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Open Fwong Phd Dissertation.Pdf
The Pennsylvania State University The Graduate School Department of Chemistry CATALYTIC NANOMOTORS AND MICROPUMP SYSTEMS UTILIZING ALTERNATE FUELS A Dissertation in Chemistry by Flory K. Wong © 2016 Flory K. Wong Submitted in Partial Fulfillment of the Requirements for the Degree of Doctor of Philosophy December 2016 ii The dissertation of Flory K. Wong was reviewed and approved* by the following: Ayusman Sen Distinguished Professor of Chemistry Dissertation Advisor Chair of Committee Thomas E. Mallouk Evan Pugh University Professor of Chemistry, Biochemistry, Molecular Biology, and Physics Head of the Department of Chemistry Raymond E. Schaak DuPont Professor of Materials Chemistry Darrell Velegol Distinguished Professor of Chemical Engineering *Signatures are on file in the Graduate School. iii ABSTRACT Colloidal assemblies of self-powered active particles have become a focus area of research. Ranging from microscopic particle suspensions to nanoscale molecules, these systems transduce chemical energy into mechanical motion across multiple length scales following a variety of mechanisms. Understanding the energy transduction processes and the subsequent nature of particle dynamics offers unprecedented opportunities to explore the physics of small-scale colloidal systems and to harness their behavior in many useful applications. However, over a decade after the initial discovery of autonomous bimetallic nanorods, we continue to struggle to bring such systems into real-world applications. Part of the setback has been the in-depth research into hydrogen peroxide fuel. While the studies have built up the fundamental knowledge necessary for the advancement of the field, we have yet to do the same for other systems that employ alternate fuels. This dissertation aims to fill that void by developing nano- and micromotor and pump systems that does not rely on traditional hydrogen peroxide fuel, uses novel material by taking inspiration in other areas of research, and complete in-depth studies to provide a clear understanding of such systems. -
The Molecular Monorail
RADBOUD UNIVERSITY NIJMEGEN RESEARCH PROPOSAL HONOURS ACADEMY FNWI The molecular monorail Authors: Robert BECKER Nadia ERKAMP Supervisor: Marieke GLAZENBURG Prof. Thomas BOLTJE Evert-Jan HEKKELMAN Lisanne SELLIES May 2017 Contents 1 Details 2 1.1 Applicants . .2 1.2 Supervisor . .2 1.3 Keywords . .2 1.4 Field of research . .2 2 Summaries 3 2.1 Scientific summary . .3 2.2 Public summary . .3 2.3 Samenvatting voor algemeen publiek . .3 3 Introduction 5 4 Background 8 4.1 The Feringa motor . .8 4.2 The ring molecule . .9 4.3 Threading of the track . 11 4.4 The track polymer . 12 5 Methods 14 5.1 Optical trapping . 14 5.2 Detection . 15 5.3 Synthesis . 16 5.3.1 Ring.................................... 16 5.3.2 Track . 17 6 Future applications 18 6.1 Further shrink down lab-on-a-chip approach . 18 6.2 Lab-on-a-chip approach in health care: Point-of-care testing (POCT) . 18 1 1 Details 1.1 Applicants Robert Becker - Biology Evert-Jan Hekkelman - Physics & Nadia Erkamp - Chemistry Mathematics Marieke Glazenburg - Physics Lisanne Sellies - Chemistry 1.2 Supervisor Name: Thomas Boltje Telephone: 024-3652331 Email: [email protected] Institute: Synthetic Organic Chemistry Radboud University Nijmegen 1.3 Keywords Nanomachine, Feringa, polymer, porphyrin, FRET 1.4 Field of research NWO division: Chemical Sciences [CW] Code Main field of research 13.20.00 Macromolecular chemistry, polymer chemistry Other fields of research 13.30.00 Organic chemistry 13.50.00 Physical chemistry 12.20.00 Nanophysics/technology 14.80.00 Nanotechnology 2 2 Summaries 2.1 Scientific summary In this proposal we present the design for a new kind of nanomachine. -
Unit VI Superconductivity JIT Nashik Contents
Unit VI Superconductivity JIT Nashik Contents 1 Superconductivity 1 1.1 Classification ............................................. 1 1.2 Elementary properties of superconductors ............................... 2 1.2.1 Zero electrical DC resistance ................................. 2 1.2.2 Superconducting phase transition ............................... 3 1.2.3 Meissner effect ........................................ 3 1.2.4 London moment ....................................... 4 1.3 History of superconductivity ...................................... 4 1.3.1 London theory ........................................ 5 1.3.2 Conventional theories (1950s) ................................ 5 1.3.3 Further history ........................................ 5 1.4 High-temperature superconductivity .................................. 6 1.5 Applications .............................................. 6 1.6 Nobel Prizes for superconductivity .................................. 7 1.7 See also ................................................ 7 1.8 References ............................................... 8 1.9 Further reading ............................................ 10 1.10 External links ............................................. 10 2 Meissner effect 11 2.1 Explanation .............................................. 11 2.2 Perfect diamagnetism ......................................... 12 2.3 Consequences ............................................. 12 2.4 Paradigm for the Higgs mechanism .................................. 12 2.5 See also ............................................... -
B.Tech. - AGRICULTURAL ENGINEERING Syllabus
B.Tech. - AGRICULTURAL ENGINEERING Syllabus I Year I – Semester (HS103) ENGINEERING MATHEMATICS – I L T P To C 3 1 - 4 4 UNIT – I Matrices : Matrices, Rank of a matrix, Solutions of system of linear equations, Gauss- Jordan, Gauss Elimination, Eigen values, Eigen vectors, Cayley-Hamilton theorem - Applications, Diagonalisation of a matrix. UNIT - II Ordinary Differential Equations: Revision of integral formulae, Formation of ordinary differential equations, Differential equations of first order and first degree – linear, Bernoulli and exact. Applications to Newton’s Law of cooling, Law of natural growth and decay, Orthogonal trajectories.Non-homogeneous linear differential equations of second and higher order with constant coefficients with RHS term of the type e, Sin ax, Cos ax, polynomials in x, method of variation of parameters UNIT – III Frobenius Series Solution: Frobenius series solution of differential equations (constant and variable coefficients) UNIT – IV Laplace Transformations : Definitions and properties, Laplace transform of standard functions, Inverse transform, first shifting Theorem, Transforms of derivatives and integrals, Unit step function, second shifting theorem, Dirac’s delta function, Convolution theorem, Differentiation and integration of transforms, Application of Laplace transforms to ordinary differential equations. UNIT - V Numerical Methods: Solutions of Algebraic and Transcendental equations: Bisection method, Regula-Falsi method, Newton-Raphson method, Numerical solutions of algebraic system of equations by Gauss-Siedel method. Interpolation: Errors in polynomial interpolation, Finite differences, Forward, backward and central differences, Newton’s formulae for interpolation, Central difference interpolation formulae, Gauss and Bessel central difference formulae, interpolation with unevenly spaced points, Lagrange’s interpolation formula. Curve fitting by least squares method, solving differential equations by numerical methods – Euler’s, Modified Eulers, RK method. -
1 Introduction
1 1 Introduction 1.1 Global Challenges Water, food, and energy security represent major challenges to the stability and continuity of human populations. However, rapid population growth and steadily improving living standards place enormous pressures on already stressed water resource and agricultural systems. Large amounts of energy are consumed to produce clean water and to treat wastewaters prior to their return to the environ- ment, which inevitably leads to a considerable amount of carbon dioxide (CO2) emissions as well as releasing other environmental pollutants. At the global scale, about 2600 km3 of water are withdrawn to supply food- driven irrigation needs every year. Viewed another way, agriculture consumes nearly 70% of total human freshwater withdrawals. This number is to increase to more than 83% by 2050 to meet the growing food demand by the rapidly growing population. In the last 25 years, access to water with potable quality has gone up from 75% to 90% of the world population, and, nevertheless, 884 million people nowadays still lack access to adequate drinking water in many geographical regions [1]. Thus, ensuring a stable and sustainable water, food, and energy supply into the future is a priority for all nations. Adding to an already dreadful situation, water pollution is becoming a major global challenge [2, 3]. From the United Nations World Water Development Report in 2018, it is said that more than 2 billion people lack access to safe drink- ing water and more than double that number lack access to safe sanitation. With a rapidly growing global population, demand for water is expected to increase by nearly one-third by 2050 [4]. -
Brushless DC Electric Motor
Please read: A personal appeal from Wikipedia author Dr. Sengai Podhuvan We now accept ₹ (INR) Brushless DC electric motor From Wikipedia, the free encyclopedia Jump to: navigation, search A microprocessor-controlled BLDC motor powering a micro remote-controlled airplane. This external rotor motor weighs 5 grams, consumes approximately 11 watts (15 millihorsepower) and produces thrust of more than twice the weight of the plane. Contents [hide] 1 Brushless versus Brushed motor 2 Controller implementations 3 Variations in construction 4 AC and DC power supplies 5 KM rating 6 Kv rating 7 Applications o 7.1 Transport o 7.2 Heating and ventilation o 7.3 Industrial Engineering . 7.3.1 Motion Control Systems . 7.3.2 Positioning and Actuation Systems o 7.4 Stepper motor o 7.5 Model engineering 8 See also 9 References 10 External links Brushless DC motors (BLDC motors, BL motors) also known as electronically commutated motors (ECMs, EC motors) are electric motors powered by direct-current (DC) electricity and having electronic commutation systems, rather than mechanical commutators and brushes. The current-to-torque and frequency-to-speed relationships of BLDC motors are linear. BLDC motors may be described as stepper motors, with fixed permanent magnets and possibly more poles on the rotor than the stator, or reluctance motors. The latter may be without permanent magnets, just poles that are induced on the rotor then pulled into alignment by timed stator windings. However, the term stepper motor tends to be used for motors that are designed specifically to be operated in a mode where they are frequently stopped with the rotor in a defined angular position; this page describes more general BLDC motor principles, though there is overlap. -
Light-Driven Nanoscale Plasmonic Motors Ming Liu1, Thomas Zentgraf1,Yongminliu1,Guybartal1 and Xiang Zhang1,2*
LETTERS PUBLISHED ONLINE: 4 JULY 2010 | DOI: 10.1038/NNANO.2010.128 Light-driven nanoscale plasmonic motors Ming Liu1, Thomas Zentgraf1,YongminLiu1,GuyBartal1 and Xiang Zhang1,2* When Sir William Crookes developed a four-vaned radiometer, the designed plasmonic structure and its interaction with the light. It also known as the light-mill, in 1873, it was believed that this does not require any predetermined angular momentum of the device confirmed the existence of linear momentum carried light, so the illuminating source can be a simple linearly polarized by photons1, as predicted by Maxwell’s equations. Although plane-wave or Gaussian beam. Reynolds later proved that the torque on the radiometer was Light-induced rotation is obtained by careful design of the phase caused by thermal transpiration2, researchers continued to retardation induced by the electron inertia18,19 and experienced by search for ways to take advantage of the momentum of the light incident on a metallic structure (see Supplementary photons and to use it for generating rotational forces. The Information). The phase retardation can be engineered to vary ability to provide rotational force at the nanoscale could open within the structure, inducing orbital angular momentum on the up a range of applications in physics, biology and chemistry, scattered light that, in turn, results in a torque imposed on the including DNA unfolding and sequencing3–6 and nanoelectro- sample. In other words, as a result of the conservation of angular mechanical systems7–10. Here, we demonstrate a nanoscale momentum, an impetus with the opposite sign is applied to the plasmonic structure that can, when illuminated with linearly plasmonic structure and provides the driving torque. -
How Molecules Became Machines
THE NOBEL PRIZE IN CHEMISTRY 2016 POPULAR SCIENCE BACKGROUND How molecules became machines The Nobel Prize in Chemistry 2016 is awarded to Jean-Pierre Sauvage, Sir J. Fraser Stoddart and Bernard L. Feringa for their development of molecular machines that are a thousand times thinner than a hair strand. This is the story of how they succeeded in linking molecules together to design everything from a tiny lift to motors and miniscule muscles. How small can you make machinery? This is the question that Nobel Laureate Richard Feynman, famed for his 1950s’ predictions of developments in nanotechnology, posed at the start of a visionary lecture in 1984. Barefoot, and wearing a pink polo top and beige shorts, he turned to the audience and said: “Now let us talk about the possibility of making machines with movable parts, which are very tiny.” He was convinced it was possible to build machines with dimensions on the nanometre scale. These already existed in nature. He gave bacterial flagella as an example, corkscrew-shaped macromole- cules which, when they spin, make bacteria move forward. But could humans – with their gigantic hands – build machines so small that you would need an electron microscope to see them? A vision of the future – molecular machines will exist within 25–30 years One possible way would be to build a pair of mechanical hands that are smaller than your own, which in turn build a pair of smaller hands, which build even smaller hands, and so on, until a pair of miniscule hands can build equally miniscule machinery. -
Design and Fabrication of Moto Autor
A. John Joseph Clinton Int. Journal of Engineering Research and Applications www.ijera.com ISSN : 2248-9622, Vol. 5, Issue 1( Part 4), January 2015, pp.07-16 RESEARCH ARTICLE OPEN ACCESS Design and Fabrication of Moto Autor A. John Joseph Clinton*, P. Rajkumar** *(Department of Mechanical Engineering, Chandy College of Engineering, Affliated to Anna University- Chennai, Tuticorin-05) ** (Department of Mechanical Engineering, Chandy College of Engineering,Affliated to Anna University- Chennai, Tuticorin-05) ABSTRACT This project is based on the need for the unconventional motor. This work will be another addition in the unconventional revolution. Our project is mainly composed of design and fabrication of the ―MOTO AUTOR‖ which is a replacement of conventional motors in many applications of it. This motoautor can run on its own without any traditional input for fuelling it except for the initiation where permanent magnets has to be installed at first. It is a perpetual motion system that can energize itself by taking up the free energy present in the nature itself. This project enables to motorize systems with very minimal expenditure of energy. Keywords–Perpetual motion, Free energy conversion, Unconventional motor, Magnetic principles, Self- energizing I. INTRODUCTION Perhaps the first electric motors were In normal motoring mode, most electric motors simple electrostatic devices created by the Scottish operate through the interaction between an electric monk Andrew Gordon in the 1740s. The theoretical motor's magnetic field and winding currents to principle behind production of mechanical force by generate force within the motor. In certain the interactions of an electric current and a magnetic applications, such as in the transportation industry field, Ampère's force law, was discovered later with traction motors, electric motors can operate in by André-Marie Ampère in 1820. -
Catalytic Nanomotors: Fabrication, Mechanism, and Applications
Front. Mater. Sci. 2011, 5(1): 25–39 DOI 10.1007/s11706-011-0120-x REVIEW ARTICLE Catalytic nanomotors: fabrication, mechanism, and applications John GIBBS (✉) and Yiping ZHAO Nanoscale Science and Engineering Center, Department of Physics and Astronomy, The University of Georgia, Athens, GA 30602, USA © Higher Education Press and Springer-Verlag Berlin Heidelberg 2011 ABSTRACT: Catalytic nanomotors are nano-to-micrometer-sized actuators that carry an on-board catalyst and convert local chemical fuel in solution into mechanical work. The location of this catalyst as well as the geometry of the structure dictate the swimming behaviors exhibited. The nanomotors can occur naturally in organic molecules, combine natural and artificial parts to form hybrid nanomotors or be purely artificial. Fabrication techniques consist of template directed electroplating, lithography, physical vapor deposition, and other advanced growth methods. Various physical and chemical propulsion mechanisms have been proposed to explain the motion behaviors including diffusiophoresis, bubble propulsion, interfacial tension gradients, and self-electropho- resis. The control and manipulation based upon external fields, catalytic alloys, and motion control through thermal modulation are discussed as well. Catalytic nanomotors represent an exciting technological challenge with the end goal being practical functional nanomachines that can perform a variety of tasks at the nanoscale. KEYWORDS: nanomotors, catalysis, glancing angle deposition (GLAD), bubble propul- sion, self-electrophoresis 1 Introduction of subfields that may greatly benefit from this research [1– 7]. Clearly, mobility and control of motion of nanoma- Recent advances in the field of catalytic nanomotors which chines and nanoactuators will have drastic consequences are capable of moving autonomously constitute a major on future technologies, and applications yet unimagined step forward to develop practicable functional nanoma- are possible rendering this research as a merited invest- chines. -
Nanomotor Mechanisms and Motive Force Distributions from Nanorotor Trajectories
PHYSICAL REVIEW E 88,062317(2013) Nanomotor mechanisms and motive force distributions from nanorotor trajectories 1,2 1 1 2,* 1,3,4, Amir Nourhani, Young-Moo Byun, Paul E. Lammert, Ali Borhan, and Vincent H. Crespi † 1Department of Physics, Pennsylvania State University, University Park, Pennsylvania 16802, USA 2Department of Chemical Engineering, Pennsylvania State University, University Park, Pennsylvania 16802, USA 3Department of Chemistry, Pennsylvania State University, University Park, Pennsylvania 16802, USA 4Department of Materials Science and Engineering, Pennsylvania State University, University Park, Pennsylvania 16802, USA (Received 27 May 2013; revised manuscript received 3 October 2013; published 30 December 2013) Nanomotors convert chemical energy into mechanical motion. For a given motor type, the underlying chemical reaction that enables motility is typically well known, but the detailed, quantitative mechanism by which this reaction breaks symmetry and converts chemical energy to mechanical motion is often less clear, since it is difficult experimentally to measure important parameters such as the spatial distribution of chemical species around the nanorotor during operation. Without this information on how motor geometry affects motor function, it is difficult to control and optimize nanomotor behavior. Here we demonstrate how one easily observable characteristic of nanomotor operation—the visible trajectory of a nanorotor—can provide quantitative information about the role of asymmetry in nanomotor operation, as well as insights into the spatial distribution of motive force along the surface of the nanomotor, the motive torques, and the effective diffusional motion. DOI: 10.1103/PhysRevE.88.062317 PACS number(s): 82.70.Dd, 47.63.mf, 05.40. a − I. INTRODUCTION In contrast to linear nanomotors, the emerging class of colloidal rotary motors remains largely unexplored theo- Chemically powered self-propelled nanomotors have retically. -
Driving Carbon Nanotube to Rotate by Diamond Wedges at Room Temperature
Driving carbon nanotube to rotate by diamond wedges at room temperature Jiao Shi 1, Aiqin Wang 1, Kun Cai 2,* 1 College of Water Resources and Architectural Engineering, the Northwest A&F University, Yangling 712100, China 2 Centre for Innovative Structures and Materials, School of Engineering, the RMIT University, Melbourne 3001, Australia *Corresponding author’s email address: [email protected] (K. C.) Abstract: A rotary nanomotor made of carbon nanostructures is introduced here. Through a rotationally symmetrical layout of diamond wedges (or needles) outside of a carbon nanotube and with the [100] direction of diamond along the tube’s axial direction, the wedge needle tips can drive the nanotube to rotate at gigahertz frequency at room temperature. During thermal vibration, some of the atoms in the nanotube collide with the needle tips. The tips provide the atoms with continuous repulsion during collision. The tangential component of the repulsion force produces a moment onto the nanotube about the tube axis. Consequently, the nanotube is driven to rotate by the moment. The rotor reaches stable rotation when the concentric outer tubes provide equivalent resistance against the repulsion from needle tips. Molecular dynamics simulation results indicate that the stability of the needle tips influences the rotational frequency of the rotor. Potential fabrication of such a nanomotor is illustrated with consideration of miniaturization. The rotary motor can act as an engine in a nanomachine. Keywords: nanomotor, carbon nanotube, diamond, molecular dynamics 1. Introduction Carbon has many natural allotropes with different configurations at nanoscale, e.g., fullerene (zero-dimension) [1, 2], nanotube (one-dimension) [3], graphene (two-dimension) [4, 5], and diamond (three-dimension).