Metamaterial Structures for Wakefield Acceleration and High Power Microwave Generation Xueying Lu

Total Page:16

File Type:pdf, Size:1020Kb

Metamaterial Structures for Wakefield Acceleration and High Power Microwave Generation Xueying Lu Metamaterial Structures for Wakefield Acceleration and High Power Microwave Generation by Xueying Lu B. S. (Engineering Physics), Tsinghua University (2012) Submitted to the Department of Physics in partial fulfillment of the requirements for the degree of Doctor of Philosophy at the MASSACHUSETTS INSTITUTE OF TECHNOLOGY February 2019 ○c Massachusetts Institute of Technology 2019. All rights reserved. Author................................................................ Department of Physics November 16, 2018 Certified by. Richard J. Temkin Senior Scientist, Department of Physics Thesis Supervisor Accepted by . Nergis Mavalvala Associate Department Head 2 Metamaterial Structures for Wakefield Acceleration and High Power Microwave Generation by Xueying Lu Submitted to the Department of Physics on November 16, 2018, in partial fulfillment of the requirements for the degree of Doctor of Philosophy Abstract This thesis presents the theoretical and experimental investigation of the interac- tion of metamaterial structures with electron beams for two applications: wakefield acceleration and high power microwave generation. Under the topic of wakefield acceleration, on the theoretical side, several meta- material structures have been designed and simulated. The novel phenomenon of reversed Cherenkov radiation has been found to enhance the beam-wave interaction in metamaterials. A metallic wagon wheel metamaterial structure was designed and built for use in an experiment at the Argonne Wakefield Accelerator (AWA) Facility. On the experimental side, this thesis presents the first demonstration of high- power, reversed Cherenkov wakefield radiation by short electron bunches passing through the wagon wheel structure at the AWA. Single 45 nC electron bunches of 65 MeV energy traversing the structure generated up to 25 MW in 2 ns pulses at 11.4 GHz, in excellent agreement with theory. Two bunches of 85 nC with appropriate temporal spacing generated up to 80 MW by coherent wakefield superposition. If this power were applied to a trailing witness bunch in a collinear wakefield accelerator, it would provide an accelerating gradient of 75 MV/m. Under the topic of high power microwave generation, on the theoretical side, an analytical theory has been developed to predict the novel Cherenkov-cyclotron in- teraction in metamaterial-based microwave devices. An S-band metamaterial-loaded waveguide with reverse symmetry has been designed and built to work with the Cherenkov-cyclotron interaction. On the experimental side, this thesis presents the experimental results of the metamaterial-loaded waveguide built at MIT. Power levels to 2.9 MW at 2.4 GHz in full 1 휇s pulses were generated by an electron beam of up to 490 kV of voltage and 84 A of current. Frequency tuning measurements verified that pulses above 1 MW of output power were only seen in the Cherenkov-cyclotron mode. With these results, this thesis demonstrates the unique features of metamaterial structures that are very attractive for high-gradient wakefield accelerators and high power microwave sources. Advantages include the high shunt impedance for intense 3 beam-wave interaction; the simple and rugged structure; and a large parameter space for various optimization goals. Thesis Supervisor: Richard J. Temkin Title: Senior Scientist, Department of Physics 4 Acknowledgments This thesis is the product of the tremendous support and help I was fortunate to receive from many people, to whom I owe a debt of gratitude. I would like to thank my thesis advisor, Dr. Richard Temkin, who has all the great things that an amazing advisor can have: knowledge, insight, patience, willingness to help, and many more. I thank Rick for bringing me to MIT and for making my PhD years enjoyable. It has been my great honor to work in the group. I would like to thank Dr. Michael Shapiro, who also closely advised my research and contributed greatly to the completion of this thesis. A quick talk with Michael would often lead to solutions to some mysteries that troubled me for days or weeks. I would like to thank Dr. Ivan Mastovsky, who always knows how to deal with misbehaving lab equipment. Ivan’s experimental expertise helped me get over all the hurdles during my time in the lab. I would like to thank my colleagues in the group past and present. I am so lucky to get to know and to work with these great people. I thank Dr. Jason Hummelt for showing me how to run the experiment in the West Cell. I thank Dr. Jacob Stephens and Dr. Guy Rosenzweig for their help and good conversations in the lab. I thank Dr. Jiexi Zhang for being a patient climbing buddy. I thank Dr. Alexander Soane for sending postcards from all over the world. I thank Dr. Sudheer Jawla, Julian Picard, Samuel Schaub and Haoran Xu for helpful discussions and comments on my work. I thank my previous officemates Dr. Sergey Arsenyev, Dr. Elizabeth Kowalski and Hannah Hoffmann for making the work environment happy. I would like to thank our collaborators at the Argonne National Laboratory, Dr. John Power, Dr. Manoel Conde, Dr. Jiahang Shao, Dr. Eric Wisniewski, Scott Doran, Charles Whiteford and Dr. Chunguang Jing, for their great help. They made my experience in Argonne both rewarding and fun. I would like to thank the MIT central machine shop, Andrew Gallant and Michael Abruzzese, for making almost all the parts for my experiments and for helping me to improve the mechanical drawings. 5 I would like to thank Dr. Miklos Porkolab and Dr. John Belcher for being on my thesis committee and my oral exam committee. Dr. Earl Marmar also served on my oral exam committee. From them I received comments and suggestions which helped greatly throughout the preparation and the review of this thesis. I would like to thank my undergraduate professors at Tsinghua University, Dr. Wenhui Huang, Dr. Jianfei Hua, Dr. Chuanxiang Tang, Dr. Huaibi Chen and Dr. Yi-Kang Pu, for encouraging me to pursue my graduate study in physics. I would like to thank all my friends, at MIT, in Boston, in the US, and in China, for sharing numerous good memories with me. I am most proud of the friends I have kept for over a decade long: Yan, Jessica Qijie, Yipeng, Zhao, Rui and Zong. During these years, we have grown separately, but we have never grown apart. Last but not least, I would like to thank my parents. My father Chao Lu intro- duced me to classical Chinese literature when I was a kid, which has taught me the great values of kindness, integrity and courage. My mother Xiaoxia Xue provides me with a great example of an independent and strong woman. I thank you for your love and support, and this thesis is dedicated to you. Xueying Lu November 15, 2018 During first snow of the season Cambridge, MA 6 Contents 1 Introduction 21 1.1 Metamaterials . 21 1.1.1 Basic Principles of Metamaterials . 23 1.1.2 Negative Refraction . 26 1.1.3 Reversed Cherenkov Radiation . 28 1.2 Wakefield Acceleration . 29 1.2.1 Motivation for High Gradient Accelerator Research . 30 1.2.2 Plasma Wakefield Acceleration . 32 1.2.3 Structure-Based Wakefield Acceleration . 33 1.2.4 Advantages of Metamaterial Structures for Wakefield Acceleration 37 1.3 High Power Microwave Generation . 38 1.3.1 Metamaterial-Based Microwave Sources . 38 1.3.2 Stimulated Cherenkov Radiation . 39 1.4 Thesis Outline . 42 2 Theory of Metamaterial Structures for Wakefield Acceleration 45 2.1 Motivation . 45 2.2 Theory of Circular Deep Corrugation Structure . 46 2.2.1 Design of the Circular Deep Corrugation Structure . 46 2.2.2 Analytical Theory . 47 2.2.3 Numerical Simulation of a Multi-Cell Structure . 50 7 2.2.4 Benchmarking . 51 2.2.5 Scaling Study . 53 2.2.6 Nominal Design . 60 2.2.7 Conclusions . 61 2.3 Design of Wagon Wheel Structure . 62 2.3.1 Motivation . 62 2.3.2 Unit Cell Design . 63 2.3.3 Double Negative Permittivity and Permeability . 66 2.3.4 Enhanced Beam-Wave Interaction . 67 2.3.5 Output Ports Design . 70 2.4 Theory of Wagon Wheel Metamaterial Structure . 72 2.4.1 Pulse Length . 72 2.4.2 Output Power from a Single Bunch . 75 2.4.3 Output Power from a Bunch Train . 75 2.5 Simulations of Wagon Wheel Metamaterial Structure . 77 2.5.1 Microwave Simulations . 77 2.5.2 Beam Simulations . 79 2.6 Theory of Volumetric 3D Metamaterial Structure . 81 2.6.1 Motivation . 82 2.6.2 Unit Cell Design . 83 2.6.3 Effective Medium Theory with Spatial Dispersion . 87 2.6.4 Wave-Beam Interaction Using Effective Medium Theory . 91 2.6.5 Radiation Pattern in a Volumetric Array of Metamaterial Unit Cells . 95 2.6.6 Application of the Volumetric Metamaterial for Wakefield Ac- celeration . 97 2.6.7 Conclusions . 98 2.7 Theory of Elliptical Deep Corrugation Structure . 100 8 3 Experiment of Metamaterial Structures for Wakefield Acceleration103 3.1 Experimental Facilities . 103 3.2 Structure Fabrication . 110 3.2.1 Full Assembly . 110 3.2.2 Metamaterial Structure Part . 111 3.2.3 Waveguides . 114 3.3 Cold Test . 116 3.3.1 Transmission Measurement . 117 3.3.2 Beadpull Measurement . 117 3.4 Beam Test Results . 124 3.4.1 Single Bunch Experiment . 124 3.4.2 Two-Bunch Experiment . 128 3.5 Conclusions . 137 4 Theory of Metamaterial Structures for High Power Microwave Gen- eration 139 4.1 Review of Previous Metamaterial-Based High Power Microwave Re- search at MIT . 140 4.2 Theory of Cherenkov-Cyclotron Instability in a Metamaterial Waveguide147 4.2.1 Motivation . 147 4.2.2 Metamaterial Loaded Waveguide Mode . 149 4.2.3 Electron Beam Interaction with the Antisymmetric Metamate- rial Waveguide Mode: Cherenkov-Cyclotron Instability .
Recommended publications
  • Influence of Angular Velocity of Pedaling on the Accuracy of The
    Research article 2018-04-10 - Rev08 Influence of Angular Velocity of Pedaling on the Accuracy of the Measurement of Cyclist Power Abstract Almost all cycling power meters currently available on the The miscalculation may be—even significantly—greater than we market are positioned on rotating parts of the bicycle (pedals, found in our study, for the following reasons: crank arms, spider, bottom bracket/hub) and, regardless of • the test was limited to only 5 cyclists: there is no technical and construction differences, all calculate power on doubt other cyclists may have styles of pedaling with the basis of two physical quantities: torque and angular velocity greater variations of angular velocity; (or rotational speed – cadence). Both these measures vary only 2 indoor trainer models were considered: other during the 360 degrees of each revolution. • models may produce greater errors; The torque / force value is usually measured many times during slopes greater than 5% (the only value tested) may each rotation, while the angular velocity variation is commonly • lead to less uniform rotations and consequently neglected, considering only its average value for each greater errors. revolution (cadence). It should be noted that the error observed in this analysis This, however, introduces an unpredictable error into the power occurs because to measure power the power meter considers calculation. To use the average value of angular velocity means the average angular velocity of each rotation. In power meters to consider each pedal revolution as perfectly smooth and that use this type of calculation, this error must therefore be uniform: but this type of pedal revolution does not exist in added to the accuracy stated by the manufacturer.
    [Show full text]
  • Basement Flood Mitigation
    1 Mitigation refers to measures taken now to reduce losses in the future. How can homeowners and renters protect themselves and their property from a devastating loss? 2 There are a range of possible causes for basement flooding and some potential remedies. Many of these low-cost options can be factored into a family’s budget and accomplished over the several months that precede storm season. 3 There are four ways water gets into your basement: Through the drainage system, known as the sump. Backing up through the sewer lines under the house. Seeping through cracks in the walls and floor. Through windows and doors, called overland flooding. 4 Gutters can play a huge role in keeping basements dry and foundations stable. Water damage caused by clogged gutters can be severe. Install gutters and downspouts. Repair them as the need arises. Keep them free of debris. 5 Channel and disperse water away from the home by lengthening the run of downspouts with rigid or flexible extensions. Prevent interior intrusion through windows and replace weather stripping as needed. 6 Many varieties of sturdy window well covers are available, simple to install and hinged for easy access. Wells should be constructed with gravel bottoms to promote drainage. Remove organic growth to permit sunlight and ventilation. 7 Berms and barriers can help water slope away from the home. The berm’s slope should be about 1 inch per foot and extend for at least 10 feet. It is important to note permits are required any time a homeowner alters the elevation of the property.
    [Show full text]
  • Simple Harmonic Motion
    [SHIVOK SP211] October 30, 2015 CH 15 Simple Harmonic Motion I. Oscillatory motion A. Motion which is periodic in time, that is, motion that repeats itself in time. B. Examples: 1. Power line oscillates when the wind blows past it 2. Earthquake oscillations move buildings C. Sometimes the oscillations are so severe, that the system exhibiting oscillations break apart. 1. Tacoma Narrows Bridge Collapse "Gallopin' Gertie" a) http://www.youtube.com/watch?v=j‐zczJXSxnw II. Simple Harmonic Motion A. http://www.youtube.com/watch?v=__2YND93ofE Watch the video in your spare time. This professor is my teaching Idol. B. In the figure below snapshots of a simple oscillatory system is shown. A particle repeatedly moves back and forth about the point x=0. Page 1 [SHIVOK SP211] October 30, 2015 C. The time taken for one complete oscillation is the period, T. In the time of one T, the system travels from x=+x , to –x , and then back to m m its original position x . m D. The velocity vector arrows are scaled to indicate the magnitude of the speed of the system at different times. At x=±x , the velocity is m zero. E. Frequency of oscillation is the number of oscillations that are completed in each second. 1. The symbol for frequency is f, and the SI unit is the hertz (abbreviated as Hz). 2. It follows that F. Any motion that repeats itself is periodic or harmonic. G. If the motion is a sinusoidal function of time, it is called simple harmonic motion (SHM).
    [Show full text]
  • Hub City Powertorque® Shaft Mount Reducers
    Hub City PowerTorque® Shaft Mount Reducers PowerTorque® Features and Description .................................................. G-2 PowerTorque Nomenclature ............................................................................................ G-4 Selection Instructions ................................................................................ G-5 Selection By Horsepower .......................................................................... G-7 Mechanical Ratings .................................................................................... G-12 ® Shaft Mount Reducers Dimensions ................................................................................................ G-14 Accessories ................................................................................................ G-15 Screw Conveyor Accessories ..................................................................... G-22 G For Additional Models of Shaft Mount Reducers See Hub City Engineering Manual Sections F & J DOWNLOAD AVAILABLE CAD MODELS AT: WWW.HUBCITYINC.COM Certified prints are available upon request EMAIL: [email protected] • www.hubcityinc.com G-1 Hub City PowerTorque® Shaft Mount Reducers Ten models available from 1/4 HP through 200 HP capacity Manufacturing Quality Manufactured to the highest quality 98.5% standards in the industry, assembled Efficiency using precision manufactured components made from top quality per Gear Stage! materials Designed for the toughest applications in the industry Housings High strength ductile
    [Show full text]
  • Rotational Motion of Electric Machines
    Rotational Motion of Electric Machines • An electric machine rotates about a fixed axis, called the shaft, so its rotation is restricted to one angular dimension. • Relative to a given end of the machine’s shaft, the direction of counterclockwise (CCW) rotation is often assumed to be positive. • Therefore, for rotation about a fixed shaft, all the concepts are scalars. 17 Angular Position, Velocity and Acceleration • Angular position – The angle at which an object is oriented, measured from some arbitrary reference point – Unit: rad or deg – Analogy of the linear concept • Angular acceleration =d/dt of distance along a line. – The rate of change in angular • Angular velocity =d/dt velocity with respect to time – The rate of change in angular – Unit: rad/s2 position with respect to time • and >0 if the rotation is CCW – Unit: rad/s or r/min (revolutions • >0 if the absolute angular per minute or rpm for short) velocity is increasing in the CCW – Analogy of the concept of direction or decreasing in the velocity on a straight line. CW direction 18 Moment of Inertia (or Inertia) • Inertia depends on the mass and shape of the object (unit: kgm2) • A complex shape can be broken up into 2 or more of simple shapes Definition Two useful formulas mL2 m J J() RRRR22 12 3 1212 m 22 JRR()12 2 19 Torque and Change in Speed • Torque is equal to the product of the force and the perpendicular distance between the axis of rotation and the point of application of the force. T=Fr (Nm) T=0 T T=Fr • Newton’s Law of Rotation: Describes the relationship between the total torque applied to an object and its resulting angular acceleration.
    [Show full text]
  • PHYS 211 Lecture 5 - Oscillations: Simple Harmonic Motion 5 - 1
    PHYS 211 Lecture 5 - Oscillations: simple harmonic motion 5 - 1 Lecture 5 - Oscillations: simple harmonic motion Text: Fowles and Cassiday, Chap. 3 Consider a power series expansion for the potential energy of an object 2 V(x) = Vo + V1x + V2x + ..., where x is the displacement of an object from its equilibrium position, and Vi, i = 0,1,2... are fixed coefficients. The leading order term in this series is unimportant to the dynamics of the object, since F = -dV/dx and the derivative of a constant vanishes. Further, if we require the equilibrium position x = 0 to be a true minimum in the energy, then V1 = 0. This doesn’t mean that potentials with odd powers in x must vanish, but just says that their minimum is not at x = 0. Thus, the simplest function that one can write is quadratic: 2 V = V2x [A slightly more complicated variant is |x| = (x2)1/2, which is not smooth at x = 0]. For small excursions from equilibrium, the quadratic term is often the leading-order piece of more complex functions such as the Morse or Lennard-Jones potentials. Quadratic potentials correspond to the familiar Hooke’s Law of ideal springs V(x) = kx 2/2 => F(x) = -dV/dx = -(2/2)kx = -kx, where k is the spring constant. Objects subject to Hooke’s Law exhibit oscillatory motion, as can be seen by solving the differential equation arising from Newton’s 2nd law: F = ma => -kx = m(d 2x/dt 2) or d 2x /dt 2 + (k/m)x = 0. We solved this equation in PHYS 120: x(t) = A sin( ot + o) Other functional forms such as cosine can be changed into this form using a suitable choice of the phase angle o.
    [Show full text]
  • Determining the Load Inertia Contribution from Different Power Consumer Groups
    energies Article Determining the Load Inertia Contribution from Different Power Consumer Groups Henning Thiesen * and Clemens Jauch Wind Energy Technology Institute (WETI), Flensburg University of Applied Sciences, 24943 Flensburg, Germany; clemens.jauch@hs-flensburg.de * Correspondence: henning.thiesen@hs-flensburg.de Received: 27 February 2020; Accepted: 25 March 2020 ; Published: 1 April 2020 Abstract: Power system inertia is a vital part of power system stability. The inertia response within the first seconds after a power imbalance reduces the velocity of which the grid frequency changes. At present, large shares of power system inertia are provided by synchronously rotating masses of conventional power plants. A minor part of power system inertia is supplied by power consumers. The energy system transformation results in an overall decreasing amount of power system inertia. Hence, inertia has to be provided synthetically in future power systems. In depth knowledge about the amount of inertia provided by power consumers is very important for a future application of units supplying synthetic inertia. It strongly promotes the technical efficiency and cost effective application. A blackout in the city of Flensburg allows for a detailed research on the inertia contribution from power consumers. Therefore, power consumer categories are introduced and the inertia contribution is calculated for each category. Overall, the inertia constant for different power consumers is in the range of 0.09 to 4.24 s if inertia constant calculations are based on the power demand. If inertia constant calculations are based on the apparent generator power, the load inertia constant is in the range of 0.01 to 0.19 s.
    [Show full text]
  • Rotation: Moment of Inertia and Torque
    Rotation: Moment of Inertia and Torque Every time we push a door open or tighten a bolt using a wrench, we apply a force that results in a rotational motion about a fixed axis. Through experience we learn that where the force is applied and how the force is applied is just as important as how much force is applied when we want to make something rotate. This tutorial discusses the dynamics of an object rotating about a fixed axis and introduces the concepts of torque and moment of inertia. These concepts allows us to get a better understanding of why pushing a door towards its hinges is not very a very effective way to make it open, why using a longer wrench makes it easier to loosen a tight bolt, etc. This module begins by looking at the kinetic energy of rotation and by defining a quantity known as the moment of inertia which is the rotational analog of mass. Then it proceeds to discuss the quantity called torque which is the rotational analog of force and is the physical quantity that is required to changed an object's state of rotational motion. Moment of Inertia Kinetic Energy of Rotation Consider a rigid object rotating about a fixed axis at a certain angular velocity. Since every particle in the object is moving, every particle has kinetic energy. To find the total kinetic energy related to the rotation of the body, the sum of the kinetic energy of every particle due to the rotational motion is taken. The total kinetic energy can be expressed as ..
    [Show full text]
  • For POWER SPEED ATHLETES
    NUTRITIONAL CONSIDERATIONS & STRATEGIES for POWER SPEED ATHLETES Landon Evans, MS, RD, CSCS 2017 USTFCCCA NATIONAL CONFERENCE University of IOWA DISCLOSURE I have no financial relationship to the audience. 2017 USTFCCCA NATIONAL CONFERENCE 2 NUTRITION POWER SPEED ATHLETES Polarizing topic (to put it mildly) Perspective tuning OUTLINE Nutritional analysis Framework (the less debatable) Special considerations 2017 USTFCCCA NATIONAL NUTRITION POWER SPEED ATHLETES CONFERENCE Top 3 Emotionally Fueled Topics on Earth 1. Religion POLARIZING TOPIC 2. Politics 3. Nutrition https://hollandsopus.files.wordpress.com/2011/05/man_yelling_at_computer.jpg Bonus #4 (in my life with 2 young daughters): Glitter 2017 USTFCCCA NATIONAL NUTRITION POWER SPEED ATHLETES CONFERENCE Coach’s mortgage depends on their athletes’ successes. Coach gets frustrated with outcomes. Coach turns to judging/critiquing lifestyle POLARIZING You need to gain You need to 30lbs to compete in this lose 10lbs TOPIC conference How do you expect to recover You should when you’re doing eat less carbs [___]?! You should stop eating gluten 2017 USTFCCCA NATIONAL NUTRITION POWER SPEED ATHLETES CONFERENCE YOU NEED TO OK [________] Coach, but how? YOU POLARIZING NEED TO OK TOPIC [________] Coach, but last time I did that and I [____] 100 possible thoughts or statements 2017 USTFCCCA NATIONAL NUTRITION POWER SPEED ATHLETES CONFERENCE ANOTHER PFAFFISM Training is overrated Henk K, Dan P 2014 Seminar PERSPECTIVE TUNING 2017 USTFCCCA NATIONAL NUTRITION POWER SPEED ATHLETES CONFERENCE PERSPECTIVE TUNING 2017 USTFCCCA NATIONAL NUTRITION POWER SPEED ATHLETES CONFERENCE (some) Dietitians are great… But the most effective nutritionists are PERSPECTIVE the ones that can COACH it. TUNING So, in a large part, YOU (coaches) are a lot more effective than I will ever be for your group/team.
    [Show full text]
  • Rotational Motion and Angular Momentum 317
    CHAPTER 10 | ROTATIONAL MOTION AND ANGULAR MOMENTUM 317 10 ROTATIONAL MOTION AND ANGULAR MOMENTUM Figure 10.1 The mention of a tornado conjures up images of raw destructive power. Tornadoes blow houses away as if they were made of paper and have been known to pierce tree trunks with pieces of straw. They descend from clouds in funnel-like shapes that spin violently, particularly at the bottom where they are most narrow, producing winds as high as 500 km/h. (credit: Daphne Zaras, U.S. National Oceanic and Atmospheric Administration) Learning Objectives 10.1. Angular Acceleration • Describe uniform circular motion. • Explain non-uniform circular motion. • Calculate angular acceleration of an object. • Observe the link between linear and angular acceleration. 10.2. Kinematics of Rotational Motion • Observe the kinematics of rotational motion. • Derive rotational kinematic equations. • Evaluate problem solving strategies for rotational kinematics. 10.3. Dynamics of Rotational Motion: Rotational Inertia • Understand the relationship between force, mass and acceleration. • Study the turning effect of force. • Study the analogy between force and torque, mass and moment of inertia, and linear acceleration and angular acceleration. 10.4. Rotational Kinetic Energy: Work and Energy Revisited • Derive the equation for rotational work. • Calculate rotational kinetic energy. • Demonstrate the Law of Conservation of Energy. 10.5. Angular Momentum and Its Conservation • Understand the analogy between angular momentum and linear momentum. • Observe the relationship between torque and angular momentum. • Apply the law of conservation of angular momentum. 10.6. Collisions of Extended Bodies in Two Dimensions • Observe collisions of extended bodies in two dimensions. • Examine collision at the point of percussion.
    [Show full text]
  • Work, Power, & Energy
    WORK, POWER, & ENERGY In physics, work is done when a force acting on an object causes it to move a distance. There are several good examples of work which can be observed everyday - a person pushing a grocery cart down the aisle of a grocery store, a student lifting a backpack full of books, a baseball player throwing a ball. In each case a force is exerted on an object that caused it to move a distance. Work (Joules) = force (N) x distance (m) or W = f d The metric unit of work is one Newton-meter ( 1 N-m ). This combination of units is given the name JOULE in honor of James Prescott Joule (1818-1889), who performed the first direct measurement of the mechanical equivalent of heat energy. The unit of heat energy, CALORIE, is equivalent to 4.18 joules, or 1 calorie = 4.18 joules Work has nothing to do with the amount of time that this force acts to cause movement. Sometimes, the work is done very quickly and other times the work is done rather slowly. The quantity which has to do with the rate at which a certain amount of work is done is known as the power. The metric unit of power is the WATT. As is implied by the equation for power, a unit of power is equivalent to a unit of work divided by a unit of time. Thus, a watt is equivalent to a joule/second. For historical reasons, the horsepower is occasionally used to describe the power delivered by a machine.
    [Show full text]
  • In-Class Problems 23-24: Harmonic Oscillation and Mechanical Energy: Solution
    MASSACHUSETTS INSTITUTE OF TECHNOLOGY Department of Physics Physics 8.01 TEAL Fall Term 2004 In-Class Problems 23-24: Harmonic Oscillation and Mechanical Energy: Solution Problem 22: Journey to the Center of the Earth Imagine that one drilled a hole with smooth sides straight through the center of the earth. If the air is removed from this tube (and it doesn’t fill up with water, liquid rock, or iron from the core) an object dropped into one end will have enough energy to just exit the other end after an interval of time. Your goal is to find that interval of time. a) The gravitational force on an object of mass m, located inside the earth a distance r < Re, from the center (Re is the radius of the earth), is due only to the mass of the earth that lies within a solid sphere of radius r. What is the gravitational force as a function of the distance r from the center? Express your answer in terms of g and Re . Note: you do not need the mass of the earth to answer this question. You only need to assume that the earth is of uniform density. Answer: Choose a radial coordinate with unit vector rˆ pointing outwards. The gravitational force on an object of mass m at the surface of the earth is given by two expressions Gmm v e ˆ ˆ Fgrav =− 2 r =−mgr . Re Therefore we can solve for the gravitational constant acceleration 1 Gme g = 2 . Re When the object is a distance r from the center of the earth, the mass of the earth that lies outside the sphere of radius r does not contribute to the gravitational force.
    [Show full text]