1. General Description of Aluminum Electrolytic Capacitors
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Imperial College London Department of Physics Graphene Field Effect
Imperial College London Department of Physics Graphene Field Effect Transistors arXiv:2010.10382v2 [cond-mat.mes-hall] 20 Jul 2021 By Mohamed Warda and Khodr Badih 20 July 2021 Abstract The past decade has seen rapid growth in the research area of graphene and its application to novel electronics. With Moore's law beginning to plateau, the need for post-silicon technology in industry is becoming more apparent. Moreover, exist- ing technologies are insufficient for implementing terahertz detectors and receivers, which are required for a number of applications including medical imaging and secu- rity scanning. Graphene is considered to be a key potential candidate for replacing silicon in existing CMOS technology as well as realizing field effect transistors for terahertz detection, due to its remarkable electronic properties, with observed elec- tronic mobilities reaching up to 2 × 105 cm2 V−1 s−1 in suspended graphene sam- ples. This report reviews the physics and electronic properties of graphene in the context of graphene transistor implementations. Common techniques used to syn- thesize graphene, such as mechanical exfoliation, chemical vapor deposition, and epitaxial growth are reviewed and compared. One of the challenges associated with realizing graphene transistors is that graphene is semimetallic, with a zero bandgap, which is troublesome in the context of digital electronics applications. Thus, the report also reviews different ways of opening a bandgap in graphene by using bi- layer graphene and graphene nanoribbons. The basic operation of a conventional field effect transistor is explained and key figures of merit used in the literature are extracted. Finally, a review of some examples of state-of-the-art graphene field effect transistors is presented, with particular focus on monolayer graphene, bilayer graphene, and graphene nanoribbons. -
Run Capacitor Info-98582
Run Cap Quiz-98582_Layout 1 4/16/15 10:26 AM Page 1 ® Run Capacitor Info WHAT IS A CAPACITOR? Very simply, a capacitor is a device that stores and discharges electrons. While you may hear capacitors referred to by a variety of names (condenser, run, start, oil, etc.) all capacitors are comprised of two or more metallic plates separated by an insulating material called a dielectric. PLATE 1 PLATE 2 A very simple capacitor can be made with two plates separated by a dielectric, in this PLATE 1 PLATE 2 case air, and connected to a source of DC current, a battery. Electrons will flow away from plate 1 and collect on plate 2, leaving it with an abundance of electrons, or a “charge”. Since current from a battery only flows one way, the capacitor plate will stay BATTERY + – charged this way unless something causes current flow. If we were to short across the plates with a screwdriver, the resulting spark would indicate the electrons “jumping” from plate 2 to plate 1 in an attempt to equalize. As soon as the screwdriver is removed, plate 2 will again collect a PLATE 1 PLATE 2 charge. + BATTERY – Now let’s connect our simple capacitor to a source of AC current and in series with the windings of an electric motor. Since AC current alternates, first one PLATE 1 PLATE 2 MOTOR plate, then the other would be charged and discharged in turn. First plate 1 is charged, then as the current reverses, a rush of electrons flow from plate 1 to plate 2 through the motor windings. -
Switched-Capacitor Circuits
Switched-Capacitor Circuits David Johns and Ken Martin University of Toronto ([email protected]) ([email protected]) University of Toronto 1 of 60 © D. Johns, K. Martin, 1997 Basic Building Blocks Opamps • Ideal opamps usually assumed. • Important non-idealities — dc gain: sets the accuracy of charge transfer, hence, transfer-function accuracy. — unity-gain freq, phase margin & slew-rate: sets the max clocking frequency. A general rule is that unity-gain freq should be 5 times (or more) higher than the clock-freq. — dc offset: Can create dc offset at output. Circuit techniques to combat this which also reduce 1/f noise. University of Toronto 2 of 60 © D. Johns, K. Martin, 1997 Basic Building Blocks Double-Poly Capacitors metal C1 metal poly1 Cp1 thin oxide bottom plate C1 poly2 Cp2 thick oxide C p1 Cp2 (substrate - ac ground) cross-section view equivalent circuit • Substantial parasitics with large bottom plate capacitance (20 percent of C1) • Also, metal-metal capacitors are used but have even larger parasitic capacitances. University of Toronto 3 of 60 © D. Johns, K. Martin, 1997 Basic Building Blocks Switches I I Symbol n-channel v1 v2 v1 v2 I transmission I I gate v1 v p-channel v 2 1 v2 I • Mosfet switches are good switches. — off-resistance near G: range — on-resistance in 100: to 5k: range (depends on transistor sizing) • However, have non-linear parasitic capacitances. University of Toronto 4 of 60 © D. Johns, K. Martin, 1997 Basic Building Blocks Non-Overlapping Clocks I1 T Von I I1 Voff n – 2 n – 1 n n + 1 tTe delay 1 I fs { --- delay V 2 T on I Voff 2 n – 32e n – 12e n + 12e tTe • Non-overlapping clocks — both clocks are never on at same time • Needed to ensure charge is not inadvertently lost. -
Syfer Capacitor Basics
Syfer Technology Limited, Old Stoke Road, Arminghall, Norwich, Norfolk, NR14 8SQ, United Kingdom Tel: +44 (0) 1603 723300 Tel. (Sales): 01603 723310 Fax: +44 (0) 1603 723301 Email: [email protected] Web: www.knowlescapacitors.com Syfer Capacitor Basics What is a Capacitor ..................................................................................2 Electrode .............................................................................................2 Dielectric .............................................................................................2 Construction ........................................................................................2 MLCC Uses ..............................................................................................3 Limitations and Factors for Consideration ....................................................3 Dielectric Types .......................................................................................4 X7R.....................................................................................................4 X5R.....................................................................................................5 X8R.....................................................................................................5 2C1 (BZ) and 2X1 (BX) .........................................................................5 C0G ....................................................................................................5 High Q .................................................................................................5 -
Kirchhoff's Laws in Dynamic Circuits
Kirchhoff’s Laws in Dynamic Circuits Dynamic circuits are circuits that contain capacitors and inductors. Later we will learn to analyze some dynamic circuits by writing and solving differential equations. In these notes, we consider some simpler examples that can be solved using only Kirchhoff’s laws and the element equations of the capacitor and the inductor. Example 1: Consider this circuit Additionally, we are given the following representations of the voltage source voltage and one of the resistor voltages: ⎧⎧10 V fortt<< 0 2 V for 0 vvs ==⎨⎨and 1 −5t ⎩⎩20 V forte>+ 0 8 4 V fort> 0 We wish to express the capacitor current, i 2 , as a function of time, t. Plan: First, apply Kirchhoff’s voltage law (KVL) to the loop consisting of the source, resistor R1 and the capacitor to determine the capacitor voltage, v 2 , as a function of time, t. Next, use the element equation of the capacitor to determine the capacitor current as a function of time, t. Solution: Apply Kirchhoff’s voltage law (KVL) to the loop consisting of the source, resistor R1 and the capacitor to write ⎧ 8 V fort < 0 vvv12+−=ss0 ⇒ v2 =−= vv 1⎨ −5t ⎩16− 8et V for> 0 Use the element equation of the capacitor to write ⎧ 0 A fort < 0 dv22 dv ⎪ ⎧ 0 A fort < 0 iC2 ==0.025 =⎨⎨d −5t =−5t dt dt ⎪0.025() 16−> 8et for 0 ⎩1et A for> 0 ⎩ dt 1 Example 2: Consider this circuit where the resistor currents are given by ⎧⎧0.8 A fortt<< 0 0 A for 0 ii13==⎨⎨−−22ttand ⎩⎩0.8et−> 0.8 A for 0 −0.8 e A fort> 0 Express the inductor voltage, v 2 , as a function of time, t. -
Ltc3225/Ltc3225-1
LTC3225/LTC3225-1 150mA Supercapacitor Charger FEATURES DESCRIPTION n Low Noise Constant Frequency Charging of Two The LTC®3225/LTC3225-1 are programmable supercapaci- Series Supercapacitors tor chargers designed to charge two supercapacitors in n Automatic Cell Balancing Prevents Capacitor series to a selectable fi xed output voltage (4.8V/5.3V for Overvoltage During Charging the LTC3225 and 4V/4.5V for the LTC3225-1) from input n Programmable Charge Current (Up to 150mA) supplies as low as 2.8V to 5.5V. Automatic cell balancing n Selectable 2.4V or 2.65V Regulation per Cell prevents overvoltage damage to either supercapacitor. No (LTC3225) balancing resistors are required. n Selectable 2V or 2.25V Regulation per Cell Low input noise, low quiescent current and low external (LTC3225-1) parts count (one fl ying capacitor, one bypass capacitor at n Automatic Recharge V and one programming resistor) make the LTC3225/ n I = 20μA in Standby Mode IN VIN LTC3225-1 ideally suited for small battery-powered n I < 1μA When Input Supply is Removed COUT applications. n No Inductors n Tiny Application Circuit (2mm × 3mm DFN Package, Charge current level is programmed with an external All Components <1mm High) resistor. When the input supply is removed, the LTC3225/ LTC3225-1 automatically enter a low current state, drawing APPLICATIONS less than 1μA from the supercapacitors. The LTC3225/LTC3225-1 are available in a 10-lead 2mm n Current Limited Applications with High Peak Power × 3mm DFN package. Loads (LED Flash, PCMCIA Tx Bursts, HDD Bursts, L, LT, LTC and LTM are registered trademarks and ThinSOT is a trademark of Linear GPRS/GSM Transmitter) Technology Corporation. -
Capacitive Voltage Transformers: Transient Overreach Concerns and Solutions for Distance Relaying
Capacitive Voltage Transformers: Transient Overreach Concerns and Solutions for Distance Relaying Daqing Hou and Jeff Roberts Schweitzer Engineering Laboratories, Inc. Revised edition released October 2010 Previously presented at the 1996 Canadian Conference on Electrical and Computer Engineering, May 1996, 50th Annual Georgia Tech Protective Relaying Conference, May 1996, and 49th Annual Conference for Protective Relay Engineers, April 1996 Previous revised edition released July 2000 Originally presented at the 22nd Annual Western Protective Relay Conference, October 1995 CAPACITIVE VOLTAGE TRANSFORMERS: TRANSIENT OVERREACH CONCERNS AND SOLUTIONS FOR DISTANCE RELAYING Daqing Hou and Jeff Roberts Schweitzer Engineering Laboratories, Inc. Pullman, W A USA ABSTRACT Capacitive Voltage Transformers (CVTs) are common in high-voltage transmission line applications. These same applications require fast, yet secure protection. However, as the requirement for faster protective relays grows, so does the concern over the poor transient response of some CVTs for certain system conditions. Solid-state and microprocessor relays can respond to a CVT transient due to their high operating speed and iflCreased sensitivity .This paper discusses CVT models whose purpose is to identify which major CVT components contribute to the CVT transient. Some surprises include a recom- mendation for CVT burden and the type offerroresonant-suppression circuit that gives the least CVT transient. This paper also reviews how the System Impedance Ratio (SIR) affects the CVT transient response. The higher the SIR, the worse the CVT transient for a given CVT . Finally, this paper discusses improvements in relaying logic. The new method of detecting CVT transients is more precise than past detection methods and does not penalize distance protection speed for close-in faults. -
Introduction What Is a Polymer Capacitor?
ECAS series (polymer-type aluminum electrolytic capacitor) No. C2T2CPS-063 Introduction If you take a look at the main board of an electronic device such as a personal computer, you’re likely to see some of the six types of capacitors shown below (Fig. 1). Common types of capacitors include tantalum electrolytic capacitors (MnO2 type and polymer type), aluminum electrolytic capacitors (electrolyte can type, polymer can type, and chip type), and MLCC. Figure 1. Main Types of Capacitors What Is a Polymer Capacitor? There are many other types of capacitors, such as film capacitors and niobium capacitors, but here we will describe polymer capacitors, a type of capacitor produced by Murata among others. In both tantalum electrolytic capacitors and aluminum electrolytic capacitors, a polymer capacitor is a type of electrolytic capacitor in which a conductive polymer is used as the cathode. In a polymer-type aluminum electrolytic capacitor, the anode is made of aluminum foil and the cathode is made of a conductive polymer. In a polymer-type tantalum electrolytic capacitor, the anode is made of the metal tantalum and the cathode is made of a conductive polymer. Figure 2 shows an example of this structure. Figure 2. Example of Structure of Conductive Polymer Aluminum Capacitor In conventional electrolytic capacitors, an electrolyte (electrolytic solution) or manganese dioxide (MnO2) was used as the cathode. Using a conductive polymer instead provides many advantages, making it possible to achieve a lower equivalent series resistance (ESR), more stable thermal characteristics, improved safety, and longer service life. As can be seen in Fig. 1, polymer capacitors have lower ESR than conventional electrolytic Copyright © muRata Manufacturing Co., Ltd. -
Synthesis of Nano-Ceramics for Supercapacitors
University of Wollongong Research Online University of Wollongong Thesis Collection 1954-2016 University of Wollongong Thesis Collections 2014 Synthesis of nano-ceramics for supercapacitors Azrin Akhter Chowdhury University of Wollongong Follow this and additional works at: https://ro.uow.edu.au/theses University of Wollongong Copyright Warning You may print or download ONE copy of this document for the purpose of your own research or study. The University does not authorise you to copy, communicate or otherwise make available electronically to any other person any copyright material contained on this site. You are reminded of the following: This work is copyright. Apart from any use permitted under the Copyright Act 1968, no part of this work may be reproduced by any process, nor may any other exclusive right be exercised, without the permission of the author. Copyright owners are entitled to take legal action against persons who infringe their copyright. A reproduction of material that is protected by copyright may be a copyright infringement. A court may impose penalties and award damages in relation to offences and infringements relating to copyright material. Higher penalties may apply, and higher damages may be awarded, for offences and infringements involving the conversion of material into digital or electronic form. Unless otherwise indicated, the views expressed in this thesis are those of the author and do not necessarily represent the views of the University of Wollongong. Recommended Citation Chowdhury, Azrin Akhter, Synthesis of nano-ceramics for supercapacitors, Doctor of Philosophy thesis, Engineering Materials Institute, University of Wollongong, 2014. https://ro.uow.edu.au/theses/4314 Research Online is the open access institutional repository for the University of Wollongong. -
Review of Technologies and Materials Used in High-Voltage Film Capacitors
polymers Review Review of Technologies and Materials Used in High-Voltage Film Capacitors Olatoundji Georges Gnonhoue 1,*, Amanda Velazquez-Salazar 1 , Éric David 1 and Ioana Preda 2 1 Department of Mechanical Engineering, École de technologie supérieure, Montreal, QC H3C 1K3, Canada; [email protected] (A.V.-S.); [email protected] (É.D.) 2 Energy Institute—HEIA Fribourg, University of Applied Sciences of Western Switzerland, 3960 Sierre, Switzerland; [email protected] * Correspondence: [email protected] Abstract: High-voltage capacitors are key components for circuit breakers and monitoring and protection devices, and are important elements used to improve the efficiency and reliability of the grid. Different technologies are used in high-voltage capacitor manufacturing process, and at all stages of this process polymeric films must be used, along with an encapsulating material, which can be either liquid, solid or gaseous. These materials play major roles in the lifespan and reliability of components. In this paper, we present a review of the different technologies used to manufacture high-voltage capacitors, as well as the different materials used in fabricating high-voltage film capacitors, with a view to establishing a bibliographic database that will allow a comparison of the different technologies Keywords: high-voltage capacitors; resin; dielectric film Citation: Gnonhoue, O.G.; Velazquez-Salazar, A.; David, É.; Preda, I. Review of Technologies and 1. Introduction Materials Used in High-Voltage Film High-voltage films capacitors are important components for networks and various Capacitors. Polymers 2021, 13, 766. electrical devices. They are used to transport and distribute high-voltage electrical energy https://doi.org/10.3390/ either for voltage distribution, coupling or capacitive voltage dividers; in electrical sub- polym13050766 stations, circuit breakers, monitoring and protection devices; as well as to improve grid efficiency and reliability. -
Suggestion of the Supercapacitor(EDLC) Application to the Electrical Characteristic Tester
Supercapacitor (EDLC) Application Note No. C2M1CXS-163A(E) Suggestion of the Supercapacitor(EDLC) Application to the Electrical Characteristic Tester 1. Summary Supercapacitor, also known as EDLC or supercap, has higher-capacity than ceramic capacitor or electrolytic capacitor. And supercapacitor is an energy storage device having longer life than a battery. In addition, Murata’s supercapacitor can handle the output power up to 50W by realizing super low ESR approximately 40mΩ (DMF series example) At the measurement environment that a high peak electric current runs through the load instantly, our supercapacitor can assist such peak current. By this effect, it is possible to downsize Fig.3 : Measurement Block Diagram with Supercapacitor and reduce power capacity of DC power supply. Besides it contributes to reduce measuring equipment cost and save the Fig.4 and Fig.5 shows each part waveform. electric power of the facilities. Top(Yellow):Load current, Middle(Green):Power line voltage, Bottom(Purple):DC power supply current. 2. Benefits Fig.4: DC power supply only. ①Downsize the DC power supply Fig.5: Supercap is added to DC power supply. Even if the power supply capacity cannot support a peak current, The effect of supercap can be confirmed because the fluctuation it does not matter because supercap can assist it. ②Supercapacitor as a power source of the input voltage is smaller and the peak current of power Because supercap can be charged quickly, it is possible to use supply decreases. supercap as power source at the time of measurement. ③Reduce the cost and Save power of measurement equipment. ④Can be mounted on limited area because of its thinner and smaller shape. -
Aluminum Electrolytic Vs. Polymer – Two Technologies – Various Opportunities
Aluminum Electrolytic vs. Polymer – Two Technologies – Various Opportunities By Pierre Lohrber BU Manager Capacitors Wurth Electronics @APEC 2017 2017 WE eiCap @ APEC PSMA 1 Agenda Electrical Parameter Technology Comparison Application 2017 WE eiCap @ APEC PSMA 2 ESR – How to Calculate? ESR – Equivalent Series Resistance ESR causes heat generation within the capacitor when AC ripple is applied to the capacitor Maximum ESR is normally specified @ 120Hz or 100kHz, @20°C ESR can be calculated like below: ͕ͨ͢ 1 1 ͍̿͌ Ɣ Ɣ ͕ͨ͢ ∗ ͒ ͒ Ɣ Ɣ 2 ∗ ∗ ͚ ∗ ̽ 2 ∗ ∗ ͚ ∗ ̽ ! ∗ ̽ 2017 WE eiCap @ APEC PSMA 3 ESR – Temperature Characteristics Electrolytic Polymer Ta Polymer Al Ceramics 2017 WE eiCap @ APEC PSMA 4 Electrolytic Conductivity Aluminum Electrolytic – Caused by the liquid electrolyte the conductance response is deeply affected – Rated up to 0.04 S/cm Aluminum Polymer – Solid Polymer pushes the conductance response to much higher limits – Rated up to 4 S/cm 2017 WE eiCap @ APEC PSMA 5 Electrical Values – Who’s Best in Class? Aluminum Electrolytic ESR approx. 85m Ω Tantalum Polymer Ripple Current rating approx. ESR approx. 200m Ω 630mA Ripple Current rating approx. 1,900mA Aluminum Polymer ESR approx. 11m Ω Ripple Current rating approx. 5,500mA 2017 WE eiCap @ APEC PSMA 6 Ripple Current >> Temperature Rise Ripple current is the AC component of an applied source (SMPS) Ripple current causes heat inside the capacitor due to the dielectric losses Caused by the changing field strength and the current flow through the capacitor 2017 WE eiCap @ APEC PSMA 7 Impedance Z ͦ 1 ͔ Ɣ ͍̿͌ ͦ + (͒ −͒ )ͦ Ɣ ͍̿͌ ͦ + 2 ∗ ∗ ͚ ∗ ͍̿͆ − 2 ∗ ∗ ͚ ∗ ̽ 2017 WE eiCap @ APEC PSMA 8 Impedance Z Impedance over frequency added with ESR ratio 2017 WE eiCap @ APEC PSMA 9 Impedance @ High Frequencies Aluminum Polymer Capacitors have excellent high frequency characteristics ESR value is ultra low compared to Electrolytic’s and Tantalum’s within 100KHz~1MHz E.g.