Laboratory Manual Physics_1. Hall effect
|
|
- Sherilyn Powers
- 6 years ago
- Views:
Transcription
1 AG niversit of Siene an Tehnoog in Crao Department of etronis Laborator Manua Phsis_ Tite: 009 r. a effet periment No. 3
2 . Goa To etermine the sampe onutivit, a oeffiient, mobiit an onentration of arriers.. What to earn? Magneti fie. Magneti fore F. a effet. Current ensit. Drift spee. esistivit. Conutivit. Mirosopi vie of Ohm's a. The reationship beteen the eetri fie an potentia ifferene. etromagnet histeresis. 3. akgroun Consier a semionutor sampe pae in the magneti fie that is in the -iretion (Fig. ). I 0 v - Fig.. Sampe onfiguration in a a measurement set up. A retanguar bok is use as the sampe. Suppose e pass a urrent through that sampe perpeniuar to the magneti fie, sa in the -iretion. The harge arriers are eetrons an the rift ith rift spee v in the opposite iretion.. At the instant shon in Fig. a, an eterna magneti fie pointing out of the pane of the figure has just been turne out. Magneti fore F ats on eah rifting eetron, pushing it toar the eft ege of the sampe.
3 As time goes on, eetrons move to the eft piing up on the eft ege of the strip, eaving unompensate positive harges in fie positions at the right ege. The separation of positive an negative harges proues an eetri fie ithin the sampe pointing from right to eft (Fig. b). This fie ats an eetri fore F on eah eetron tening to push it to the eft. In an equiibrium, the eetri fore F baanes the magneti fore F so as to keep urrent foing aong the -iretion. F q F ev v F ( v ) (,0,0), ( 0,0, ) v q F e, (,0) 0 psurge of the eetria fie in the -iretion is ae a ffet. A a potentia ifferene is assoiate ith the eetri fie aross the sampe of ith as foos: Consiering the baane of fores on the harge arriers e see that : e ev The tota urrent ensit is aoring to the mirosopi Ohm s La ies: e j e ne j j ne j nev hih The a oeffiient is efine as: j ne Note that the sign of iniates if the sampe is n-tpe or p-tpe. When the arriers are eetrons, the a oeffiient is negative. When the arriers are hoes, the a oeffiient is 3
4 positive. The a oeffiient enabes aso estabishing the onentration of the arriers in the sampe n. Carrier onentration is the number or arriers per unit voume. I I - v - F F F Fig.. The iea of a effet etron veoit v is taken to var inear ith the fie : v µ hih is on true uner ohmi onition. The proportionait onstant beteen v an is µ mobiit - an it an be epresse as : µ v j ne j ne j j Votage is ae the onutivit votage i.e. votage beteen the ontats in the iretion of the urrent an is ae the a votage an it is the resutant votage beteen the ontats that are perpeniuar to the iretion of the urrent. The mobiit µ is use to epress onutivit σ neµ. Taking into aount the imensions of the sampe, the tota urrent is reate to the ensit of harge arriers n an their rift veoit v as: I j S j ( env )( ) 4
5 i.e. as the prout of the urrent ensit j an the ross-setiona area of the sampe S. Fina, e obtain the fooing epressions for the : µ σ j I I I σ neµ µ I 4. quipment etromagnet. a probe. Measurement pane ontaining DC poer supp to furnish urrent to a probe, votmeter of high input impeane to measure a votage, votmeters to measure onutivit votage an votmeter to measure votage aross the resistor 000 Ω ±Ω onnete in series ith the a probe. 5. Measurements Fig. 3 shos the measurement set-up. I Z V mv. mv Fig. 3. The measurement set-up. Fig. 4 shos the vie of the front of the measurement pane. eetromagnet. Fig. 5 shos the vie of 5
6 Fig. 4. Measurement pane Knob to set the iretion of urrent in ois Sith on/off Varia to ontro urrent in eetromagnet ois Fig. 5. etromagnet. Turn the measurement pane on (Fig. 4).. Push the knob an then set ith the oer potentiometer on the front of the measurement pane. The instrutor i hoose the ertain vaues of for our eperiment. 6
7 is a votage aross the resistor 000 Ω ±%, hih is onnete in series ith the a probe an it is use to auate urrent I foing through the a probe: I. 3. Turn the eetromagnet on (Fig. 5). Varia to ontro urrent in eetromagnet ois shou be set for ero urrent. 4. Set the iretion of urrent through the eetromagnet ois " to the right" using the knob ith a hite arro on the front of eetromagnet. 5. Push the knob an using the upper potentiometer on the front of the measurement pane set for ero. 6. Set the urrent through the eetromagnet ois for a ertain vaues given b the instrutor. Do not eee eetromagnet urrent of 6A. Aas graua inrease an erease urrent in eetromagnet ois. Large inutive votage surges ma amage the insuation of ois. 7. For ever setting of the urrent measure an votage using votmeters inue in the measurement pane. Push the knob an measure the a votage. Push the knob an measure the votage onutivit. 8. Derease the urrent in eetromagneti ois to ero an hange the iretion of urrent in ois "to the eft" using the knob ith hite arros on the front of eetromagnet. After this hange ajust a votage to ero using the upper potentiometer on the front of the measurement pane. 9. Set the urrent through the eetromagnet ois for the same vaues as in the point 7. For ever setting of the urrent measure an votage. 0. se the eetromagnet harateristi f(i em ) to estabish the magneti fie beteen the eetromagnet poes on the basis of urrent I em in eetromagnet ois (Fig. 6).. Write on the resuts in the Tabe. 7
8 6. Data haning. Write on the resuts in the Tabe. Dra the reationships: f( ), f( ), f( ) for eah that orrespons to I em,.5,,.5, 3.0, 3.5, 4.0 A, respetive. 3. For eah reationship fin the "best fit" straight ine through the ata using the inear regression metho, fin the regression oeffiients of the ine a an b an the unertainties of oeffiients a an b. 4. Fin the arrier mobiit µ, a oeffiient an onutivit σ of the a probe using the reationships: µ σ an the proper inear regression equations. e arefu: use the one parameter inear regression (b0) 5. Fin the onentration of arriers n on the basis of the reationship 6. Cauate the unertainties µ,, σ, n.. ne Literature:. aia, esnik Funamentas of Phsis - 8 th eition, John Wie 007, 8
9 Tabe. esuts [V] I em [A] [Wb/m] [mv] [mv] [mv] [mv] [mv] [mv] 4,5,5 3 3,5 4 5,5,5 3 3,5 4 6,5,5 3 3,5 4 +, + Dimensions of the a probe: (3,7 ± 0,) 0 3 m, (,7 ± 0,) 0 3 m, (,5 ± 0,) 0 3 m, 0 (,4 ± 0,) 0 3 m. 9
10 etromagnet harateristi f(i em ) 0,45 0,4 0,35 0,3 [Wb/m ] 0,5 0, 0,5 0, I em [A] Fig. 6. etromagnet harateristi 0
11 6. ints to the report.. f( ) for onst. On the basis of Tabe reate the sub-tabe: I em [A] A [mv] [mv] µ [...].. Wb/m µ [...] µ Dra the pot f( ). Fin the regression oeffiient a an the unertaint σ a for these ata. se the one parameter inear regression (b0) Compare the sopes: a µ a µ µ a [ m] m m Fin the unit of µ: [ µ ] Wb Wb Vs m m Cauate the unertaint µ/µ using the metho of ogarithmi erivative: µ a Cauate ogarithm of the both sies of the equation: n µ n a + n n n Derivate both sies of the equation: µ µ a a here: a σ a is the unertaint of the regression oeffiient a 3 3 0, 0 m, b 0, 0 m are the geometria unertainties of the probe,
12 is the unertaint of the estabishe on the basis of the eetromagnet harateristi. ui-up suh sub-tabes for eah vaues of I em,.5,,.5, 3.0, 3.5, 4.0 A an respetive. Cauate µ an µ/µ in eah ase an oet the resuts in one fina tabe [Wb/m] µ [...] µ [...] µ.. f( ) for onst. On the basis of Tabe reate the sub-tabe: I em [A] A [mv] [mv] Η [...].. Wb/m [...] Dra the pot f( ). Fin the regression oeffiient a an the unertaint σ a for these ata. se the one parameter inear regression (b0). Compare the sopes: a a a Fin the unit of. Cauate the unertaint of / using the metho of ogarithmi erivative: ui-up suh sub-tabes for eah vaues of I em,.5,,.5, 3.0, 3.5, 4.0 A an respetive. Cauate an / in eah ase an oet the resuts in one fina tabe
13 [Wb/m ] [...] / [...] 3. f( _average ) On the basis of Tabe reate the subtabe: I em [A] A [mv] [mv] σ [...].. Wb/m σ [...] σ Dra the pot f( ). Fin the regression oeffiient a an the unertaint σ a for these ata. se the one parameter inear regression (b0) Compare the sopes: a σ a σ a σ Fin the unit of σ. Cauate the unertaint of σ /σ using the metho of ogarithmi erivative: ui-up suh sub-tabes for eah vaues of I em,.5,,.5, 3.0, 3.5, 4.0 A an respetive. Cauate an / in eah ase an oet the resuts in one fina tabe [Wb/m ] σ [...] σ /σ[...] 3
14 4. n e emember: e C. Determine the unit of n. Cauate the unertaint n using the tota ifferentia metho: n δn δ Coet the resuts in the fina tabe: [Wb/m ] n [...] n [...] pate: , b arbara Diuria 4
Chapter 2: One-dimensional Steady State Conduction
1 Chapter : One-imensional Steay State Conution.1 Eamples of One-imensional Conution Eample.1: Plate with Energy Generation an Variable Conutivity Sine k is variable it must remain insie the ifferentiation
More informationCSIR-UGC NET/JRF JUNE - 6 PHYSICAL SCIENCES OOKLET - [A] PART. The raius of onvergene of the Taylor series epansion of the funtion (). The value of the ontour integral the anti-lokwise iretion, is 4z e
More informationThe Square of the Dirichlet-to-Neumann map equals minus Laplacian
The Square of the Dirihet-to-Neumann map equas minus Lapaian D V Ingerman Abstrat. The Dirihet-to-Neumann maps onnet boundary vaues of harmoni funtions. It is an amazing fat that the square of the non-oa
More informationMath 225B: Differential Geometry, Homework 6
ath 225B: Differential Geometry, Homework 6 Ian Coley February 13, 214 Problem 8.7. Let ω be a 1-form on a manifol. Suppose that ω = for every lose urve in. Show that ω is exat. We laim that this onition
More informationMoment - Axial Force Interaction Report and Program
oment - Aia Fore Interation Report and rogram ehdi Vojoudi Vojoudi@vojoudi.om THINK GLOBAL, ACT LOCAL Spring 3 Strutura Stabiity rojet. Sope Cauate the moment aia fore interation urve for a hinged oumn
More informationSupporting Information
Supporting Information Multiple-beam interferene enable broaban metamaterial wave plates Junhao Li, Huijie Guo, Tao Xu, 3 Lin Chen,, * Zhihong Hang, 3 Lei Zhou, an Shuqi Chen 4 Wuhan National Laborator
More informationSure Shot 2016 Electric Current By M K Ezaz
Sure Shot 06 Eectric Current B M K Ezaz. A 0 V batter of negigibe interna resistance is connected across a 00 V batter and a resistance of 38 Ω. Find the vaue of the current in circuit. () E 00 0 A: I
More informationELECTROCHEMISTRY Lecture/Lession Plan -1
Chapter 4 ELECTROCHEMISTRY Leture/Lession Plan -1 ELECTROCHEMISTRY 4.1 Conept of eletrohemistry Eletrohemistry is a branh of hemistry where we will study how hemial energy an be transformed into eletrial
More informationCAPACITANCE AND INDUCTANCE
APAITANE AND INDUTANE Inroduces wo passive, energy soring devices: apaciors and Inducors APAITORS Sore energy in heir elecric field (elecrosaic energy) Model as circui elemen INDUTORS Sore energy in heir
More informationChapter 26 - Capacitance
Chapter 26 Capacitance Probem Set #5 ue: Ch 26 2, 3, 5, 7, 9, 5, 22, 26, 29, 6, 63, 64 The ieas of energy storage in fies can be carrie a step further by unerstaning the concept of "Capacitance." Lecture
More informationMass Transfer 2. Diffusion in Dilute Solutions
Mass Transfer. iffusion in ilute Solutions. iffusion aross thin films and membranes. iffusion into a semi-infinite slab (strength of weld, tooth deay).3 Eamples.4 ilute diffusion and onvetion Graham (85)
More informationThe numbers inside a matrix are called the elements or entries of the matrix.
Chapter Review of Matries. Definitions A matrix is a retangular array of numers of the form a a a 3 a n a a a 3 a n a 3 a 3 a 33 a 3n..... a m a m a m3 a mn We usually use apital letters (for example,
More informationSTRUCTURE AND ELECTRICAL PROPERTIES OF ELECTRON IRRADIATED CdSe THIN FILMS
Journal of Optoeletronis an Avane Materials ol. 6, o. 1, Marh 24, p. 113-119 STRUCTURE AD ELECTRICAL PROPERTIES OF ELECTRO IRRADIATED C THI FILMS L. Ion a*, S. Antohe a, M. Popesu b, F. Sarlat, F. Sava
More informationExtended Spectral Nonlinear Conjugate Gradient methods for solving unconstrained problems
International Journal of All Researh Euation an Sientifi Methos IJARESM ISSN: 55-6 Volume Issue 5 May-0 Extene Spetral Nonlinear Conjuate Graient methos for solvin unonstraine problems Dr Basim A Hassan
More informationENGINE CONTROL (1MZ-FE)
ENGINE ONTRO (MZ-FE) SSTEM OUTINE THIS SSTEM UTIIZES N ENGINE ONTRO MOUE N MINTINS OVER ONTRO OF THE ENGINE, TRNSMISSION N SO ON. N OUTINE OF THE ENGINE ONTRO IS EPINE HERE.. INPUT SIGNS ( ) ENGINE OONT
More information1 st Meetng of EcosimPro Users, UNED, Madrid, 3-4 May 2001 C7 MODELLING AND SIMULATION OF DISTRIBUTED PROCESSES: DIFFUSERS IN THE SUGAR INDUSTRY
C7 MODELLING AND SIMULATION OF DISTRIBUTED PROCESSES: DIFFUSERS IN THE SUGAR INDUSTRY Merino Gómez, Alejanro Centro e Tenología Azuarera. Universia e Vallaoli C/ Real e Burgos. Eifiio Alfonso VIII. Planta
More informationDeveloping a Convenient Balance Beam for Unknown Loads
Deveoping a Convenient Baane Bea for Unknon s Keon Young Yi* Assoiate Professor Yong Jun Ki* Graduate student Sa Yong Chung** Tea Leader Song Soo Han** Senior Researher/Ph.D Sang Heon Lee** Senior Researher/Ph.D
More information1. A dependent variable is also known as a(n). a. explanatory variable b. control variable c. predictor variable d. response variable ANSWER:
1. A epenent variale is also known as a(n). a. explanatory variale. ontrol variale. preitor variale. response variale FEEDBACK: A epenent variale is known as a response variale. Definition of the Simple
More informationStrain Energy in Linear Elastic Solids
Strain Energ in Linear Eastic Soids CEE L. Uncertaint, Design, and Optimiation Department of Civi and Environmenta Engineering Duke Universit Henri P. Gavin Spring, 5 Consider a force, F i, appied gradua
More informationSeveral Rules about the Magnetic Moment of Rotational Charged Bodies
IES ONLINE, VOL. 3, NO. 6, 007 81 Severa ues about the Magnetic Moment of otationa Charged Bodies Guo-Quan Zhou Department of hsics, Wuhan Universit, Wuhan 43007, China Abstract A strict and deicate anaog
More informationMeasuring & Inducing Neural Activity Using Extracellular Fields I: Inverse systems approach
Measuring & Induing Neural Ativity Using Extraellular Fields I: Inverse systems approah Keith Dillon Department of Eletrial and Computer Engineering University of California San Diego 9500 Gilman Dr. La
More informationChapter 2 Lecture 5 Longitudinal stick fixed static stability and control 2 Topics
hapter 2 eture 5 ongitudinal stik fied stati stability and ontrol 2 Topis 2.2 mg and mα as sum of the ontributions of various omponent 2.3 ontributions of ing to mg and mα 2.3.1 orretion to mα for effets
More informationPN Code Tracking Loops
Wireless Information Transmission System Lab. PN Coe Traking Loops Institute of Communiations Engineering National Sun Yat-sen University Introution Coe synhronization is generally arrie out in two steps
More information= 1 u 6x 2 4 2x 3 4x + 5. d dv (3v2 + 9v) = 6v v + 9 3v 2 + 9v dx = ln 3v2 + 9v + C. dy dx ay = eax.
Math 220- Mock Eam Soutions. Fin the erivative of n(2 3 4 + 5). To fin the erivative of n(2 3 4+5) we are going to have to use the chain rue. Let u = 2 3 4+5, then u = 62 4. (n(2 3 4 + 5) = (nu) u u (
More informationDevelopment of Truss Equations
MANE & CIV Introuction to Finite Eeents Prof. Suvranu De Deveopent of Truss Equations Reaing assignent: Chapter : Sections.-.9 + ecture notes Suar: Stiffness atri of a bar/truss eeent Coorinate transforation
More informationVariable Impedance Control with an Artificial Muscle Manipulator Using Instantaneous Force and MR Brake
1 IEEE/RSJ International Conferene on Intelligent Robots an Systems (IROS) November -7, 1. Tokyo, Japan ariable Impeane Control with an Artifiial Musle Manipulator Using Instantaneous Fore an MR Brake
More informationMCG 3341 FLUID MECHANICS II LABORATORY MANUAL
MG 334 UI MEHANIS II ABORATORY MANUA January Professor S. Tavoularis epartment of Mehanial Engineering University of Ottawa MG 334 UI MEHANIS II / aboratory Manual / Professor S. Tavoularis /p.. Objetive
More informationAO NO 'e~.0. c;;:o~
Bt 6 9 PG Subitted by: hairan of the Asseby at the Request of the Mayor Prepared by: Anhorage ater & ' aeak's OFFE Da te: pj9 4 5 6 7 9 4 5 6 7 9 4 5 6 7 9 4 5 6 7 9 4 4 Utiity Oh't For reading : SEPTEMBER
More informationGeneral Equilibrium. What happens to cause a reaction to come to equilibrium?
General Equilibrium Chemial Equilibrium Most hemial reations that are enountered are reversible. In other words, they go fairly easily in either the forward or reverse diretions. The thing to remember
More informationECE Microwave Engineering
ECE 5317-6351 Mirowave Engineering Aapte from notes by Prof. Jeffery T. Williams Fall 18 Prof. Davi R. Jakson Dept. of ECE Notes 7 Waveguiing Strutures Part : Attenuation ε, µσ, 1 Attenuation on Waveguiing
More informationAnalytic Model for Area-Constrained Optimal Repeater Insertion
Anayti Mode for Area-Constrained Optima Repeater Insertion G.S. Garea, N.P. van der Meijs and R.H.J.M Otten* Eetria Engineering / CAS Deft University of Tehnoogy Deft, The Netherands *Eindhoven University
More informationClass 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 informationCAPACITANCE AND INDUCTANCE
APAITANE AND INDUTANE Inroduces wo passive, energy soring devices: apaciors and Inducors EARNING GOAS APAITORS Sore energy in heir elecric field (elecrosaic energy) Model as circui elemen INDUTORS Sore
More informationPhysicsAndMathsTutor.com
. Two points A and B ie on a smooth horizonta tabe with AB = a. One end of a ight eastic spring, of natura ength a and moduus of easticity mg, is attached to A. The other end of the spring is attached
More information2 Parallel-Plate Transmission Line (Geometric Model) = c Assume it s a plane wave propagate in the z with polarization in y direction. d dz ~ ˆ.
Tansmission ines 1 ntoution When the soue aiates in a ie aea, the eneg speas out. The aiate eneg is not guie an the tansmission of eneg though aiation is ineffiient. Dietive antenna oul have huge imensions
More informationInterim Exam 1 5AIB0 Sensing, Computing, Actuating , Location AUD 11
Interim Exam 1 5AIB0 Sensing, Computing, Actuating 3-5-2015, 14.00-15.00 Location AUD 11 Name: ID: This interim exam consists of 1 question for which you can score at most 30 points. The fina grade for
More informationVersion 2.2 NE03 - Faraday's Law of Induction
Definition Version. Laboratory Manua Department of Physics he University of Hong Kong Aims o demonstrate various properties of Faraday s Law such as: 1. Verify the aw.. Demonstrate the ighty damped osciation
More information"Research Note" ANALYSIS AND OPTIMIZATION OF A FISSION CHAMBER DETECTOR USING MCNP4C AND SRIM MONTE CARLO CODES *
Iranian Journal of Siene & Tehnology, Transation A, Vol. 33, o. A3 Printed in the Islami Republi of Iran, 9 Shiraz University "Researh ote" AALYSIS AD OPTIMIZATIO OF A FISSIO CHAMBER DETECTOR USIG MCP4C
More information15. MAGNETIC EFFECT OF ELECTRIC CURRENT
15. MAGNETIC EFFECT OF ELECTRIC CURRENT HOMEWORK SOLUTIONS 1. Given : Effetive area, na 0.121 m 2 na 1.21 x -1 m 2 B -4 Wb/m 2 i 0 ma i -1 A τ D? τ D niab Defleting torque ating on MCG is τ D niab τ D
More informationMC74VHC574. Octal D Type Flip Flop with 3 State Output. ON Semiconductor
ON Semiconductor Octal Type Flip Flop with 3 State Output The M74H574 is an advanced high speed MOS octal flip flip with 3 state output fabricated with silicon gate MOS technology. It achieves high speed
More informationField dependence of magnetic susceptibility of crystals under conditions of degeneracy of their electron energy bands
Engish transation of our paper pubished in Fiz. Nizk. Temp. This transation orrets that made in Low Temp. Phys., 58-59 (1996). Fied dependene of magneti suseptibiity of rystas under onditions of degeneray
More informationChemical Kinetics Part 2. Chapter 16
Chemica Kinetics Part 2 Chapter 16 Integrated Rate Laws The rate aw we have discussed thus far is the differentia rate aw. Let us consider the very simpe reaction: a A à products The differentia rate reates
More informationDetermination the Invert Level of a Stilling Basin to Control Hydraulic Jump
Global Avane Researh Journal of Agriultural Siene Vol. (4) pp. 074-079, June, 0 Available online http://garj.org/garjas/inex.htm Copyright 0 Global Avane Researh Journals Full Length Researh Paper Determination
More informationPractical Approach to Polymer Electrolyte Fuel Cell Modeling
39 Researh Report Pratia Approah to Poymer Eetroyte Fue Ce odeing Haruhiko Yamada, Yu orimoto A simpe simuation method to predit the urrent distribution in a poymer eetroyte fue e is presented. This method
More informationVITA FIELDS OF STUDY. Computer-Aided Design. Modeling and Simulation of Cam Mechanisms
ACKNOWLEDGEMEN VIA September, 96 Born Haimen, Jiang Su Provine, China 983 B.S.M.E. Mehania Engineering East China Universit of Metaurg Ma An Shan, China 983-985 Assistant East China Universit of Metaurg
More informationA 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 informationChemical Kinetics Part 2
Integrated Rate Laws Chemica Kinetics Part 2 The rate aw we have discussed thus far is the differentia rate aw. Let us consider the very simpe reaction: a A à products The differentia rate reates the rate
More informationMetal: a free electron gas model. Drude theory: simplest model for metals Sommerfeld theory: classical mechanics quantum mechanics
Metal: a free eletron gas model Drude theory: simplest model for metals Sommerfeld theory: lassial mehanis quantum mehanis Drude model in a nutshell Simplest model for metal Consider kinetis for eletrons
More informationLongitudinal Static Stability
ongitudinal Stati Stability Some definitions C m M V S pithing moment without dimensions (so without influene of ρ, V and S) it is a shape parameter whih varies with the angle of attak. Note the hord in
More informationCandidate Number. General Certificate of Education Advanced Level Examination June 2010
Centre Number Surname Candidate Number For Examiner s Use Other Names Candidate Signature Examiner s Initias Genera Certificate of Education Advanced Leve Examination June 2010 Question 1 2 Mark Physics
More informationRELUCTANCE The resistance of a material to the flow of charge (current) is determined for electric circuits by the equation
INTRODUCTION Magnetism pays an integra part in amost every eectrica device used today in industry, research, or the home. Generators, motors, transformers, circuit breakers, teevisions, computers, tape
More informationA NEW KIRCHHOFF PLATE MODEL BASED ON A MODIFIED COUPLE STRESS THEORY
7 th GRACM Internationa Congress on Computationa Mehanis Athens, 30 June Ju 0 A NEW KIRCHHOFF PLATE MODEL BASED ON A MODIFIED COUPLE STRESS THEORY George C. Tsiatas Shoo of Civi Engineering Nationa Tehnia
More informationarxiv: v1 [math-ph] 19 Apr 2009
arxiv:0904.933v1 [math-ph] 19 Apr 009 The relativisti mehanis in a nonholonomi setting: A unifie approah to partiles with non-zero mass an massless partiles. Olga Krupková an Jana Musilová Deember 008
More informationI. Aim of the experiment
Task VIII TRAUBE S RULE I. Aim of the eperiment The purpose of this task is to verify the Traube s rule for a homologous series of apillary ative substane solutions (i.e. alohols or arboyli aids) on the
More informationMining Statistically Significant Attribute Associations in Attributed Graphs
Mining Statistiall Signifiant Attriute Assoiations in Attriute Graphs Jihan Lee Department of Computer Siene Purue Universit West Lafaette, IN Email: jihan@purue.eu Keehan Park Department of Computer Siene
More informationExperiment 3: Basic Electronic Circuits II (tbc 1/7/2007)
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
More informationFour-dimensional equation of motion for viscous compressible substance with regard to the acceleration field, pressure field and dissipation field
Four-dimensional equation of motion for visous ompressible substane with regard to the aeleration field, pressure field and dissipation field Sergey G. Fedosin PO box 6488, Sviazeva str. -79, Perm, Russia
More informationChapter 15 Chemical Equilibrium
Chapter 5 Chemial Equilibrium 5. The Conept of Equilibrium Figure: 3. from Chemistry by MMurray & Fey Figure 3.(a) NO 4( g) NO( g) olorless brown we start with reatant, N O 4, so the solution is olorless
More informationThe gravitational phenomena without the curved spacetime
The gravitational phenomena without the urved spaetime Mirosław J. Kubiak Abstrat: In this paper was presented a desription of the gravitational phenomena in the new medium, different than the urved spaetime,
More information14 - OSCILLATIONS Page 1
14 - OSCILLATIONS Page 1 14.1 Perioic an Osciator otion Motion of a sste at reguar interva of tie on a efinite path about a efinite point is known as a perioic otion, e.g., unifor circuar otion of a partice.
More informationIn Coulomb gauge, the vector potential is then given by
Physics 505 Fa 007 Homework Assignment #8 Soutions Textbook probems: Ch. 5: 5.13, 5.14, 5.15, 5.16 5.13 A sphere of raius a carries a uniform surface-charge istribution σ. The sphere is rotate about a
More informationSensitivity analysis for linear optimization problem with fuzzy data in the objective function
Sensitivity analysis for linear optimization problem with fuzzy data in the objetive funtion Stephan Dempe, Tatiana Starostina May 5, 2004 Abstrat Linear programming problems with fuzzy oeffiients in the
More informationOn the Reverse Problem of Fechnerian Scaling
On the Reverse Prolem of Fehnerian Saling Ehtiar N. Dzhafarov Astrat Fehnerian Saling imposes metris on two sets of stimuli relate to eah other y a isrimination funtion sujet to Regular Minimality. The
More informationOn the sustainability of collusion in Bertrand supergames with discrete pricing and nonlinear demand
PRA unih Personal RePE Arhive On the sustainability of ollusion in Bertran supergames with isrete priing an nonlinear eman Paul R. Zimmerman US Feeral Trae Commission 25. January 2010 Online at http://mpra.ub.uni-muenhen.e/20249/
More informationSensitivity Analysis of Resonant Circuits
1 Sensitivity Analysis of Resonant Ciruits Olivier Buu Abstrat We use first-orer perturbation theory to provie a loal linear relation between the iruit parameters an the poles of an RLC network. The sensitivity
More informationCandidate Number. General Certificate of Education Advanced Level Examination January 2012
entre Number andidate Number Surname Other Names andidate Signature Genera ertificate of Education dvanced Leve Examination January 212 Physics PHY4/1 Unit 4 Fieds and Further Mechanics Section Tuesday
More informationRadiation processes and mechanisms in astrophysics 3. R Subrahmanyan Notes on ATA lectures at UWA, Perth 22 May 2009
Radiation proesses and mehanisms in astrophysis R Subrahmanyan Notes on ATA letures at UWA, Perth May 009 Synhrotron radiation - 1 Synhrotron radiation emerges from eletrons moving with relativisti speeds
More informationSome Useful Results for Spherical and General Displacements
E 5 Fall 997 V. Kumar Some Useful Results for Spherial an General Displaements. Spherial Displaements.. Eulers heorem We have seen that a spherial isplaement or a pure rotation is esribe by a 3 3 rotation
More informationPerformance Evaluation of atall Building with Damped Outriggers Ping TAN
Performane Evaluation of atall Builing with Dampe Outriggers Ping TAN Earthquake Engineering Researh an Test Center Guangzhou University, Guangzhou, China OUTLINES RESEARCH BACKGROUND IMPROVED ANALYTICAL
More informationPHYSICS 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 informationChapter 9. There are 7 out of 50 measurements that are greater than or equal to 5.1; therefore, the fraction of the
Pratie questions 6 1 a y i = 6 µ = = 1 i = 1 y i µ i = 1 ( ) = 95 = s n 95 555. x i f i 1 1+ + 5+ n + 5 5 + n µ = = = f 11+ n 11+ n i 7 + n = 5 + n = 6n n = a Time (minutes) 1.6.1.6.1.6.1.6 5.1 5.6 6.1
More informationRelated Topics Maxwell s equations, electrical eddy field, magnetic field of coils, coil, magnetic flux, induced voltage
Magnetic induction TEP Reated Topics Maxwe s equations, eectrica eddy fied, magnetic fied of cois, coi, magnetic fux, induced votage Principe A magnetic fied of variabe frequency and varying strength is
More informationarxiv: v1 [math.mg] 17 Jun 2008
arxiv:86.789v [math.mg] 7 Jun 8 Chromogeometr an reativistic conics N J Wiberger Schoo of Mathematics an Statistics UNSW Sne 5 ustraia This paper shows how a recent reformuation of the basics of cassica
More information(Specifications A and B)
Centre Number Surname Candidate Number For Examiner s Use Other Names Candidate Signature Examiner s Initias Genera Certificate of Education Advanced Subsidiary Examination June 2011 Question 1 2 Mark
More informationTRANSMISSION 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 informationTHE EQUATION CONSIDERING CONCRETE STRENGTH AND STIRRUPS FOR DIAGONAL COMPRESSIVE CAPACITY OF RC BEAM
- Tehnial Paper - THE EQUATION CONSIDERING CONCRETE STRENGTH AND STIRRUPS FOR DIAGONAL COMPRESSIE CAPACITY OF RC BEAM Patarapol TANTIPIDOK *, Koji MATSUMOTO *, Ken WATANABE *3 and Junihiro NIWA *4 ABSTRACT
More informationElements of Kinetic Theory
Eements of Kinetic Theory Statistica mechanics Genera description computation of macroscopic quantities Equiibrium: Detaied Baance/ Equipartition Fuctuations Diffusion Mean free path Brownian motion Diffusion
More informationτ = 10 seconds . In a non-relativistic N 1 = N The muon survival is given by the law of radioactive decay N(t)=N exp /.
Muons on the moon Time ilation using ot prouts Time ilation using Lorentz boosts Cheking the etor formula Relatiisti aition of eloities Why you an t eee the spee of light by suessie boosts Doppler shifts
More informationAn Integer Solution of Fractional Programming Problem
Gen. Math. Notes, Vol. 4, No., June 0, pp. -9 ISSN 9-784; Copyright ICSRS Publiation, 0 www.i-srs.org Available free online at http://www.geman.in An Integer Solution of Frational Programming Problem S.C.
More informationThe 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 informationChapter 15: Chemical Equilibrium
Chapter 5: Chemial Equilibrium ahoot!. At eq, the rate of the forward reation is the rate of the reverse reation. equal to, slower than, faster than, the reverse of. Selet the statement that BEST desribes
More informationAnnouncements. Office Hours Swap: OH schedule has been updated to reflect this.
SA Solving Announements Offie Hours Swap: Zavain has offie hours from 4-6PM toay in builing 460, room 040A. Rose has offie hours tonight from 7-9PM in Gates B26B. Keith has offie hours hursay from 2-4PM
More informationReview for Exam #2. Specific Heat, Thermal Conductivity, and Thermal Diffusivity. Conduction
Review for Exam # Speifi Heat, Thermal Condutivity, and Thermal Diffusivity Speifi heat ( p ) A measure of how muh energy is required to raise the temperature of an objet Thermal ondutivity (k) A measure
More informationHong Xu. School of Business and Management, Hong Kong University of Science and Technology, Clearwater Bay, Kowloon, HONG KONG
RESEARCH ARTICLE IDETITY MAAGEMET AD TRADABLE REPUTATIO Hong Xu Scoo of Business an Management, Hong Kong University of Science an Tecnoogy, Cearater Bay, Kooon, HOG KOG {xu@ust.} Jianqing Cen Jina Scoo
More informationECE507 - Plasma Physics and Applications
ECE57 - Plasma Phsis and Appliations Leture 4 Prof. Jorge Roa and Dr. Fernando Tomasel Department of Eletrial and Computer Engineering Constant, uniform Let s align with the -ais, so = k. Then we an write
More informationMC74VHC574. Octal D-Type Flip-Flop with 3-State Output
M74H574 Octal -Type Flip-Flop with 3-State Output The M74H574 is an advanced high speed MOS octal flip flip with 3 state output fabricated with silicon gate MOS technology. It achieves high speed operation
More informationTowards an Absolute Cosmic Distance Gauge by using Redshift Spectra from Light Fatigue.
Towards an Absolute Cosmi Distane Gauge by using Redshift Spetra from Light Fatigue. Desribed by using the Maxwell Analogy for Gravitation. T. De Mees - thierrydemees @ pandora.be Abstrat Light is an eletromagneti
More informationEXPERIMENT 5 MOLAR CONDUCTIVITIES OF AQUEOUS ELECTROLYTES
EXPERIMENT 5 MOLR CONDUCTIVITIES OF QUEOUS ELECTROLYTES Objective: To determine the conductivity of various acid and the dissociation constant, K for acetic acid a Theory. Eectrica conductivity in soutions
More informationELECTROMAGNETIC WAVES WITH NONLINEAR DISPERSION LAW. P. М. Меdnis
ELECTROMAGNETIC WAVES WITH NONLINEAR DISPERSION LAW P. М. Меdnis Novosibirs State Pedagogial University, Chair of the General and Theoretial Physis, Russia, 636, Novosibirs,Viljujsy, 8 e-mail: pmednis@inbox.ru
More informationThe homopolar generator: an analytical example
The homopolar generator: an analytial example Hendrik van Hees August 7, 214 1 Introdution It is surprising that the homopolar generator, invented in one of Faraday s ingenious experiments in 1831, still
More informationQ c, Q f denote the outputs of good C and F, respectively. The resource constraints are: T since the technology implies: Tc = Qc
Fall 2008 Eon 455 Ansers - Problem Set 3 Harvey Lapan 1. Consider a simpliied version o the Heksher-Ohlin model ith the olloing tehnology: To produe loth: three units o labor and one unit o land are required
More informationBrazilian Journal of Physics ISSN: Sociedade Brasileira de Física Brasil
Brazilian Journal of Physis ISSN: 3-9733 luizno.bj@gmail.om Soieae Brasileira e Físia Brasil Araujo, Vanilse S.; Coutinho, F.A.B.; Perez, J. Fernano On the elta funtion normalization of the wave funtions
More informationClassical Diamagnetism and the Satellite Paradox
Classial Diamagnetism and the Satellite Paradox 1 Problem Kirk T. MDonald Joseph Henry Laboratories, Prineton University, Prineton, NJ 08544 (November 1, 008) In typial models of lassial diamagnetism (see,
More informationDetermination of the reaction order
5/7/07 A quote of the wee (or amel of the wee): Apply yourself. Get all the eduation you an, but then... do something. Don't just stand there, mae it happen. Lee Iaoa Physial Chemistry GTM/5 reation order
More informationThe optimization of kinematical response of gear transmission
Proeeings of the 7 WSEAS Int. Conferene on Ciruits, Systems, Signal an Teleommuniations, Gol Coast, Australia, January 7-9, 7 The optimization of inematial response of gear transmission VINCENZO NIOLA
More informationHorizontal Distribution of Forces to Individual Shear Walls
Horizontal Distribtion of Fores to ndividal Shear Walls nteration of Shear Walls ith Eah Other n the shon figre the slabs at as horizontal diaphragms etending beteen antilever alls and the are epeted to
More informationName Solutions to Test 1 September 23, 2016
Name Solutions to Test 1 September 3, 016 This test onsists of three parts. Please note that in parts II and III, you an skip one question of those offered. Possibly useful formulas: F qequb x xvt E Evpx
More information(Refer Slide Time: 2:34) L C V
Microwave Integrated Circuits Professor Jayanta Mukherjee Department of Eectrica Engineering Indian Intitute of Technoogy Bombay Modue 1 Lecture No 2 Refection Coefficient, SWR, Smith Chart. Heo wecome
More informationA New Hybrid Synchronous Machine Capable of Ultra-High Output Power.
A New Hybri Synhronous Mahine Capable o Ultra-High Output ower. L.U. Anih, h.d. *, C.U. Ogbuka, M.Eng., an M. Ewelum, B.Teh. Department o Eletrial Engineering, University o Nigeria, Nsukka, Nigeria. Department
More informationTransport Cost and Optimal Number of Public Facilities
Transport Cost an Optima Number of Pubic Faciities Kazuo Yamaguchi Grauate Schoo of Economics, University of Tokyo June 14, 2006 Abstract We consier the number an ocation probem of pubic faciities without
More information