Experiment 3: Basic Electronic Circuits II (tbc 1/7/2007)

Size: px
Start display at page:

Download "Experiment 3: Basic Electronic Circuits II (tbc 1/7/2007)"

Transcription

1 Experiment 3: Basi Eletroni iruits II (tb /7/007) Objetive: a) To study the first-order dynamis of a apaitive iruits with the appliation of Kirhoff s law, Ohm s law and apaitane formula. b) To learn how to do data-logging using Labview 8 and the USB-6009 devie. I. apaitors A. Definitions and Units B. Symbols apaitane () ratio of eletrial harge (Q) to voltage () Units: farad (F) oulomb/volt apaitors are eletrial omponents with onstant apaitane: Q dq d dq d I d I d aution: some apaitors (speially eletrolyti types) are polarized. Figure. Symbols for apaitors.

2 II. Experimental Setup Figure. 0µF, MΩ II. Labview Setup Figure. Front Panel onfiguration

3 Figure 3. Blok Diagram onfiguration. Proedure to inlude the ead apaitor blok shown in Figure 3:. In the Blok Diagram window, aess the Funtions palette and expand the [Express] [Input] ion subdiretory. Selet the [DAQ Assistant] blok and drop into the While loop box.. A onfiguration window should pop out. [lik] the [Analog Input] item to expand the menu hoies, then selet [oltage]. (see Figure 4) 3. A menu of available hannels and devies should appear. ( Make sure the USB devie is onneted to the omputer). Selet the item ai0 then [lik] the [Finish] button to move on to the onfiguration window. lik this to expand the menu hoies. Figure 4. 3

4 4. In the onfiguration window, math the values given in Table. Table. Settings for DAQ Assistant blok. Settings Input ange Min -5 Max 5 Saled Units olts Terminal onfiguration Differential Task Timing Aquisition Model ontinuous lok Settings Samples to ead 0 ate (Hz) [lik] the [OK] button to finish. (You may need to move the onfiguration window to the left to show the [OK] button on the lower right orner of the window.) 6. hange to ion view and rename the blok as ead apaitor, if desired. III. Tasks/Proedure. onstrut both the experimental setup and the Labview I setup.. With the power supply off, run the Labview I. Make sure that the voltage reading of the apaitor voltage starts at zero. ( If not, wait until the voltage settles to zero then stop and repeat the Labview run ) 3. At a hosen elapsed time (e.g. 0 seonds), turn the power supply on 4. Wait until the voltage settles to a new steady state then stop the Labview run. 5. Load the data into an Exel spreadsheet similar to the one shown in Figure 5. The model for the estimated apaitor voltage will be a first order model: d τ ) final ( t ) 0) initial () where τ is the time onstant, and t ) is the time elapsed after step hange. Assuming ap initial for t ) <0, the solution is given by: final ( ) initial initial final if t < tstart t tstart exp τ if t tstart () 4

5 (8-D8)^ AEAGE(E8: E37) IF( B8<$$, $$3, $$4($$3-$$4)* EXP(-(B8-$$)/$$5) Figure 4. Sample spreadsheet. 6. Use SOLE to minimize the root mean square (MS) error, by modifying the values of t start, initial, final and τ. Plot the data together with the estimated voltages to see if the fit is visually aeptable. Fill-in the values in Table. 7. Using the voltmeter, measure: a) the atual resistane of the MΩ resistor b) the apparent resistane of the USB-6009 devie ) the atual apaitane of the 0 µf apaitor d) s the voltage of the power supply and fill-in the values in Table ompare the value of time onstant τ and final,obtained from the parameter estimation in step 6, with the alulated values uisng equation (5) below, whih are based on Kirhoff s law, Ohm s law and the apaitane formula. Let, and be the voltages aross the MΩ resistor, the USB-6009 devie and the apaitor, respetively. Likewise, let I, I and I be the urrent flowing aross the MΩ resistor, the USB-6009 devie and the apaitor, respetively. Thus, I I I d Sine s and, we have (3) 5

6 6 s s s d d d (4) After omparing the oeffiients of (4) with (), final s τ (5) Table. From Data Fitting alulated from Eqn (5) % elative Error τ final initial t start

7 Table 3. s alulation for τ and final using equation (5): 7

EE 321 Project Spring 2018

EE 321 Project Spring 2018 EE 21 Projet Spring 2018 This ourse projet is intended to be an individual effort projet. The student is required to omplete the work individually, without help from anyone else. (The student may, however,

More information

The simulation analysis of the bridge rectifier continuous operation in AC circuit

The simulation analysis of the bridge rectifier continuous operation in AC circuit Computer Appliations in Eletrial Engineering Vol. 4 6 DOI 8/j.8-448.6. The simulation analysis of the bridge retifier ontinuous operation in AC iruit Mirosław Wiślik, Paweł Strząbała Kiele University of

More information

Capacitors. The charge Q on a capacitor s plate is proportional to the potential difference V across the Q = C V (1)

Capacitors. The charge Q on a capacitor s plate is proportional to the potential difference V across the Q = C V (1) apacitors THEORY The charge Q on a capacitor s plate is proportional to the potential difference V across the capacitor. We express this with Q = V (1) where is a proportionality constant known as the

More information

Models for the simulation of electronic circuits with hysteretic inductors

Models for the simulation of electronic circuits with hysteretic inductors Proeedings of the 5th WSEAS Int. Conf. on Miroeletronis, Nanoeletronis, Optoeletronis, Prague, Czeh Republi, Marh 12-14, 26 (pp86-91) Models for the simulation of eletroni iruits with hystereti indutors

More information

PHYSICS 212 FINAL EXAM 21 March 2003

PHYSICS 212 FINAL EXAM 21 March 2003 PHYSIS INAL EXAM Marh 00 Eam is losed book, losed notes. Use only the provided formula sheet. Write all work and answers in eam booklets. The baks of pages will not be graded unless you so ruest on the

More information

DIGITAL DISTANCE RELAYING SCHEME FOR PARALLEL TRANSMISSION LINES DURING INTER-CIRCUIT FAULTS

DIGITAL DISTANCE RELAYING SCHEME FOR PARALLEL TRANSMISSION LINES DURING INTER-CIRCUIT FAULTS CHAPTER 4 DIGITAL DISTANCE RELAYING SCHEME FOR PARALLEL TRANSMISSION LINES DURING INTER-CIRCUIT FAULTS 4.1 INTRODUCTION Around the world, environmental and ost onsiousness are foring utilities to install

More information

Simplified Modeling, Analysis and Simulation of Permanent Magnet Brushless Direct Current Motors for Sensorless Operation

Simplified Modeling, Analysis and Simulation of Permanent Magnet Brushless Direct Current Motors for Sensorless Operation Amerian Journal of Applied Sienes 9 (7): 1046-1054, 2012 ISSN 1546-9239 2012 Siene Publiations Simplified Modeling, Analysis and Simulation of Permanent Magnet Brushless Diret Current Motors for Sensorless

More information

Heat exchangers: Heat exchanger types:

Heat exchangers: Heat exchanger types: Heat exhangers: he proess of heat exhange between two fluids that are at different temperatures and separated by a solid wall ours in many engineering appliations. he devie used to implement this exhange

More information

UTC. Engineering 329. Proportional Controller Design. Speed System. John Beverly. Green Team. John Beverly Keith Skiles John Barker.

UTC. Engineering 329. Proportional Controller Design. Speed System. John Beverly. Green Team. John Beverly Keith Skiles John Barker. UTC Engineering 329 Proportional Controller Design for Speed System By John Beverly Green Team John Beverly Keith Skiles John Barker 24 Mar 2006 Introdution This experiment is intended test the variable

More information

A Theorem of Mass Being Derived From Electrical Standing Waves (Adapted for a test by Jerry E. Bayles)

A Theorem of Mass Being Derived From Electrical Standing Waves (Adapted for a test by Jerry E. Bayles) EleMaEMCD A Theorem of Mass Being Derived From Eletrial Standing Waves (Adapted for a test by Jerry E Bayles) - by - Jerry E Bayles May 1, 000 This paper formalizes a onept presented in my book, "Eletrogravitation

More information

Part G-4: Sample Exams

Part G-4: Sample Exams Part G-4: Sample Exams 1 Cairo University M.S.: Eletronis Cooling Faulty of Engineering Final Exam (Sample 1) Mehanial Power Engineering Dept. Time allowed 2 Hours Solve as muh as you an. 1. A heat sink

More information

MATLAB/Simulink Based Study of Different Approaches Using Mathematical Model of Differential Equations

MATLAB/Simulink Based Study of Different Approaches Using Mathematical Model of Differential Equations I.J. Intelligent Systems and Appliations, 04, 05, -4 Published Online April 04 in MECS (http://www.mes-press.org/) DOI: 0.585/ijisa.04.05.0 MATLAB/Simulink Based Study of Different Approahes Using Mathematial

More information

Combined Electric and Magnetic Dipoles for Mesoband Radiation, Part 2

Combined Electric and Magnetic Dipoles for Mesoband Radiation, Part 2 Sensor and Simulation Notes Note 53 3 May 8 Combined Eletri and Magneti Dipoles for Mesoband Radiation, Part Carl E. Baum University of New Mexio Department of Eletrial and Computer Engineering Albuquerque

More information

max min z i i=1 x j k s.t. j=1 x j j:i T j

max min z i i=1 x j k s.t. j=1 x j j:i T j AM 221: Advaned Optimization Spring 2016 Prof. Yaron Singer Leture 22 April 18th 1 Overview In this leture, we will study the pipage rounding tehnique whih is a deterministi rounding proedure that an be

More information

Final Review. A Puzzle... Special Relativity. Direction of the Force. Moving at the Speed of Light

Final Review. A Puzzle... Special Relativity. Direction of the Force. Moving at the Speed of Light Final Review A Puzzle... Diretion of the Fore A point harge q is loated a fixed height h above an infinite horizontal onduting plane. Another point harge q is loated a height z (with z > h) above the plane.

More information

CAPACITANCE AND INDUCTANCE

CAPACITANCE AND INDUCTANCE APAITANE AND INDUTANE Inroduces wo passve, energy sorng devces: apacors and Inducors LEARNING GOALS APAITORS Sore energy n her elecrc feld (elecrosac energy) Model as crcu elemen INDUTORS Sore energy n

More information

System Identification of RTD Dynamics (Tom Co, 11/26/2006; 11/25/2007, 11/15/2009)

System Identification of RTD Dynamics (Tom Co, 11/26/2006; 11/25/2007, 11/15/2009) System Identification of RTD Dynamics (Tom Co, 11/26/26; 11/25/27, 11/15/29) Laboratory Objective: To obtain a mathematical model of RTD dynamics General procedures for mathematical modeling of dynamic

More information

University of TN Chattanooga Physics 1040L 8/18/2012 PHYSICS 1040L LAB LAB 4: R.C. TIME CONSTANT LAB

University of TN Chattanooga Physics 1040L 8/18/2012 PHYSICS 1040L LAB LAB 4: R.C. TIME CONSTANT LAB PHYSICS 1040L LAB LAB 4: R.C. TIME CONSTANT LAB OBJECT: To study the discharging of a capacitor and determine the time constant for a simple circuit. APPARATUS: Capacitor (about 24 μf), two resistors (about

More information

Experiment 03: Work and Energy

Experiment 03: Work and Energy MASSACHUSETTS INSTITUTE OF TECHNOLOGY Physis Department Physis 8.01 Purpose of the Experiment: Experiment 03: Work and Energy In this experiment you allow a art to roll down an inlined ramp and run into

More information

Capacitor in the AC circuit with Cobra3

Capacitor in the AC circuit with Cobra3 Capacitor in the AC circuit with Cobra3 LEP Related Topics Capacitance, Kirchhoff s laws, Maxwell s equations, AC impedance, Phase displacement Principle A capacitor is connected in a circuit with a variable-frequency

More information

Example Calculations of Uncertainty

Example Calculations of Uncertainty nertainty Examples. Example alulations of nertainty Instrument Bias nertainty Example # A D voltage of -.65 volts is measured with an Agilent #05A Multimeter. Aording to the data sheet (p.5.) the D auray

More information

CAPACITANCE AND INDUCTANCE

CAPACITANCE AND INDUCTANCE APAITANE AND INDUTANE Inroduces wo passive, energy soring devices: apaciors and Inducors LEARNING GOALS APAITORS Sore energy in heir elecric field (elecrosaic energy) Model as circui elemen INDUTORS Sore

More information

Special Relativity Electromagnetic and Gravitation combined Into one theory

Special Relativity Electromagnetic and Gravitation combined Into one theory --5 Speial Relatiity Eletromagneti and Graitation ombined Into one theory Mourii Shahter mourii@gmail.om mourii@walla.o.il ISRAE, HOON 54-54855 Introdution In this paper, I try to ombine Eletromagneti

More information

Thin Airfoil Theory Lab

Thin Airfoil Theory Lab Thin Airfoil Theory Lab AME 3333 University of Notre Dame Spring 26 Written by Chris Kelley and Grady Crahan Deember, 28 Updated by Brian Neiswander and Ryan Kelly February 6, 24 Updated by Kyle Heintz

More information

Speed-feedback Direct-drive Control of a Low-speed Transverse Flux-type Motor with Large Number of Poles for Ship Propulsion

Speed-feedback Direct-drive Control of a Low-speed Transverse Flux-type Motor with Large Number of Poles for Ship Propulsion Speed-feedbak Diret-drive Control of a Low-speed Transverse Flux-type Motor with Large Number of Poles for Ship Propulsion Y. Yamamoto, T. Nakamura 2, Y. Takada, T. Koseki, Y. Aoyama 3, and Y. Iwaji 3

More information

Comparison of Alternative Equivalent Circuits of Induction Motor with Real Machine Data

Comparison of Alternative Equivalent Circuits of Induction Motor with Real Machine Data Comparison of Alternative Equivalent Ciruits of Indution Motor with Real Mahine Data J. radna, J. auer, S. Fligl and V. Hlinovsky Abstrat The algorithms based on separated ontrol of the motor flux and

More information

BS7671:2008 +A3:2015 (Answers references to On-Site Guide) You may find it helpful to have a copy of BS7671:2008 +A3:2015 On-Site Guide.

BS7671:2008 +A3:2015 (Answers references to On-Site Guide) You may find it helpful to have a copy of BS7671:2008 +A3:2015 On-Site Guide. Eletrial supply systems: (Covering Outome 2 of Unit 304 Understand the priniples of internal and external earthing arrangements for eletrial installations for buildings, strutures and the environment (Level

More information

Motor Sizing Application Note

Motor Sizing Application Note PAE-TILOGY Linear Motors 70 Mill orest d. Webster, TX 77598 (8) 6-7750 ax (8) 6-7760 www.trilogysystems.om E-mail emn_support_trilogy@parker.om Motor Sizing Appliation Note By Jak Marsh Introdution Linear

More information

The universal model of error of active power measuring channel

The universal model of error of active power measuring channel 7 th Symposium EKO TC 4 3 rd Symposium EKO TC 9 and 5 th WADC Workshop nstrumentation for the CT Era Sept. 8-2 Kosie Slovakia The universal model of error of ative power measuring hannel Boris Stogny Evgeny

More information

Developing Excel Macros for Solving Heat Diffusion Problems

Developing Excel Macros for Solving Heat Diffusion Problems Session 50 Developing Exel Maros for Solving Heat Diffusion Problems N. N. Sarker and M. A. Ketkar Department of Engineering Tehnology Prairie View A&M University Prairie View, TX 77446 Abstrat This paper

More information

Hankel Optimal Model Order Reduction 1

Hankel Optimal Model Order Reduction 1 Massahusetts Institute of Tehnology Department of Eletrial Engineering and Computer Siene 6.245: MULTIVARIABLE CONTROL SYSTEMS by A. Megretski Hankel Optimal Model Order Redution 1 This leture overs both

More information

If velocity of A relative to ground = velocity of B relative to ground = the velocity of A relative to B =

If velocity of A relative to ground = velocity of B relative to ground = the velocity of A relative to B = L Physis MC nswers Year:1989 Question Number: 3,0,,4,6,9,30,31,36,40,4 1989MC (3) If eloity of relatie to ground = and eloity of relatie to ground =, then the eloity of relatie to = X X Y Y Suppose that

More information

Atomic and Nuclear Physics

Atomic and Nuclear Physics Atomi and Nulear Physis X-ray physis Compton effet and X-ray physis LD Physis Leaflets P6.3.7. Compton effet: Measuring the energy of the sattered photons as a funtion of the sattering angle Objets of

More information

Atomic and Nuclear Physics

Atomic and Nuclear Physics Atomi and Nulear Physis X-ray physis Compton effet and X-ray physis LD Physis Leaflets P6.3.7. Compton effet: Measuring the energy of the sattered photons as a funtion of the sattering angle Objets of

More information

3B SCIENTIFIC PHYSICS

3B SCIENTIFIC PHYSICS 3B SCIENTIFIC PHYSICS Peltier Heat Pump 0076 Instrution manual 05/7 TL/JS Transport ase Semati view 3 Stirrer unit 4 Connetor for stirrer unit 5 Connetor for power supply 6 Stirring rod old side 7 Peltier

More information

Pre/Post Charge Control using IGBT for Relay Contact Protection in Electric Vehicle

Pre/Post Charge Control using IGBT for Relay Contact Protection in Electric Vehicle WSEAS TRANSATONS on POWER SYSTEMS Surahai Wongfookeat, Thanathai Kulworawanihpong Pre/Post har ontrol using GBT for Relay ontat Protetion in Eletri ehile Shool of Eletrial Engineering, nstitute of Engineering

More information

TeSys contactors. Rated operational. current in AC V up to. kw kw kw kw kw kw kw A kg

TeSys contactors. Rated operational. current in AC V up to. kw kw kw kw kw kw kw A kg Referenes TeSys ontators TeSys D ontators for motor ontrol up to kw at 00 V, in ategory AC- For onnetion y srew lamp terminals and lugs D0pp Dpp -pole ontators Standard power ratings of -phase motors 0-0

More information

Directional Coupler. 4-port Network

Directional Coupler. 4-port Network Diretional Coupler 4-port Network 3 4 A diretional oupler is a 4-port network exhibiting: All ports mathed on the referene load (i.e. S =S =S 33 =S 44 =0) Two pair of ports unoupled (i.e. the orresponding

More information

Advances in Radio Science

Advances in Radio Science Advanes in adio Siene 2003) 1: 99 104 Copernius GmbH 2003 Advanes in adio Siene A hybrid method ombining the FDTD and a time domain boundary-integral equation marhing-on-in-time algorithm A Beker and V

More information

ENERGY AND MOMENTUM IN ELECTROMAGNETIC WAVES

ENERGY AND MOMENTUM IN ELECTROMAGNETIC WAVES MISN-0-211 z ENERGY AND MOMENTUM IN ELECTROMAGNETIC WAVES y È B` x ENERGY AND MOMENTUM IN ELECTROMAGNETIC WAVES by J. S. Kovas and P. Signell Mihigan State University 1. Desription................................................

More information

Natural Convection Experiment Measurements from a Vertical Surface

Natural Convection Experiment Measurements from a Vertical Surface OBJECTIVE Natural Convetion Experiment Measurements from a Vertial Surfae 1. To demonstrate te basi priniples of natural onvetion eat transfer inluding determination of te onvetive eat transfer oeffiient.

More information

+Ze. n = N/V = 6.02 x x (Z Z c ) m /A, (1.1) Avogadro s number

+Ze. n = N/V = 6.02 x x (Z Z c ) m /A, (1.1) Avogadro s number In 1897, J. J. Thomson disovered eletrons. In 1905, Einstein interpreted the photoeletri effet In 1911 - Rutherford proved that atoms are omposed of a point-like positively harged, massive nuleus surrounded

More information

Subject: Introduction to Component Matching and Off-Design Operation % % ( (1) R T % (

Subject: Introduction to Component Matching and Off-Design Operation % % ( (1) R T % ( 16.50 Leture 0 Subjet: Introdution to Component Mathing and Off-Design Operation At this point it is well to reflet on whih of the many parameters we have introdued (like M, τ, τ t, ϑ t, f, et.) are free

More information

RC Circuits. Equipment: Capstone with 850 interface, RLC circuit board, 2 voltage sensors (no alligator clips), 3 leads V C = 1

RC Circuits. Equipment: Capstone with 850 interface, RLC circuit board, 2 voltage sensors (no alligator clips), 3 leads V C = 1 R ircuits Equipment: apstone with 850 interface, RL circuit board, 2 voltage sensors (no alligator clips), 3 leads 1 Introduction The 3 basic linear circuits elements are the resistor, the capacitor, and

More information

I D based Two-Stage Amplifier Design

I D based Two-Stage Amplifier Design m D based Two-Stae Amplifier Desin honli ai 9/0/04 Motivation d/(w/l) VS VG is sensitive to Vbs Motivation m/d vs VG is also sensitive to Vbs Motivation But m/d vs D/(W/L) has fixed shape With a ertain

More information

23.1 Tuning controllers, in the large view Quoting from Section 16.7:

23.1 Tuning controllers, in the large view Quoting from Section 16.7: Lesson 23. Tuning a real ontroller - modeling, proess identifiation, fine tuning 23.0 Context We have learned to view proesses as dynami systems, taking are to identify their input, intermediate, and output

More information

9 Geophysics and Radio-Astronomy: VLBI VeryLongBaseInterferometry

9 Geophysics and Radio-Astronomy: VLBI VeryLongBaseInterferometry 9 Geophysis and Radio-Astronomy: VLBI VeryLongBaseInterferometry VLBI is an interferometry tehnique used in radio astronomy, in whih two or more signals, oming from the same astronomial objet, are reeived

More information

Lightning electromagnetic environment in the presence of a tall grounded strike object

Lightning electromagnetic environment in the presence of a tall grounded strike object JOURNAL OF GEOPHYSICAL RESEARCH, VOL.,, doi:.9/4jd555, 5 Lightning eletromagneti environment in the presene of a tall grounded strike objet Yoshihiro Baba Department of Eletrial Engineering, Doshisha University,

More information

Speed Regulation of a Small BLDC Motor using Genetic-Based Proportional Control

Speed Regulation of a Small BLDC Motor using Genetic-Based Proportional Control World Aademy of Siene, Engineering and Tehnology 47 8 Speed Regulation of a Small BLDC Motor using Geneti-Based Proportional Control S. Poonsawat, and T. Kulworawanihpong Abstrat This paper presents the

More information

COMPUTER METHODS FOR THE DETERMINATION OF THE CRITICAL PARAMETERS OF POLLUTED INSULATORS

COMPUTER METHODS FOR THE DETERMINATION OF THE CRITICAL PARAMETERS OF POLLUTED INSULATORS COMPUTER METHODS FOR THE DETERMINATION OF THE CRITICAL PARAMETERS OF POLLUTED INSULATORS I. F. GONOS S. A. SUFLIS F. V. TOPALIS I.A. STATHOPULOS NATIONAL TECHNICAL UNIVERSITY OF ATHENS DEPARTMENT OF ELECTRICAL

More information

IZM circuit-breakers IN switch-disconnectors up to 6300 A

IZM circuit-breakers IN switch-disconnectors up to 6300 A Contents 11/1 IZM iruit-breaers IN swith-disonnetors up to 6300 A Modern protetion tehnology overing the rated urrent range. This overview will assist you to effiiently use the Moeller onept for the open

More information

Analysis of discretization in the direct simulation Monte Carlo

Analysis of discretization in the direct simulation Monte Carlo PHYSICS OF FLUIDS VOLUME 1, UMBER 1 OCTOBER Analysis of disretization in the diret simulation Monte Carlo iolas G. Hadjionstantinou a) Department of Mehanial Engineering, Massahusetts Institute of Tehnology,

More information

Relativistic Dynamics

Relativistic Dynamics Chapter 7 Relativisti Dynamis 7.1 General Priniples of Dynamis 7.2 Relativisti Ation As stated in Setion A.2, all of dynamis is derived from the priniple of least ation. Thus it is our hore to find a suitable

More information

Lab 10: DC RC circuits

Lab 10: DC RC circuits Name: Lab 10: DC RC circuits Group Members: Date: TA s Name: Objectives: 1. To understand current and voltage characteristics of a DC RC circuit 2. To understand the effect of the RC time constant Apparatus:

More information

Precision, Quad, SPDT, CMOS Analog Switch

Precision, Quad, SPDT, CMOS Analog Switch 19-0189; Rev 1; 6/99 Precision, Quad, SPDT, MOS Analog Switch General Description The is a precision, quad, single-pole doublethrow (SPDT) analog switch. The four independent switches operate with bipolar

More information

Maximum Entropy and Exponential Families

Maximum Entropy and Exponential Families Maximum Entropy and Exponential Families April 9, 209 Abstrat The goal of this note is to derive the exponential form of probability distribution from more basi onsiderations, in partiular Entropy. It

More information

BME/ISE 3511 Bioelectronics - Test Six Course Notes Fall 2016

BME/ISE 3511 Bioelectronics - Test Six Course Notes Fall 2016 BME/ISE 35 Bioelectronics - Test Six ourse Notes Fall 06 Alternating urrent apacitive & Inductive Reactance and omplex Impedance R & R ircuit Analyses (D Transients, Time onstants, Steady State) Electrical

More information

Techniques for Including Dielectrics when Extracting Passive Low-Order Models of High Speed Interconnect

Techniques for Including Dielectrics when Extracting Passive Low-Order Models of High Speed Interconnect Tehniques for Inluding Dieletris when Extrating Passive Low-Order Models of High Speed Interonnet Lua Daniel University of California, Berkeley dlua@ees.berkeley.edu Alberto Sangiovanni-Vinentelli Univ.

More information

AIC431/TL431A/TL431. Adjustable Precision Shunt Regulators FEATURES DESCRIPTION TYPICAL APPLICATION CIRCUIT. Precision Regulator

AIC431/TL431A/TL431. Adjustable Precision Shunt Regulators FEATURES DESCRIPTION TYPICAL APPLICATION CIRCUIT. Precision Regulator /TL431A/TL431 Adjustable Precision Shunt Regulators FEATURES Unconditionally Stable. Precision Reference Voltage. :2.495V ±0.5% TL431A :2.495V ±1.0% TL431 :2.495V ±1.6% Sink urrent apability: 200mA. Minimum

More information

Relativity in Classical Physics

Relativity in Classical Physics Relativity in Classial Physis Main Points Introdution Galilean (Newtonian) Relativity Relativity & Eletromagnetism Mihelson-Morley Experiment Introdution The theory of relativity deals with the study of

More information

Experiment 5: Thermocouples (tbc 1/14/2007, revised 3/16/2007, 3/22,2007, 2/23/2009, 3/13/2011)

Experiment 5: Thermocouples (tbc 1/14/2007, revised 3/16/2007, 3/22,2007, 2/23/2009, 3/13/2011) Experiment 5: Thermocouples (tbc 1/14/2007, revised 3/16/2007, 3/22,2007, 2/23/2009, 3/13/2011) Objective: To implement a thermocouple circuit for temperature sensing. I. Introduction to Thermocouples

More information

An Improved State Space Average Model of Buck DC-DC Converter with all of the System Uncertainties

An Improved State Space Average Model of Buck DC-DC Converter with all of the System Uncertainties International Journal on Eletrial Engineering and Informatis - Volume 5, Number 1, Marh 2013 An Improed State Spae Aerage Model of Buk DC-DC Conerter with all of the System Unertainties Mohammad Reza Modabbernia

More information

A NETWORK SIMPLEX ALGORITHM FOR THE MINIMUM COST-BENEFIT NETWORK FLOW PROBLEM

A NETWORK SIMPLEX ALGORITHM FOR THE MINIMUM COST-BENEFIT NETWORK FLOW PROBLEM NETWORK SIMPLEX LGORITHM FOR THE MINIMUM COST-BENEFIT NETWORK FLOW PROBLEM Cen Çalışan, Utah Valley University, 800 W. University Parway, Orem, UT 84058, 801-863-6487, en.alisan@uvu.edu BSTRCT The minimum

More information

Robust Flight Control Design for a Turn Coordination System with Parameter Uncertainties

Robust Flight Control Design for a Turn Coordination System with Parameter Uncertainties Amerian Journal of Applied Sienes 4 (7): 496-501, 007 ISSN 1546-939 007 Siene Publiations Robust Flight ontrol Design for a urn oordination System with Parameter Unertainties 1 Ari Legowo and Hiroshi Okubo

More information

COMBINED PROBE FOR MACH NUMBER, TEMPERATURE AND INCIDENCE INDICATION

COMBINED PROBE FOR MACH NUMBER, TEMPERATURE AND INCIDENCE INDICATION 4 TH INTERNATIONAL CONGRESS OF THE AERONAUTICAL SCIENCES COMBINED PROBE FOR MACH NUMBER, TEMPERATURE AND INCIDENCE INDICATION Jiri Nozika*, Josef Adame*, Daniel Hanus** *Department of Fluid Dynamis and

More information

Line Radiative Transfer

Line Radiative Transfer http://www.v.nrao.edu/ourse/astr534/ineradxfer.html ine Radiative Transfer Einstein Coeffiients We used armor's equation to estimate the spontaneous emission oeffiients A U for À reombination lines. A

More information

Differential Equations 8/24/2010

Differential Equations 8/24/2010 Differential Equations A Differential i Equation (DE) is an equation ontaining one or more derivatives of an unknown dependant d variable with respet to (wrt) one or more independent variables. Solution

More information

Experiment 4. RC Circuits. Observe and qualitatively describe the charging and discharging (decay) of the voltage on a capacitor.

Experiment 4. RC Circuits. Observe and qualitatively describe the charging and discharging (decay) of the voltage on a capacitor. Experiment 4 RC Circuits 4.1 Objectives Observe and qualitatively describe the charging and discharging (decay) of the voltage on a capacitor. Graphically determine the time constant τ for the decay. 4.2

More information

CAPACITORS / CAPACITANCE ECET11

CAPACITORS / CAPACITANCE ECET11 APAITORS / APAITANE - apacitance - apacitor types - apacitors in series & parallel - R ircuit harging phase - R ircuit Discharging phase - R ircuit Steady State model - Source onversions - Superposition

More information

TRANSMISSION AND DISTRIBUTION LINES & CABLES

TRANSMISSION AND DISTRIBUTION LINES & CABLES ELEC46 Power ystem Analysis TANMON AND DTBUTON LNE & CABLE eading: hapters 4 and 5 of textbook (Glover et al). EE ETANCE Current in ondutor real power losses k = skin effet fator (.0) l = resistivity k

More information

HIGH speed interconnects both on-board and on-chip that

HIGH speed interconnects both on-board and on-chip that Eigenmode-based Capaitane Calulations with Appliations in Passivation Layer Design Thomas Demeester and Daniël De Zutter, Fellow, IEEE Abstrat The design of high-speed metalli interonnets suh as mirostrips

More information

What s New in ChemSep TM 6.8

What s New in ChemSep TM 6.8 What s New in ChemSep TM 6.8 January 2011 (Updated Marh 2011) Harry Kooijman and Ross Taylor In this doument we identify and desribe the most important new features in ChemSep. 1. New: GUI an diretly load

More information

Supplementary Materials

Supplementary Materials Supplementary Materials Neural population partitioning and a onurrent brain-mahine interfae for sequential motor funtion Maryam M. Shanehi, Rollin C. Hu, Marissa Powers, Gregory W. Wornell, Emery N. Brown

More information

CAPACITANCE. Capacitor. Because of the effect of capacitance, an electrical circuit can store energy, even after being de-energized.

CAPACITANCE. Capacitor. Because of the effect of capacitance, an electrical circuit can store energy, even after being de-energized. D ircuits APAITANE APAITANE Because of the effect of capacitance, an electrical circuit can store energy, even after being de-energized. EO 1.5 EO 1.6 EO 1.7 EO 1.8 EO 1.9 DESRIBE the construction of a

More information

Class XII - Physics Electromagnetic Waves Chapter-wise Problems

Class XII - Physics Electromagnetic Waves Chapter-wise Problems Class XII - Physis Eletromagneti Waves Chapter-wise Problems Multiple Choie Question :- 8 One requires ev of energy to dissoiate a arbon monoxide moleule into arbon and oxygen atoms The minimum frequeny

More information

Millennium Relativity Acceleration Composition. The Relativistic Relationship between Acceleration and Uniform Motion

Millennium Relativity Acceleration Composition. The Relativistic Relationship between Acceleration and Uniform Motion Millennium Relativity Aeleration Composition he Relativisti Relationship between Aeleration and niform Motion Copyright 003 Joseph A. Rybzyk Abstrat he relativisti priniples developed throughout the six

More information

Chapter 3 Church-Turing Thesis. CS 341: Foundations of CS II

Chapter 3 Church-Turing Thesis. CS 341: Foundations of CS II CS 341: Foundations of CS II Marvin K. Nakayama Computer Siene Department New Jersey Institute of Tehnology Newark, NJ 07102 CS 341: Chapter 3 3-2 Contents Turing Mahines Turing-reognizable Turing-deidable

More information

Control Theory association of mathematics and engineering

Control Theory association of mathematics and engineering Control Theory assoiation of mathematis and engineering Wojieh Mitkowski Krzysztof Oprzedkiewiz Department of Automatis AGH Univ. of Siene & Tehnology, Craow, Poland, Abstrat In this paper a methodology

More information

A Unified View on Multi-class Support Vector Classification Supplement

A Unified View on Multi-class Support Vector Classification Supplement Journal of Mahine Learning Researh??) Submitted 7/15; Published?/?? A Unified View on Multi-lass Support Vetor Classifiation Supplement Ürün Doğan Mirosoft Researh Tobias Glasmahers Institut für Neuroinformatik

More information

International Journal of Electronics and Computer Science Engineering 817. Available Online at ISSN

International Journal of Electronics and Computer Science Engineering 817. Available Online at   ISSN International Journal of Eletronis and Computer Siene Engineering 817 Available Online at www.ijese.org ISSN- 2277-1956 A Duly Synhronized, Straightforward Approah For Realizing the General Charateristis

More information

California University of Pennsylvania. Department of Applied Engineering & Technology. Electrical / Computer Engineering Technology

California University of Pennsylvania. Department of Applied Engineering & Technology. Electrical / Computer Engineering Technology California University of Pennsylvania Department of Applied Engineering & Technology Electrical / Computer Engineering Technology EET 215: Introduction to Instrumentations Lab No.7 Temperature Measurement

More information

To determine the biasing conditions needed to obtain a specific gain each stage must be considered.

To determine the biasing conditions needed to obtain a specific gain each stage must be considered. PHYSIS 56 Experiment 9: ommon Emitter Amplifier A. Introdution A ommon-emitter oltage amplifier will be tudied in thi experiment. You will inetigate the fator that ontrol the midfrequeny gain and the low-and

More information

Modes are solutions, of Maxwell s equation applied to a specific device.

Modes are solutions, of Maxwell s equation applied to a specific device. Mirowave Integrated Ciruits Prof. Jayanta Mukherjee Department of Eletrial Engineering Indian Institute of Tehnology, Bombay Mod 01, Le 06 Mirowave omponents Welome to another module of this NPTEL mok

More information

First Order RC and RL Transient Circuits

First Order RC and RL Transient Circuits First Order R and RL Transient ircuits Objectives To introduce the transients phenomena. To analyze step and natural responses of first order R circuits. To analyze step and natural responses of first

More information

Arithmetic Circuits. Comp 120, Spring 05 2/10 Lecture. Today s BIG Picture Reading: Study Chapter 3. (Chapter 4 in old book)

Arithmetic Circuits. Comp 120, Spring 05 2/10 Lecture. Today s BIG Picture Reading: Study Chapter 3. (Chapter 4 in old book) omp 2, pring 5 2/ Leture page Arithmeti iruits Didn t I learn how to do addition in the seond grade? UN ourses aren t what they used to be... + Finally; time to build some serious funtional bloks We ll

More information

An Adaptive Optimization Approach to Active Cancellation of Repeated Transient Vibration Disturbances

An Adaptive Optimization Approach to Active Cancellation of Repeated Transient Vibration Disturbances An aptive Optimization Approah to Ative Canellation of Repeated Transient Vibration Disturbanes David L. Bowen RH Lyon Corp / Aenteh, 33 Moulton St., Cambridge, MA 138, U.S.A., owen@lyonorp.om J. Gregory

More information

UPPER-TRUNCATED POWER LAW DISTRIBUTIONS

UPPER-TRUNCATED POWER LAW DISTRIBUTIONS Fratals, Vol. 9, No. (00) 09 World Sientifi Publishing Company UPPER-TRUNCATED POWER LAW DISTRIBUTIONS STEPHEN M. BURROUGHS and SARAH F. TEBBENS College of Marine Siene, University of South Florida, St.

More information

Heat propagation and stability in a small high T superconductor. coil

Heat propagation and stability in a small high T superconductor. coil Ž. Physia C 310 1998 372 376 Heat propagation and stability in a small high T superondutor oil T. Kiss a,), V.S. Vysotsky a, H. Yuge a, H. Saho a, Yu.A. Ilyin a, M. Takeo a, K. Watanabe b, F. Irie a Graduate

More information

LECTURE 5 PER-PHASE CIRCUITS AND MAGNETICS (1)

LECTURE 5 PER-PHASE CIRCUITS AND MAGNETICS (1) ECE 330 POWER CIRCUITS AND ELECTROMECHANICS LECTURE 5 PER-PHASE CIRCUITS AND MAGNETICS (1) Aknowledgment-These handouts and leture notes given in lass are based on material from Prof. Peter Sauer s ECE

More information

Case I: 2 users In case of 2 users, the probability of error for user 1 was earlier derived to be 2 A1

Case I: 2 users In case of 2 users, the probability of error for user 1 was earlier derived to be 2 A1 MUTLIUSER DETECTION (Letures 9 and 0) 6:33:546 Wireless Communiations Tehnologies Instrutor: Dr. Narayan Mandayam Summary By Shweta Shrivastava (shwetash@winlab.rutgers.edu) bstrat This artile ontinues

More information

dy dx 1 P a g e

dy dx 1 P a g e . India is a ountry of rih heritage and ultural diversity. Whih one of the following fats best supports the laim made in the above sentene? India is a union of 8 states and 7 union territories. India has

More information

CALIFORNIA STATE UNIVERSITY, BAKERSFIELD (CSUB) Laboratory 3

CALIFORNIA STATE UNIVERSITY, BAKERSFIELD (CSUB) Laboratory 3 ALIFORNIA STATE UNIERSITY, BAKERSFIELD (SUB) DEPARTMENT OF ELETRIAL & OMPUTER ENGINEERING & OMPUTER SIENE EE 3320: FIELDS AND WAES Laboratory 3 First, get familiar with the oscilloscope It is a powerful

More information

Circuits. 1. The Schematic

Circuits. 1. The Schematic + ircuits 1. The Schematic 2. Power in circuits 3. The Battery 1. eal Battery vs. Ideal Battery 4. Basic ircuit nalysis 1. oltage Drop 2. Kirchoff s Junction Law 3. Series & Parallel 5. Measurement Tools

More information

LATTICE BOLTZMANN METHOD FOR MICRO CHANNEL AND MICRO ORIFICE FLOWS TAIHO YEOM. Bachelor of Science in Mechanical Engineering.

LATTICE BOLTZMANN METHOD FOR MICRO CHANNEL AND MICRO ORIFICE FLOWS TAIHO YEOM. Bachelor of Science in Mechanical Engineering. LATTICE BOLTZMANN METHOD FOR MICRO CHANNEL AND MICRO ORIFICE FLOWS By TAIHO YEOM Bahelor of Siene in Mehanial Engineering Ajou University Suwon, South Korea 2005 Submitted to the Faulty of the Graduate

More information

Power-speed Trade-off in Parallel Prefix Circuits

Power-speed Trade-off in Parallel Prefix Circuits Power-speed Trade-off in Parallel Prefix Ciruits ITCom 00 High-Performane Pervasive Computing Conferene Boston, MA July 9 August, 00 by S. Vanihayobon, S. K. Dhall, S. Lakshmivarahan, J. K. Antonio Shool

More information

QNET Experiment #05: HVAC System Identification. Heating, Ventilation, and Air Conditioning Trainer (HVACT) Student Manual

QNET Experiment #05: HVAC System Identification. Heating, Ventilation, and Air Conditioning Trainer (HVACT) Student Manual Quanser NI-ELVIS Trainer (QNET) Series: QNET Experiment #05: HVAC System Identification Heating, Ventilation, and Air Conditioning Trainer (HVACT) Student Manual Table of Contents 1. Laboratory Objectives...1

More information

A Spatiotemporal Approach to Passive Sound Source Localization

A Spatiotemporal Approach to Passive Sound Source Localization A Spatiotemporal Approah Passive Sound Soure Loalization Pasi Pertilä, Mikko Parviainen, Teemu Korhonen and Ari Visa Institute of Signal Proessing Tampere University of Tehnology, P.O.Box 553, FIN-330,

More information

Elimination of Chaotic Ferroresonance in power transformers including Nonlinear Core Losses applying of Neutral Resistance

Elimination of Chaotic Ferroresonance in power transformers including Nonlinear Core Losses applying of Neutral Resistance Elimination of haoti Ferroresonane in power transformers inluding Nonlinear ore Losses applying of Neutral Resistane A.Abbasi M.Rostami H.Radmanesh H.Abbasi abbasi@shahed.a.ir Rostami@shahed.a.ir hamid.nsa@gmail.om

More information

On the Geometrical Conditions to Determine the Flat Behaviour of the Rotational Curves in Galaxies

On the Geometrical Conditions to Determine the Flat Behaviour of the Rotational Curves in Galaxies On the Geometrial Conditions to Determine the Flat Behaviour of the Rotational Curves in Galaxies Departamento de Físia, Universidade Estadual de Londrina, Londrina, PR, Brazil E-mail: andrenaves@gmail.om

More information

Lecture 7: September 19th, The following slides were derived from those prepared by Professor Oldham for EE40 in Fall 01. Version Date 9/19/01

Lecture 7: September 19th, The following slides were derived from those prepared by Professor Oldham for EE40 in Fall 01. Version Date 9/19/01 EES Intro. electronics for S Fall Lecture 7: September 9th, Lecture 7: 9/9/ A.. Neureuther Version Date 9/9/ harging and Discharging of ircuits (Transients) A) Mathematical Method B) EE Easy Method ) Logic

More information