UNIVERSITY of CALIFONIA SANTA CRUZ HIGH TEMPERATURE EXPERIMENTAL CHARACTERIZATION of MICROSCALE THERMOELECTRIC EFFECTS a Dissert

Total Page:16

File Type:pdf, Size:1020Kb

UNIVERSITY of CALIFONIA SANTA CRUZ HIGH TEMPERATURE EXPERIMENTAL CHARACTERIZATION of MICROSCALE THERMOELECTRIC EFFECTS a Dissert UNIVERSITY OF CALIFONIA SANTA CRUZ HIGH TEMPERATURE EXPERIMENTAL CHARACTERIZATION OF MICROSCALE THERMOELECTRIC EFFECTS A dissertation submitted in partial satisfaction of the requirements for the degree of DOCTOR OF PHILOSOPHY in ELECTRICAL ENGINEERING by Tela Favaloro September 2014 The Dissertation of Tela Favaloro is approved: Professor Ali Shakouri, Chair Professor Joel Kubby Professor Nobuhiko Kobayashi Tyrus Miller Vice Provost and Dean of Graduate Studies Copyright © by Tela Favaloro 2014 This work is licensed under a Creative Commons Attribution- NonCommercial-NoDerivatives 4.0 International License Table of Contents List of Figures ............................................................................................................................ vi List of Tables ........................................................................................................................... xiv Nomenclature .......................................................................................................................... xv Abstract ................................................................................................................................. xviii Acknowledgements and Collaborations ................................................................................. xxi Chapter 1 Introduction .......................................................................................................... 1 1.1 Applications of thermoelectric devices for energy conversion ................................... 1 1.2 Physical Effects ............................................................................................................ 6 Seebeck Coefficient ........................................................................................................... 6 Peltier Effect ...................................................................................................................... 8 Joule heating ..................................................................................................................... 9 1.3 Thermoelectric material properties governing efficiency ......................................... 10 Thermoelectric module design ....................................................................................... 10 Material Figure of Merit.................................................................................................. 12 1.4 Advances in material synthesis ................................................................................. 14 Interdependence of thermoelectric material properties ............................................... 14 Material nanostructuring theory .................................................................................... 16 1.5 Advanced materials in this work ............................................................................... 18 III-V films with embedded nanostructures ..................................................................... 18 Nitride superlattices ........................................................................................................ 20 Nanostructured bulk Mg2Si ............................................................................................. 21 Vanadium dioxide nanobeams ....................................................................................... 22 1.6 High temperature material characterization methodologies and scope of work ..... 24 In-plane and cross-plane measurements........................................................................ 24 Thermoreflectance imaging microscopy ........................................................................ 25 Transient Harman technique .......................................................................................... 27 High temperature considerations ................................................................................... 28 Chapter 2 Characterization techniques for thermoelectric material and device properties 29 2.1 In-plane measurements .......................................................................................... 30 Van der Pauw method for electrical conductivity .......................................................... 30 Differential Seebeck coefficient measurement .............................................................. 33 iii Consolidation of in-plane measurements ....................................................................... 39 2.2 Cross-plane measurements .................................................................................... 41 3ω method for measurement of thermal conductivity .................................................. 41 Extension to measurement of the cross-plane Seebeck coefficient .............................. 48 Chapter 3 Thermoreflectance Thermal Imaging.................................................................. 52 3.1 General Principle ..................................................................................................... 53 4-bucket approach to thermal imaging: homodyne method ......................................... 55 8-bucket technique: simultaneous imaging of Peltier and Joule .................................... 59 Transient thermal imaging: pulsed boxcar averaging ..................................................... 61 3.2 Applications of thermal mapping: Peltier and Joule surface thermal profiles for high temperature imaging .................................................................................................. 63 3.3 High temperature experimental calibration method ............................................. 69 Room temperature calibration measurements .............................................................. 69 High temperature calibration methodology ................................................................... 72 Gold ................................................................................................................................. 79 Platinum .......................................................................................................................... 84 Aluminum ........................................................................................................................ 86 Equations governing temperature dependence and the effect of passivation .............. 88 Chapter 4 Transient Harman technique for direct measurement of the cross-plane figure of merit of thin films at high temperatures ............................................................................ 95 4.1 Theory and measurement requirements .................................................................. 96 4.2 Optimization of device design ................................................................................... 98 4.3 Measurement Details and Results .......................................................................... 103 Application of the transient Harman technique ........................................................... 103 Thermoreflectance imaging .......................................................................................... 107 High temperature experimental results and cross-plane Seebeck ............................... 109 4.4 Finite Element Modelling ........................................................................................ 114 Chapter 5 High magnification imaging of vanadium dioxide nanobeams .......................... 121 5.1 VO2 material background information ...................................................................... 121 5.2 Measurement Specifics ............................................................................................. 123 5.3 Measurement results: periodic domain organization .............................................. 125 5.4 Measurement results: irregular domain configuration ............................................ 129 5.5 Discussion .................................................................................................................. 133 Chapter 6 Design and fabrication of high temperature vacuum thermostat ................... 139 iv 6.1 General Considerations ......................................................................................... 139 6.2 Bulk measurement stage ...................................................................................... 141 6.3 Chamber for optical measurement ....................................................................... 144 Chapter 7 Conclusions ......................................................................................................... 147 High temperature thermoreflectance imaging and transient Harman characterization of thermoelectric energy conversion devices ....................................................................... 150 Characterization of the temperature dependence of the thermoreflectance coefficient for conductive thin films ......................................................................................................... 151 Direct observation of nanoscale Peltier and Joule effects at metal-insulator domain walls in vanadium dioxide nanobeams ...................................................................................... 152 References ............................................................................................................................ 155 v List of Figures Figure 1.1: Radioisotope thermoelectric generator used by NASA to power the Curiosity Mars rover. Right hand side is a picture taken by the rover
Recommended publications
  • Potential Energyenergy Isis Storedstored Energyenergy Duedue Toto Anan Objectobject Location.Location
    TypesTypes ofof EnergyEnergy && EnergyEnergy TransferTransfer HeatHeat (Thermal)(Thermal) EnergyEnergy HeatHeat (Thermal)(Thermal) EnergyEnergy . HeatHeat energyenergy isis thethe transfertransfer ofof thermalthermal energy.energy. AsAs heatheat energyenergy isis addedadded toto aa substances,substances, thethe temperaturetemperature goesgoes up.up. MaterialMaterial thatthat isis burning,burning, thethe Sun,Sun, andand electricityelectricity areare sourcessources ofof heatheat energy.energy. HeatHeat (Thermal)(Thermal) EnergyEnergy Thermal Energy Explained - Study.com SolarSolar EnergyEnergy SolarSolar EnergyEnergy . SolarSolar energyenergy isis thethe energyenergy fromfrom thethe Sun,Sun, whichwhich providesprovides heatheat andand lightlight energyenergy forfor Earth.Earth. SolarSolar cellscells cancan bebe usedused toto convertconvert solarsolar energyenergy toto electricalelectrical energy.energy. GreenGreen plantsplants useuse solarsolar energyenergy duringduring photosynthesis.photosynthesis. MostMost ofof thethe energyenergy onon thethe EarthEarth camecame fromfrom thethe Sun.Sun. SolarSolar EnergyEnergy Solar Energy - Defined and Explained - Study.com ChemicalChemical (Potential)(Potential) EnergyEnergy ChemicalChemical (Potential)(Potential) EnergyEnergy . ChemicalChemical energyenergy isis energyenergy storedstored inin mattermatter inin chemicalchemical bonds.bonds. ChemicalChemical energyenergy cancan bebe released,released, forfor example,example, inin batteriesbatteries oror food.food. ChemicalChemical (Potential)(Potential)
    [Show full text]
  • An Overview on Principles for Energy Efficient Robot Locomotion
    REVIEW published: 11 December 2018 doi: 10.3389/frobt.2018.00129 An Overview on Principles for Energy Efficient Robot Locomotion Navvab Kashiri 1*, Andy Abate 2, Sabrina J. Abram 3, Alin Albu-Schaffer 4, Patrick J. Clary 2, Monica Daley 5, Salman Faraji 6, Raphael Furnemont 7, Manolo Garabini 8, Hartmut Geyer 9, Alena M. Grabowski 10, Jonathan Hurst 2, Jorn Malzahn 1, Glenn Mathijssen 7, David Remy 11, Wesley Roozing 1, Mohammad Shahbazi 1, Surabhi N. Simha 3, Jae-Bok Song 12, Nils Smit-Anseeuw 11, Stefano Stramigioli 13, Bram Vanderborght 7, Yevgeniy Yesilevskiy 11 and Nikos Tsagarakis 1 1 Humanoids and Human Centred Mechatronics Lab, Department of Advanced Robotics, Istituto Italiano di Tecnologia, Genova, Italy, 2 Dynamic Robotics Laboratory, School of MIME, Oregon State University, Corvallis, OR, United States, 3 Department of Biomedical Physiology and Kinesiology, Simon Fraser University, Burnaby, BC, Canada, 4 Robotics and Mechatronics Center, German Aerospace Center, Oberpfaffenhofen, Germany, 5 Structure and Motion Laboratory, Royal Veterinary College, Hertfordshire, United Kingdom, 6 Biorobotics Laboratory, École Polytechnique Fédérale de Lausanne, Lausanne, Switzerland, 7 Robotics and Multibody Mechanics Research Group, Department of Mechanical Engineering, Vrije Universiteit Brussel and Flanders Make, Brussels, Belgium, 8 Centro di Ricerca “Enrico Piaggio”, University of Pisa, Pisa, Italy, 9 Robotics Institute, Carnegie Mellon University, Pittsburgh, PA, United States, 10 Applied Biomechanics Lab, Department of Integrative Physiology,
    [Show full text]
  • Benefits and Challenges of Mechanical Spring Systems for Energy Storage Applications
    Available online at www.sciencedirect.com ScienceDirect Energy Procedia 82 ( 2015 ) 805 – 810 ATI 2015 - 70th Conference of the ATI Engineering Association Benefits and challenges of mechanical spring systems for energy storage applications Federico Rossia, Beatrice Castellania*, Andrea Nicolinia aUniversity of Perugia, Department of Engineering, CIRIAF, Via G. Duranti 67, Perugia Abstract Storing the excess mechanical or electrical energy to use it at high demand time has great importance for applications at every scale because of irregularities of demand and supply. Energy storage in elastic deformations in the mechanical domain offers an alternative to the electrical, electrochemical, chemical, and thermal energy storage approaches studied in the recent years. The present paper aims at giving an overview of mechanical spring systems’ potential for energy storage applications. Part of the appeal of elastic energy storage is its ability to discharge quickly, enabling high power densities. This available amount of stored energy may be delivered not only to mechanical loads, but also to systems that convert it to drive an electrical load. Mechanical spring systems’ benefits and limits for storing macroscopic amounts of energy will be assessed and their integration with mechanical and electrical power devices will be discussed. ©© 2015 2015 The The Authors. Authors. Published Published by Elsevier by Elsevier Ltd. This Ltd. is an open access article under the CC BY-NC-ND license (Selectionhttp://creativecommons.org/licenses/by-nc-nd/4.0/ and/or peer-review under responsibility). of ATI Peer-review under responsibility of the Scientific Committee of ATI 2015 Keywords:energy storage; mechanical springs; energy storage density. 1.
    [Show full text]
  • Mechanical Energy
    Chapter 2 Mechanical Energy Mechanics is the branch of physics that deals with the motion of objects and the forces that affect that motion. Mechanical energy is similarly any form of energy that’s directly associated with motion or with a force. Kinetic energy is one form of mechanical energy. In this course we’ll also deal with two other types of mechanical energy: gravitational energy,associated with the force of gravity,and elastic energy, associated with the force exerted by a spring or some other object that is stretched or compressed. In this chapter I’ll introduce the formulas for all three types of mechanical energy,starting with gravitational energy. Gravitational Energy An object’s gravitational energy depends on how high it is,and also on its weight. Specifically,the gravitational energy is the product of weight times height: Gravitational energy = (weight) × (height). (2.1) For example,if you lift a brick two feet off the ground,you’ve given it twice as much gravitational energy as if you lift it only one foot,because of the greater height. On the other hand,a brick has more gravitational energy than a marble lifted to the same height,because of the brick’s greater weight. Weight,in the scientific sense of the word,is a measure of the force that gravity exerts on an object,pulling it downward. Equivalently,the weight of an object is the amount of force that you must exert to hold the object up,balancing the downward force of gravity. Weight is not the same thing as mass,which is a measure of the amount of “stuff” in an object.
    [Show full text]
  • Thermal Interface Material Catalog
    Thermal Interface Materials One Company, Many Solutions www.boydcorp.com BC012021 Thermal Interface Materials TABLE OF CONTENTS Title Page Introduction . 2 Gap Fillers . 3 Gap Rubber Pads . 12 Graphite . 16 Phase Change Materials . 18 Tapes . 21 Thermal Epoxy. 24 Thermal Grease . 25 Lorem ipsum 1 BC012021 Thermal Interface Materials INTRODUCTION Thermal Interface Materials (TIMs) are a critical portion to any effective thermal management system as they transfer heat between solid surfaces. Boyd provides a full array of thermal interface materials, from soft materials like gap fillers, phase change materials, and thermal grease to less compliant materials like thermal rubber pads, films, and thermally conductive hardware. Our broad portfolio contains many options that include electrical isolating properties, adhesives, reinforcements, carriers, and a variety of hardnesses to meet varying application requirements. Boyd's engineering team is well-equipped to help you determine the best material to meet your project’s needs. We leverage our relationships with suppliers and our TIM expertise, developed from decades of tests and projects, to pick the material best suited for your application. Boyd’s precision converting and assembly expertise can custom fabricate and pre-apply Thermal Interface Materials on Aavid’s thermal management solutions like liquid cold plates or heat sinks. By providing complete, ready-to-install thermal Lorem ipsum management solutions, we help customers reduce assembly time and costs with a complete and integrated thermal solution. 2 BC012021 TECHNICAL DATASHEET Transtherm® Thermally Conductive Gap Filler TRANSTHERM® THERMALLY CONDUCTIVE GAP FILLERS Transtherm® Thermally Conductive Gap Fillers are soft, malleable interface materials with high thermal conductivity. Gap fillers are ideal for applications with significant distances between the heat source and cooling surface, varying component heights, high tolerance stack up variability, and uneven or rough surfaces.
    [Show full text]
  • Energy Dissipation Mechanism and Damage Model of Marble Failure Under Two Stress Paths
    L. Zhang et alii, Frattura ed Integrità Strutturale, 30 (2014) 515-525; DOI: 10.3221/IGF-ESIS.30.62 Energy dissipation mechanism and damage model of marble failure under two stress paths Liming Zhang College of Science, Qingdao Technological University, Qingdao, Shandong 266033, China; [email protected] Co-operative Innovation Center of Engineering Construction and Safety in Shandong Peninsula blue economic zone, Qingdao Technological University ; Qingdao, Shandong 266033, China; [email protected] Mingyuan Ren, Shaoqiong Ma, Zaiquan Wang College of Science, Qingdao Technological University, Qingdao, Shandong 266033, China; Email: [email protected], [email protected], [email protected] ABSTRACT. Marble conventional triaxial loading and unloading failure testing research is carried out to analyze the elastic strain energy and dissipated strain energy evolutionary characteristics of the marble deformation process. The study results show that the change rates of dissipated strain energy are essentially the same in compaction and elastic stages, while the change rate of dissipated strain energy in the plastic segment shows a linear increase, so that the maximum sharp point of the change rate of dissipated strain energy is the failure point. The change rate of dissipated strain energy will increase during unloading confining pressure, and a small sharp point of change rate of dissipated strain energy also appears at the unloading point. The damage variable is defined to analyze the change law of failure variable over strain. In the loading test, the damage variable growth rate is first rapid then slow as a gradual process, while in the unloading test, a sudden increase appears in the damage variable before reaching the rock peak strength.
    [Show full text]
  • Noncuring Graphene Thermal Interface Materials for Advanced Electronics
    FULL PAPER www.advelectronicmat.de Noncuring Graphene Thermal Interface Materials for Advanced Electronics Sahar Naghibi, Fariborz Kargar,* Dylan Wright, Chun Yu Tammy Huang, Amirmahdi Mohammadzadeh, Zahra Barani, Ruben Salgado, and Alexander A. Balandin* development of next generation of compact Development of next-generation thermal interface materials (TIMs) with high and flexible electronics.[1] The increase in thermal conductivity is important for thermal management and packaging computer usage and ever-growing depend- ence on cloud systems require better of electronic devices. The synthesis and thermal conductivity measurements methods for dissipating heat away from of noncuring thermal paste, i.e., grease, based on mineral oil with a mixture electronic components. The important of graphene and few-layer graphene flakes as the fillers, is reported. The ingredients of thermal management are the graphene thermal paste exhibits a distinctive thermal percolation threshold thermal interface materials (TIMs). Various with the thermal conductivity revealing a sublinear dependence on the filler TIMs interface two uneven solid surfaces loading. This behavior contrasts with the thermal conductivity of curing where air would be a poor conductor of heat, and aid in heat transfer from one medium graphene TIMs, based on epoxy, where superlinear dependence on the filler into another. Two important classes of TIMs loading is observed. The performance of the thermal paste is benchmarked include curing and noncuring composites. against top-of-the-line commercial thermal pastes. The obtained results show Both of them consist of a base, i.e., matrix that noncuring graphene TIMs outperforms the best commercial pastes in materials, and thermally conducting fillers. terms of thermal conductivity, at substantially lower filler concentration of Commonly, the studies of new fillers for the use in TIMs start with the curing epoxy- ϕ = 27 vol%.
    [Show full text]
  • Dissipation Potentials from Elastic Collapse
    Dissipation potentials from royalsocietypublishing.org/journal/rspa elastic collapse Joe Goddard1 and Ken Kamrin2 1Department of Mechanical and Aerospace Engineering, University Research of California, San Diego, CA, USA 2 Cite this article: Goddard J, Kamrin K. 2019 Department of Mechanical Engineering, Massachusetts Institute of Dissipation potentials from elastic collapse. Technology, Cambridge, MA, USA Proc.R.Soc.A475: 20190144. JG, 0000-0003-4181-4994 http://dx.doi.org/10.1098/rspa.2019.0144 Generalizing Maxwell’s (Maxwell 1867 IV. Phil. Trans. Received: 7 March 2019 R. Soc. Lond. 157, 49–88 (doi:10.1098/rstl.1867.0004)) classical formula, this paper shows how the Accepted: 9 May 2019 dissipation potentials for a dissipative system can be derived from the elastic potential of an elastic system Subject Areas: undergoing continual failure and recovery. Hence, stored elastic energy gives way to dissipated elastic mechanics energy. This continuum-level response is attributed broadly to dissipative microscopic transitions over Keywords: a multi-well potential energy landscape of a type dissipative systems, nonlinear Onsager studied in several previous works, dating from symmetry, elastic failure, energy landscape Prandtl’s (Prandtl 1928 Ein Gedankenmodell zur kinetischen Theorie der festen Körper. ZAMM 8, Author for correspondence: 85–106) model of plasticity. Such transitions are assumed to take place on a characteristic time scale Joe Goddard T, with a nonlinear viscous response that becomes a e-mail: [email protected] plastic response for T → 0. We consider both discrete mechanical systems and their continuum mechanical analogues, showing how the Reiner–Rivlin fluid arises from nonlinear isotropic elasticity. A brief discussion is given in the conclusions of the possible extensions to other dissipative processes.
    [Show full text]
  • The Relationship Between Energy Demand and Real GDP Growth Rate: the Role of Price Asymmetries and Spatial Externalities Within 34 Countries Across the Globe
    The relationship between energy demand and real GDP growth rate: the role of price asymmetries and spatial externalities within 34 countries across the globe Panagiotis Fotis a Hellenic Competition Commission Commissioner Sotiris Karkalakos b University of Piraeus and DePaul University Department of Economics Dimitrios Asteriou c Oxford Brookes University Department of Accounting, Finance and Economics Abstract The aim of this paper is to empirically explore the relationship between energy demand and real Gross Domestic Product (GDP) growth and to investigate the role of asymmetries (price and GDP growth asymmetries) and regional externalities on Final Energy Consumption (FEC ) in 34 countries during the period from 2005 to 2013. The paper utilizes a Panel Generalized Method of Moments approach in order to analyse the effect of real GDP growth rate on FEC through an Error Correction Model (ECM) and spatial econometric techniques in order to examine clustered patterns of energy consumption. The results show that a) the demand is elastic both in the industrial and the household/services sectors, b) electricity and natural gas are demand substitutes, c) the relationship between real GDP growth rate and energy consumption exhibits an inverted U – shape, d) price (electricity and gas) and GDP growth asymmetries are supported from the employed parametric and non – parametric tests, and e) distance does not affect FEC, but economic neighbors have a strong positive effect. Keywords: energy demand; dynamic panel data; error correction model; spatial externalities. JEL classification C21; C23; C51; L16; R12 a Corresponding Author , Hellenic Competition Commission, Commissionner, 5 P. Ioakim St., 12132, Peristeri, Greece, Tel.: +30 6947609741, E-mail: [email protected] .
    [Show full text]
  • US5198189.Pdf
    |||||||||||| USOO598 89A United States Patent (19) 11 Patent Number: 5,198,189 Booth et al. r (45) Date of Patent: Mar. 30, 1993 54) LIQUID METAL MATRIXTHERMAL PASTE FOREIGN PATENT DOCUMENTS (75) Inventors: Richard B. Booth, Wappingers Falls; 0009605 4/1980 European Pat. Off. Gary W. Grube, Washingtonville; 332981 4/1972 U.S.S.R. ............................. 420/.555 Peter A. Gruber, Mohegan Lake; Igor Y. Khandros, Peekskill; Arthur OTHER PUBLICATIONS R. Zingher, White Plains, all of N.Y. Patent Abstracts of Japan, vol. 12, No. 342 (E-658), 73 Assignee: International Business Machines Sep. 14th, 1988; JP-A-63 102 345 (Fujitsu Ltd) May 7, 1988. Corporation, Armonk, N.Y. Patent Abstracts of Japan, vol. 8, No. 236 (C-249), Oct. 21 Appl. No.: 870,152 30th, 1984; and JP-A-59 16 357 (Hitachi Seisakusho K.K.) Jul. 5, 1984. (22 Filed: Apr. 13, 1992 Patent Abstracts of Japan, vol. 7, No. 218 (E-200), Sep. 28th, 1983; and JP-A-58 111 354 (Hitachi Seisakusho Related U.S. Application Data K.K.) Jul. 2, 1983. a Patent Abstracts of Japan, vol. 11, No. 3 (C-395), Jan. 63 Continuation of Ser. No. 389,131, Aug. 3, 1989. 7th, 1987; and JP-A-61 179 844 (Tokuriki Honten Co., 51) Int. C. .............................................. C22C 28/00 Ltd) Aug. 12, 1986. 52 U.S. Cl. ..................................... 420/555; 252/387 Primary Examiner-Peter D. Rosenberg 58 Field of Search ..................... 420/555; 228/1802; Attorney, Agent, or Firm-Philip J. Feig 252/38 7 57 ABSTRACT (56) References Cited A liquid metal matrix thermal paste comprises a disper U.S.
    [Show full text]
  • Energy Regenerative Damping in Variable Impedance Actuators for Long-Term Robotic Deployment
    XXXX, VOL. X, NO. X, JANUARY 2020 1 Energy regenerative damping in variable impedance actuators for long-term robotic deployment Fan Wu and Matthew Howard∗† Abstract—Energy efficiency is a crucial issue towards long- Recently, much research effort has gone into the design term deployment of compliant robots in the real world. In of variable physical damping actuation, based on different the context of variable impedance actuators (VIAs), one of the principles of damping force generation (see [4], [5] for a main focuses has been on improving energy efficiency through reduction of energy consumption. However, the harvesting of review). Variable physical damping has proven to be necessary dissipated energy in such systems remains under-explored. This to achieve better task performance, for example, in eliminat- study proposes a variable damping module design enabling ing undesired oscillations caused by the elastic elements of energy regeneration in VIAs by exploiting the regenerative VSAs [6], [7]. It has also been demonstrated that variable braking effect of DC motors. The proposed damping module physical damping plays an important role in terms of energy uses four switches to combine regenerative and dynamic braking, in a hybrid approach that enables energy regeneration without efficiency for actuators that are required to operate at different a reduction in the range of damping achievable. A physical frequencies, to optimally exploit the natural dynamics [6]. implementation on a simple VIA mechanism is presented in However, while these studies represent important advances which the regenerative properties of the proposed module are in terms of improving the efficiency of energy consumption characterised and compared against theoretical predictions.
    [Show full text]
  • What Is Elastic Potential Energy?
    What is Elastic Potential Energy? Elastic Potential Energy Elasticity is energy stored in something that has is the ability of a material or an object to elasticity. resume its normal shape after being compressed or stretched. Objects that can be stretched and compressed can hold elastic energy. The amount of elastic potential energy is determined by the extent to which the object can stretch or compress. The more you stretch or compress it the higher the elastic potential energy. Why does a ball bounce? A balls ability to bounce has to do with its elasticity. The elasticity of a ball is determined by its material. Its round shape guarantees an equal, uniform response – no matter on which point the ball hits the ground. What happens during a bounce? By lifting it up, the ball receives potential energy which is transformed into kinetic energy It pushes back on the when you drop it. ground and shoots back up into the air. When the ball hits Due to its elasticity the ground it quickly returns to it gets compressed. its original shape. For this experiment you will need: Different types of balls, e.g. a tennisball, golfball, marble, basketball… Tape measure Masking tape Pencil Instructions 1) Choose an area next to a wall or table where the ground is rather hard and flat. 2) Use the masking tape and the tape measure to mark different heights: 10’’, 15’’, 20’’, 25’’, 30’’ 3) Start with the first ball: Have a partner drop it from 30’’ DROP the ball – and record the height of the bounce in the Bounce Tracker below.
    [Show full text]