Mechanical Energy
Total Page:16
File Type:pdf, Size:1020Kb
Load more
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) -
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, -
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 -
Energy Literacy Essential Principles and Fundamental Concepts for Energy Education
Energy Literacy Essential Principles and Fundamental Concepts for Energy Education A Framework for Energy Education for Learners of All Ages About This Guide Energy Literacy: Essential Principles and Intended use of this document as a guide includes, Fundamental Concepts for Energy Education but is not limited to, formal and informal energy presents energy concepts that, if understood and education, standards development, curriculum applied, will help individuals and communities design, assessment development, make informed energy decisions. and educator trainings. Energy is an inherently interdisciplinary topic. Development of this guide began at a workshop Concepts fundamental to understanding energy sponsored by the Department of Energy (DOE) arise in nearly all, if not all, academic disciplines. and the American Association for the Advancement This guide is intended to be used across of Science (AAAS) in the fall of 2010. Multiple disciplines. Both an integrated and systems-based federal agencies, non-governmental organizations, approach to understanding energy are strongly and numerous individuals contributed to the encouraged. development through an extensive review and comment process. Discussion and information Energy Literacy: Essential Principles and gathered at AAAS, WestEd, and DOE-sponsored Fundamental Concepts for Energy Education Energy Literacy workshops in the spring of 2011 identifies seven Essential Principles and a set of contributed substantially to the refinement of Fundamental Concepts to support each principle. the guide. This guide does not seek to identify all areas of energy understanding, but rather to focus on those To download this guide and related documents, that are essential for all citizens. The Fundamental visit www.globalchange.gov. Concepts have been drawn, in part, from existing education standards and benchmarks. -
STARS in HYDROSTATIC EQUILIBRIUM Gravitational Energy
STARS IN HYDROSTATIC EQUILIBRIUM Gravitational energy and hydrostatic equilibrium We shall consider stars in a hydrostatic equilibrium, but not necessarily in a thermal equilibrium. Let us define some terms: U = kinetic, or in general internal energy density [ erg cm −3], (eql.1a) U u ≡ erg g −1 , (eql.1b) ρ R M 2 Eth ≡ U4πr dr = u dMr = thermal energy of a star, [erg], (eql.1c) Z Z 0 0 M GM dM Ω= − r r = gravitational energy of a star, [erg], (eql.1d) Z r 0 Etot = Eth +Ω = total energy of a star , [erg] . (eql.1e) We shall use the equation of hydrostatic equilibrium dP GM = − r ρ, (eql.2) dr r and the relation between the mass and radius dM r =4πr2ρ, (eql.3) dr to find a relations between thermal and gravitational energy of a star. As we shall be changing variables many times we shall adopt a convention of using ”c” as a symbol of a stellar center and the lower limit of an integral, and ”s” as a symbol of a stellar surface and the upper limit of an integral. We shall be transforming an integral formula (eql.1d) so, as to relate it to (eql.1c) : s s s GM dM GM GM ρ Ω= − r r = − r 4πr2ρdr = − r 4πr3dr = (eql.4) Z r Z r Z r2 c c c s s s dP s 4πr3dr = 4πr3dP =4πr3P − 12πr2P dr = Z dr Z c Z c c c s −3 P 4πr2dr =Ω. Z c Our final result: gravitational energy of a star in a hydrostatic equilibrium is equal to three times the integral of pressure within the star over its entire volume. -
Energy Conservation in a Spring
Part II: Energy Conservation in a Spring Activity 4 Title: Forces and Energy in a Spring Summary: Students will use the “Masses and Springs” simulation from PhET to investigate the relationship between gravitational potential energy, spring potential energy, and mass. Standard: PS2 (Ext) - 5 Students demonstrate an understanding of energy by… 5aa Identifying, measuring, calculating and analyzing qualitative and quantitative relationships associated with energy transfer or energy transformation. Specific Learning Goals: 1. Understand how to calculate the force constant of a spring using the formula F = -k ∆x 2. Understand that even though energy is transformed during the oscillation of a spring among gravitational potential energy, elastic potential energy, and kinetic energy, the total energy in the system remains constant. 3. Understand how to calculate the gravitational potential energy for a mass which is lifted to a height above a table. 4. Understand how to calculate the elastic potential energy for a spring which has been displaced by a certain distance. Prior Knowledge: 1. The restoring force that a spring exerts on a mass is proportional to the displacement of the spring and the spring constant and is in a direction opposite the displacement: F = -k ∆x 2. Gravitational potential energy is calculated by the formula: PEg = mgΔh 2 3. Elastic potential energy is calculated by the formula: PEs = ½ k ∆x 4. In a mass and spring system at equilibrium, the restoring force is equal to the gravitational force on the suspended mass (Fg = mg) Schedule: 40-50 minutes Materials: “Masses and Springs 2.02 PhET” Engage: Three different masses are suspended from a spring. -
Work and Energy Summary Sheet Chapter 6
Work and Energy Summary Sheet Chapter 6 Work: work is done when a force is applied to a mass through a displacement or W=Fd. The force and the displacement must be parallel to one another in order for work to be done. F (N) W =(Fcosθ)d F If the force is not parallel to The area of a force vs. the displacement, then the displacement graph + W component of the force that represents the work θ d (m) is parallel must be found. done by the varying - W d force. Signs and Units for Work Work is a scalar but it can be positive or negative. Units of Work F d W = + (Ex: pitcher throwing ball) 1 N•m = 1 J (Joule) F d W = - (Ex. catcher catching ball) Note: N = kg m/s2 • Work – Energy Principle Hooke’s Law x The work done on an object is equal to its change F = kx in kinetic energy. F F is the applied force. 2 2 x W = ΔEk = ½ mvf – ½ mvi x is the change in length. k is the spring constant. F Energy Defined Units Energy is the ability to do work. Same as work: 1 N•m = 1 J (Joule) Kinetic Energy Potential Energy Potential energy is stored energy due to a system’s shape, position, or Kinetic energy is the energy of state. motion. If a mass has velocity, Gravitational PE Elastic (Spring) PE then it has KE 2 Mass with height Stretch/compress elastic material Ek = ½ mv 2 EG = mgh EE = ½ kx To measure the change in KE Change in E use: G Change in ES 2 2 2 2 ΔEk = ½ mvf – ½ mvi ΔEG = mghf – mghi ΔEE = ½ kxf – ½ kxi Conservation of Energy “The total energy is neither increased nor decreased in any process. -
Potential Energy
Potential Energy • So far: Considered all forces equal, calculate work done by net force only => Change in kinetic energy. – Analogy: Pure Cash Economy • But: Some forces seem to be able to “store” the work for you (when they do negative work) and “give back” the same amount (when they do positive work). – Analogy: Bank Account. You pay money in (ending up with less cash) - the money is stored for you - you can withdraw it again (get cash back) • These forces are called “conservative” (they conserve your work/money for you) Potential Energy - Example • Car moving up ramp: Weight does negative work ΔW(grav) = -mgΔh • Depends only on initial and final position • Can be retrieved as positive work on the way back down • Two ways to describe it: 1) No net work done on car on way up F Pull 2) Pulling force does positive F Normal y work that is stored as gravitational x potential energy ΔU = -ΔW(grav) α F Weight Total Mechanical Energy • Dimension: Same as Work Unit: Nm = J (Joule) Symbol: E = K.E. + U 1) Specify all external *) forces acting on a system 2) Multiply displacement in the direction of the net external force with that force: ΔWext = F Δs cosφ 3) Set equal to change in total energy: m 2 m 2 ΔE = /2vf - /2vi + ΔU = ΔWext ΔU = -Wint *) We consider all non-conservative forces as external, plus all forces that we don’t want to include in the system. Example: Gravitational Potential Energy *) • I. Motion in vertical (y-) direction only: "U = #Wgrav = mg"y • External force: Lift mass m from height y i to height y f (without increasing velocity) => Work gets stored as gravitational potential energy ΔU = mg (yf -yi)= mg Δy ! • Free fall (no external force): Total energy conserved, change in kinetic energy compensated by change in m 2 potential energy ΔK.E. -
How Long Would the Sun Shine? Fuel = Gravitational Energy? Fuel
How long would the Sun shine? Fuel = Gravitational Energy? • The mass of the Sun is M = 2 x 1030 kg. • The Sun needs fuel to shine. – The amount of the fuel should be related to the amount of – The Sun shines by consuming the fuel -- it generates energy mass. from the fuel. • Gravity can generate energy. • The lifetime of the Sun is determined by – A falling body acquires velocity from gravity. – How fast the Sun consumes the fuel, and – Gravitational energy = (3/5)GM2/R – How much fuel the Sun contains. – The radius of the Sun: R = 700 million m • How fast does the Sun consume the fuel? – Gravitational energy of the Sun = 2.3 x 1041 Joules. – Energy radiated per second is called the “luminosity”, which • How long could the Sun shine on gravitational energy? is in units of watts. – Lifetime = (Amount of Fuel)/(How Fast the Fuel is – The solar luminosity is about 3.8 x 1026 Watts. Consumed) 41 26 • Watts = Joules per second – Lifetime = (2.3 x 10 Joules)/(3.8 x 10 Joules per second) = 0.6 x 1015 seconds. • Compare it with a light bulb! – Therefore, the Sun lasts for 20 million years (Helmholtz in • What is the fuel?? 1854; Kelvin in 1887), if gravity is the fuel. Fuel = Nuclear Energy Burning Hydrogen: p-p chain • Einstein’s Energy Formula: E=Mc2 1 1 2 + – The mass itself can be the source of energy. • H + H -> H + e + !e 2 1 3 • If the Sun could convert all of its mass into energy by • H + H -> He + " E=Mc2… • 3He + 3He -> 4He + 1H + 1H – Mass energy = 1.8 x 1047 Joules. -
On the First Electromagnetic Measurement of the Velocity of Light by Wilhelm Weber and Rudolf Kohlrausch
Andre Koch Torres Assis On the First Electromagnetic Measurement of the Velocity of Light by Wilhelm Weber and Rudolf Kohlrausch Abstract The electrostatic, electrodynamic and electromagnetic systems of units utilized during last century by Ampère, Gauss, Weber, Maxwell and all the others are analyzed. It is shown how the constant c was introduced in physics by Weber's force of 1846. It is shown that it has the unit of velocity and is the ratio of the electromagnetic and electrostatic units of charge. Weber and Kohlrausch's experiment of 1855 to determine c is quoted, emphasizing that they were the first to measure this quantity and obtained the same value as that of light velocity in vacuum. It is shown how Kirchhoff in 1857 and Weber (1857-64) independently of one another obtained the fact that an electromagnetic signal propagates at light velocity along a thin wire of negligible resistivity. They obtained the telegraphy equation utilizing Weber’s action at a distance force. This was accomplished before the development of Maxwell’s electromagnetic theory of light and before Heaviside’s work. 1. Introduction In this work the introduction of the constant c in electromagnetism by Wilhelm Weber in 1846 is analyzed. It is the ratio of electromagnetic and electrostatic units of charge, one of the most fundamental constants of nature. The meaning of this constant is discussed, the first measurement performed by Weber and Kohlrausch in 1855, and the derivation of the telegraphy equation by Kirchhoff and Weber in 1857. Initially the basic systems of units utilized during last century for describing electromagnetic quantities is presented, along with a short review of Weber’s electrodynamics. -
Gravitational Potential Energy
An easy way for numerical calculations • How long does it take for the Sun to go around the galaxy? • The Sun is travelling at v=220 km/s in a mostly circular orbit, of radius r=8 kpc REVISION Use another system of Units: u Assume G=1 Somak Raychaudhury u Unit of distance = 1kpc www.sr.bham.ac.uk/~somak/Y3FEG/ u Unit of velocity= 1 km/s u Then Unit of time becomes 109 yr •Course resources 5 • Website u And Unit of Mass becomes 2.3 × 10 M¤ • Books: nd • Sparke and Gallagher, 2 Edition So the time taken is 2πr/v = 2π × 8 /220 time units • Carroll and Ostlie, 2nd Edition Gravitational potential energy 1 Measuring the mass of a galaxy cluster The Virial theorem 2 T + V = 0 Virial theorem Newton’s shell theorems 2 Potential-density pairs Potential-density pairs Effective potential Bertrand’s theorem 3 Spiral arms To establish the existence of SMBHs are caused by density waves • Stellar kinematics in the core of the galaxy that sweep • Optical spectra: the width of the spectral line from around the broad emission lines Galaxy. • X-ray spectra: The iron Kα line is seen is clearly seen in some AGN spectra • The bolometric luminosities of the central regions of The Winding some galaxies is much larger than the Eddington Paradox (dilemma) luminosity is that if galaxies • Variability in X-rays: Causality demands that the rotated like this, the spiral structure scale of variability corresponds to an upper limit to would be quickly the light-travel time erased. -
Lawrence Berkeley National Laboratory Recent Work
Lawrence Berkeley National Laboratory Recent Work Title E.E. REVIEW COURSE - LECTURE VIII. Permalink https://escholarship.org/uc/item/733807j5 Authors Martinelli, E. Leppard, J. Perl, H. Publication Date 1952-04-21 eScholarship.org Powered by the California Digital Library University of California UNIVERSITY OF CALIFORNIA UCRT. 1888 Radiation Laboratory Berkeley, California ELECTRICAL ENGINEERING REVIEW COURSE LECTURE VIII April 21, 1952 E. Martinelli (Notes by: J. Leppard, H. -Perl) I. MAG1TETIC FIELDS A. Electrostatic Case Coulomb's Law which is given for th~ electrostatic case can be stated thus~ 2 ~ F = f e1 e2 / r in which F is in dynes, r in centimeters, f = 1 (dimensionless}j'l-gives the value of the charge e, in electro static units (ESU). B. Magnetic Case The magnetic case has an equivalent which was first determined "experi mentally by Ampere. Given two closed loops of wire of length~. Using electromagnetic units (EMU) i is measured in ab amperes = 10 amperes. r is measured in centimeters.· C = 1 (dimensionless). DISCLAIMER This document was prepared as an account of work sponsored by the United States Government. While this document is believed to contain correct information, neither the United States Government nor any agency thereof, nor the Regents of the University of California, nor any of their employees, makes any warranty, express or implied, or assumes any legal responsibility for the accuracy, completeness, or usefulness of any information, apparatus, product, or process disclosed, or represents that its use would not infringe privately owned rights. Reference herein to any specific commercial product, process, or service by its trade name, trademark, manufacturer, or otherwise, does not necessarily constitute or imply its endorsement, recommendation, or favoring by the United States Government or any agency thereof, or the Regents of the University of California.