The Smart Energy Network: Electricity's Third Great Revolution
Total Page:16
File Type:pdf, Size:1020Kb
Load more
Recommended publications
-
(Nxpowerlite).Ppt
MAP/Ming Professorship, Engineering School, Stanford University, 29 March 2007 CEE 173L/273L: Advanced Energy End-Use Efficiency Public Lectures in Advanced Energy Efficiency: 4. Implementation “To be truly radical is to make hope possible, not despair convincing.” — Raymond Williams Amory B. Lovins Chairman and Chief Scientist Rocky Mountain Institute www .rmi.org [email protected] Copyright © 2007 Stanford University. All rights reserved. Distribution licensed to Rocky Mountain Institute. Osage (Iowa) municipal utilities ◊ 11 employees serving ~3,800 population ◊ A decade of demand-side management advice to homes and small businesses: Prepaid all the debt and built a $2.5M emergency fund Cut the rates 5 times in 5 y (by 1/3 real, to 1/2 IA av.) Kept existing factories competitive & attracted two more Kept >$1,000/household-y in town, supporting local jobs and multipliers Made Osage noticeably more prosperous than comparable neighboring towns ◊ If you can’t keep the bathtub full because the water keeps running out…do you need a bigger water-heater, or do you need a plug? U.S. energy/GDP already cut 46%, to very nearly the 1976 “soft path” 250 primary energy consumption (quadrillion BTU/year) 200 "hard path" projected by industry and government ~1975 government USEIA Annual 150 Energy Outlook actual total actual total energy saved 86 q/y = Reference Case, consumption 2004 and 2006 reported by USEIAconsumption 2.12× 2005 oil 100 "soft path" proposed by Lovins, Foreign Affairs , Fall 1976 coal gas oil and gas 50 soft technologies oil -
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. -
University of Cincinnati
UNIVERSITY OF CINCINNATI 05/29/08 Date:___________________ Carl Sterner I, _________________________________________________________, hereby submit this work as part of the requirements for the degree of: Master in: Architecture It is entitled: A Sustainable Pattern Language: A Comprehensive Approach to Sustainable Design This work and its defense approved by: Chair: T_om__ _Bible___________________________ Elizabeth______ _Riorden________________________ Michael_____ _Zaretsky_________________________ _______________________________ _______________________________ A Sustainable Pattern Language: A Comprehensive Approach to Sustainable Design Carl S. Sterner Bachelor of Architecture University of Cincinnati, 2006 Submitted in partial fulfillment of the requirements for the degree of Master of Architecture University of Cincinnati College of Design, Architecture, Art & Planning School of Architecture & Interior Design Committee Members: G. Thomas Bible Elizabeth Riorden Michael Zaretsky May 2008 Copyright © 2008 by Carl S. Sterner All rights reserved. Please direct reprint requests and questions to: Carl S. Sterner, [email protected] Abstract Sustainable design as presently prac- ticed focuses on technical solutions, ignoring the socio-cultural dimensions of sustainability. A truly sustainable society will require substantial change to our economic structure and social order. Architecture must therefore en- gage both the social and technical di- mensions of sustainability. This thesis attempts to understand the architectural implications -
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]. -
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. -
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. -
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. -
Cleaner Energy, Greener Profits
Cleaner Energy, Greener Profits: Fuel Cells as Cost-Effective Distributed Energy Resources Contents: Executive Summary . 2 By Joel N. Swisher, Ph.D., P.E. Introduction . 4 Rocky Mountain Institute Fuel cells: A small, clean,reliable This publication and its underlying research were funded power source . 6 by the grants from the W. Alton Jones Foundation, What is different Pew Charitable Trusts, and Energy Foundation. about today’s electricity problems? The author, a civil and mechanical engineer with a . 8 Stanford doctorate in civil and environmental engineering, is an authority on distributed generation Changing Trends in and leads RMI’s Energy and Resource Services team. the Electricity Industry . 9 Small is profitable: the economic benefits of distributed generation . 13 Early markets and commercialization paths . 32 Cleaner Energy, Greener Profits Executive Summary The electric power industry is undergoing centrally focused “generation-transmission- major changes that are reshaping the traditional distribution” companies into a more heteroge- roles of utilities, creating opportunities for new neous structure. The new industry will be made technologies, and redefining the scope and up of companies fulfilling various traditional character of government regulation. These roles, including independent power producers, changes are arising out of the interaction of electric service providers, energy brokers and several driving forces: marketers, transmission operators, and local distribution companies. • An emerging technological shift could offer distributed generation sources economic One of the most promising and exciting distrib- benefits unavailable to traditional, central- uted generation (DG) options is fuel cell ized sources of electricity. technology, which converts fuel to electricity at • Regulatory and public policy support is high efficiency, without combustion, and with growing for competition over traditional negligible emissions. -
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. -
Principles of HVDC Transmission
Principles of HVDC Transmission Course No: E04-036 Credit: 4 PDH Velimir Lackovic, Char. Eng. Continuing Education and Development, Inc. 22 Stonewall Court Woodcliff Lake, NJ 07677 P: (877) 322-5800 [email protected] PRINCIPLES OF HVDC TRANSMISSION The question that is frequently discussed is: “Why does anyone want to use D.C. transmission?” One reply is that electric losses are lower, but this is not true. Amount of losses is determined by the rating and size of chosen conductors. Both D.C. and A.C. conductors, either as transmission circuits or submarine cables can generate lower power losses but at increased cost since the bigger cross-sectional conductors will typically lead to lower power losses but will unfortunately cost more. When power converters are utilized for D.C. electrical transmission in preference to A.C. electrical transmission, it is commonly impacted by one of the causes: An overhead D.C. line with associated overhead line towers can be made as less pricey per unit of length than the same A.C. transmission line made to transfer the equivalent amount of electric power. Nevertheless the D.C. converter stations at transmission line terminal ends are more expensive than the stations at terminals of an A.C. transmission line. Therefore there is a breakeven length above which the overall price of D.C. electrical transmission is lower than its A.C. electrical transmission option. The D.C. electrical transmission line can have a lower visual impact than the same A.C. transmission line, producing lower environmental effect. There are additional environmental advantages to a D.C. -
High Dielectric Permittivity Materials in the Development of Resonators Suitable for Metamaterial and Passive Filter Devices at Microwave Frequencies
ADVERTIMENT. Lʼaccés als continguts dʼaquesta tesi queda condicionat a lʼacceptació de les condicions dʼús establertes per la següent llicència Creative Commons: http://cat.creativecommons.org/?page_id=184 ADVERTENCIA. El acceso a los contenidos de esta tesis queda condicionado a la aceptación de las condiciones de uso establecidas por la siguiente licencia Creative Commons: http://es.creativecommons.org/blog/licencias/ WARNING. The access to the contents of this doctoral thesis it is limited to the acceptance of the use conditions set by the following Creative Commons license: https://creativecommons.org/licenses/?lang=en High dielectric permittivity materials in the development of resonators suitable for metamaterial and passive filter devices at microwave frequencies Ph.D. Thesis written by Bahareh Moradi Under the supervision of Dr. Juan Jose Garcia Garcia Bellaterra (Cerdanyola del Vallès), February 2016 Abstract Metamaterials (MTMs) represent an exciting emerging research area that promises to bring about important technological and scientific advancement in various areas such as telecommunication, radar, microelectronic, and medical imaging. The amount of research on this MTMs area has grown extremely quickly in this time. MTM structure are able to sustain strong sub-wavelength electromagnetic resonance and thus potentially applicable for component miniaturization. Miniaturization, optimization of device performance through elimination of spurious frequencies, and possibility to control filter bandwidth over wide margins are challenges of present and future communication devices. This thesis is focused on the study of both interesting subject (MTMs and miniaturization) which is new miniaturization strategies for MTMs component. Since, the dielectric resonators (DR) are new type of MTMs distinguished by small dissipative losses as well as convenient conjugation with external structures; they are suitable choice for development process.