Technical Information

Size: px
Start display at page:

Download "Technical Information"

Transcription

1

2 Technica Infomation BECKER Designation Diamon Gaes TFC IO Designation PD Desciption oi poycystaine CVD-iamon without bine an without cabie einfocement, pefect cutting ege shapness an cutting eges without any micoamage. No cutting pessue an smaest toeances. Highest wea esistance an vey high thema conuctivity (HC an HPC), highe toughness. Appication Fom supe-finishing to semifinishing of a non-feous metas an non-feous composites with high content of abasive einfocement o siicon. PDC DP Compoun Poycystaine iamon (compoun cutting mateia), cabie einfoce iamon of fine git size, goo cutting ege shapness an ow cutting pessue aowing fo mino toeances. Lowe wea esistance at highe toughness. Finishing of a non-feous metas an non-metaics with ow content of abasive einfocement o siicon. PDC- DP Compoun Poycystaine iamon (compoun cutting mateia), cabie einfoce iamon of coase git size, goo ege shapness an ow cutting pessue aowing fo mino toeances. Iea fo miing. Lowe wea esistance at highe toughness. Finishing an miing of a nonfeous an non-metaics with meium content of abasive einfocement o siicon. PDC-CU- DP Compoun oi poycystaine iamon (compoun cutting mateia) without cabie einfocement, coase git size, goo cutting ege shapness an ow cutting pessue aowing fo mino toeances. We suite fo miing toos with high epth of cut. High wea esistance at highe toughness ue to age iamon voume. Finishing an miing of a nonfeous metas an non-metaics with high content of abasive einfocement o siicon. Chipbeake Designation Appication Chipbeake Cutting Infomation CB1 CB2 Meium to finish machining with ow cutting foces fo ow bu, high toeance, high suface quaity. Genea pupose machining. tong, shap cutting ege fo high epths of cut an fee ates poucing goo suface quaity. Raius D.O.C. (ap) Min. - Max. FEED (ip) Min. - Max " 0.002" " " " 0.008" " " " " 0.016" 0.004" " 0.003" " 0.031" 0.006" " 0.003" " 0.047" 0.012" " " " 0.004" " 0.020" " 0.003" " 0.016" 0.024" " 0.003" " 0.031" 0.028" " 0.006" " 0.047" 0.032" " 0.008" " pee Infomation Mateias TFC (Vc : FM) PDC (Vc : FM) PDC- (Vc : FM) PDC-CU- (Vc : FM) Non-feous metas, auminum aoys without siicon Non-feous metas, auminum aoys with ess than 12% siicon Non-feous metas, auminum aoys with moe than 12 % siicon Bass, bonze, coppe, coppe aoys, pecious metas Non-metaics, pue pastics without einfocements Non-metaics, pastics with einfocements

3 BECKER DIAMOND TOOL of Gemany intouces evoutionay 3D PCD chipbeaking technoogy fo the machining of non-feous mateias. Though the use of avance popietay technoogy, tue 3D PCD chipbeake foms ae pouce at the cutting point of the PCD segment. The pefomance esuts of this amatic innovation, which is avaiabe in oughing an finishing foms, ae unsupasse chip conto an amaticay incease too ife. The highe shea anges integate within the chipbeake pouces owe cutting pessues an ess heat expansion of the wokpiece. The by-pouct of this machining ynamic is pecise imensiona accuacy, eiminating the nee fo seconay opeations whie both inceasing pouctivity an eucing opeating costs. The contoe shot chips coming off the wokpiece aow fo uninteupte pouction uns an pacticay eiminates costy maintenance stoppages taitionay equie when ceaing machines of ong uncontoe swaf. CCGT-CB1 Positive Neuta (with Chip Conto) TFC PDC PDC- PDC-CU- CCGT CB g g CCGT CB g g CCGT CB g g CCGT CB g CCGT CB g g CCGT CB g CCGT-431-CB g CCGT-432-CB g CCGT-CB1 Positive Neuta (with Chip Conto) TFC PDC PDC- PDC-CU- ¹ ¹ CCGT W-CB1* g CCGT-21.51W-CB1* g g CCGT W-CB1* g CCGT-32.51W-CB1* g g CCGT-430.5W-CB1* g CCGT-431W-CB1* g g *= 95 Hoe CCGT-CB2 Positive Neuta (with Chip Conto) TFC PDC PDC- PDC-CU- CCGT CB g g CCGT CB g g g CCGT CB g g CCGT CB g g CCGT CB g g CCGT CB g g CCGT-431-CB g g CCGT-432-CB g g CCGT-CB2 Positive Neuta (with Chip Conto) TFC PDC PDC- PDC-CU- *= 95 Hoe ¹ ¹ CCGT W-CB2* g g g CCGT-21.51W-CB2* g g g CCGT W-CB2* g g g CCGT-32.51W-CB2* g g g CCGT-430.5W-CB2* g g g CCGT-431W-CB2* g g g

4 CCGW Neuta (Fat Top Inset) TFC PDC PDC- PDC-CU- CCGW g g CCGW g g g g CCGW g g g g CCGW g CCGW g g g CCGW g g g g CCGW g g g CCGW Neuta (Fat Top Inset) TFC PDC PDC- PDC-CU- *= 95 Hoe ¹ ¹ CCGW-21.50W* g g CCGW W* g g CCGW-21.51W* g CCGW-32.50W* g g CCGW W* g g CCGW-32.51W* g CPGT-CB1 Positive Neuta (with Chip Conto) TFC PDC PDC- PDC-CU- ¹ CPGT CB g ¹ 11 CPGT CB g CPGT-CB2 Positive Neuta (with Chip Conto) TFC PDC PDC- PDC-CU- ¹ CPGT CB g g ¹ 11 CPGT CB g DCGT-CB1 Positive Neuta (with Chip Conto) TFC PDC PDC- PDC-CU- DCGT CB g g DCGT CB g g g g DCGT CB g g g g DCGT CB g g DCGT CB g g DCGT CB g g g DCGT CB g g g g DCGT CB g g g g

5 DCGT-CB2 Positive Neuta (with Chip Conto) TFC PDC PDC- PDC-CU- DCGT CB g DCGT CB g g g DCGT CB g g g DCGT CB g g DCGT CB g DCGT CB g g DCGT CB g g g DCGT CB g g g DCGW Neuta (Fat Top Inset) TFC PDC PDC- PDC-CU- DCGW g DCGW g g g DCGW g g g g DCGW g g g g DCGW g DCGW g g g DCGW g g g g DCGW g g g g DCGW g g RCGT-CB1 Fuface (with Chip Conto) TFC PDC PDC- PDC-CU- Designation ¹ s PDC TFC PD DP ¹ RCGT-0602MO-VM-CB FULL g g RCGT-10T3MO-VM-CB FULL g g RCGT-CB2 Fuface (with Chip Conto) TFC PDC PDC- PDC-CU- Designation ¹ s PDC TFC PD DP ¹ RCGT-0602MO-VM-CB FULL g RCGT-10T3MO-VM-CB FULL g RCGW Neuta (Fat Top Inset) TFC PDC PDC- PDC-CU- Designation ¹ s PDC TFC PD DP RCGW-0602MO-VM FULL g g RCGW-0803MO-VM FULL g g g ¹ RCGW-1003MO-VM FULL g g RCGW-10T3MO-VM FULL g g RCGW-1204MO-VM FULL g

6 CGT-CB1 Positive Neuta (with Chip Conto) TFC PDC PDC- PDC-CU- CGT CB g g CGT CB g g CGT-CB2 Positive Neuta (with Chip Conto) TFC PDC PDC- PDC-CU- CGT CB g g CGT CB g g CGW Neuta (Fat Top Inset) TFC PDC PDC- PDC-CU- CGW g CGW g g g CGW g g CGW g CGW g g CGW g g CGW g g TCGT-CB1 Positive Neuta (with Chip Conto) TFC PDC PDC- PDC-CU- TCGT CB g g TCGT CB g g TCGT CB g g TCGT CB g g TCGT CB g g TCGT CB g g TCGT-CB2 Positive Neuta (with Chip Conto) TFC PDC PDC- PDC-CU- TCGT CB g g TCGT CB g g TCGT CB g g TCGT CB g g TCGT CB g g TCGT CB g g

7 TCGW Neuta (Fat Top Inset) TFC PDC PDC- PDC-CU- TCGW g g g TCGW g g g TCGW g g TCGW g g g TCGW g g g g TCGW g g g TCGW g g g TCGW g g g VBGT-CB1 Positive Neuta (with Chip Conto) TFC PDC PDC- PDC-CU- VBGT CB g g g VBGT-331-CB g g g VBGT-332-CB g g g VBGT-333-CB g g g VBGT-CB2 Positive Neuta (with Chip Conto) TFC PDC PDC- PDC-CU- VBGT CB g g VBGT-331-CB g g g VBGT-332-CB g g g VBGT-333-CB g g VBGW Neuta (Fat Top Inset) TFC PDC PDC- PDC-CU- VBGW g VBGW g VBGW g VBGW g g VBGW g g g VBGW g g g VBGW g g

8 VCGT-CB1 Positive Neuta (with Chip Conto) TFC PDC PDC- PDC-CU- VCGT-220-CB g g VCGT CB g g g VCGT-221-CB g g g VCGT CB g g VCGT-331-CB g g g VCGT-332-CB g g g VCGT-333-CB g g g VCGT-CB2 Positive Neuta (with Chip Conto) TFC PDC PDC- PDC-CU- VCGT-220-CB g g g VCGT CB g g g VCGT-221-CB g g VCGT CB g g g VCGT-331-CB g g g VCGT-332-CB g g VCGT-333-CB g g VCGW Neuta (Fat Top Inset) TFC PDC PDC- PDC-CU- VCGW g VCGW g g g g VCGW g g g g VCGW g g VCGW g VCGW g g g g VCGW g g g g VCGW g g g VCGW g g g can hee fo ou BECKER chipbeake vieo can hee fo BECKER bochues & cataogs Avaiabe Fom: pecifications ae subject to change without notice. No esponsibiity fo eos an/o pinting eos wi be accepte.

Application field. PBC-10S - for high cutting speed and long tool life in machining of grey cast irons

Application field. PBC-10S - for high cutting speed and long tool life in machining of grey cast irons cutting mateias utaha Appication fie - fo high cutting spee an ong too ife in machining of gey cast ions Fo exampe: ive whee, GG 25, iamete 480 mm Use inset type: DCGW11T308-D-10-2MC upefinishing: v c

More information

Equilibria of a cylindrical plasma

Equilibria of a cylindrical plasma // Miscellaneous Execises Cylinical equilibia Equilibia of a cylinical plasma Consie a infinitely long cyline of plasma with a stong axial magnetic fiel (a geat fusion evice) Plasma pessue will cause the

More information

FI 2201 Electromagnetism

FI 2201 Electromagnetism F Eectomagnetism exane. skana, Ph.D. Physics of Magnetism an Photonics Reseach Goup Magnetostatics MGNET VETOR POTENTL, MULTPOLE EXPNSON Vecto Potentia Just as E pemitte us to intouce a scaa potentia V

More information

FACTORS EFFECTING ELASTICITY

FACTORS EFFECTING ELASTICITY Synopsis : ELASTICITY. Defoming foce : The extena foce acting on a body on account of which its size o shape o both change is defined as the defoming foce.. Restoing foce : The foce which estoes the size

More information

[ ] [ ] 3.3 Given: turning corner radius, r ε = 0 mm lead angle, ψ r = 15 back rake angle, γ p = 5 side rake angle, γ f = 5

[ ] [ ] 3.3 Given: turning corner radius, r ε = 0 mm lead angle, ψ r = 15 back rake angle, γ p = 5 side rake angle, γ f = 5 33 Given: tuning cone adius, ε = 0 mm lead angle, ψ = 5 back ake angle, γ p = 5 side ake angle, γ f = 5 initial wokpiece diamete, D w = 00 mm specific cutting and thust enegy models feed ate, f = 020 mm/ev

More information

2.25 Advanced Fluid Mechanics

2.25 Advanced Fluid Mechanics MIT Depatment of Mechanical Engineeing.5 Advanced Fluid Mechanics Poblem 6.1 This poblem is fom Advanced Fluid Mechanics Poblems by A.H. Shapio and A.A. Sonin The sketch shows a cicula beaing pad which

More information

Topic 4a Introduction to Root Finding & Bracketing Methods

Topic 4a Introduction to Root Finding & Bracketing Methods /8/18 Couse Instucto D. Raymond C. Rumpf Office: A 337 Phone: (915) 747 6958 E Mail: cumpf@utep.edu Topic 4a Intoduction to Root Finding & Backeting Methods EE 4386/531 Computational Methods in EE Outline

More information

Shank 8 mm. GL 55.5 mm, with heel, Z 2 / V 2 WB ID mm. RPM: n = min -1. GL 67 mm, with heel, Z 2 / V 2 WB

Shank 8 mm. GL 55.5 mm, with heel, Z 2 / V 2 WB ID mm. RPM: n = min -1. GL 67 mm, with heel, Z 2 / V 2 WB . riing. owe riing.. owe ris Shank Appication For riing owe hoes, especiay owe hoes in cabinetry. Suitabe for machines with insufficient bit guiance. Machine centres, hinge boring machines, muti-spine

More information

Homework 1 Solutions CSE 101 Summer 2017

Homework 1 Solutions CSE 101 Summer 2017 Homewok 1 Soutions CSE 101 Summe 2017 1 Waming Up 1.1 Pobem and Pobem Instance Find the smaest numbe in an aay of n integes a 1, a 2,..., a n. What is the input? What is the output? Is this a pobem o a

More information

22.615, MHD Theory of Fusion Systems Prof. Freidberg Lecture 4: Toroidal Equilibrium and Radial Pressure Balance

22.615, MHD Theory of Fusion Systems Prof. Freidberg Lecture 4: Toroidal Equilibrium and Radial Pressure Balance .615, MHD Theoy of Fusion Systems Pof. Feidbeg Lectue 4: Tooidal Equilibium and Radial Pessue Balance Basic Poblem of Tooidal Equilibium 1. Radial pessue balance. Tooidal foce balance Radial Pessue Balance

More information

Physics 4A Chapter 8: Dynamics II Motion in a Plane

Physics 4A Chapter 8: Dynamics II Motion in a Plane Physics 4A Chapte 8: Dynamics II Motion in a Plane Conceptual Questions and Example Poblems fom Chapte 8 Conceptual Question 8.5 The figue below shows two balls of equal mass moving in vetical cicles.

More information

A Deep Convolutional Neural Network Based on Nested Residue Number System

A Deep Convolutional Neural Network Based on Nested Residue Number System A Deep Convolutional Neual Netwok Based on Nested Residue Numbe System Hioki Nakahaa Ehime Univesity, Japan Tsutomu Sasao Meiji Univesity, Japan Abstact A pe-tained deep convolutional neual netwok (DCNN)

More information

15. SIMPLE MHD EQUILIBRIA

15. SIMPLE MHD EQUILIBRIA 15. SIMPLE MHD EQUILIBRIA In this Section we will examine some simple examples of MHD equilibium configuations. These will all be in cylinical geomety. They fom the basis fo moe the complicate equilibium

More information

Cylindrical Ro ller Bearings

Cylindrical Ro ller Bearings Pat 4 2. CYLINRICAL ROLLER EARINGS ouble Row Cylinical Rolle eaings Cylinical Rolle eaings Single Row Cylinical Rolle eaings Cylinical Rolle eaings P78- Featues Stana Seies Numbeing System eaing Tables

More information

Pressure in the Average-Atom Model

Pressure in the Average-Atom Model Pessue in the Aveage-Atom Moe W.. Johnson Depatment of Physics, 225 Nieuwan Science Ha Note Dame Univesity, Note Dame, IN 46556 Febuay 28, 2002 Abstact The (we-known) quantum mechanica expession fo the

More information

T1500Z. General Purpose Coated Cermet for Steel Turning

T1500Z. General Purpose Coated Cermet for Steel Turning TOOLING NEWS E-125 P M K N S H General Purpose Coated Cermet for Steel Turning Brilliant Coat for glossy finished surface and excellent wear resistance Expanded chip breaker lineup with newly developed

More information

B. Spherical Wave Propagation

B. Spherical Wave Propagation 11/8/007 Spheical Wave Popagation notes 1/1 B. Spheical Wave Popagation Evey antenna launches a spheical wave, thus its powe density educes as a function of 1, whee is the distance fom the antenna. We

More information

( )( )( ) ( ) + ( ) ( ) ( )

( )( )( ) ( ) + ( ) ( ) ( ) 3.7. Moel: The magnetic fiel is that of a moving chage paticle. Please efe to Figue Ex3.7. Solve: Using the iot-savat law, 7 19 7 ( ) + ( ) qvsinθ 1 T m/a 1.6 1 C. 1 m/s sin135 1. 1 m 1. 1 m 15 = = = 1.13

More information

LINEAR AND NONLINEAR ANALYSES OF A WIND-TUNNEL BALANCE

LINEAR AND NONLINEAR ANALYSES OF A WIND-TUNNEL BALANCE LINEAR AND NONLINEAR ANALYSES O A WIND-TUNNEL INTRODUCTION BALANCE R. Kakehabadi and R. D. Rhew NASA LaRC, Hampton, VA The NASA Langley Reseach Cente (LaRC) has been designing stain-gauge balances fo utilization

More information

JAPAN HIGH PERFORMANCE CERAMIC BEARING FOR SPECIAL ENVIRONMENTS NATEC. Regional Distributor NATEC CORPORATION.,LTD.

JAPAN HIGH PERFORMANCE CERAMIC BEARING FOR SPECIAL ENVIRONMENTS NATEC. Regional Distributor NATEC CORPORATION.,LTD. NATEC JAPAN HIGH PERFORMAN RAMIC EARING NATEC FOR SPECIAL ENVIRONMENTS JAPAN Regional istibuto NATEC CORPORATION.,LT. NATEC JAPAN INEX AVANTAGEPROUCT CATEGORY............ RAMIC MATERIALS........................

More information

of Technology: MIT OpenCourseWare). (accessed MM DD, YYYY). License: Creative Commons Attribution- Noncommercial-Share Alike.

of Technology: MIT OpenCourseWare).   (accessed MM DD, YYYY). License: Creative Commons Attribution- Noncommercial-Share Alike. MIT OpenCouseWae http://ocw.mit.eu 6.013/ESD.013J Electomagnetics an Applications, Fall 005 Please use the following citation fomat: Makus Zahn, Eich Ippen, an Davi Staelin, 6.013/ESD.013J Electomagnetics

More information

CBE Transport Phenomena I Final Exam. December 19, 2013

CBE Transport Phenomena I Final Exam. December 19, 2013 CBE 30355 Tanspot Phenomena I Final Exam Decembe 9, 203 Closed Books and Notes Poblem. (20 points) Scaling analysis of bounday laye flows. A popula method fo measuing instantaneous wall shea stesses in

More information

3-7 FLUIDS IN RIGID-BODY MOTION

3-7 FLUIDS IN RIGID-BODY MOTION 3-7 FLUIDS IN IGID-BODY MOTION S-1 3-7 FLUIDS IN IGID-BODY MOTION We ae almost eady to bein studyin fluids in motion (statin in Chapte 4), but fist thee is one cateoy of fluid motion that can be studied

More information

Reasons to Build a Hydraulic Model

Reasons to Build a Hydraulic Model Reasons to Build a Hydaulic Model Detemine dischage coefficient fo lage flow measuement stuctue (spillway o wei) Develop effective method fo enegy dissipation at outlet of hydaulic stuctue Development

More information

MAE 210B. Homework Solution #6 Winter Quarter, U 2 =r U=r 2 << 1; ) r << U : (1) The boundary conditions written in polar coordinates,

MAE 210B. Homework Solution #6 Winter Quarter, U 2 =r U=r 2 << 1; ) r << U : (1) The boundary conditions written in polar coordinates, MAE B Homewok Solution #6 Winte Quate, 7 Poblem a Expecting a elocity change of oe oe a aial istance, the conition necessay fo the ow to be ominate by iscous foces oe inetial foces is O( y ) O( ) = =

More information

MECHANICAL PULPING REFINER MECHANICAL PULPS

MECHANICAL PULPING REFINER MECHANICAL PULPS MECHANICAL PULPING REFINER MECHANICAL PULPS Histoy of efine mechanical pulping Fo many yeas all mechanical pulp was made fom stone goundwood (SGW). This equied whole logs. Stating in the 950s, but eally

More information

Objectives. We will also get to know about the wavefunction and its use in developing the concept of the structure of atoms.

Objectives. We will also get to know about the wavefunction and its use in developing the concept of the structure of atoms. Modue "Atomic physics and atomic stuctue" Lectue 7 Quantum Mechanica teatment of One-eecton atoms Page 1 Objectives In this ectue, we wi appy the Schodinge Equation to the simpe system Hydogen and compae

More information

CHAPTER 3 DIODES. NTUEE Electronics L. H. Lu 3-1

CHAPTER 3 DIODES. NTUEE Electronics L. H. Lu 3-1 CHAPER 3 OE Chapte Outline 3.1 he eal ioe 3.2 eminal Chaacteistics of Junction ioes 3.3 Moeling the ioe Fowa Chaacteistics 3.4 Opeation in the Reese Beakown Region ene ioes 3.5 Rectifie Cicuits 3.6 Limiting

More information

Faraday s Law. Faraday s Law. Faraday s Experiments. Faraday s Experiments. Magnetic Flux. Chapter 31. Law of Induction (emf( emf) Faraday s Law

Faraday s Law. Faraday s Law. Faraday s Experiments. Faraday s Experiments. Magnetic Flux. Chapter 31. Law of Induction (emf( emf) Faraday s Law Faaday s Law Faaday s Epeiments Chapte 3 Law of nduction (emf( emf) Faaday s Law Magnetic Flu Lenz s Law Geneatos nduced Electic fields Michael Faaday discoeed induction in 83 Moing the magnet induces

More information

Physics: Work & Energy Beyond Earth Guided Inquiry

Physics: Work & Energy Beyond Earth Guided Inquiry Physics: Wok & Enegy Beyond Eath Guided Inquiy Elliptical Obits Keple s Fist Law states that all planets move in an elliptical path aound the Sun. This concept can be extended to celestial bodies beyond

More information

Jackson 3.3 Homework Problem Solution Dr. Christopher S. Baird University of Massachusetts Lowell

Jackson 3.3 Homework Problem Solution Dr. Christopher S. Baird University of Massachusetts Lowell Jackson 3.3 Homewok Pobem Soution D. Chistophe S. Baid Univesity of Massachusetts Lowe POBLEM: A thin, fat, conducting, cicua disc of adius is ocated in the x-y pane with its cente at the oigin, and is

More information

Page 1 of 6 Physics II Exam 1 155 points Name Discussion day/time Pat I. Questions 110. 8 points each. Multiple choice: Fo full cedit, cicle only the coect answe. Fo half cedit, cicle the coect answe and

More information

Phys102 Second Major-182 Zero Version Monday, March 25, 2019 Page: 1

Phys102 Second Major-182 Zero Version Monday, March 25, 2019 Page: 1 Monday, Mach 5, 019 Page: 1 Q1. Figue 1 shows thee pais of identical conducting sphees that ae to be touched togethe and then sepaated. The initial chages on them befoe the touch ae indicated. Rank the

More information

1 2 U CV. K dq I dt J nqv d J V IR P VI

1 2 U CV. K dq I dt J nqv d J V IR P VI o 5 o T C T F 9 T K T o C 7.5 L L T V VT Q mct nct Q F V ml F V dq A H k TH TC dt L pv nt Kt nt CV ideal monatomic gas 5 CV ideal diatomic gas w/o vibation V W pdv V U Q W W Q e Q Q e Canot H C T T S C

More information

Flux. Area Vector. Flux of Electric Field. Gauss s Law

Flux. Area Vector. Flux of Electric Field. Gauss s Law Gauss s Law Flux Flux in Physics is used to two distinct ways. The fist meaning is the ate of flow, such as the amount of wate flowing in a ive, i.e. volume pe unit aea pe unit time. O, fo light, it is

More information

EKT 356 MICROWAVE COMMUNICATIONS CHAPTER 2: PLANAR TRANSMISSION LINES

EKT 356 MICROWAVE COMMUNICATIONS CHAPTER 2: PLANAR TRANSMISSION LINES EKT 356 MICROWAVE COMMUNICATIONS CHAPTER : PLANAR TRANSMISSION LINES 1 Tansmission Lines A device used to tansfe enegy fom one point to anothe point efficiently Efficiently minimum loss, eflection and

More information

10. Groundwater in geotechnical problems

10. Groundwater in geotechnical problems . Goundwate in geotechnical poblems Goundwate plays a key ole in many geotechnical poblems. We will look at; - land subsidence - dewateing open pits - Consolidation of sediments Remembe the stoage of wate

More information

Numerical Integration

Numerical Integration MCEN 473/573 Chapte 0 Numeical Integation Fall, 2006 Textbook, 0.4 and 0.5 Isopaametic Fomula Numeical Integation [] e [ ] T k = h B [ D][ B] e B Jdsdt In pactice, the element stiffness is calculated numeically.

More information

Method for Approximating Irrational Numbers

Method for Approximating Irrational Numbers Method fo Appoximating Iational Numbes Eic Reichwein Depatment of Physics Univesity of Califonia, Santa Cuz June 6, 0 Abstact I will put foth an algoithm fo poducing inceasingly accuate ational appoximations

More information

Faraday s Law (continued)

Faraday s Law (continued) Faaday s Law (continued) What causes cuent to flow in wie? Answe: an field in the wie. A changing magnetic flux not only causes an MF aound a loop but an induced electic field. Can wite Faaday s Law: ε

More information

Determining solar characteristics using planetary data

Determining solar characteristics using planetary data Detemining sola chaacteistics using planetay data Intoduction The Sun is a G-type main sequence sta at the cente of the Sola System aound which the planets, including ou Eath, obit. In this investigation

More information

Force and Work: Reminder

Force and Work: Reminder Electic Potential Foce and Wok: Reminde Displacement d a: initial point b: final point Reminde fom Mechanics: Foce F if thee is a foce acting on an object (e.g. electic foce), this foce may do some wok

More information

Mechanics and Special Relativity (MAPH10030) Assignment 3

Mechanics and Special Relativity (MAPH10030) Assignment 3 (MAPH0030) Assignment 3 Issue Date: 03 Mach 00 Due Date: 4 Mach 00 In question 4 a numeical answe is equied with pecision to thee significant figues Maks will be deducted fo moe o less pecision You may

More information

Technical Data for Profiles. Groove position, external dimensions and modular dimensions

Technical Data for Profiles. Groove position, external dimensions and modular dimensions Technica Data for Profies Extruded Profie Symbo A Mg Si 0.5 F 25 Materia number.206.72 Status: artificiay aged Mechanica vaues (appy ony in pressing direction) Tensie strength Rm min. 245 N/mm 2 Yied point

More information

Conservation of Linear Momentum using RTT

Conservation of Linear Momentum using RTT 07/03/2017 Lectue 21 Consevation of Linea Momentum using RTT Befoe mi-semeste exam, we have seen the 1. Deivation of Reynols Tanspot Theoem (RTT), 2. Application of RTT in the Consevation of Mass pinciple

More information

EELE 3331 Electromagnetic I Chapter 4. Electrostatic fields. Islamic University of Gaza Electrical Engineering Department Dr.

EELE 3331 Electromagnetic I Chapter 4. Electrostatic fields. Islamic University of Gaza Electrical Engineering Department Dr. EELE 3331 Electomagnetic I Chapte 4 Electostatic fields Islamic Univesity of Gaza Electical Engineeing Depatment D. Talal Skaik 212 1 Electic Potential The Gavitational Analogy Moving an object upwad against

More information

working pages for Paul Richards class notes; do not copy or circulate without permission from PGR 2004/11/3 10:50

working pages for Paul Richards class notes; do not copy or circulate without permission from PGR 2004/11/3 10:50 woking pages fo Paul Richads class notes; do not copy o ciculate without pemission fom PGR 2004/11/3 10:50 CHAPTER7 Solid angle, 3D integals, Gauss s Theoem, and a Delta Function We define the solid angle,

More information

Mutual Inductance. If current i 1 is time varying, then the Φ B2 flux is varying and this induces an emf ε 2 in coil 2, the emf is

Mutual Inductance. If current i 1 is time varying, then the Φ B2 flux is varying and this induces an emf ε 2 in coil 2, the emf is Mutua Inductance If we have a constant cuent i in coi, a constant magnetic fied is ceated and this poduces a constant magnetic fux in coi. Since the Φ B is constant, thee O induced cuent in coi. If cuent

More information

Sensing, Computing, Actuating

Sensing, Computing, Actuating Sensing, Computing, Actuating Sande Stuij (s.stuij@tue.nl) Depatment of Electical Engineeing Electonic Systems SENSING TEMPEATUE, SELF-HEATING (Chapte.,., 5.) 3 Engine coolant tempeatue senso https://www.youtube.com/watch?=q5637fsca

More information

r cos, and y r sin with the origin of coordinate system located at

r cos, and y r sin with the origin of coordinate system located at Lectue 3-3 Kinematics of Rotation Duing ou peious lectues we hae consideed diffeent examples of motion in one and seeal dimensions. But in each case the moing object was consideed as a paticle-like object,

More information

ACCURATE FLOATING-POINT SUMMATION IN CUB

ACCURATE FLOATING-POINT SUMMATION IN CUB ACCURATE FLOATING-POINT SUMMATION IN CUB URI VERNER Summe inten OUTLINE Who need accuate floating-point ummation?! Round-off eo: ouce and ecovey A new method fo accuate FP ummation on a GPU Added a a function

More information

Fluid flow in curved geometries: Mathematical Modeling and Applications

Fluid flow in curved geometries: Mathematical Modeling and Applications Fluid flow in cuved geometies: Mathematical Modeling and Applications D. Muhammad Sajid Theoetical Plasma Physics Division PINSTECH, P.O. Niloe, PAEC, Islamabad Mach 01-06, 010 Islamabad, Paistan Pesentation

More information

Stress, Cauchy s equation and the Navier-Stokes equations

Stress, Cauchy s equation and the Navier-Stokes equations Chapte 3 Stess, Cauchy s equation and the Navie-Stokes equations 3. The concept of taction/stess Conside the volume of fluid shown in the left half of Fig. 3.. The volume of fluid is subjected to distibuted

More information

( ) ( ) Review of Force. Review of Force. r = =... Example 1. What is the dot product for F r. Solution: Example 2 ( )

( ) ( ) Review of Force. Review of Force. r = =... Example 1. What is the dot product for F r. Solution: Example 2 ( ) : PHYS 55 (Pat, Topic ) Eample Solutions p. Review of Foce Eample ( ) ( ) What is the dot poduct fo F =,,3 and G = 4,5,6? F G = F G + F G + F G = 4 +... = 3 z z Phs55 -: Foce Fields Review of Foce Eample

More information

F-IF Logistic Growth Model, Abstract Version

F-IF Logistic Growth Model, Abstract Version F-IF Logistic Gowth Model, Abstact Vesion Alignments to Content Standads: F-IFB4 Task An impotant example of a model often used in biology o ecology to model population gowth is called the logistic gowth

More information

Spiral Magnetic Gradient Motor Using Axial Magnets

Spiral Magnetic Gradient Motor Using Axial Magnets Spial Magnetic Gadient Moto Using Axial Magnets Cedit: Tom Schum fo spial stato constuction Thomas Valone, PhD, PE Integity Reseach Institute Pape on Science Diect, Physics Gadients Ae Used fo All Powe

More information

Numerical Simulation of Launch Tube Based on Container type Missile Launch Technology

Numerical Simulation of Launch Tube Based on Container type Missile Launch Technology Avaiabe onine at www.scienceirect.com Proceia Engineering 31 (2012) 302 307 Internationa Conference on Avances in Computationa oeing an Simuation Numerica Simuation of Launch Tube Base on Container type

More information

Magnetohydrodynamics (MHD) I

Magnetohydrodynamics (MHD) I Magnetohydodynamics (MHD) I Yong-Su Na National Fusion Reseach Cente POSTECH, Koea, 8-10 May, 006 Contents 1. Review Confinement & Single Paticle Motion. Plasmas as Fluids Fluid Equations 3. MHD Equations

More information

Insulated Bearings MEGAOHM TM Series

Insulated Bearings MEGAOHM TM Series Fo ew Technology etwok copoation R Insulated eaings MEGAOHM TM Seies Insulated eaings MEGAOHM TM Seies : Offeing Enhanced Safety and Reliability eaings used in electical equipment such as motos and powe

More information

High precision computer simulation of cyclotrons KARAMYSHEVA T., AMIRKHANOV I. MALININ V., POPOV D.

High precision computer simulation of cyclotrons KARAMYSHEVA T., AMIRKHANOV I. MALININ V., POPOV D. High pecision compute simulation of cyclotons KARAMYSHEVA T., AMIRKHANOV I. MALININ V., POPOV D. Abstact Effective and accuate compute simulations ae highly impotant in acceleatos design and poduction.

More information

(1) It increases the break down potential of the surrounding medium so that more potential can be applied and hence more charge can be stored.

(1) It increases the break down potential of the surrounding medium so that more potential can be applied and hence more charge can be stored. Cpcito Cpcito: Cpcito ( o conense ) is evice fo stoing chge. It essentilly consists of two conucting sufces such s two pltes o two spheicl shell o two cylines etc. kept exctly pllel to ech othe septe y

More information

4/18/2005. Statistical Learning Theory

4/18/2005. Statistical Learning Theory Statistical Leaning Theoy Statistical Leaning Theoy A model of supevised leaning consists of: a Envionment - Supplying a vecto x with a fixed but unknown pdf F x (x b Teache. It povides a desied esponse

More information

EKT 345 MICROWAVE ENGINEERING CHAPTER 2: PLANAR TRANSMISSION LINES

EKT 345 MICROWAVE ENGINEERING CHAPTER 2: PLANAR TRANSMISSION LINES EKT 345 MICROWAVE ENGINEERING CHAPTER : PLANAR TRANSMISSION LINES 1 Tansmission Lines A device used to tansfe enegy fom one point to anothe point efficiently Efficiently minimum loss, eflection and close

More information

Introduction to Dielectric Properties and Magnetism

Introduction to Dielectric Properties and Magnetism Intoduction to Dielectic opeties and Magnetism At the end of the last lectue we looked at some of the electical popeties of matte and intoduces the notions of electic field and electical conductivity.

More information

Geometry and statistics in turbulence

Geometry and statistics in turbulence Geomety and statistics in tubulence Auoe Naso, Univesity of Twente, Misha Chetkov, Los Alamos, Bois Shaiman, Santa Babaa, Alain Pumi, Nice. Tubulent fluctuations obey a complex dynamics, involving subtle

More information

Construction Figure 10.1: Jaw clutches

Construction Figure 10.1: Jaw clutches CHAPTER TEN FRICTION CLUTCHES The wod clutch is a geneic tem descibing any one wide vaiety of devices that is capable of causing a machine o mechanism to become engaged o disengaged. Clutches ae of thee

More information

Equations to Calculate Characteristic Frequencies of Multiple Chamber Aligned in Parallel Cavity Resonator (MCAP-CR)

Equations to Calculate Characteristic Frequencies of Multiple Chamber Aligned in Parallel Cavity Resonator (MCAP-CR) MCAPE Equations to Calculate Chaacteistic Fequencies of Multiple Chabe Aligne in Paallel Cavity Resonato (MCAP-CR) Shigeu Suzui Mach, (Revise in ovebe, ). Peface It is necessay to solve the equations of

More information

18.06 Problem Set 4 Solution

18.06 Problem Set 4 Solution 8.6 Poblem Set 4 Solution Total: points Section 3.5. Poblem 2: (Recommended) Find the lagest possible numbe of independent vectos among ) ) ) v = v 4 = v 5 = v 6 = v 2 = v 3 =. Solution (4 points): Since

More information

Passivity-Based Control of Saturated Induction Motors

Passivity-Based Control of Saturated Induction Motors Passivity-Base Contol of Satuate Inuction otos Levent U. Gökee, embe, IEEE, awan A. Simaan, Fellow, IEEE, an Chales W. Bice, Senio embe, IEEE Depatment of Electical Engineeing Univesity of South Caolina

More information

Graphite. Graphite

Graphite. Graphite igh-performance en mills with CV iamon coating for of graphite. ochleistungs-schaftfräser mit CV-iamant Beschichtung für ie von Graphit. 115-124 www.nkotool.com 115 ew ew ew Tool coe GE 235 GEL 435 GBLS

More information

Current Balance Warm Up

Current Balance Warm Up PHYSICS EXPERIMENTS 133 Cuent Balance-1 Cuent Balance Wam Up 1. Foce between cuent-caying wies Wie 1 has a length L (whee L is "long") and caies a cuent I 0. What is the magnitude of the magnetic field

More information

Theorem 2: Proof: Note 1: Proof: Note 2:

Theorem 2: Proof: Note 1: Proof: Note 2: A New 3-Dimenional Polynomial Intepolation Method: An Algoithmic Appoach Amitava Chattejee* and Rupak Bhattachayya** A new 3-dimenional intepolation method i intoduced in thi pape. Coeponding to the method

More information

= ρ. Since this equation is applied to an arbitrary point in space, we can use it to determine the charge density once we know the field.

= ρ. Since this equation is applied to an arbitrary point in space, we can use it to determine the charge density once we know the field. Gauss s Law In diffeentia fom D = ρ. ince this equation is appied to an abita point in space, we can use it to detemine the chage densit once we know the fied. (We can use this equation to ve fo the fied

More information

Merging to ordered sequences. Efficient (Parallel) Sorting. Merging (cont.)

Merging to ordered sequences. Efficient (Parallel) Sorting. Merging (cont.) Efficient (Paae) Soting One of the most fequent opeations pefomed by computes is oganising (soting) data The access to soted data is moe convenient/faste Thee is a constant need fo good soting agoithms

More information

Conducting fuzzy division by using linear programming

Conducting fuzzy division by using linear programming WSES TRNSCTIONS on INFORMTION SCIENCE & PPLICTIONS Muat pe Basaan, Cagdas Hakan adag, Cem Kadia Conducting fuzzy division by using inea pogamming MURT LPER BSRN Depatment of Mathematics Nigde Univesity

More information

Recap. Centripetal acceleration: v r. a = m/s 2 (towards center of curvature)

Recap. Centripetal acceleration: v r. a = m/s 2 (towards center of curvature) a = c v 2 Recap Centipetal acceleation: m/s 2 (towads cente of cuvatue) A centipetal foce F c is equied to keep a body in cicula motion: This foce poduces centipetal acceleation that continuously changes

More information

Supplementary Figure 1. Circular parallel lamellae grain size as a function of annealing time at 250 C. Error bars represent the 2σ uncertainty in

Supplementary Figure 1. Circular parallel lamellae grain size as a function of annealing time at 250 C. Error bars represent the 2σ uncertainty in Supplementay Figue 1. Cicula paallel lamellae gain size as a function of annealing time at 50 C. Eo bas epesent the σ uncetainty in the measued adii based on image pixilation and analysis uncetainty contibutions

More information

Title. Author(s)Y. IMAI; T. TSUJII; S. MOROOKA; K. NOMURA. Issue Date Doc URL. Type. Note. File Information

Title. Author(s)Y. IMAI; T. TSUJII; S. MOROOKA; K. NOMURA. Issue Date Doc URL. Type. Note. File Information Title CALCULATION FORULAS OF DESIGN BENDING OENTS ON TH APPLICATION OF THE SAFETY-ARGIN FRO RC STANDARD TO Autho(s)Y. IAI; T. TSUJII; S. OROOKA; K. NOURA Issue Date 013-09-1 Doc URL http://hdl.handle.net/115/538

More information

Exam 3, vers Physics Spring, 2003

Exam 3, vers Physics Spring, 2003 1 of 9 Exam 3, ves. 0001 - Physics 1120 - Sping, 2003 NAME Signatue Student ID # TA s Name(Cicle one): Michael Scheffestein, Chis Kelle, Paisa Seelungsawat Stating time of you Tues ecitation (wite time

More information

2.25 Advanced Fluid Mechanics

2.25 Advanced Fluid Mechanics MIT Depatment of Mechanical Engineeing 2.25 Advanced Fluid Mechanics Poblem 4.27 This poblem is fom Advanced Fluid Mechanics Poblems by A.H. Shapio and A.A. Sonin u(,t) pg Gas Liquid, density Conside a

More information

PHYS 1444 Lecture #5

PHYS 1444 Lecture #5 Shot eview Chapte 24 PHYS 1444 Lectue #5 Tuesday June 19, 212 D. Andew Bandt Capacitos and Capacitance 1 Coulom s Law The Fomula QQ Q Q F 1 2 1 2 Fomula 2 2 F k A vecto quantity. Newtons Diection of electic

More information

Phys-272 Lecture 17. Motional Electromotive Force (emf) Induced Electric Fields Displacement Currents Maxwell s Equations

Phys-272 Lecture 17. Motional Electromotive Force (emf) Induced Electric Fields Displacement Currents Maxwell s Equations Phys-7 Lectue 17 Motional Electomotive Foce (emf) Induced Electic Fields Displacement Cuents Maxwell s Equations Fom Faaday's Law to Displacement Cuent AC geneato Magnetic Levitation Tain Review of Souces

More information

Course Updates. Reminders: 1) Assignment #10 due next Wednesday. 2) Midterm #2 take-home Friday. 3) Quiz # 5 next week. 4) Inductance, Inductors, RLC

Course Updates. Reminders: 1) Assignment #10 due next Wednesday. 2) Midterm #2 take-home Friday. 3) Quiz # 5 next week. 4) Inductance, Inductors, RLC Couse Updates http://www.phys.hawaii.edu/~vane/phys7-sp10/physics7.htm Remindes: 1) Assignment #10 due next Wednesday ) Midtem # take-home Fiday 3) Quiz # 5 next week 4) Inductance, Inductos, RLC Mutua

More information

Lecture 8 - Gauss s Law

Lecture 8 - Gauss s Law Lectue 8 - Gauss s Law A Puzzle... Example Calculate the potential enegy, pe ion, fo an infinite 1D ionic cystal with sepaation a; that is, a ow of equally spaced chages of magnitude e and altenating sign.

More information

Visit us on the Web : Copyright 2011 Pearson Education,Inc.

Visit us on the Web :   Copyright 2011 Pearson Education,Inc. The authos and the publishe have taken cae in the pepaation of this book but make no expessed o implied waanty of any kind and assume no esponsibility fo eos o omissions. No liability is assumed fo the

More information

Potential Energy and Conservation of Energy

Potential Energy and Conservation of Energy Potential Enegy and Consevation of Enegy Consevative Foces Definition: Consevative Foce If the wok done by a foce in moving an object fom an initial point to a final point is independent of the path (A

More information

Multiphase Flow and Heat Transfer

Multiphase Flow and Heat Transfer Multiphase Flow and Heat Tansfe ME546 -Sudhee Siddapueddy sudhee@iitp.ac.in Pendant and Sessile Dops Pendant doplet detachment sequence Sessile wate doplet immesed in oil and esting on a bass suface Inteface

More information

DQ Modeling Of Induction Motor With Broken Rotor Bars In MATLAB Simulink

DQ Modeling Of Induction Motor With Broken Rotor Bars In MATLAB Simulink DQ Moeling Of Inuction Moto With Boken Roto Bas In MATLAB Simulink Pincy P 1 an Gayathi Vijayachanan 2 1,2 Depatment. Of Electical an Electonics, See Buha College of Engineeing, Keala Abstact To analyze

More information

General Railgun Function

General Railgun Function Geneal ailgun Function An electomagnetic ail gun uses a lage Loentz foce to fie a pojectile. The classic configuation uses two conducting ails with amatue that fits between and closes the cicuit between

More information

Review of Potential Energy. The Electric Potential. Plotting Fields and Potentials. Electric Potential of a Point Charge

Review of Potential Energy. The Electric Potential. Plotting Fields and Potentials. Electric Potential of a Point Charge eview of Potential negy Potential enegy U() can be used to descibe a consevative foce. efeence point (U) can be chosen fo convenience. Wok done by F : W F d s F d (1D) Change in P.. : U U f U i W Foce

More information

L6 Energy Conversion. EIEN20 Design of Electrical Machines, IEA, Previous lecture. L6: Energy conversion. Today s goal

L6 Energy Conversion. EIEN20 Design of Electrical Machines, IEA, Previous lecture. L6: Energy conversion. Today s goal L: Enegy convesion a potentia fo causing a change R Ω u i L σ e R μ N i Pevious ectue R δ N i e L σ R Ω u i E x(y), i eectomagnetism eecto- and magnetomotive foce Induction action tansfomed o motiona votage

More information

A scaling-up methodology for co-rotating twin-screw extruders

A scaling-up methodology for co-rotating twin-screw extruders A scaling-up methodology fo co-otating twin-scew extudes A. Gaspa-Cunha, J. A. Covas Institute fo Polymes and Composites/I3N, Univesity of Minho, Guimaães 4800-058, Potugal Abstact. Scaling-up of co-otating

More information

Algebra-based Physics II

Algebra-based Physics II lgebabased Physics II Chapte 19 Electic potential enegy & The Electic potential Why enegy is stoed in an electic field? How to descibe an field fom enegetic point of view? Class Website: Natual way of

More information

SAMPLE QUIZ 3 - PHYSICS For a right triangle: sin θ = a c, cos θ = b c, tan θ = a b,

SAMPLE QUIZ 3 - PHYSICS For a right triangle: sin θ = a c, cos θ = b c, tan θ = a b, SAMPLE QUIZ 3 - PHYSICS 1301.1 his is a closed book, closed notes quiz. Calculatos ae pemitted. he ONLY fomulas that may be used ae those given below. Define all symbols and justify all mathematical expessions

More information

Section 11. Timescales Radiation transport in stars

Section 11. Timescales Radiation transport in stars Section 11 Timescales 11.1 Radiation tanspot in stas Deep inside stas the adiation eld is vey close to black body. Fo a black-body distibution the photon numbe density at tempeatue T is given by n = 2

More information

ECE 3318 Applied Electricity and Magnetism. Spring Prof. David R. Jackson Dept. Of ECE. Notes 20 Dielectrics

ECE 3318 Applied Electricity and Magnetism. Spring Prof. David R. Jackson Dept. Of ECE. Notes 20 Dielectrics ECE 3318 Applied Electicity and Magnetism Sping 218 Pof. David R. Jackson Dept. Of ECE Notes 2 Dielectics 1 Dielectics Single H 2 O molecule: H H Wate ε= εε O 2 Dielectics (cont.) H H Wate ε= εε O Vecto

More information

PHY 213. General Physics II Test 2.

PHY 213. General Physics II Test 2. Univesity of Kentucky Depatment of Physics an Astonomy PHY 3. Geneal Physics Test. Date: July, 6 Time: 9:-: Answe all questions. Name: Signatue: Section: Do not flip this page until you ae tol to o so.

More information

AP-C WEP. h. Students should be able to recognize and solve problems that call for application both of conservation of energy and Newton s Laws.

AP-C WEP. h. Students should be able to recognize and solve problems that call for application both of conservation of energy and Newton s Laws. AP-C WEP 1. Wok a. Calculate the wok done by a specified constant foce on an object that undegoes a specified displacement. b. Relate the wok done by a foce to the aea unde a gaph of foce as a function

More information

Sensors and Actuators Introduction to sensors

Sensors and Actuators Introduction to sensors Sensos an ctuatos Intouction to sensos Sane Stuijk (s.stuijk@tue.nl) Depatment of Electical Engineeing Electonic Systems PITIE SENSORS (hapte 3., 7., 9.,.6, 3., 3.) 3 Senso classification type / quantity

More information

Description of TEAM Workshop Problem 33.b: Experimental Validation of Electric Local Force Formulations.

Description of TEAM Workshop Problem 33.b: Experimental Validation of Electric Local Force Formulations. 1 Desciption of TEAM Wokshop Poblem 33.b: Expeimental Validation of Electic Local Foce Fomulations. Olivie Baé, Pascal Bochet, Membe, IEEE Abstact Unde extenal stesses, the esponse of any mateial is a

More information