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The Effects of High Frequency Current Ripple on Electric Vehicle Battery Performance
Original citation: Uddin, Kotub , Moore, Andrew D. , Barai, Anup and Marco, James. (2016) The effects of high frequency current ripple on electric vehicle battery performance. Applied Energy, 178 . pp. 142-154. Permanent WRAP URL: http://wrap.warwick.ac.uk/80006 Copyright and reuse: The Warwick Research Archive Portal (WRAP) makes this work of researchers of the University of Warwick available open access under the following conditions. This article is made available under the Creative Commons Attribution 4.0 International license (CC BY 4.0) and may be reused according to the conditions of the license. For more details see: http://creativecommons.org/licenses/by/4.0/ A note on versions: The version presented in WRAP is the published version, or, version of record, and may be cited as it appears here. For more information, please contact the WRAP Team at: [email protected] warwick.ac.uk/lib-publications Applied Energy 178 (2016) 142–154 Contents lists available at ScienceDirect Applied Energy journal homepage: www.elsevier.com/locate/apenergy The effects of high frequency current ripple on electric vehicle battery performance ⇑ Kotub Uddin , Andrew D. Moore, Anup Barai, James Marco WMG, International Digital Laboratory, The University of Warwick, Coventry CV4 7AL, UK highlights Experimental study into the impact of current ripple on li-ion battery degradation. 15 cells exercised with 1200 cycles coupled AC–DC signals, at 5 frequencies. Results highlight a greater spread of degradation for cells exposed to AC excitation. Implications for BMS control, thermal management and system integration. article info abstract Article history: The power electronic subsystems within electric vehicle (EV) powertrains are required to manage both Received 8 April 2016 the energy flows within the vehicle and the delivery of torque by the electrical machine. -
Emotion Perception and Recognition: an Exploration of Cultural Differences and Similarities
Emotion Perception and Recognition: An Exploration of Cultural Differences and Similarities Vladimir Kurbalija Department of Mathematics and Informatics, Faculty of Sciences, University of Novi Sad Trg Dositeja Obradovića 4, 21000 Novi Sad, Serbia +381 21 4852877, [email protected] Mirjana Ivanović Department of Mathematics and Informatics, Faculty of Sciences, University of Novi Sad Trg Dositeja Obradovića 4, 21000 Novi Sad, Serbia +381 21 4852877, [email protected] Miloš Radovanović Department of Mathematics and Informatics, Faculty of Sciences, University of Novi Sad Trg Dositeja Obradovića 4, 21000 Novi Sad, Serbia +381 21 4852877, [email protected] Zoltan Geler Department of Media Studies, Faculty of Philosophy, University of Novi Sad dr Zorana Đinđića 2, 21000 Novi Sad, Serbia +381 21 4853918, [email protected] Weihui Dai School of Management, Fudan University Shanghai 200433, China [email protected] Weidong Zhao School of Software, Fudan University Shanghai 200433, China [email protected] Corresponding author: Vladimir Kurbalija, tel. +381 64 1810104 ABSTRACT The electroencephalogram (EEG) is a powerful method for investigation of different cognitive processes. Recently, EEG analysis became very popular and important, with classification of these signals standing out as one of the mostly used methodologies. Emotion recognition is one of the most challenging tasks in EEG analysis since not much is known about the representation of different emotions in EEG signals. In addition, inducing of desired emotion is by itself difficult, since various individuals react differently to external stimuli (audio, video, etc.). In this article, we explore the task of emotion recognition from EEG signals using distance-based time-series classification techniques, involving different individuals exposed to audio stimuli. -
Lesson 22: Determining Control Stability Using Bode Plots
11/30/2015 Lesson 22: Determining Control Stability Using Bode Plots 1 ET 438A AUTOMATIC CONTROL SYSTEMS TECHNOLOGY lesson22et438a.pptx Learning Objectives 2 After this presentation you will be able to: List the control stability criteria for open loop frequency response. Identify the gain and phase margins necessary for a stable control system. Use a Bode plot to determine if a control system is stable or unstable. Generate Bode plots of control systems the include dead-time delay and determine system stability. lesson22et438a.pptx 1 11/30/2015 Bode Plot Stability Criteria 3 Open loop gain of less than 1 (G<1 or G<0dB) at Stable Control open loop phase angle of -180 degrees System Oscillatory Open loop gain of exactly 1 (G=1 or G= 0dB) at Control System open loop phase angle of -180 degrees Marginally Stable Unstable Control Open loop gain of greater than 1 (G>1 or G>0dB) System at open loop phase angle of -180 degrees lesson22et438a.pptx Phase and Gain Margins 4 Inherent error and inaccuracies require ranges of phase shift and gain to insure stability. Gain Margin – Safe level below 1 required for stability Minimum level : G=0.5 or -6 dB at phase shift of 180 degrees Phase Margin – Safe level above -180 degrees required for stability Minimum level : f=40 degree or -180+ 40=-140 degrees at gain level of 0.5 or 0 dB. lesson22et438a.pptx 2 11/30/2015 Determining Phase and Gain Margins 5 Define two frequencies: wodB = frequency of 0 dB gain w180 = frequency of -180 degree phase shift Open Loop Gain 0 dB Gain Margin -m180 bodB Phase Margin -180+b0dB -180o Open Loop w w Phase odB 180 lesson22et438a.pptx Determining Phase and Gain Margins 6 Procedure: 1) Draw vertical lines through 0 dB on gain and -180 on phase plots. -
EE C128 Chapter 10
Lecture abstract EE C128 / ME C134 – Feedback Control Systems Topics covered in this presentation Lecture – Chapter 10 – Frequency Response Techniques I Advantages of FR techniques over RL I Define FR Alexandre Bayen I Define Bode & Nyquist plots I Relation between poles & zeros to Bode plots (slope, etc.) Department of Electrical Engineering & Computer Science st nd University of California Berkeley I Features of 1 -&2 -order system Bode plots I Define Nyquist criterion I Method of dealing with OL poles & zeros on imaginary axis I Simple method of dealing with OL stable & unstable systems I Determining gain & phase margins from Bode & Nyquist plots I Define static error constants September 10, 2013 I Determining static error constants from Bode & Nyquist plots I Determining TF from experimental FR data Bayen (EECS, UCB) Feedback Control Systems September 10, 2013 1 / 64 Bayen (EECS, UCB) Feedback Control Systems September 10, 2013 2 / 64 10 FR techniques 10.1 Intro Chapter outline 1 10 Frequency response techniques 1 10 Frequency response techniques 10.1 Introduction 10.1 Introduction 10.2 Asymptotic approximations: Bode plots 10.2 Asymptotic approximations: Bode plots 10.3 Introduction to Nyquist criterion 10.3 Introduction to Nyquist criterion 10.4 Sketching the Nyquist diagram 10.4 Sketching the Nyquist diagram 10.5 Stability via the Nyquist diagram 10.5 Stability via the Nyquist diagram 10.6 Gain margin and phase margin via the Nyquist diagram 10.6 Gain margin and phase margin via the Nyquist diagram 10.7 Stability, gain margin, and -
Switching-Ripple-Based Current Sharing for Paralleled Power Converters
Switching-ripple-based current sharing for paralleled power converters The MIT Faculty has made this article openly available. Please share how this access benefits you. Your story matters. Citation Perreault, D.J., K. Sato, R.L. Selders, and J.G. Kassakian. “Switching-Ripple-Based Current Sharing for Paralleled Power Converters.” IEEE Transactions on Circuits and Systems I: Fundamental Theory and Applications 46, no. 10 (1999): 1264–1274. © 1999 IEEE As Published http://dx.doi.org/10.1109/81.795839 Publisher Institute of Electrical and Electronics Engineers (IEEE) Version Final published version Citable link http://hdl.handle.net/1721.1/86985 Terms of Use Article is made available in accordance with the publisher's policy and may be subject to US copyright law. Please refer to the publisher's site for terms of use. 1264 IEEE TRANSACTIONS ON CIRCUITS AND SYSTEMS—I: FUNDAMENTAL THEORY AND APPLICATIONS, VOL. 46, NO. 10, OCTOBER 1999 Switching-Ripple-Based Current Sharing for Paralleled Power Converters David J. Perreault, Member, IEEE, Kenji Sato, Member, IEEE, Robert L. Selders, Jr., and John G. Kassakian, Fellow, IEEE Abstract— This paper presents the implementation and ex- perimental evaluation of a new current-sharing technique for paralleled power converters. This technique uses information naturally encoded in the switching ripple to achieve current sharing and requires no intercell connections for communicating this information. Practical implementation of the approach is addressed and an experimental evaluation, based on a three-cell prototype system, is also presented. It is shown that accurate and stable load sharing is obtained over a wide load range. Finally, an alternate implementation of this current-sharing technique is described and evaluated. -
IIR Filterdesign
UNIVERSITY OF OSLO IIR filterdesign Sverre Holm INF34700 Digital signalbehandling DEPARTMENT OF INFORMATICS UNIVERSITY OF OSLO Filterdesign 1. Spesifikasjon • Kjenne anven de lsen • Kjenne designmetoder (hva som er mulig, FIR/IIR) 2. Apppproksimas jon • Fokus her 3. Analyse • Filtre er som rege l spes ifiser t i fre kvens domene t • Også analysere i tid (fase, forsinkelse, ...) 4. Realisering • DSP, FPGA, PC: Matlab, C, Java ... DEPARTMENT OF INFORMATICS 2 UNIVERSITY OF OSLO Sources • The slides about Digital Filter Specifications have been a dap te d from s lides by S. Mitra, 2001 • Butterworth, Chebychev, etc filters are based on Wikipedia • Builds on Oppenheim & Schafer with Buck: Discrete-Time Signal Processing, 1999. DEPARTMENT OF INFORMATICS 3 UNIVERSITY OF OSLO IIR kontra FIR • IIR filtre er mer effektive enn FIR – færre koe ffisi en ter f or samme magnitu de- spesifikasjon • Men bare FIR kan gi eksakt lineær fase – Lineær fase symmetrisk h[n] ⇒ Nullpunkter symmetrisk om |z|=1 – Lineær fase IIR? ⇒ Poler utenfor enhetssirkelen ⇒ ustabilt • IIR kan også bli ustabile pga avrunding i aritme tikken, de t kan ikke FIR DEPARTMENT OF INFORMATICS 4 UNIVERSITY OF OSLO Ideal filters • Lavpass, høypass, båndpass, båndstopp j j HLP(e ) HHP(e ) 1 1 – 0 c c – c 0 c j j HBS(e ) HBP (e ) –1 1 – –c1 – – c2 c2 c1 c2 c2 c1 c1 DEPARTMENT OF INFORMATICS 5 UNIVERSITY OF OSLO Prototype low-pass filter • All filter design methods are specificed for low-pass only • It can be transformed into a high-pass filter • OiOr it can be p lace -
I Introduction and Background
Final Design Report Platform Motion Measurement System ELEC 492 A Senior Design Project, 2005 Between University of San Diego And Trex Enterprises Submitted to: Dr. Lord at USD Prepared by: YAZ Zlatko Filipovic Yoshitaka Yano August 12, 2005 University of San Diego Final Design Report USD August 12, 2005 Platform Motion Measurement System Table of Contents I. Acknowledgments…………...…………………………………………………………4 II. Executive Summary……..…………………………………………………………….5 III. Introduction and Background…...………………………...………………………….6 IV. Project Requirements…………….................................................................................8 V. Methodology of Design Plan……….…..……………..…….………….…..…….…..11 VI. Testing….……………………………………..…..…………………….……...........21 VII. Deliverables and Project Results………...…………...…………..…….…………...24 VIII. Budget………………………………………...……..……………………………..25 IX. Personnel…………………..………………………………………....….……….......28 X. Design Schedule………….…...……………………………….……...…………........29 XI. Reference and Bibliography…………..…………..…………………...…………….31 XII. Summary…………………………………………………………………………....32 Appendices Appendix 1. Simulink Simulations…..………………………….…….33 Appendix 2. VisSim Simulations..........……………………………….34 Appendix 3. Frequency Response and VisSim results……………......36 Appendix 4. Vibration Measurements…………..………………….….38 Appendix 5. PCB Layout and Schematic……………………………..39 Appendix 6. User’s Manual…………………………………………..41 Appendix 7. PSpice Simulations of Hfilter…………………………….46 1 Final Design Report USD August 12, 2005 Platform Motion Measurement System -
Output Ripple Voltage for Buck Switching Regulator (Rev. A)
Application Report SLVA630A–January 2014–Revised October 2014 Output Ripple Voltage for Buck Switching Regulator Surinder P. Singh, Ph.D., Manager, Power Applications Group............................. WEBENCH® Design Center ABSTRACT Switched-mode power supplies (SMPSs) are used to regulate voltage to a certain level. SMPSs have an inherent switching action, which causes the currents and voltages in the circuit to switch and fluctuate. The output voltage also has ripple on top of the regulated steady-state DC value. Designers of power systems consider the output voltage ripple to be both a key parameter for design considerations and a key figure of merit. The online WEBENCH® Power Designer recognizes the key importance of peak-to-peak voltage output ripple voltage—the ripple voltage is calculated and reported in the visualizer [1]. This application report presents a closed-form analytical formulation for the output voltage ripple waveform and the peak-to-peak ripple voltage. This formulation is accurate over all regions of operation and harmonizes the peak-to-peak ripple voltage calculation over all regions of operation. The new analytical formulation presented in this application report gives an accurate evaluation of the output ripple as compared to the simplified linear or root-mean square (RMS) approximations often used. In this application report, the analytical model for output voltage waveform and peak-to-peak ripple voltage for buck is derived. This model is validated against SPICE TINA-TI simulations. This report presents the behavior of ripple peak-to-voltage for various input conditions and choices of output capacitor and compare it against SPICE TINA-TI results. -
Meeting Design Specifications
NDSU Meeting Design Specs using Bode Plots ECE 461 Meeting Design Specs using Bode Plots When designing a compensator to meet design specs including: Steady-state error for a step input Phase Margin 0dB gain frequency the procedure using Bode plots is about the same as it was for root-locus plots. Add a pole at s = 0 if needed (making the system type-1) Start cancelling zeros until the system is too fast For every zero you added, add a pole. Place these poles so that the phase adds up. When using root-locus techniques, the phase adds up to 180 degrees at some spot on the s-plane. When using Bode plot techniques, the phase adds up to give you your phase margin at some spot on the jw axis. Example 1: Problem: Given the following system 1000 G(s) = (s+1)(s+3)(s+6)(s+10) Design a compensator which result in No error for a step input 20% overshoot for a step input, and A settling time of 4 second Solution: First, convert to Bode Plot terminology No overshoot means make this a type-1 system. Add a pole at s = 0. 20% overshoot means ζ = 0.4559 Mm = 1.2322 GK = 1∠ − 132.120 Phase Margin = 47.88 degrees A settling time of 4 seconds means s = -1 + j X s = -1 + j2 (from the damping ratio) The 0dB gain frequency is 2.00 rad/sec In short, design K(s) so that the system is type-1 and 0 (GK)s=j2 = 1∠ − 132.12 JSG 1 rev June 22, 2016 NDSU Meeting Design Specs using Bode Plots ECE 461 Start with s+1 K(s) = s At 4 rad/sec 1000 0 GK = s(s+3)(s+6)(s+10) = 2.1508∠ − 153.43 s=j2 There is too much phase shift, so start cancelling zeros. -
13.2 Analog Elliptic Filter Design
CHAPTER 13 IIR FILTER DESIGN 13.2 Analog Elliptic Filter Design This document carries out design of an elliptic IIR lowpass analog filter. You define the following parameters: fp, the passband edge fs, the stopband edge frequency , the maximum ripple Mathcad then calculates the filter order and finds the zeros, poles, and coefficients for the filter transfer function. Background Elliptic filters, so called because they employ elliptic functions to generate the filter function, are useful because they have equiripple characteristics in the pass and stopband regions. This ensures that the lowest order filter can be used to meet design constraints. For information on how to transform a continuous-time IIR filter to a discrete-time IIR filter, see Section 13.1: Analog/Digital Lowpass Butterworth Filter. For information on the lowest order polynomial (as opposed to elliptic) filters, see Section 14: Chebyshev Polynomials. Mathcad Implementation This document implements an analog elliptic lowpass filter design. The definitions below of elliptic functions are used throughout the document to calculate filter characteristics. Elliptic Function Definitions TOL ≡10−5 Im (ϕ) Re (ϕ) ⌠ 1 ⌠ 1 U(ϕ,k)≡1i⋅ ⎮――――――dy+ ⎮―――――――――dy ‾‾‾‾‾‾‾‾‾‾‾‾2‾ ‾‾‾‾‾‾‾‾‾‾‾‾‾‾‾‾‾‾2‾ ⎮ 2 ⎮ 2 ⌡ 1−k ⋅sin(1j⋅y) ⌡ 1−k ⋅sin(1j⋅ Im(ϕ)+y) 0 0 ϕ≡1i sn(uk, )≡sin(root(U(ϕ,k)−u,ϕ)) π ― 2 ⌠ 1 L(k)≡⎮――――――dy ‾‾‾‾‾‾‾‾‾‾2‾ ⎮ 2 ⌡ 1−k ⋅sin(y) 0 ⎛⎛ ⎞⎞ 2 1− ‾1‾−‾k‾2‾ V(k)≡――――⋅L⎜⎜――――⎟⎟ 1+ ‾1‾−‾k‾2‾ ⎝⎜⎝⎜ 1+ ‾1‾−‾k‾2‾⎠⎟⎠⎟ K(k)≡if(k<.9999,L(k),V(k)) Design Specifications First, the passband edge is normalized to 1 and the maximum passband response is set at one. -
Applications Academic Program Distributing Vissim Models
VISSIM VisSim is a visual block diagram language for simulation of dynamical systems and Model Based Design of embedded systems. It is developed by Visual Solutions of Westford, Massachusetts. Applications VisSim is widely used in control system design and digital signal processing for multidomain simulation and design. It includes blocks for arithmetic, Boolean, and transcendental functions, as well as digital filters, transfer functions, numerical integration and interactive plotting. The most commonly modeled systems are aeronautical, biological/medical, digital power, electric motor, electrical, hydraulic, mechanical, process, thermal/HVAC and econometric. Academic program The VisSim Free Academic Program allows accredited educational institutions to site license VisSim v3.0 for no cost. The latest versions of VisSim and addons are also available to students and academic institutions at greatly reduced pricing. Distributing VisSim models VisSim viewer screenshot with sample model. The free Vis Sim Viewer is a convenient way to share VisSim models with colleagues and clients not licensed to use VisSim. The VisSim Viewer will execute any VisSim model, and allows changes to block and simulation parameters to illustrate different design scenarios. Sliders and buttons may be activated if included in the model. Code generation The VisSim/C-Code add-on generates efficient, readable ANSI C code for algorithm acceleration and real-time implementation of embedded systems. The code is more efficient and readable than most other code generators. VisSim's author served on the X3J11 ANSI C committee and wrote several C compilers, in addition to co-authoring a book on C. [2] This deep understanding of ANSI C, and the nature of the resulting machine code when compiled, is the key to the code generator's efficiency. -
Advanced Electronic Systems Damien Prêle
Advanced Electronic Systems Damien Prêle To cite this version: Damien Prêle. Advanced Electronic Systems . Master. Advanced Electronic Systems, Hanoi, Vietnam. 2016, pp.140. cel-00843641v5 HAL Id: cel-00843641 https://cel.archives-ouvertes.fr/cel-00843641v5 Submitted on 18 Nov 2016 (v5), last revised 26 May 2021 (v8) HAL is a multi-disciplinary open access L’archive ouverte pluridisciplinaire HAL, est archive for the deposit and dissemination of sci- destinée au dépôt et à la diffusion de documents entific research documents, whether they are pub- scientifiques de niveau recherche, publiés ou non, lished or not. The documents may come from émanant des établissements d’enseignement et de teaching and research institutions in France or recherche français ou étrangers, des laboratoires abroad, or from public or private research centers. publics ou privés. advanced electronic systems ST 11.7 - Master SPACE & AERONAUTICS University of Science and Technology of Hanoi Paris Diderot University Lectures, tutorials and labs 2016-2017 Damien PRÊLE [email protected] Contents I Filters 7 1 Filters 9 1.1 Introduction . .9 1.2 Filter parameters . .9 1.2.1 Voltage transfer function . .9 1.2.2 S plane (Laplace domain) . 11 1.2.3 Bode plot (Fourier domain) . 12 1.3 Cascading filter stages . 16 1.3.1 Polynomial equations . 17 1.3.2 Filter Tables . 20 1.3.3 The use of filter tables . 22 1.3.4 Conversion from low-pass filter . 23 1.4 Filter synthesis . 25 1.4.1 Sallen-Key topology . 25 1.5 Amplitude responses . 28 1.5.1 Filter specifications . 28 1.5.2 Amplitude response curves .