Novel Food Processing Technologies

Total Page:16

File Type:pdf, Size:1020Kb

Novel Food Processing Technologies 23 Advances in Ohmic Heating and Moderate Electric Field (MEF) Processing Sudhir K. Sastry The Ohio State University, Columbus, Ohio, U.S.A. I. INTRODUCTION The technology of heating materials by passing a current through them has been variously termed Ohmic or Joule heating, in honor of Georg Ohm (who elucidated the Ohm’s law) and James Prescott Joule (who showed that passage of electricity resulted in heating effects).In the latter part of the 19th century, a number of inventions were developed for the heating of flowable materials.The technology saw periodic revival with industrial applications, for example, in milk pasteurization in the 1930s, before being discontinued. In the 1980s, the technology was again revived, and it has achieved some industrial applications that include the pasteurization of liquid eggs and processing of fruit products. New developments in various areas have improved the prospects for future use of this technology.Developments in power supply technology in the past 5 years have shown promise in significantly decreasing costs.The control of electrolytic effects has been greatly advanced by recent developments.Further, the emergence of new manufacturers of low-cost ohmic heaters on the market suggests that the technology is undergoing improvement and refinement.Moreover, research on ohmic heating has identified new applications in the area of moderate electric field (MEF) processing. The basic principle of ohmic heating is the dissipation of electrical energy into heat, which is proportional to the square of the electric field strength and electrical conductivity (Sastry and Palaniappan, 1992a; Sastry and Li, 1996). uÁ ¼ AjVA2r ð1Þ where the electrical conductivity U is a function of temperature, the material, and the method of heating.For cellular materials, electrical conductivity undergoes a sharp increase in the temperature range of 70jC because of the breakdown of cell wall constituents.When an electric field is applied, cell wall breakdown occurs at lower temperatures, and the increase of electrical conductivity occurs over a wider range of temperatures (Palaniappan and Sastry, 1991a; Fig.1). 491 Copyright © 2005 by Marcel Dekker. 492 Sastry Figure 1 Electrical conductivity of carrot subjected to various electric field strengths.(From Palaniappan and Sastry, 1991a.) Above a certain electric field strength, or when the material has been previously thermally treated (Wang and Sastry, 1997a), the electrical conductivity–temperature curve often becomes linear. Because electrical conductivity increases with temperature, ohmic heating becomes more effective at higher temperatures.The electrical conductivity of liquid foods tends to follow a linear trend, regardless of the mode of heating.Because no cellular structure exists, the properties remain the same (Palaniappan and Sastry, 1991b; Fig. 2). Because the rate of heating may be affected by varying the electric field strength or the product’s electrical conductivity, the technology provides opportunities for creativity on the part of the process engineer or product developer.It is possible to design heaters for materials of relatively low electrical conductivity if the electric field strength is made sufficiently large.It is also possible to heat materials at extremely rapid rates.Further, for Figure 2 Electrical conductivity of orange juice subjected to various electric field strengths.The decrease at high temperatures is due to evaporation and boiling within an unpressurized heater. (From Palaniappan and Sastry, 1991b.) Copyright © 2005 by Marcel Dekker. Advances in Ohmic Heating and MEF Processing 493 materials with uniform electrical conductivity, the energy generation is far more uniform than in microwave heating.These basic principles have been addressed by Palaniappan and Sastry (1991a), de Alwis and Fryer (1990), Halden et al.(1990), and Sastry (1992), among others. II. MICROBIAL DEATH KINETICS The question of whether a nonthermal contribution to microbial lethality exists has been addressed in a number of studies in the literature. Early literature was inconclusive (Palaniappan et al., 1990), because most studies either did not specify sample temperatures or failed to eliminate it as a variable.It is essential that studies comparing conventional and ohmic heating be conducted under temperature histories that are as close as possible.Palaniappan et al.(1992) found no difference between ohmic and conventional heat treatments on the death kinetics of yeast cells (Zygosaccha- romyces bailii) under identical thermal histories.They found, however, that a mild electrical pretreatment of Escherichia coli decreased the subsequent inactivation requirement in certain cases. Recent studies suggest that mild electroporation might occur even under the relatively low field strengths encountered during ohmic heating.The presence of pore-forming mechanisms in cellular tissue has been confirmed by recent work (Imai et al., 1995; Wang, 1995; Kulshrestha and Sastry, 1999).Another recent study (Cho et al.,1999), which was conducted under near-identical temperature conditions, indicates that the inactivation Table 1 Decimal Reduction Times (D Values) and Kinetic Reaction Rate Constants (k) for B. subtilis Spores Under Conventional and Ohmic Heating D values for k for D values for conventional conventional ohmic heating k for ohmic Temperature (jC) heating (minÀ1) heating (secÀ1) (minÀ1) heating (secÀ1) 88 32.8 0.00117 30.2 0.001271 90 (stage 1 of 17.1 0.002245 14.2 0.002703 two-stage heating) (stage 2 of 9.2 0.004172 8.5 0.004516 two-stage heating) 92.3 9.87 0.003889 8.55 0.004489 95 5.06 0.007586 95.5 4.38 0.008763 97 3.05 0.012585 99.1 1.76 0.021809 Z value (C) 8.74a 70.0b 9.16a 67.5b or activation energy (Ea) (kcal/mol) a Z value. b Activation energy. Source: Cho et al.(1999). Copyright © 2005 by Marcel Dekker. 494 Sastry Table 2 Reaction Rate Constants (k) for Z. bailii Under Conventional and Ohmic Heating D values for D values for conventional k for conventional ohmic heating k for ohmic Temperature (jC) heating (minÀ1) heating (secÀ1) (minÀ1) heating (secÀ1) 49.8 294.6 0.008 274.0 0.009 52.3 149.7 0.016 113.0 0.021 55.8 47.21 0.049 43.11 0.054 58.8 16.88 0.137 17.84 0.130 Z values (C) or 7.19a 29.63b 7.68a 27.77b activation energy (Ea) (kcal/mol) a Z value. b Activation energy. Source: Palaniappan et al.(1992). kinetics of Bacillus subtilis spores can be accelerated by ohmic treatment.A two-stage ohmic treatment (ohmic treatment followed by a holding time, before second heat treatment) accelerated the death rates further.Lee and Yoon (1999) have indicated that leakage of intracellular constituents of Saccharomyces cerevisiae was found to be enhanced under ohmic heating, as compared to conventional heating in boiling water. The additional effect of ohmic treatment may be because of the low frequency used (50–60 Hz), which allows cell walls to build up charges and form pores.This effect is less apparent in high-frequency methods such as radiofrequency or microwave heating.In such cases, the electric field is reversed before sufficient charge buildup occurs, so the cell membrane does not break down because of electrical effects (Tables 1 and 2). III. ELECTROLYTIC EFFECTS It is necessary to consider any electrolytic reactions that may occur at the electrode–solution interface.When direct current is used, different reactions occur at the cathode and anode; under alternating currents, however, the cathode and anode are periodically reversed, and both cathodic and anodic products may occur at either electrode.Electrolytic processes can be prevented if the potential drop at the electrode–solution interface can be kept below the critical electrode potential for the system.This implies that either the frequency is sufficiently increased, or the electrode capacitance is increased for such minimization to occur.A detailed analysis of these phenomena has been presented by Amatore et al.(1998) and Bazhal et al.(1983a).An important consideration in developing ohmic technology is the need to address such issues economically. IV. OHMIC AND MODERATE ELECTRIC FIELD (MEF) PROCESSING APPLICATIONS While a wealth of potential applications exist for ohmic heating, most are still awaiting commercial exploitation.These include sterilization, pasteurization, processing of fouling- Copyright © 2005 by Marcel Dekker. Advances in Ohmic Heating and MEF Processing 495 sensitive material, blanching, thawing, on-line detection of starch gelatinization, and ohmic heating as a pretreatment for drying and extraction.Additionally, the presence of an electric field has various interesting effects on bacterial cells.The effects of the electric field are worthy of note with or without any attendant heating effects.Thus we may loosely define the area of moderate electric field processing as processes conducted using an electric field in the range from about 1–1000 V/cm, or arbitrary waveform, and with or without ohmic heating effects.Processes in this category have shown many significant results. A. Sterilization Uniform heating has resulted in great expectations for sterilization technology for partic- ulate foods.Typical systems for this purpose involve a material flowing through a suitably designed set of electrodes.One common commercial embodiment is the APV ohmic heater, where the field is aligned with the flow (Fig.3a).A coaxial design is shown in Fig.3b. Commercial sterilization requires that all parts of the flowing material be exposed to a sufficient temperature for a time adequate to destroy pathogenic spore-formers.When the
Recommended publications
  • Laboratory Manual Physics 166, 167, 168, 169
    Laboratory Manual Physics 166, 167, 168, 169 Lab manual, part 2 For PHY 167 and 169 students Department of Physics and Astronomy HERBERT LEHMAN COLLEGE Spring 2018 TABLE OF CONTENTS Writing a laboratory report ............................................................................................................................... 1 Introduction: Measurement and uncertainty ................................................................................................. 3 Introduction: Units and conversions ............................................................................................................ 11 Experiment 1: Density .................................................................................................................................... 12 Experiment 2: Acceleration of a Freely Falling Object .............................................................................. 17 Experiment 3: Static Equilibrium .................................................................................................................. 22 Experiment 4: Newton’s Second Law .......................................................................................................... 27 Experiment 5: Conservation Laws in Collisions ......................................................................................... 33 Experiment 6: The Ballistic Pendulum ......................................................................................................... 41 Experiment 7: Rotational Equilibrium ........................................................................................................
    [Show full text]
  • GEORG OHM - Ω Physicist and Mathematician
    GEORG OHM - Ω Physicist and Mathematician The start Georg Simon Ohm was born on 16th of March 1789 in Erlangen in Germany and died on 6th of July 1854 in Munich, Germany. He was born into a Protestant family and was the son of Johann Wolfgang Ohm and Maria Elizabeth Beck. The family had seven children, but only three survived: Georg, his younger brother Martin and his sister Elizabeth Barbara. His mother died when Georg was only 10 years old. Education Georg and Martin were taught by their father who brought them to a high standard in mathematics, physics, chemistry and philosophy. Georg Simon attended Erlangen Gymnasium from age eleven to fifteen where he hardly received any scientific education. After the Gymnasium, he was sent to Switzerland as his father was concerned that his son was wasting his educational opportunity. In September 1806 Ohm accepted a position as a mathematics teacher in a school in Gottstadt. Ohm restarted his mathematical studies, left his teaching post in March 1809 and became a private tutor in Neuchâtel. For two years he carried out his duties as a tutor while he followed private studies of mathematics. Then in April 1811 he returned to the University of Erlangen. Teaching Ohm received his doctorate from the University of Erlangen on October 25, 1811. He immediately joined the faculty there as a lecturer in mathematics but left after three semesters because of unpromising prospects. He could not survive on his salary as a lecturer. He had a few more teaching jobs after that and unhappy with his job, Georg began writing an elementary textbook on geometry as a way to prove his abilities.
    [Show full text]
  • Student Pages Part B 3C P2
    Fat: Who Says? Measuring Obesity by Bioelectrical Impedance Analysis Circuitous Adventures-Measuring Electrical Values Student Information Page 3C Part B Activity Introduction: Surge ahead and learn how to use a multimeter device to measure voltage, amps, and resistance. Resistance is futile! Activity Background: Whenever charged particles are taken from one object and given to another object, an imbalance of charge occurs. This imbalance of charge is called voltage (or potential difference). Voltage is measured in units called Volts (V), named after Alessandro Volta. An electric current is nothing more than the flow of electric charges from one location to another. The measure of how much flow is occurring at any given point is called the amperage and is measured in units called amps (A), named after André-Marie Ampère. Electric charges can only flow through certain materials, called conductors. Materials that resist the flow of current are called insulators. Materials offer resistance to the flow of current. This resistance is measured in units called ohms (Ω), named after its discovered Georg Ohm. Ohm’s law states that the amount of current (I) flowing through a conductor times the resistance (R) of the conductor is equal to voltage (V) of the source of power (i.e. batteries). This law is often expressed in the following form: V = I X R Note: V = voltage, I = current, and R = resistance Activity Materials: • 2 batteries • 1 battery holder • Several electrical wires (stripped) or with alligator clips • 1 buzzer • 1 switch • 1 Analog multimeter • 1 Copy Student Information Page • 1 Copy Student Data Page • Transparency of Figure 3 Part B LESSON 3 ® Positively Aging /M.O.R.E.
    [Show full text]
  • Energy Pioneers
    Providing energy education to students in the communities we serve. That’s our Promise to Michigan. Energy Pioneers The following pages will give an overview about famous people in history who studied energy and invented useful things we still use today. Read about these people then complete the matching activity on the last page. For more great energy resources visit: www.ConsumersEnergy.com/kids © 2015 Consumers Energy. All rights reserved. Providing energy education to students in the communities we serve. That’s our Promise to Michigan. Thomas Edison (1847) Information comes from the Department of Energy, including sourced pictures. Source: Wikimedia Commons (Public Domain) Born in 1847. Not a very good student. Created many inventions including the phonograph (similar to a record player), the light bulb, the first power plant and the first movie camera. One of his most famous quotes is, “Invention is one percent inspiration and ninety-nine percent perspiration.” For more great energy resources visit: www.ConsumersEnergy.com/kids © 2015 Consumers Energy. All rights reserved. Providing energy education to students in the communities we serve. That’s our Promise to Michigan. Marie Curie (1867) Information comes from the Department of Energy, including sourced pictures. Source: Nobel Foundation, Wikimedia Commons (Public Domain) Born in 1867. Learned to read at 4. There were no universities in her native Poland that accepted women, so she had to move to France to attend college. She, along with her husband, discovered the first radioactive element. In 1903, she was awarded the Nobel Prize in Physics for the discovery of radium. Marie Curie was the first woman to win a Nobel Prize in Physics.
    [Show full text]
  • Electrical Basics
    Electrical Basics Power & Ohm’s Law Group 1 • Work together to understand the informaon in your secon. • You will have 10 minutes to review the material and present it to the class. • With some applied force, electrons will move from a negatively charged atom to a positively charged atom. This flow of electrons between atoms is called current. • Current is represented by the symbol I 3 • When there is a lack of electrons at one end of a conductor and an abundance at the other end, current will flow through the conductor. This difference in “pressure” is referred to as voltage. • This “pressure” is sometimes referred to as “electromotive force” or EMF. • Voltage is represented by the symbol E 4 • Resistance is the opposition to the flow of electrons (aka “current”). • Every material offers some resistance. • Conductors offer very low resistance. • Insulators offer high resistance. • Resistance is represented by the Symbol R • Resistance is measured in Ohms Ω 5 • Current is measured by literally counting the number of electrons that pass a given point. • Current will be the same at any point of a wire. • The basic unit for counting electrons is the "coulomb“. (French physicist Charles Augustin de Coulomb in 1780’s) 6 • 1 coulomb = 6.24 x 1018 electrons = 6,240,000,000,000,000,000 = more than 6 billion billion electrons! If 1 coulomb of electrons go by each second, then we say that the current is 1 "ampere" or 1 amp (Named after André-Marie Ampère, 1826) 7 • Voltage is measured in volts. • A voltage of 1 volt means that 1 "Joule" of energy is being delivered for each coulomb of charge that flows through the circuit.
    [Show full text]
  • Electric Currents on the Body Current in Amperes Effect 0.001 Can Be Felt 0.005 Painful 0.010 Involuntary Muscle Contractions 0.015 Loss of Muscle Control
    Chapter 20 - Electric Circuits Physics Electric Current • Electric current is simply the flow of electric charges • Charge flows when there is an electric potential difference, or difference in potential (voltage), between the ends of a conductor. (Think of water pipes. Water can only flow if there a difference in gravitational potential energy between two points) • The flow of charge will continue until both ends reach a common electric potential. When there is no potential difference, there is no longer a flow of charge through the conductor • The unit of electric current is called the ampere (A) – named after André-Marie Ampère (1775–1836), French mathematician and physicist flow of charge - When the rate of flow of charge past any cross section of wire cross section is 1coulomb per second, the current is 1 ampere ( ) => Electric current(I) = rate of charge flow = ( ) amount of charge q I = [A]change in time t 풒 휟풕 Q1) A wire carries a current of 2.0A. How much charge passes by a point in 55 seconds? a) 110C b) 100C c) 90C d) 80C Q2) 175C of charge pass a point in a wire in 35s. What is the current in the wire? a) 1A b) 3A c) 5A d) 8A Q3) How much charge, in coulombs, passes through a cross section of a particular wire every second if the current in the wire is 3A? How many electrons would this charge be equivalent to? (q= ne, 1e = 1.6×10-19C) a) 5C, 3.2×1019e-/s b) 3C, 1.9×1019e-/s c) 5C, 1.9×1019e-/s d) 3C, 3.2×1019e-/s 1 Voltage Sources and Resistance i) Voltage Sources • Charges do not flow unless there is a potential difference(=Voltage) • A battery is one example of a voltage source.
    [Show full text]
  • The Short History of Science
    PHYSICS FOUNDATIONS SOCIETY THE FINNISH SOCIETY FOR NATURAL PHILOSOPHY PHYSICS FOUNDATIONS SOCIETY THE FINNISH SOCIETY FOR www.physicsfoundations.org NATURAL PHILOSOPHY www.lfs.fi Dr. Suntola’s “The Short History of Science” shows fascinating competence in its constructively critical in-depth exploration of the long path that the pioneers of metaphysics and empirical science have followed in building up our present understanding of physical reality. The book is made unique by the author’s perspective. He reflects the historical path to his Dynamic Universe theory that opens an unparalleled perspective to a deeper understanding of the harmony in nature – to click the pieces of the puzzle into their places. The book opens a unique possibility for the reader to make his own evaluation of the postulates behind our present understanding of reality. – Tarja Kallio-Tamminen, PhD, theoretical philosophy, MSc, high energy physics The book gives an exceptionally interesting perspective on the history of science and the development paths that have led to our scientific picture of physical reality. As a philosophical question, the reader may conclude how much the development has been directed by coincidences, and whether the picture of reality would have been different if another path had been chosen. – Heikki Sipilä, PhD, nuclear physics Would other routes have been chosen, if all modern experiments had been available to the early scientists? This is an excellent book for a guided scientific tour challenging the reader to an in-depth consideration of the choices made. – Ari Lehto, PhD, physics Tuomo Suntola, PhD in Electron Physics at Helsinki University of Technology (1971).
    [Show full text]
  • I. Electricity and Magnetism 2______3
    Electricity and Magnetism 2 By Henri RASOLONDRAMANITRA African Virtual university Université Virtuelle Africaine Universidade Virtual Africana African Virtual University NOTICE This document is published under the conditions of the Creative Commons http://en.wikipedia.org/wiki/Creative_Commons Attribution http://creativecommons.org/licenses/by/2.5/ License (abbreviated “cc-by”), Version 2.5. African Virtual University Table of conTenTs I. Electricity and Magnetism 2 __________________________________ 3 II. Prerequisite Course or knowledge _____________________________ 3 III. Time ____________________________________________________ 3 IV. Material __________________________________________________ 3 V. Module Rationale __________________________________________ 4 VI. Content __________________________________________________ 4 6.1 Overview ______________________________________________ 4 6.2 Outline________________________________________________ 5 6.3 Graphic Organizer _______________________________________ 5 VII. General Objective(s) ________________________________________ 6 VIII. Specific Learning Objectives __________________________________ 7 IX. Teaching and Learning Activities _______________________________ 9 X. Learning Activities _________________________________________ 20 XI. Key Concepts (Glossary) ___________________________________ 161 XII. Compulsory Readings _____________________________________ 164 XIII. Useful Links ____________________________________________ 167 XIV. Synthesis of the Module ___________________________________
    [Show full text]
  • A Guide to Low Resistance Measurement Contents
    Tried. Tested. Trusted. A Guide to Low Resistance Measurement Contents 02-03 Introduction 04-05 Applications 06 Resistance 06-09 Principles of Resistance Measurement 09-10 Methods of 4 Terminal Connections 10-19 Possible Measurement Errors 14-18 Choosing the Right Instrument 18-24 Application Examples 25-33 Useful Formulas and Charts 34 Find out more Tried. Tested. Trusted. With resistance measurement, precision is everything. This guide is what we know about achieving the highest quality measurements possible. The measurement of very large or very small cable characteristics, temperature coefficients quantities is always difficult, and resistance and various formulas to ensure you make the best measurement is no exception. Values above 1G possible choice when selecting your measuring Ω and values below 1 both present measurement instrument and measurement technique. Ω problems. We hope you will find this booklet a valuable Cropico is a world leader in low resistance addition to your toolkit. measurement; we produce a comprehensive range of low resistance ohmmeters and accessories which cover most measurement applications. This handbook gives an overview of low resistance measurement techniques, explains common causes of errors and how to avoid them. We have also included useful tables of wire and 2 Tried. Tested. Trusted. 3 Applications There are many reasons why the resistance of material is measured. Here are a few. Manufacturers of components thus avoiding the joint or contact from Resistors, inductors and chokes all have to becoming excessively hot, a poor cable joint or verify that their product meets the specified switch contact will soon fail due to this heating resistance tolerance, end of production line and effect.
    [Show full text]
  • Electrical Circuits
    Electrical Circuits This guide covers the following: ● What is a circuit? ● Circuit Symbols ● Series and Parallel Circuits ● Electrical Charge ● Voltage ● Current ● Current and Voltage in Series and Parallel circuits ● Resistance ● Ohm’s Law ● Electrical Power What is a Circuit? To power an electrical device we need a few things. 1. Power source (cell/battery/wall socket etc.) 2. An electrical circuit for the electricity to travel round. We know that electricity is the flow of electrons. If the electrons cannot move there is now electricity. For electrons to move much like a scalextric car they need a track or wire to move along. What is a Circuit? Electrical Circuits are the “tracks” that the electrons travel round. This “track” must start AND end with the power source. Spread around the “track” are the devices you want to power such as bulbs and motors etc. Circuit Symbols It can be difficult to draw a circuit that is easy to follow. Because of this a system has been developed to simplify the drawing of circuits. These are called Circuit Diagrams. Circuit Diagrams are easy to read and easy to draw! Circuit Diagrams replace components in the circuit with Circuit Symbols. Circuit Symbols Circuit Symbols Below are the most common circuit symbols. Types of Circuit Electrical Circuits come in three forms: 1. Series Circuits 2. Parallel Circuits 3. A combination of Series and Parallel Circuits These relate to how the components in the circuit are arranged. Series Circuits In Series Circuits the components are joined together in a chain. Like a daisy chain! Parallel Circuits In Parallel Circuits the components are joined so that each component has its own loop back to the battery.
    [Show full text]
  • What Is Ohm's Law?
    What is Ohm’s Law? Ohm’s Law is a formula used to calculate the relationship between voltage, current and resistance in an electrical circuit. To students of electronics, Ohm’s Law (E = IR) is as fundamentally important as Einstein’s Relativity equation (E = mc2) is to physicists. E = I x R When spelled out, it means voltage = current x resistance, or volts = amps x ohms, or V = A x Ω. Named for German physicist Georg Ohm (1789-1854), Ohm’s Law addresses the key quantities at work in circuits: Quantity Ohm’s Law Unit of measure Role in circuits In case you’re wondering: symbol (abbreviation) Voltage E Volt (V) Pressure that triggers E = electromotive force (old- electron flow school term) Current I Ampere, amp (A) Rate of electron flow I = intensity Resistance R Ohm (Ω) Flow inhibitor Ω = Greek letter omega If two of these values are known, technicians can reconfigure Ohm’s Law to calculate the third. Just modify the pyramid as follows: If you know voltage (E) and current (I) and want to know resistance (R), X-out the R in the pyramid and calculate the remaining equation (see the first, or far left, pyramid above). Note: Resistance cannot be measured in an operating circuit, so Ohm’s Law is especially useful when it needs to be calculated. Rather than shutting off the circuit to measure resistance, a technician can determine R using the above variation of Ohm’s Law. Now, if you know voltage (E) and resistance (R) and want to know current (I), X-out the I and calculate the remaining two symbols (see the middle pyramid above).
    [Show full text]
  • Electricity Is a Type of Energy That Can Build up in One Place Or Flow from One Place to Another
    Electricity is a type of energy that can build up in one place or flow from one place to another. A science that deals with the phenomena and laws of electricity Keen contagious excitement! Knowledge of electric eels dates back to 2750 BC. A Greek philosopher named Thales of Miletus made some observations about static electricity around 600 BC. Static electricity was generated by rubbing amber against fur in experiments and magic tricks. The word “Electricus” was first used in 1600, by an English scientist named William Gilbert. He took the word from the Greek word for amber: ήλεκτρον [elektron]. The word “Electricity” was first printed in 1646. 1752: Benjamin Franklin supposedly did the famous Key in a lightning storm experiment. We know for sure he did a lot of research. 1792: Luigi Galvani demonstrated that animals’ bodies run on electricity. 1800: Alessandro Volta's invented an early type of battery. 1820: Hans Christian Ørsted and André-Marie Ampère researched how magnets and electricity work together. 1821: Michael Faraday invented the electric motor. 1827: Georg Ohm mathematically analyzed the electrical circuit. Mid 1800’s and beyond: Nikola Tesla, Thomas Edison, George Westinghouse, Ernst Werner von Siemens, Alexander Graham Bell, Lord Kelvin, and others, all did very influential work in electricity. We have to look really close – at ATOMS! They have protons, neutrons, and electrons. Protons are POSITIVELY charged. Electrons are NEGATIVELY charged. Neutrons are NEUTRAL. When an electron gets removed from an atom, it’s still an atom of the same element, but the CHARGE is different! All atoms want to be neutral – they want to get that electron back! Opposites attract, so a positively charged atom will attract a negatively charged one.
    [Show full text]