 35 ( 2018-09-04), p. 10426-10433
    Type of Medium: Online Resource
    ISSN: 0743-7463 , 1520-5827
    RVK:
    Language: English
    Publisher: American Chemical Society (ACS)
    Publication Date: 2018
    detail.hit.zdb_id: 2005937-1
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  • 10
    In: Acta Physica Sinica, Acta Physica Sinica, Chinese Physical Society and Institute of Physics, Chinese Academy of Sciences, Vol. 65, No. 22 ( 2016), p. 220201-
    Abstract: A Janus particle is a general term for a non-uniform particle that has different properties on different sides of particle. For a Pt-SiO2 type of Janus microsphere, Pt side serves as the catalysis surface to decompose H2O2 solution, leading to the self-propulsion motion of particle. In this paper, the relevant experimental phenomena in two driven modes are compared first. The results show that under the same concentration of solution, the microsphere with a diameter of about 1 m experiences self-diffusiophoresis propulsion; whereas, the one with an about 20 m diameter experiences bubble self-propulsion. Significant differences in motional trajectory and propulsion velocity are found between them. Then, the dominated physical factors are analyzed and the multi-field coupling numerical model is constructed based on the simplified force balance analysis. Subsequently, the velocity field distribution and O2 concentration distribution around Janus microsphere are also studied. According to these studies, we explain the position and size of the bubble generated. Further more, we infer that the wall slip coefficient is a key matching parameter in the numerical model, and two slip coefficients with a difference of an order of magnitude are given corresponding to the two types of self-propulsion modes. Then we explain the possible mechanism for the changes of wall slip coefficient under different particle sizes. The present study is beneficial to the in-depth exploration of the self-propulsion mechanism and also provides the theoretical foundation for improving the performance of self-propellant device.
    Type of Medium: Online Resource
    ISSN: 1000-3290 , 1000-3290
    Language: Unknown
    Publisher: Acta Physica Sinica, Chinese Physical Society and Institute of Physics, Chinese Academy of Sciences
    Publication Date: 2016
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