Voltage Doubler Circuit with 555 Timer
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History and Progress of Fractional–Order Element
296 A. KARTCI, N. HERENCSAR, J. T. MACHADO, L. BRANCIK, HISTORY AND PROGRESS OF FRACTIONAL–ORDER ELEMENT . History and Progress of Fractional–Order Element Passive Emulators: A Review Aslihan KARTCI 1;2, Norbert HERENCSAR 1, Jose Tenreiro MACHADO 3, Lubomir BRANCIK 4 1 Dept. of Telecommunications, Brno University of Technology, Technicka 3082/12, 616 00 Brno, Czech Republic 2 Computer, Electrical and Mathematical Sciences and Engineering Division, King Abdullah University of Science and Technology, Thuwal 23955-6900, Saudi Arabia 3 Institute of Engineering, Polytechnic of Porto, Dept. of Electrical Engineering, Porto, Portugal 4 Dept. of Radio Electronics, Brno University of Technology, Technicka 3082/12, 616 00 Brno, Czech Republic {kartci, herencsn, brancik}@feec.vutbr.cz, [email protected] Submitted April 5, 2020 / Accepted April 19, 2020 Abstract. This paper presents a state-of-the-art survey where Iαv¹tº denotes the "fractional-order time integral" [3] in the area of fractional-order element passive emulators with an order 0 < α < 1. Figure 1 shows these funda- adopted in circuits and systems. An overview of the different mental components in the frequency domain and possible approximations used to estimate the passive element values fractional-order elements (FOEs) in the four quadrants of by means of rational functions is also discussed. A short com- the complex plane [4]. Their impedance is described as parison table highlights the significance of recent methodolo- Z¹sº = Ksα, where ! is the angular frequency with s = j! gies and their potential for further research. Moreover, the and the phase is given in radians (φ = απ/2) or in degrees pros and cons in emulation of FOEs are analyzed. -
Basic Electrical Engineering
BASIC ELECTRICAL ENGINEERING V.HimaBindu V.V.S Madhuri Chandrashekar.D GOKARAJU RANGARAJU INSTITUTE OF ENGINEERING AND TECHNOLOGY (Autonomous) Index: 1. Syllabus……………………………………………….……….. .1 2. Ohm’s Law………………………………………….…………..3 3. KVL,KCL…………………………………………….……….. .4 4. Nodes,Branches& Loops…………………….……….………. 5 5. Series elements & Voltage Division………..………….……….6 6. Parallel elements & Current Division……………….………...7 7. Star-Delta transformation…………………………….………..8 8. Independent Sources …………………………………..……….9 9. Dependent sources……………………………………………12 10. Source Transformation:…………………………………….…13 11. Review of Complex Number…………………………………..16 12. Phasor Representation:………………….…………………….19 13. Phasor Relationship with a pure resistance……………..……23 14. Phasor Relationship with a pure inductance………………....24 15. Phasor Relationship with a pure capacitance………..……….25 16. Series and Parallel combinations of Inductors………….……30 17. Series and parallel connection of capacitors……………...…..32 18. Mesh Analysis…………………………………………………..34 19. Nodal Analysis……………………………………………….…37 20. Average, RMS values……………….……………………….....43 21. R-L Series Circuit……………………………………………...47 22. R-C Series circuit……………………………………………....50 23. R-L-C Series circuit…………………………………………....53 24. Real, reactive & Apparent Power…………………………….56 25. Power triangle……………………………………………….....61 26. Series Resonance……………………………………………….66 27. Parallel Resonance……………………………………………..69 28. Thevenin’s Theorem…………………………………………...72 29. Norton’s Theorem……………………………………………...75 30. Superposition Theorem………………………………………..79 31. -
The Essential Component of a Toaster Is an Electrical Element (A Resistor) That Converts Electrical Energy to Heat Energy
Electric Circuits I Circuit Elements Dr. Firas Obeidat 1 Independent Voltage Sources An independent voltage source is characterized by a terminal voltage which is completely independent of the current through it or other circuit elements. The independent voltage source is an ideal source and does not represent exactly any real physical device, because the ideal source could theoretically deliver an infinite amount of energy from its terminals. Physical sources such as batteries and generators may be regarded as approximations to ideal voltage sources. 2 Dr. Firas Obeidat – Philadelphia University Independent Current Sources Independent current source is characterized by a current which is completely independent of the voltage across it or other circuit elements. The independent current source is at best a reasonable approximation for a physical element. In theory it can deliver infinite power from its terminals because it produces the same finite current for any voltage across it, no matter how large that voltage may be. It is, however, a good approximation for many practical sources, particularly in electronic circuits. 3 Dr. Firas Obeidat – Philadelphia University Dependent Voltage & Current Sources Dependent, or controlled, source, in which the source quantity is determined by a voltage or current existing at some other location in the system being analyzed. (a) current-controlled current source; (b) voltage-controlled current source; (c) voltage-controlled voltage source; (d) current-controlled voltage source. Sources such as these appear in the equivalent electrical models for many electronic devices, such as transistors, operational amplifiers, and integrated circuits. Dependent and independent voltage and current sources are active elements; they are capable of delivering power to some external device. -
Mcnearney, Eugene Master's Thesis
Analysis of Droplet-target interactions in electrostatically charged spraying systems A thesis submitted in partial fulfilment of the requirements for the degree of Master of Engineering, in Electrical and Electronic Engineering at the university of Canterbury by E. J. McNearney, B.E. Hons University of Canterbury, Christchurch, New Zealand December 2020. Abstract Increasing demands for food production and other agricultural products push demands for improved crop yields. Chemical pest management in the form of pesticides is a widely used method of increasing crop yields, over 90% of which is applied as liquid sprays. Poor application efficacy of these pesticides onto the target plant introduce concerns for both the environment and human health for those that come into contact. Traditional spraying techniques result in up to 70% off target losses, with less than 1% of the active chemical reaching the target pest. These losses are highly configuration dependent needing to be selected for the target plant and environmental conditions. One method to improve spray efficacy, electrostatically charging the liquid spray, has been previously introduced to market. This thesis has investigated factors influencing the liquid spray deposition onto the target, looking into plant impedances and using computer vision to quantify depositions with the ESS electrostatic nozzle. A high voltage power supply has also been developed to allow control of nozzle voltage. Leaf to ground impedances of potted grapevines were investigated as well as potential sources for the found values. It was found that the frequency and impedance relationship appears to follow dispersions found in other living tissues. It was also found that physical junctions in the plant where plant fibres intersect provided the largest impedance contributions with apparent linear regions in between. -
Numerical Modeling of a Lumped Acoustic Source Actuated by A
NUMERICAL MODELING OF A LUMPED ACOUSTIC SOURCE ACTUATED BY A PIEZOELECTRIC STACK DEVICE THAT IS DRIVEN BY A SWITCHING AMPLIFIER Farnaz Tajdari University of Twente, Faculty of Engineering Technology, Enschede, The Netherlands email: [email protected] Arthur P. Berkhoff TNO Technical Sciences, Acoustics and Sonar, Den Haag, The Netherlands André de Boer University of Twente, Faculty of Engineering Technology, Enschede, The Netherlands This paper studies an acoustic source with a relatively small thickness and high bending stiff- ness. Piezoelectric actuators are used to drive the moving component of the acoustic source. In the current study, a lumped model is used to represent the acoustic source that is excited by a piezoelectric stacked actuator. The equivalent electrical circuit of the lumped acoustic source can directly be connected to the electrical circuit of a switching amplifier. Various methods are used to estimate the radiation impedance of the acoustic source. The effectiveness of these methods is investigated when they are used in combination with the equivalent electrical circuit of the lumped acoustic source, the actuator and the amplifier. Finally, result of a numerical finite element simu- lation is compared with the results of the fully-lumped equivalent electrical circuit. Keywords: thin acoustic source, radiation impedance 1. Introduction Thin acoustic sources operating at low frequencies can have specific applications. For instance, they can be used as sources with severe space constraints, in active sound absorption or active noise control. A thin acoustic source is introduced in Ref. [1] and is implemented in Ref. [2]. In this acous- tic source, a high bending stiffness is obtained by attaching the source to a sandwich structure. -
Unit-I Electrical Circuits Introduction
Unit-I Electrical Circuits Introduction 1. Electric charge(Q) In all atoms there exists number of electrons which are very loosely bounded to its nucleus. Such electrons are free to wander when specific forces are applied. If any of these electrons is removed, the atom becomes positively charged. And if excess electrons are added to the atom it becomes positively charged. The total deficiency or addition of electrons in an atom is called its charge. A charged atom is called Ion. An element containing a number of ionized atoms is said to be charged. And accordingly the element consisting of that atom is said to be positively or negatively charged. Particle Electric charge possessed by Atomic charge particle of one number (C) Protons +1.6022X 10-19 +1 Neutrons 0 0 Electrons 1.6022X 10-19 -1 The unit of measurement of charge is Coulomb (C). It can be defined as the charge possessed by number of electrons. Hence if an element has a positive charge of one coulomb then that element has a deficiency of number of electrons. Conductors: The atoms of different materials differ in the number of electrons, protons and neutrons, which they contain. They also differ in how tightly the electrons in the outer orbit are bound to the nucleus. The electrons, which are loosely bound to their nuclei, are called free electrons. These free electrons may be dislodged from an atom by giving them additional energy. Thus they may be transferred from one atom to another. The electrical properties of materials largely depend upon the number of free electrons available. -
Zero-Voltage Switching Flyback-Boost Converter with Voltage-Doubler Rectifier for High Step-Up Applications
Zero-Voltage Switching Flyback-Boost Converter with Voltage-Doubler Rectifier for High Step-up Applications Hyun-Wook Seong, Hyoung-Suk Kim, Ki-Bum Park, Gun-Woo Moon, and Myung-Joong Youn Department of Electrical Engineering, KAIST 373-1 Guseong-dong, Yuseong-gu, Daegeon, Republic of Korea, 305-701 [email protected] Abstract -- A zero-voltage switching (ZVS) flyback-boost (FB) output rectifier produces the high voltage spike. Thus, the converter with a voltage-doubler rectifier (VDR) has been snubber network is required across the output rectifier, which proposed. By combining the common part between a flyback results in a degraded efficiency. converter and a boost converter as a parallel-input/series-output As an attractive solution over aforementioned topologies, (PISO) configuration, this proposed circuit can increase a step- up ratio and clamp the surge voltage of switches. The secondary the flyback-boost (FB) converter was proposed as shown in VDR provides a further extended step-up ratio as well as its Fig. 1 [5], [6]. It can achieve a higher step-up ratio due to voltage stress to be clamped. An auxiliary switch instead of a both a transformer and a parallel-input/series-output (PISO) boost diode enables all switches to be turned on under ZVS configuration. Since the voltage spike across the switch is conditions. The zero-current turn-off of the secondary VDR limited to the output voltage of the boost converter, no alleviates its reverse-recovery losses. The operation principles, protection circuit is required. Furthermore, since the energy the theoretical analysis, and the design consideration are investigated. -
DESIGN and SIMULATION of a HIGH PERFORMANCE CMOS VOLTAGE DOUBLERS USING CHARGE REUSE TECHNIQUE 1. Introduction
Journal of Engineering Science and Technology Vol. 12, No. 12 (2017) 3344 - 3357 © School of Engineering, Taylor’s University DESIGN AND SIMULATION OF A HIGH PERFORMANCE CMOS VOLTAGE DOUBLERS USING CHARGE REUSE TECHNIQUE SHAMIL H. HUSSEIN Dept. of Electrical Engineering, College of Engineering, University of Mosul, Mosul, Iraq E-mail: [email protected] Abstract Voltage doubler (VD) structure plays an important role in charge pump (CP) circuits. It provides a voltages that is higher than the voltage of the power supply or a voltage of reverse polarity. In many applications such as the power IC and switched-capacitor transformers. This paper presents the design and analysis for VD using charge reuse technique CMOS 0.35µm tech. with high performance. Bootstrapped and charge reuse techniques is used to improve performance of integrated VD. Charge reusing method is based on equalizing the voltages of the pumping capacitances in each stage of CP. As a consequence, it reduces the load independent losses, improve the efficiency. Simulation using Orcad is applied for various VD structures shows improvement in charge reuse technique compared with existing counterpart. The results obtained show that the VD can be used in a wide band frequencies (0-100 MHz) or greater. The charge reuse VD circuit provided a good efficiency about (87.6%) and (83.5%) for one stage and two stage respectively at pump capacitance of 57pf, load current of 1mA, frequency of 10 MHz and supply voltage is 3.5 V compared with one stage and two stage of a latched VD are (85.4%) and (80%) respectively. -
HIGH VOLTAGE DC up to 2 KV from AC by USING CAPACITORS and DIODES in LADDER NETWORK Mr
[Prasad * et al., 5(6): June, 2018] ISSN: 2349-5197 Impact Factor: 3.765 INTERNATIONAL JOURNAL OF RESEARCH SCIENCE & MANAGEMENT HIGH VOLTAGE DC UP TO 2 KV FROM AC BY USING CAPACITORS AND DIODES IN LADDER NETWORK Mr. A. Raghavendra Prasad, Mr.K.Rajasekhara Reddy & Mr.M.Siva sankar Asst. Prof., Santhiram Engineering college, Nandyal Asst. Prof., Santhiram Engineering college, Nandyal Asst. Prof., Santhiram Engineering college, Nandyal DOI: 10.5281/zenodo.1291902 Abstract The aim of this project is designed to develop a high voltage DC around 2KV from a supply source of 230V AC using the capacitors and diodes in a ladder network based on voltage multiplier concept. The method for stepping up the voltage is commonly done by a step-up transformer. The output of the secondary of the step up transformer increases the voltage and decreases the current. The other method for stepping up the voltage is a voltage multiplier but from AC to DC. Voltage multipliers are primarily used to develop high voltages where low current is required. This project describes the concept to develop high voltage DC (even till 10KV output and beyond) from a single phase AC. For safety reasons our project restricts the multiplication factor to 8 such that the output would be within 2KV. This concept of generation is used in electronic appliances like the CRT’s, TV Picture tubes, oscilloscope and also used in industrial applications. The design of the circuit involves voltage multiplier, whose principle is to go on doubling the voltage for each stage. Thus, the output from an 8 stage voltage multiplier can generate up to 2KV. -
A Review of Charge Pump Topologies for the Power Management of Iot Nodes
electronics Review A Review of Charge Pump Topologies for the Power Management of IoT Nodes Andrea Ballo , Alfio Dario Grasso * and Gaetano Palumbo Dipartimento di Ingegneria Elettrica Elettronica e Informatica (DIEEI), University of Catania, I-95125 Catania, Italy; [email protected] (A.B.); [email protected] (G.P.) * Correspondence: [email protected]; Tel.: +39-095-738-2317 Received: 11 April 2019; Accepted: 24 April 2019; Published: 29 April 2019 Abstract: With the aim of providing designer guidelines for choosing the most suitable solution, according to the given design specifications, in this paper a review of charge pump (CP) topologies for the power management of Internet of Things (IoT) nodes is presented. Power management of IoT nodes represents a challenging task, especially when the output of the energy harvester is in the order of few hundreds of millivolts. In these applications, the power management section can be profitably implemented, exploiting CPs. Indeed, presently, many different CP topologies have been presented in literature. Finally, a data-driven comparison is also provided, allowing for quantitative insight into the state-of-the-art of integrated CPs. Keywords: charge pump (CP); Dickson charge pump; energy harvesting; IoT node; power management; switched-capacitors boost converter 1. Introduction The Internet of Things (IoT) paradigm is expected to have a pervasive impact in the next years. The ubiquitous character of IoT nodes implies that they must be untethered and energy autonomous. In IoT nodes, power-autonomy is achieved by scavenging energy from the ambient using transducers, such as photovoltaic (PV) cells, thermoelectric generators (TEG), and vibration sensors [1–4]. -
Electrical Engineering Dictionary
ratio of the power per unit solid angle scat- tered in a specific direction of the power unit area in a plane wave incident on the scatterer R from a specified direction. RADHAZ radiation hazards to personnel as defined in ANSI/C95.1-1991 IEEE Stan- RS commonly used symbol for source dard Safety Levels with Respect to Human impedance. Exposure to Radio Frequency Electromag- netic Fields, 3 kHz to 300 GHz. RT commonly used symbol for transfor- mation ratio. radial basis function network a fully R-ALOHA See reservation ALOHA. connected feedforward network with a sin- gle hidden layer of neurons each of which RL Typical symbol for load resistance. computes a nonlinear decreasing function of the distance between its received input and Rabi frequency the characteristic cou- a “center point.” This function is generally pling strength between a near-resonant elec- bell-shaped and has a different center point tromagnetic field and two states of a quan- for each neuron. The center points and the tum mechanical system. For example, the widths of the bell shapes are learned from Rabi frequency of an electric dipole allowed training data. The input weights usually have transition is equal to µE/hbar, where µ is the fixed values and may be prescribed on the electric dipole moment and E is the maxi- basis of prior knowledge. The outputs have mum electric field amplitude. In a strongly linear characteristics, and their weights are driven 2-level system, the Rabi frequency is computed during training. equal to the rate at which population oscil- lates between the ground and excited states. -
Electrical Engineering and the 4-H Engineering Design Challenge Level 2
MINNESOTA 4-H STEM PROGRAM Electrical Engineering and the 4-H Engineering Design Challenge Level 2 One of the exciting aspects of building the 4-H Engineering Design Challenge Level 2 machine is learning about the various categories of machine construction. This information addresses the Electrical element. WHAT IS ELECTRICITY? At its most basic, electricity is the presence and flow of electrical charges. Since all atoms have charges, electricity is all around us. While certain aspects of electricity had been observed for centuries, like lightning and static electricity, it wasn't until the 1600s that people tried to harness this energy. Today electricity is used for a lot more than powering appliances and lighting your home. All home devices communicate with each other using electrical impulses. Home stereo speakers are connected to TV with cables, audio visual cables each carry an electrical signal which allows televisions to communicate with different peripherals. None of that would be possible without electricity. ELECTRICITY AND OHM’S LAW Georg Ohm found that, at a constant temperature, the electrical current flowing through a fixed linear resistance is directly proportional to the voltage applied across it and inversely proportional to the resistance. This relationship between the Voltage, Current and Resistance forms the basis of Ohm's Law. Ohm's Law Relationship By knowing any two values of the Voltage, Current or Resistance quantities we can use Ohm's Law to find the third missing value. Ohm's Law is used extensively in electronics formulas and calculations and can provide some insight into how electricity may be involved in your machine.