ETD Template
Total Page:16
File Type:pdf, Size:1020Kb
Load more
Recommended publications
-
Analysis and Measurement of Anti-Reciprocal Systems By
ANALYSIS AND MEASUREMENT OF ANTI-RECIPROCAL SYSTEMS BY NOORI KIM DISSERTATION Submitted in partial fulfillment of the requirements for the degree of Doctor of Philosophy in Electrical and Computer Engineering in the Graduate College of the University of Illinois at Urbana-Champaign, 2014 Urbana, Illinois Doctoral Committee: Associate Professor Jont B. Allen, Chair Professor Stephen Boppart Professor Steven Franke Associate Professor Michael Oelze ABSTRACT Loudspeakers, mastoid bone-drivers, hearing-aid receivers, hybrid cars, and more – these “anti-reciprocal” systems are commonly found in our daily lives. However, the depth of understanding about the systems has not been well addressed since McMillan in 1946. The goal of this study is to provide an intuitive and clear understanding of the systems, beginning from modeling one of the most popular hearing-aid receivers, a balanced armature receiver (BAR). Models for acoustic transducers are critical in many acoustic applications. This study analyzes a widely used commercial hearing-aid receiver, manufactured by Knowles Electron- ics, Inc (ED27045). Electromagnetic transducer modeling must consider two key elements: a semi-inductor and a gyrator. The semi-inductor accounts for electromagnetic eddy cur- rents, the “skin effect” of a conductor, while the gyrator accounts for the anti-reciprocity characteristic of Lenz’s law. Aside from the work of Hunt, to our knowledge no publications have included the gyrator element in their electromagnetic transducer models. The most prevalent method of transducer modeling evokes the mobility method, an ideal transformer alternative to a gyrator followed by the dual of the mechanical circuit. The mobility ap- proach greatly complicates the analysis. The present study proposes a novel, simplified, and rigorous receiver model. -
SSB-Filters (PART 4)
--------- ELECTRONICS --------------------- SSB-FilterS (PART 4) ELECTRONICS This is the fourth article of a tivity and stability characteristics, with mtmaturization of equipment. This is the fourth article of a series from a training course written but their large size makes them Also to the advantage of the me series from a training course written by Collins Radio Company for per subject to shock or vibration de· chanical filter is a Q in the order by Collins Radio Company for per- sonnel concerned with single side terioration. Also, their cost is of 10,000 which is about 100 times sonnel concerned with single side- band communications. quite high. the Q obtainable with electrical band communications. Both SSB transmitters and SSB Newer crystal filters are being elements. Both SSB transmitters and SSB developed that have extended fre receivers require very selective receivers require very selective Although the commercial use of bandpass filters in the region of bandpass filters in the region of quency range and are smaller. These mechanical filters is relatively 100 to 500 kilocycles. 100 to 500 kilocycles. newer crystal filters are more ac new, the basic principles on which In receivers, a high order of ad- In receivers, a high order of ad ceptable for use in SSB equipment. they are based is well established. jacent channel rejection is required jacent channel rejection is required LC Filters The mechanical filter is a me if channels are to be closely spaced if channels are to be closely spaced LC filters have been used at IF chanically resonant device that re to conserve spectrum space. -
A Centrality Measure for Electrical Networks
Carnegie Mellon Electricity Industry Center Working Paper CEIC-07 www.cmu.edu/electricity 1 A Centrality Measure for Electrical Networks Paul Hines and Seth Blumsack types of failures. Many classifications of network structures Abstract—We derive a measure of “electrical centrality” for have been studied in the field of complex systems, statistical AC power networks, which describes the structure of the mechanics, and social networking [5,6], as shown in Figure 2, network as a function of its electrical topology rather than its but the two most fruitful and relevant have been the random physical topology. We compare our centrality measure to network model of Erdös and Renyi [7] and the “small world” conventional measures of network structure using the IEEE 300- bus network. We find that when measured electrically, power model inspired by the analyses in [8] and [9]. In the random networks appear to have a scale-free network structure. Thus, network model, nodes and edges are connected randomly. The unlike previous studies of the structure of power grids, we find small-world network is defined largely by relatively short that power networks have a number of highly-connected “hub” average path lengths between node pairs, even for very large buses. This result, and the structure of power networks in networks. One particularly important class of small-world general, is likely to have important implications for the reliability networks is the so-called “scale-free” network [10, 11], which and security of power networks. is characterized by a more heterogeneous connectivity. In a Index Terms—Scale-Free Networks, Connectivity, Cascading scale-free network, most nodes are connected to only a few Failures, Network Structure others, but a few nodes (known as hubs) are highly connected to the rest of the network. -
Electrical Impedance Tomography
INSTITUTE OF PHYSICS PUBLISHING INVERSE PROBLEMS Inverse Problems 18 (2002) R99–R136 PII: S0266-5611(02)95228-7 TOPICAL REVIEW Electrical impedance tomography Liliana Borcea Computational and Applied Mathematics, MS 134, Rice University, 6100 Main Street, Houston, TX 77005-1892, USA E-mail: [email protected] Received 16 May 2002, in final form 4 September 2002 Published 25 October 2002 Online at stacks.iop.org/IP/18/R99 Abstract We review theoretical and numerical studies of the inverse problem of electrical impedance tomographywhich seeks the electrical conductivity and permittivity inside a body, given simultaneous measurements of electrical currents and potentials at the boundary. (Some figures in this article are in colour only in the electronic version) 1. Introduction Electrical properties such as the electrical conductivity σ and the electric permittivity , determine the behaviour of materials under the influence of external electric fields. For example, conductive materials have a high electrical conductivity and both direct and alternating currents flow easily through them. Dielectric materials have a large electric permittivity and they allow passage of only alternating electric currents. Let us consider a bounded, simply connected set ⊂ Rd ,ford 2and, at frequency ω, let γ be the complex admittivity function √ γ(x,ω)= σ(x) +iω(x), where i = −1. (1.1) The electrical impedance is the inverse of γ(x) and it measures the ratio between the electric field and the electric current at location x ∈ .Electrical impedance tomography (EIT) is the inverse problem of determining the impedance in the interior of ,givensimultaneous measurements of direct or alternating electric currents and voltages at the boundary ∂. -
Nonreciprocal Wavefront Engineering with Time-Modulated Gradient Metasurfaces J
Nonreciprocal Wavefront Engineering with Time-Modulated Gradient Metasurfaces J. W. Zang1,2, D. Correas-Serrano1, J. T. S. Do1, X. Liu1, A. Alvarez-Melcon1,3, J. S. Gomez-Diaz1* 1Department of Electrical and Computer Engineering, University of California Davis One Shields Avenue, Kemper Hall 2039, Davis, CA 95616, USA. 2School of Information and Electronics, Beijing Institute of Technology, Beijing 100081, China 3 Universidad Politécnica de Cartagena, 30202 Cartagena, Spain *E-mail: [email protected] We propose a paradigm to realize nonreciprocal wavefront engineering using time-modulated gradient metasurfaces. The essential building block of these surfaces is a subwavelength unit-cell whose reflection coefficient oscillates at low frequency. We demonstrate theoretically and experimentally that such modulation permits tailoring the phase and amplitude of any desired nonlinear harmonic and determines the behavior of all other emerging fields. By appropriately adjusting the phase-delay applied to the modulation of each unit-cell, we realize time-modulated gradient metasurfaces that provide efficient conversion between two desired frequencies and enable nonreciprocity by (i) imposing drastically different phase-gradients during the up/down conversion processes; and (ii) exploiting the interplay between the generation of certain nonlinear surface and propagative waves. To demonstrate the performance and broad reach of the proposed platform, we design and analyze metasurfaces able to implement various functionalities, including beam steering and focusing, while exhibiting strong and angle-insensitive nonreciprocal responses. Our findings open a new direction in the field of gradient metasurfaces, in which wavefront control and magnetic-free nonreciprocity are locally merged to manipulate the scattered fields. 1. Introduction Gradient metasurfaces have enabled the control of electromagnetic waves in ways unreachable with conventional materials, giving rise to arbitrary wavefront shaping in both near- and far-fields [1-6]. -
Mechanical Engineering 310 Documentation 2018-2019
P a g e | 1 X Y L E M MECHANICAL ENGINEERING 310 DOCUMENTATION 2018-2019 Mechanical Engineering Design Group 416 Escondido Mall Stanford University Stanford, CA 94305- 2203 http://me310.stanford.edu Team Xylem: Adit Desai Fay Nicole Colah Okkeun Lee Tin Jing jie Dai Jiang Mika Julin Nina Saarikoski Samuel Moy Timo Moyer 1 Executive Summary This report summarizes the work completed by the Stanford University (SU) and Aalto University (AU) Teams during the 2018-19 Academic Year for ME310 with our corporate sponsor Xylem Inc. In Autumn Quarter 2018, the SU team explored the concept of a modified drip irrigation system designed to reduce the amount of water lost due to evaporation during irrigation, and an oyster based water filtration system which aimed to replicate the mucus in oysters to trap contaminants to purify water. In Winter Quarter 2019, the SU team explored the concept of a human powered personal and floor-based filtration system, which achieved flow rates of up to 80 times faster as compared to gravity fed methods. In Spring Quarter 2019 after the Winter Break in Aalto University, the SU and AU teams converged on a final product design concept and user, which was a low cost, modular and highly maintainable water filtration system which could remove heavy metals, pathogens and sediments from contaminated waters. The filtration system was designed such that clean drinking water could be provided to rural children in developing countries who did not have access to an electrical supply. A key nature-inspired filtration technology of this system was the usage of microalgae (Chlorella Vulgaris) for batch removal of heavy metals, where literature research reported that small quantities of such algae are able to remove significant quantities (~88%) of heavy metals from contaminated waters within 30 minutes. -
Electric Currents in Infinite Networks
Electric currents in infinite networks Peter G. Doyle Version dated 25 October 1988 GNU FDL∗ 1 Introduction. In this survey, we will present the basic facts about conduction in infinite networks. This survey is based on the work of Flanders [5, 6], Zemanian [17], and Thomassen [14], who developed the theory of infinite networks from scratch. Here we will show how to get a more complete theory by paralleling the well-developed theory of conduction on open Riemann surfaces. Like Flanders and Thomassen, we will take as a test case for the theory the problem of determining the resistance across an edge of a d-dimensional grid of 1 ohm resistors. (See Figure 1.) We will use our borrowed network theory to unify, clarify and extend their work. 2 The engineers and the grid. Engineers have long known how to compute the resistance across an edge of a d-dimensional grid of 1 ohm resistors using only the principles of symmetry and superposition: Given two adjacent vertices p and q, the resistance across the edge from p to q is the voltage drop along the edge when a 1 amp current is injected at p and withdrawn at q. Whether or not p and q are adjacent, the unit current flow from p to q can be written as the superposition of the unit ∗Copyright (C) 1988 Peter G. Doyle. Permission is granted to copy, distribute and/or modify this document under the terms of the GNU Free Documentation License, as pub- lished by the Free Software Foundation; with no Invariant Sections, no Front-Cover Texts, and no Back-Cover Texts. -
Note on Mechanical Filtration and Gravitation Filtration (Paper & Discussion)
69 Victorian Institute of Engineers. A FEW NOTES ON MECHANICAL FILTRATION IN CONNECTION WITH WATER SUPPLIES. Read by MR. GEORGE SWINBURNE, 7M August, 1901. In this short paper I make no pretence at originality, but with a view to initiating discussion, will endeavour to give the result of a few enquiries on this important matter in which I have taken a little interest. The system adopted in older countries of filtering through sand beds is not adaptable to Australian conditions in the great majority of cases; yet there is no doubt that something must be done in the near future to better the condition of water supply in the smaller towns of Australia. In the large centres of population, where watershed areas are preserved, a good state of things _ mày exist, but in the country districts, the only available supplies are from doubtful springs, lather stagnant rivers which have already been polluted further up, or dams open to dust storms and all kinds of impurities, which are only filled when it rains in the immediate neighbourhood. It is rarely that the people themselves take much interest in the question, except to grumble when things are very bad. To engineers and sanitary authorities it is one of the most important questions in our modern life. Pure water means good health, but half the population of this continent is content to put up with Typhoid and the ills attending a supply of bad water, rather than help or pay to have the supply placed on the best possible footing. In my opinion this state of things exists on account of the supplies being in the hands of the local authorities or trusts, and the members not realising the importance of the matter. -
Modelling of Anisotropic Electrical Conduction in Layered Structures 3D-Printed with Fused Deposition Modelling
sensors Article Modelling of Anisotropic Electrical Conduction in Layered Structures 3D-Printed with Fused Deposition Modelling Alexander Dijkshoorn 1,* , Martijn Schouten 1 , Stefano Stramigioli 1,2 and Gijs Krijnen 1 1 Robotics and Mechatronics Group (RAM), University of Twente, 7500 AE Enschede, The Netherlands; [email protected] (M.S.); [email protected] (S.S.); [email protected] (G.K.) 2 Biomechatronics and Energy-Efficient Robotics Lab, ITMO University, 197101 Saint Petersburg, Russia * Correspondence: [email protected] Abstract: 3D-printing conductive structures have recently been receiving increased attention, es- pecially in the field of 3D-printed sensors. However, the printing processes introduce anisotropic electrical properties due to the infill and bonding conditions. Insights into the electrical conduction that results from the anisotropic electrical properties are currently limited. Therefore, this research focuses on analytically modeling the electrical conduction. The electrical properties are described as an electrical network with bulk and contact properties in and between neighbouring printed track elements or traxels. The model studies both meandering and open-ended traxels through the application of the corresponding boundary conditions. The model equations are solved as an eigenvalue problem, yielding the voltage, current density, and power dissipation density for every position in every traxel. A simplified analytical example and Finite Element Method simulations verify the model, which depict good correspondence. The main errors found are due to the limitations of the model with regards to 2D-conduction in traxels and neglecting the resistance of meandering Citation: Dijkshoorn, A.; Schouten, ends. Three dimensionless numbers are introduced for the verification and analysis: the anisotropy M.; Stramigioli, S.; Krijnen, G. -
Inf 5490 Rf Mems
INF 5490 RF MEMS LN10: Micromechanical filters Spring 2011, Oddvar Søråsen Jan Erik Ramstad Department of Informatics, UoO 1 Today’s lecture • Properties of mechanical filters • Visualization and working principle • Modeling • Examples • Design procedure • Mixer 2 Mechanical filters • Well-known for several decades – Jmfr. book: ”Mechanical filters in electronics”, R.A. Johnson, 1983 • Miniaturization of mechanical filters makes it more interesting to use – Possible by using micromachining – Motivation Fabrication of small integrated filters: ”system-on-chip” with good filter performance 3 Filter response 4 Several resonators used • One silingle resonathtor has a narrow BP- response – Good for d e fini ng oscill a tor frequency – Not good for BP-filter • BP-filters are implemented by coupling resonators in cascade – Gives a wider pass band than using one single resonating structure – 2 or more micro resonators are used • Each of comb type or c-c beam type (or other types) – Connected by soft springs 5 Filter order • NbNumber o f resonators, n, defines the filter order – Order = 2 * n – Sharper ”roll-off” to stop band when several resonators are used • ”sharper filter” 6 Micromachined filter properties • + CtCompact ilimplemen ttitation – ”on-chip” filter bank possible • + Hig h Q -ftfactor can bbidbe obtained • + Low-loss BP-filters can be implemented – The individual resonators have low loss – Low total ”Insertion loss, IL” • IL: Degraded for small bandwidth • IL: Improved for high Q-factor 7 ”Insertion loss ” IL: Degraded for small -
Thermal-Electrical Analogy: Thermal Network
Chapter 3 Thermal-electrical analogy: thermal network 3.1 Expressions for resistances Recall from circuit theory that resistance �"#"$ across an element is defined as the ratio of electric potential difference Δ� across that element, to electric current I traveling through that element, according to Ohm’s law, � � = "#"$ � (3.1) Within the context of heat transfer, the respective analogues of electric potential and current are temperature difference Δ� and heat rate q, respectively. Thus we can establish “thermal circuits” if we similarly establish thermal resistances R according to Δ� � = � (3.2) Medium: λ, cross-sectional area A Temperature T Temperature T Distance r Medium: λ, length L L Distance x (into the page) Figure 3.1: System geometries: planar wall (left), cylindrical wall (right) Planar wall conductive resistance: Referring to Figure 3.1 left, we see that thermal resistance may be obtained according to T1,3 − T1,5 � �, $-./ = = (3.3) �, �� The resistance increases with length L (it is harder for heat to flow), decreases with area A (there is more area for the heat to flow through) and decreases with conductivity �. Materials like styrofoam have high resistance to heat flow (they make good thermal insulators) while metals tend to have high low resistance to heat flow (they make poor insulators, but transmit heat well). Cylindrical wall conductive resistance: Referring to Figure 3.1 right, we have conductive resistance through a cylindrical wall according to T1,3 − T1,5 ln �5 �3 �9 $-./ = = (3.4) �9 2��� Convective resistance: The form of Newton’s law of cooling lends itself to a direct form of convective resistance, valid for either geometry. -
S-Parameter Techniques – HP Application Note 95-1
H Test & Measurement Application Note 95-1 S-Parameter Techniques Contents 1. Foreword and Introduction 2. Two-Port Network Theory 3. Using S-Parameters 4. Network Calculations with Scattering Parameters 5. Amplifier Design using Scattering Parameters 6. Measurement of S-Parameters 7. Narrow-Band Amplifier Design 8. Broadband Amplifier Design 9. Stability Considerations and the Design of Reflection Amplifiers and Oscillators Appendix A. Additional Reading on S-Parameters Appendix B. Scattering Parameter Relationships Appendix C. The Software Revolution Relevant Products, Education and Information Contacting Hewlett-Packard © Copyright Hewlett-Packard Company, 1997. 3000 Hanover Street, Palo Alto California, USA. H Test & Measurement Application Note 95-1 S-Parameter Techniques Foreword HEWLETT-PACKARD JOURNAL This application note is based on an article written for the February 1967 issue of the Hewlett-Packard Journal, yet its content remains important today. S-parameters are an Cover: A NEW MICROWAVE INSTRUMENT SWEEP essential part of high-frequency design, though much else MEASURES GAIN, PHASE IMPEDANCE WITH SCOPE OR METER READOUT; page 2 See Also:THE MICROWAVE ANALYZER IN THE has changed during the past 30 years. During that time, FUTURE; page 11 S-PARAMETERS THEORY AND HP has continuously forged ahead to help create today's APPLICATIONS; page 13 leading test and measurement environment. We continuously apply our capabilities in measurement, communication, and computation to produce innovations that help you to improve your business results. In wireless communications, for example, we estimate that 85 percent of the world’s GSM (Groupe Speciale Mobile) telephones are tested with HP instruments. Our accomplishments 30 years hence may exceed our boldest conjectures.