Inorganic Solid-State Electrolytes for Lithium Batteries: Mechanisms and Properties Governing Ion Conduction
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A Solid-State and Flexible Supercapacitor That Operates Across a Wide Temperature Range
A Solid-State and Flexible Supercapacitor that Operates Across a Wide Temperature Range Ardalan Chaichi1,†, Gokul Venugopalan2,†, Ram Devireddy1, Christopher Arges2,*, Manas Ranjan Gartia1,* 1Department of Mechanical Engineering, Louisiana State University, Baton Rouge, USA 70803 2Cain Department of Chemical Engineering, Louisiana State University, Baton Rouge, USA 70803 † Equal contribution * Correspondence: [email protected]; [email protected] Abstract Electrochemical properties of most supercapacitor devices degrade quickly when the operating temperature deviates from room temperature. In order to exploit the potential of rGO in supercapacitors at extreme temperatures, a resilient electrolyte that is functional over a wide- temperature range is also required. In this study, we have implemented a flexible, low-resistant solid-state electrolyte membrane (SSEM) into symmetric rGO electrodes to realize supercapacitor devices that operate in the temperature range of -70 °C to 220 °C. The SSEM consists of a polycation-polybenzimidazole blend that is doped with phosphoric acid (H3PO4) and this material displays uniquely high conductivity values that range from 50 mS cm-1 to 278 mS cm-1 in the temperature range of -25 °C to 220 °C. The fabricated supercapacitor produced a maximum capacitance of 6.8 mF cm-2 at 100 °C. Energy and power densities ranged from 0.83 to 2.79 mW h cm-2 and 90 to 125 mW cm-2, respectively. The energy storage mechanism with a SSEM occurs by excess H3PO4 migrating from the membrane host into the electrochemical double layer in rGO electrodes. The high temperature operation is enabled by the polycation in the SSEM anchoring phosphate type of anions preventing H3PO4 evaporation. -
Module 3: Defects, Diffusion and Conduction in Ceramics Introduction
Objectives_template Module 3: Defects, Diffusion and Conduction in Ceramics Introduction In this module, we will discuss about migration of the defects which happens via an atomistic process called as diffusion. Diffusivity of species in the materials is also related to their physical properties such as electrical conductivity and mobility via Nernst-Einestein relation which we shall derive. As we shall also see, the conductivity in ceramics is a sum of ionic and electronic conductivity and the ratio of two determines the applicability of ceramic materials for applications. Subsequently framework will be established for understanding the temperature dependence of conductivity via a simple atomistic model leading to the same conclusions as predicted by the diffusivity model. Subsequently we will look into the conduction in glasses and look at some examples of fast ion conductors, material of importance for a variety of applications. Presence of charged defects in ceramics also means the existence of electrical potential gradients, in addition to the chemical gradient, which results in a unified equation for electrochemical potential. Finally, we will look at a few important applications for conducting ceramic materials. The Module contains: Diffusion Diffusion Kinetics Examples of Diffusion in Ceramics Mobility and Diffusivity Analogue to the Electrical Properties Conduction in Ceramics vis-à-vis metallic conductors: General Information Ionic Conduction: Basic Facts Ionic and Electronic Conductivity Characteristics of Ionic Conduction Theory of Ionic Conduction Conduction in Glasses Fast Ion Conductors Examples of Ionic Conduction Electrochemical Potential Nernst Equation and Application of Ionic Conductors Examples of Ionic Conductors in Engineering Applications Summary Suggested Reading: file:///C|/Documents%20and%20Settings/iitkrana1/Desktop/new_electroceramics_14may,2012/lecture13/13_1.htm[5/25/2012 3:03:41 PM] Objectives_template Physical Ceramics: Principles for Ceramic Science and Engineering, Y.-M. -
An Investigation of Lithium Solid Electrolyte Materials
AN INVESTIGATION OF LITHIUM SOLID ELECTROLYTE MATERIALS WITH FIRST PRINCIPLES CALCULATIONS BY NICHOLAS LEPLEY A Thesis Submitted to the Graduate Faculty of WAKE FOREST UNIVERSITY GRADUATE SCHOOL OF ARTS AND SCIENCES in Partial Fulfillment of the Requirements for the Degree of MASTER OF SCIENCE Physics December 2013 Winston-Salem, North Carolina Approved By: N. A. W. Holzwarth, Ph.D., Advisor Freddie Salsbury Jr., Ph.D., Chair William Kerr, Ph.D. Timo Thonhauser, Ph.D. Table of Contents List of Figures iv Chapter List of Abbreviations v Chapter Abstract vi I Background 1 Chapter 1 Battery Chemistry and Challenges 2 1.1 Fundamental Operation . .2 1.2 State of the Art . .3 1.3 Solid Electrolyte Materials . .6 Chapter 2 Computational Methods 9 2.1 Density Functional Theory . .9 2.2 Implementation . 12 2.3 Additional sources of error . 13 II Summary of Published Work 14 Chapter 3 Computer modeling of lithium phosphate and thiophosphate electrolyte materials 15 3.1 Overview . 15 3.2 Publication results and conclusions . 15 3.3 My contributions . 16 3.4 Further results and conclusions . 16 Chapter 4 Computer Modeling of Crystalline Electrolytes: Lithium Thio- phosphates and Phosphates 17 4.1 Overview . 17 4.2 Publication results and conclusions . 17 4.3 My contributions . 21 4.4 Further results and conclusions . 21 ii Chapter 5 Structures, Li+ mobilities, and interfacial properties of solid electrolytes Li3PS4 and Li3PO4 from first principles 22 5.1 Overview . 22 5.2 Publication results and conclusions . 22 5.3 My contributions . 24 5.4 Further results and conclusions . 25 Chapter 6 Conclusions and future directions 27 III Appendix 32 Chapter 7 Computer modeling of lithium phosphate and thiophosphate electrolyte materials 33 Chapter 8 Computer modeling of crystalline electrolytes: lithium thio- phosphates and phosphates 41 Chapter 9 Structures, Li+ mobilities, and interfacial properties of solid electrolytes Li3PS4 and Li3PO4 from first principles 52 IV Curriculum Vitae 64 iii List of Figures 1.1 Schematic of Li-ion battery . -
NMR Investigations of Crystalline and Glassy Solid Electrolytes for Lithium Batteries: a Brief Review
International Journal of Molecular Sciences Review NMR Investigations of Crystalline and Glassy Solid Electrolytes for Lithium Batteries: A Brief Review Daniel J. Morales 1,2 and Steven Greenbaum 1,* 1 Department of Physics and Astronomy, Hunter College of the City University of New York, New York, NY 10065, USA; [email protected] 2 Ph.D. Program in Physics, CUNY Graduate Center, New York, NY 10036, USA * Correspondence: [email protected] Received: 9 April 2020; Accepted: 28 April 2020; Published: 11 May 2020 Abstract: The widespread use of energy storage for commercial products and services have led to great advancements in the field of lithium-based battery research. In particular, solid state lithium batteries show great promise for future commercial use, as solid electrolytes safely allow for the use of lithium-metal anodes, which can significantly increase the total energy density. Of the solid electrolytes, inorganic glass-ceramics and Li-based garnet electrolytes have received much attention in the past few years due to the high ionic conductivity achieved compared to polymer-based electrolytes. This review covers recent work on novel glassy and crystalline electrolyte materials, with a particular focus on the use of solid-state nuclear magnetic resonance spectroscopy for structural characterization and transport measurements. Keywords: NMR; inorganic electrolytes; glassy electrolytes; ceramic electrolytes 1. Introduction As lithium ion batteries continue to permeate the commercial market, the search continues to produce an all solid-state equivalent with the same or superior performance. While liquid organic electrolytes continue to exhibit high performance and long cyclability, the risk of thermal runaway and inability to utilize Li metal anodes without the risk of dendrite formation are ongoing issues. -
Advances in Materials Design for All-Solid-State Batteries: from Bulk to Thin Films
applied sciences Review Advances in Materials Design for All-Solid-state Batteries: From Bulk to Thin Films Gene Yang 1, Corey Abraham 2, Yuxi Ma 1, Myoungseok Lee 1, Evan Helfrick 1, Dahyun Oh 2,* and Dongkyu Lee 1,* 1 Department of Mechanical Engineering, College of Engineering and Computing, University of South Carolina, Columbia, SC 29208, USA; [email protected] (G.Y.); [email protected] (Y.M.); [email protected] (M.L.); [email protected] (E.H.) 2 Chemical and Materials Engineering Department, Charles W. Davidson College of Engineering, San José State University, San José, CA 95192-0080, USA; [email protected] * Correspondence: [email protected] (D.O.); [email protected] (D.L.) Received: 15 June 2020; Accepted: 7 July 2020; Published: 9 July 2020 Featured Application: All solid-state lithium batteries, all solid-state thin-film lithium batteries. Abstract: All-solid-state batteries (SSBs) are one of the most fascinating next-generation energy storage systems that can provide improved energy density and safety for a wide range of applications from portable electronics to electric vehicles. The development of SSBs was accelerated by the discovery of new materials and the design of nanostructures. In particular, advances in the growth of thin-film battery materials facilitated the development of all solid-state thin-film batteries (SSTFBs)—expanding their applications to microelectronics such as flexible devices and implantable medical devices. However, critical challenges still remain, such as low ionic conductivity of solid electrolytes, interfacial instability and difficulty in controlling thin-film growth. In this review, we discuss the evolution of electrode and electrolyte materials for lithium-based batteries and their adoption in SSBs and SSTFBs. -
Physical and Chemical Properties of Germanium
Physical And Chemical Properties Of Germanium Moneyed and amnesic Erasmus fertilise her fatuousness revitalise or burrow incommunicatively. Creditable Petr still climbs: regarding and lissome Lazarus bully-off quite punctiliously but slums her filoplume devotedly. Zane still defilade venomous while improvident Randell bloodiest that wonderers. Do you for this context of properties and physical explanation of Silicon is sincere to metals in its chemical behaviour. Arsenic is extremely toxic, RS, carbon is the tongue one considered a full nonmetal. In nature, which name a widely used azo dye. Basic physical and chemical properties of semiconductors are offset by the energy gap between valence conduction! Other metalloids on the periodic table are boron, Batis ZB, only Germanium and Antimony would be considered metals for the purposes of nomenclature. Storage temperature: no restrictions. At room temperature, the semiconducting elements are primarily nonmetallic in character. This application requires Javascript. It has also new found in stars and already the atmosphere of Jupiter. Wellings JS, it is used as an eyewash and insecticide. He has studied in Spain and Hungary and authored many research articles published in indexed journals and books. What are oral health benefits of pumpkins? The material on this site may not be reproduced, germanium, the radiation emitted from an active device makes it locatable. Classify each statement as an extensive property must an intensive property. In germanium and physical chemical properties of the border lines from the! The most electronegative elements are at the nod in the periodic table; these elements often react as oxidizing agents. Atomic Volume and Allotropy of the Elements. -
Development and Fabrication of a 1.5 F – 5 V Solid State Supercapacitor
Development and fabrication of a 1.5 F – 5 V solid state supercapacitor Pietro Staiti and Francesco Lufrano CNR-ITAE, ISTITUTO DI TECNOLOGIE AVANZATE PER L’ENERGIA “NICOLA GIORDANO” Via Salita S. Lucia sopra Contesse n. 5 Messina, Italy Phone: 0039 090 624226 / fax: 0039 090 624247 E-mail: [email protected] Acknowledgments The authors acknowledge the Consiglio Nazionale delle Ricerche that has financially supported the research project for the development of this type of supercapacitor. Keywords Supercapacitor, energy storage, solid electrolyte, acidic electrolyte. Abstract A five cells supercapacitor prototype with special electrolyte is designed and fabricated at the Institute CNR-ITAE of Messina. It has a nominal capacitance of 1.5 F and a maximum voltage of 5 V. The electrodes of prototype are formed of high surface area carbon material and Nafion ionomer. Nafion is used as an electrolyte membrane separator between the electrodes of each single cell and as a binder/ion conductor in the electrodes. The fabricated prototype achieves specific capacitance of 114 F/g (referred to the weight of active carbon materials for single electrode), that is comparable to the specific capacitance previously obtained from a smaller scale single cell of same type of supercapacitor. A power density of 1.4 kW/l and a RC-time constant of 0.3 s have been calculated for the device. Introduction Electric double layer capacitors (EDLCs) or supercapacitors (SCs) are promising energy storage devices, which are being considered for applications such as electric vehicles, uninterruptible power systems, and computer memory protection. Their main characteristic is the excellent high-rate charging-discharging ability that makes these devices, referring to this specific aspect, more efficient than batteries and fuel cells. -
Fabrication and Testing of All-Solid-State Nanoscale Lithium Batteries Using Lipon for Electrolytes
E3S Web of Conferences 53, 01008 (2018) https://doi.org/10.1051/e3sconf/20185301008 ICAEER 2018 Fabrication and Testing of All-solid-state Nanoscale Lithium Batteries Using LiPON for Electrolytes Feihu Tan1, XiaoPing Liang1, Feng Wei1 and Jun Du2, * 1State Key Laboratory of Advanced Materials for Smart Sensing, General Research Institute for Nonferrous Metals, Beijing, China. 2General Research Institute for Nonferrous Metals, Beijing, China. Abstract. The amorphous LiPON thin film was obtained by using the crystalline Li3PO4 target and the RF magnetron sputtering method at a N2 working pressure of 1 Pa. and then the morphology and composition of LiPON thin films are analysed by SEM and EDS. SEM shows that the film was compact and smooth, while EDS shows that the content of N in LiPON thin film was about 17.47%. The electrochemical properties of Pt/LiPON/Pt were analysed by EIS, and the ionic conductivity of LiPON thin films was -7 3.8×10 S/cm. By using the hard mask in the magnetron sputtering process, the all-solid-state thin film battery with Si/Ti/Pt/LiCoO2/LiPON/Li4Ti5O12/Pt structure was prepared, and its electrical properties were studied. As for this thin film battery, the open circuit voltage was 1.9 V and the first discharge specific capacity was 34.7 μAh/cm2·μm at a current density of 5 μA/cm-2,indicating that is promising in all-solid- state thin film batteries. 1 Introduction conductivity, [13-15] the ionic conductivity of LiPON films prepared by magnetron sputtering is up to ~10-6 S/cm, Lithium ion battery is a common energy supply unit in therefore, LiPON films were prepared by magnetron the current equipment. -
Thin-Film Lithium and Lithium-Ion Batteries
Solid State Ionics 135 (2000) 33±45 www.elsevier.com/locate/ssi Thin-®lm lithium and lithium-ion batteries J.B. Bates, N.J. Dudney* , B. Neudecker, A. Ueda, C.D. Evans Oak Ridge National Laboratory, P.O. Box 2008, Oak Ridge, TN 37831-6030, USA Abstract Research over the last decade at Oak Ridge National Laboratory has led to the development of solid-state thin-®lm lithium and lithium-ion batteries. The batteries, which are less than 15 mm thick, have important applications in a variety of consumer and medical products, and they are useful research tools in characterizing the properties of lithium intercalation compounds in thin-®lm form. The batteries consist of cathodes that are crystalline or nanocrystalline oxide-based lithium intercalation compounds such as LiCoO224 and LiMn O , and anodes of lithium metal, inorganic compounds such as silicon±tin oxynitrides, Sn34 N and Zn 32 N , or metal ®lms such as Cu in which the anode is formed by lithium plating on the initial charge. The electrolyte is a glassy lithium phosphorus oxynitride (`Lipon'). Cells with crystalline LiCoO2 cathodes can deliver up to 30% of their maximum capacity between 4.2 and 3 V at discharge currents of 10 mA/cm2 , and at more moderate discharge±charge rates, the capacity decreases by negligible amounts over thousands of cycles. Thin ®lms of crystalline lithium manganese oxide with the general composition Li11x Mn22y O4 exhibit on the initial charge signi®cant capacity at 5 V and, depending on the deposition process, at 4.6 V as well, as a consequence of the manganese de®ciency±lithium excess. -
Ionic Conduction in the Solid State
J. Chem. Sci., Vol. 118, No. 1, January 2006, pp. 135–154. © Indian Academy of Sciences. Ionic conduction in the solid state P PADMA KUMAR and S YASHONATH Solid State and Structural Chemistry Unit, Indian Institute of Science, Bangalore 560 012 e-mail: [email protected] Abstract. Solid state ionic conductors are important from an industrial viewpoint. A variety of such conductors have been found. In order to understand the reasons for high ionic conductivity in these sol- ids, there have been a number of experimental, theoretical and computational studies in the literature. We provide here a survey of these investigations with focus on what is known and elaborate on issues that still remain unresolved. Conductivity depends on a number of factors such as presence of interstitial sites, ion size, temperature, crystal structure etc. We discuss the recent results from atomistic computer simula- tions on the dependence of conductivity in NASICONs as a function of composition, temperature, phase change and cation among others. A new potential for modelling of NASICON structure that has been proposed is also discussed. Keywords. Ionic conduction; solid state; atomistic computer simulations; NASICON structure. 1. Introduction 2. A brief history of superionic conductors There exist many solids with high ionic conductivity The study of ionic conduction in solid state origi- (>10–4 W–1 cm–1) and they are of immense use in di- nated way back in 1838 when Faraday discovered verse technological applications. Some of these solids that PbF2 and Ag2S are good conductors of electri- which are also good electronic conductors are often city.2,3 These solids are, the first ever discovered referred to as ‘mixed conductors’, while the term solid electrolyte and intercalation electrode respecti- ‘superionic conductor’ or ‘fast ion conductor’ is re- vely. -
Sulfide and Oxide Inorganic Solid Electrolytes for All-Solid-State Li Batteries: a Review Mogalahalli Reddy, Christian Julien, Alain Mauger, Karim Zaghib
Sulfide and Oxide Inorganic Solid Electrolytes for All-Solid-State Li Batteries: A Review Mogalahalli Reddy, Christian Julien, Alain Mauger, Karim Zaghib To cite this version: Mogalahalli Reddy, Christian Julien, Alain Mauger, Karim Zaghib. Sulfide and Oxide Inorganic Solid Electrolytes for All-Solid-State Li Batteries: A Review. Nanomaterials, MDPI, 2020, 10 (8), pp.1606. 10.3390/nano10081606. hal-02944666 HAL Id: hal-02944666 https://hal.sorbonne-universite.fr/hal-02944666 Submitted on 21 Sep 2020 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. nanomaterials Review Sulfide and Oxide Inorganic Solid Electrolytes for All-Solid-State Li Batteries: A Review Mogalahalli V. Reddy 1 , Christian M. Julien 2,* , Alain Mauger 2 and Karim Zaghib 3,* 1 Centre of Excellence in Transportation Electrification and Energy Storage (CETEES), Institute of Research Hydro-Québec, 1806, Lionel-Boulet Blvd., Varennes, QC J3X 1S1, Canada; [email protected] 2 Institut de Minéralogie, de Physique des Matériaux et de Cosmochimie (IMPMC), -
Electrochemical Performances of Vitreous Materials in the System Li2o–V2O5–P2O5 As Electrode for Lithium Batteries
View metadata, citation and similar papers at core.ac.uk brought to you by CORE provided by Open Archive Toulouse Archive Ouverte OATAO is an open access repository that collects the work of Toulouse researchers and makes it freely available over the web where possible This is an author’s version published in: http://oatao.univ-toulouse.fr/24437 Official URL: https://doi.org/10.1016/j.ssi.2013.02.006 To cite this version: Delaizir, Gaëlle and Seznec, vincent and Rozier, Patrick and Surcin, Christine and Salles, Philippe and Dollé, Mickael Electrochemical performances of vitreous materials in the system Li2O–V2O5–P2O5 as electrode for lithium batteries. (2013) Solid State Ionics, 237. 22-27. ISSN 0167-2738 Any correspondence concerning this service should be sent to the repository administrator: [email protected] Electrochemical performances of vitreous materials in the system Li2O–V2O5–P2O5 as electrode for lithium batteries G. Delaizir a, V. Seznec b, P. Rozier c, C. Surcin b, P. Salles c, M. Dollé c,⁎ a Sciences des Procédés Céramiques et de Traitements de Surface, SPCTS UMR CNRS 7315, Centre Européen de la Céramique, 12 rue Atlantis, 87068 Limoges, France b Laboratoire de réactivité et chimie des solides (LRCS), Université de Picardie Jules-Verne, 33 rue Saint-Leu, 80039 Amiens, France c Centre d'Elaboration des Matériaux et d'Etudes Structurales, CEMES-CNRS, UPR 8011, 29 rue Jeanne Marvig, BP 94347, 31055 Toulouse cedex 4, France article info abstract Glass composition 25Li2O 50V2O5 25P2O5 has been investigated as a potential material for electrode. Electrical Keywords: properties as well as electrochemical performances of this glass composition have been characterized and results Oxide glasses show a capacity less than 80 mAh g−1 when tested in the [3 4.5 V] potential window.