OBSTACLE DETECTION USING RING BEAM SYSTEM

Size: px
Start display at page:

Download "OBSTACLE DETECTION USING RING BEAM SYSTEM"

Transcription

1 OBSTACLE DETECTION USING RING BEAM SYSTEM M. Hiaki, K. Takamasu and S. Ozono Depatment of Peision Engineeing, The Univesity of Tokyo Hongo, Bunkyo-ku, Tokyo, Japan Abstat: In this pape, we popose a novel obstale detetion system using Ring Beam System (RBS) fo mobile obots. This system onsists of RBS with a one mio, a spheial mio and a CCD amea. The piniple of this system is same as tiangulation. The advantages ae having no moving pats and deteting all obstales aound the obot simultaneously. Fistly, we alulate a elationship between the position of bight point on pitue fom CCD amea and the distane to obstales. Next, we show developed expeimental devie and esults of obstale detetion. Keywods: Obstale detetion, Tiangulation, Mobile obots 1 INTRODUCTION Thee ae many eseahes about omni-dietional mobile obots, espeially fo indoo use. So, it is neessay fo autonomous mobile obots to detet obstales aound it. The obstale detetion systems ae vaious, fo example, image poessing using CCD amea [1], ultasoni wave system, and so on. A tiangulation using lase slit and CCD amea is used fo obstale detetion beause thee-dimensional shapes of objets an be measued easily [2]. In this eseah, using Ring Beam System (RBS) [3] that an pojet lase slit to all dietion, we develop the novel obstale detetion system that has no moving pats. 2 CALCULATING DISTANCE USING GEOMETRIC MODEL Figue 1 shows the geometi model of ou expeimental devie. The ente of spheial mio whose adius is is egaded as an oigin and oodinates ae deided as the figue. Moeove, it is assumed that the CCD amea and the RBS ae distane l and d away fom the oigin, espetively. Hee, a distane x to the obstales is alulated by following equations: φ = sin 1 α = os 1 l sinθ osθ sinθ 1 [ 2os( θ + φ ) osφ osθ ] l 2 sinθ x = sinφ + ( d osφ) tanα (3) (1) (2) Figue 1. Geometi model of obstale detetion system.

2 Figue 2. Expeimental devie. Figue 3. Example of obtained pitue. Figue 4. Pitue of inside of a box in ase of applying lase slit by RBS Figue 5. Deteting esult of bight line. 3 EXPERIMENT (1) The expeimental devie onsists of a spheial mio, a CCD amea and a RBS with a one mio. Developed expeimental devie is shown in figue 2 and an example of obtained pitue using this obstale detetion system is shown in figue 3. This pitue is obtained while this expeimental system is put on a desk in ou laboatoy.

3 Figue 6. Measuing esult of inside of box. Figue 7. New geometial model with geometial eos. In this expeiment, we measue inside of a box with sides 300mm long as an obstale. Fistly, we obtain two pitues by the CCD amea and a pitue boad in PC: one is a pitue in ase of applying lase slit by RBS (figue 4) and anothe is in ase of no lase beam. Seondly, we alulate diffeenes of these two pitues to detet the bight line on obstales. Figue 5 shows the deteting esult of bight line. Finally, we alulate anglesθ fo eah bight point in figue 5 and alulate the distane x to obstales using equations (1) (3). Figue 6 shows measuing esult of inside of the box. In this figue, solid lines give the position of the eal obstales and small iles give the position of deteted obstales. This esult shows the possibility of deteting obstales using ou system. 4 CONSIDERATION OF GEOMETRICAL ERRORS In the expeiment, a maximum measuing eo is 15.4 mm. We think that fatos of this eo ae eos of ente axis of eah devie and paameti eos, fo example, the length between the CCD amea and the spheial mio. Theefoe, we build a new geometial model with geometial eos in figue 7. Same as figue.2, the ente of spheial mio whose adius is is egaded as an oigin and oodinates ae deided as the figue. Moeove, it is assumed that the CCD amea and the RBS ae distane l and d away fom the oigin, espetively. As geometial eos, we intodue a position eo of CCD amea e, an oientation eo of CCD amea ψ and an oientation eo of RBS ψ. The position eos and the oientation eos ae 3 degees of feedom. Howeve, it seems that the position eos along z-axis ae inluded position l and d. Position eos x and y of RBS an be ignoed beause the slit ay fom RBS extends hoizontally. Hee, we disuss about influene that

4 eo fatos give to esults of measuement, so we use easie 2 DOF model. A elationship between a distane x to the obstales and θ is alulated by following equations: 2 1 l sin( θ ψ ) + e os( θ ψ ) l sin( θ ψ ) + e os( θ ψ ) φ = sin os sin( θ ψ ) 1 (4) α = os 1 [ 2os( θ ψ + φ)osφ os( θ ψ )] sinφ + ( d osφ) tanα x = (6) 1+ sinψ tanα 5 ANALYSIS OF ERRORS We disuss about the influene that eah geometial paamete gives to the esults of measuement. Using equations (4) - (6), diffeentials between distane x and geometial paametes ae as follows: = 2.23, = 1.46, = 14.8, = 8.87, when x = 150. l d e Hee, eah value of diffeential epesents an eo of deteting distane fo a small vaiation of the geometial paamete. We an find out that an influene of position eo of CCD amea e is biggest. About oientation eos, following equations shows diffeentials. = 2270, = 219, when x = 150. ψ ψ These diffeentials annot be ompaed with above position eos shown by equation (7), beause a unit of equation (7) is diffeent fom a unit of equation (8). Howeve, we an ealize that an influene of oientation eo of CCD amea ψ is bigge than an influene of oientation eo of RBS ψ. 6 PARAMETER IDENTIFICATION AND EXPERIMENT (2) We identify the paamete e that is the position eo of CCD amea. In fat, it is neessay to onside an eo in x-axis e and in y-axis x e fo position eos of CCD amea. Howeve, the y measuement esult of inside of box in figue 5 is almost symmety with espet to y-axis. Theefoe, we identified only the paamete e. Figue 8 shows a esult of measuing expeiment afte the y identifiation of the paamete. Using modified geometial model, we aied out an expeiment of deteting obstales. We seleted passageway in font of ou laboatoy fo the measuing envionment, beause poposed sensing system was loaded on mobile obot fo indoo use. The measuing envionment is shown by figue 9. In this figue, the lase slit fom RBS an be seen on a wall and a doo. (5) (7) (8) y mm x mm Figue 8. Measuing esult of inside of box afte paamete identifiation.

5 1000 y mm Figue 9. Measued Envionment x mm Figue 10. Result of deteting obstales Figue 10 shows a esult of an expeiment of deteting obstales. The developed measuing system is put at a position (0,0). The fou deteted points aound it ae esults of deteting the fou poles inluded in the measuing system. The points on the ight side of the oigin ae esults of deteting a box that is fixed in ode to put a ompute. This esult of expeiment shows the possibility of deteting obstales unde the eal envionment using ou developed system. 7 CONCLUSIONS We poposed a novel obstale detetion system using RBS (Ring Beam System), a spheial mio and CCD amea fo indoo use mobile obots. We showed the alulating method of distane to obstales and aied out the expeiment of deteting obstales. The esult of expeiment shows the possibility of deteting obstales using ou system, howeve, thee ae some eos fom paameti eos o geometial eos. Theefoe, we build anothe geometial model inlude geometial eos and identified paametes based on the esult of expeiment. Afte the identifiation of unknown paametes, we aied out the othe expeiment of deteting obstales and the esult of expeiment shows the possibility of deteting obstales aound this system simultaneously unde the eal envionment. REFERENCES [1] Y. Yagi, Real-time Omnidietional Image Sensos, Jounal of the Robotis Soiety of Japan 13 (3) (1995) (Japanese). [2] S. Kato and S. Tsugawa, Obstale Region Detetion Senso by Extended Slit-Ray Pojetion: Detetion Tehnique and Ahitetue fo a High-Speed Poessing Realization, Poeedings of the 5th Symposium on Robot Sensos (1996) 109 (Japanese). [3] Y. Kawaguhi, J. Mizuno and K. Ito, Piniple of Ring Beam System (R.B.S.) and Its Appliations, O plus E 210 (1997) (Japanese). AUTHORS: Reseah Assoiate D. Masahiko HIRAKI, Assoiate Pof. D. Kiyoshi TAKAMASU, Pof. D. Shigeo OZONO, Depatment of Peision Engineeing, Shool of Engineeing, The Univesity of Tokyo, Hongo, Bunkyo-ku, Tokyo, Japan, Phone Int , Fax Int , hiaki@ozono.pe.u-tokyo.a.jp

Photographing a time interval

Photographing a time interval Potogaping a time inteval Benad Rotenstein and Ioan Damian Politennia Univesity of imisoaa Depatment of Pysis imisoaa Romania benad_otenstein@yaoo.om ijdamian@yaoo.om Abstat A metod of measuing time intevals

More information

COMPARING MORE THAN TWO POPULATION MEANS: AN ANALYSIS OF VARIANCE

COMPARING MORE THAN TWO POPULATION MEANS: AN ANALYSIS OF VARIANCE COMPARING MORE THAN TWO POPULATION MEANS: AN ANALYSIS OF VARIANCE To see how the piniple behind the analysis of vaiane method woks, let us onside the following simple expeiment. The means ( 1 and ) of

More information

Determine the Stress Calculating Mode of Sliding Failure of Soil Mass under the Push-Extend Multi-under-Reamed Pile

Determine the Stress Calculating Mode of Sliding Failure of Soil Mass under the Push-Extend Multi-under-Reamed Pile Engineeing, 014, 6, 54-59 Published Online Apil 014 in SiRes. http://www.sip.og/jounal/eng http://dx.doi.og/10.436/eng.014.6509 Deteine the Stess Calulating Mode of Sliding Failue of Soil Mass unde the

More information

Vision Sensor. Vision. (Phase 1) pre-shaping. Actuator. Tactile Sensor. Vision. (Phase 2) shaping. Actuator. Tactile Sensor.

Vision Sensor. Vision. (Phase 1) pre-shaping. Actuator. Tactile Sensor. Vision. (Phase 2) shaping. Actuator. Tactile Sensor. Optimal Gasping using Visual and Tatile Feedbak Akio NAMIKI Masatoshi ISHIKAWA Depatment of Mathematial Engineeing and Infomation Physis Univesity of Tokyo Tokyo 3, Japan namik@k.t.u-tokyo.a.jp Abstat

More information

Physics 218, Spring March 2004

Physics 218, Spring March 2004 Today in Physis 8: eleti dipole adiation II The fa field Veto potential fo an osillating eleti dipole Radiated fields and intensity fo an osillating eleti dipole Total satteing oss setion of a dieleti

More information

From E.G. Haug Escape Velocity To the Golden Ratio at the Black Hole. Branko Zivlak, Novi Sad, May 2018

From E.G. Haug Escape Velocity To the Golden Ratio at the Black Hole. Branko Zivlak, Novi Sad, May 2018 Fom E.G. Haug Esape eloity To the Golden Ratio at the Blak Hole Banko Zivlak, bzivlak@gmail.om Novi Sad, May 018 Abstat Esape veloity fom the E.G. Haug has been heked. It is ompaed with obital veloity

More information

Red Shift and Blue Shift: A realistic approach

Red Shift and Blue Shift: A realistic approach Red Shift and Blue Shift: A ealisti appoah Benhad Rothenstein Politehnia Uniesity of Timisoaa, Physis Dept., Timisoaa, Romania E-mail: benhad_othenstein@yahoo.om Coina Nafonita Politehnia Uniesity of Timisoaa,

More information

Special Relativity in Acoustic and Electromagnetic Waves Without Phase Invariance and Lorentz Transformations 1. Introduction n k.

Special Relativity in Acoustic and Electromagnetic Waves Without Phase Invariance and Lorentz Transformations 1. Introduction n k. Speial Relativit in Aousti and Eletomagneti Waves Without Phase Invaiane and Loentz Tansfomations Benhad Rothenstein bothenstein@gmail.om Abstat. Tansfomation equations fo the phsial quantities intodued

More information

SKP-2 ALGORITHM: ON FORMING PART AND MACHINE CLUSTERS SEPARATELY

SKP-2 ALGORITHM: ON FORMING PART AND MACHINE CLUSTERS SEPARATELY Poeedings of the 1998 Paifi Confeene on Manufatuing, August 18-20, 1998, Bisbane, Queensland, Austalia SKP-2 ALGORITHM: ON FORMING PART AND MACHINE CLUSTERS SEPARATELY Susanto,S., Kennedy,R.D. and Pie,

More information

An analytic calculation method on air gap flux in permanent magnet. brushless DC motor with ironless rotor

An analytic calculation method on air gap flux in permanent magnet. brushless DC motor with ironless rotor Intenational Confeene on Enegy and Envionmental Potetion ICEEP 6 An analyti alulation method on ai gap flux in pemanent magnet bushless DC moto with ionless oto Xinghua Wang,Yaolong Sheng andshugang Zhao,,

More information

Recitation PHYS 131. must be one-half of T 2

Recitation PHYS 131. must be one-half of T 2 Reitation PHYS 131 Ch. 5: FOC 1, 3, 7, 10, 15. Pobles 4, 17, 3, 5, 36, 47 & 59. Ch 5: FOC Questions 1, 3, 7, 10 & 15. 1. () The eloity of a has a onstant agnitude (speed) and dietion. Sine its eloity is

More information

(conservation of momentum)

(conservation of momentum) Dynamis of Binay Collisions Assumptions fo elasti ollisions: a) Eletially neutal moleules fo whih the foe between moleules depends only on the distane between thei entes. b) No intehange between tanslational

More information

PLEASE DO NOT REMOVE THIS PAGE

PLEASE DO NOT REMOVE THIS PAGE Thank you fo downloading this doument fom the RMIT ReseahR Repositoy Citation: Davy, J, Mahn, J, Kaji, L, Waeing, R and Pease, J 205, 'Compaison of theoetial peditions of adiation effiieny with expeimental

More information

Extra Examples for Chapter 1

Extra Examples for Chapter 1 Exta Examples fo Chapte 1 Example 1: Conenti ylinde visomete is a devie used to measue the visosity of liquids. A liquid of unknown visosity is filling the small gap between two onenti ylindes, one is

More information

Revised Newtonian Formula of Gravity and Equation of Cosmology in Flat Space-Time Transformed from Schwarzschild Solution

Revised Newtonian Formula of Gravity and Equation of Cosmology in Flat Space-Time Transformed from Schwarzschild Solution Intenational Jounal of Astonomy and Astophysis,,, 6-8 http://dx.doi.og/.46/ijaa.. Published Online Mah (http://www.sip.og/jounal/ijaa) evised Newtonian Fomula of Gavity and Equation of Cosmology in Flat

More information

Experiment 1 Electric field and electric potential

Experiment 1 Electric field and electric potential Expeiment 1 Eleti field and eleti potential Pupose Map eleti equipotential lines and eleti field lines fo two-dimensional hage onfiguations. Equipment Thee sheets of ondutive papes with ondutive-ink eletodes,

More information

Lab 10: Newton s Second Law in Rotation

Lab 10: Newton s Second Law in Rotation Lab 10: Newton s Second Law in Rotation We can descibe the motion of objects that otate (i.e. spin on an axis, like a popelle o a doo) using the same definitions, adapted fo otational motion, that we have

More information

1 Fundamental Solutions to the Wave Equation

1 Fundamental Solutions to the Wave Equation 1 Fundamental Solutions to the Wave Equation Physial insight in the sound geneation mehanism an be gained by onsideing simple analytial solutions to the wave equation One example is to onside aousti adiation

More information

SAMPLE LABORATORY SESSION FOR JAVA MODULE B. Calculations for Sample Cross-Section 2

SAMPLE LABORATORY SESSION FOR JAVA MODULE B. Calculations for Sample Cross-Section 2 SAMPLE LABORATORY SESSION FOR JAVA MODULE B Calulations fo Sample Coss-Setion. Use Input. Setion Popeties The popeties of Sample Coss-Setion ae shown in Figue and ae summaized below. Figue : Popeties of

More information

Solving Problems of Advance of Mercury s Perihelion and Deflection of. Photon Around the Sun with New Newton s Formula of Gravity

Solving Problems of Advance of Mercury s Perihelion and Deflection of. Photon Around the Sun with New Newton s Formula of Gravity Solving Poblems of Advance of Mecuy s Peihelion and Deflection of Photon Aound the Sun with New Newton s Fomula of Gavity Fu Yuhua (CNOOC Reseach Institute, E-mail:fuyh945@sina.com) Abstact: Accoding to

More information

Natural Convection Heat Transfer Effects with Micro Finned Structures

Natural Convection Heat Transfer Effects with Micro Finned Structures Natual Convetion Heat Tansfe Effets with Mio Finned Stutues Saad MAHMOUD, Raya AL-DADAH*, David ASPINWALL, Leung SOO * Coesponding autho: Tel.: ++44(0)114143513; Fax: ++44(0)114143958; Email:.k.aldadah@bham.a.uk

More information

Time Dilation in Gravity Wells

Time Dilation in Gravity Wells Time Dilation in Gavity Wells By Rihad R. Shiffman Digital Gaphis Asso. 038 Dunkik Ave. L.A., Ca. 9005 s@isi.edu This doument disusses the geneal elativisti effet of time dilation aused by a spheially

More information

Special relativity with clock synchronization

Special relativity with clock synchronization Speial elativity with lok synhonization Benhad Rothenstein ), Stefan Popesu ) and Geoge J. Spi 3) ) Politehnia Univesity of Timisoaa, Physis Depatment, Timisoaa, Romania, benhad_othenstein@yahoo.om ) Siemens

More information

8.022 (E&M) Lecture 13. What we learned about magnetism so far

8.022 (E&M) Lecture 13. What we learned about magnetism so far 8.0 (E&M) Letue 13 Topis: B s ole in Mawell s equations Veto potential Biot-Savat law and its appliations What we leaned about magnetism so fa Magneti Field B Epeiments: uents in s geneate foes on hages

More information

APPLICATION OF MAC IN THE FREQUENCY DOMAIN

APPLICATION OF MAC IN THE FREQUENCY DOMAIN PPLICION OF MC IN HE FREQUENCY DOMIN D. Fotsch and D. J. Ewins Dynamics Section, Mechanical Engineeing Depatment Impeial College of Science, echnology and Medicine London SW7 2B, United Kingdom BSRC he

More information

Levitation force analysis of ring and disk shaped permanent magnet-high temperature superconductor

Levitation force analysis of ring and disk shaped permanent magnet-high temperature superconductor Inn Jounal of Pue & Applied Physics Vol. 55, Apil 017, pp. 61-68 Levitation foce analysis of ing and disk shaped pemanent magnet-high tempeatue supeconducto Sinan Basaan & Selim Sivioglu* Depatment of

More information

Physics 2020, Spring 2005 Lab 5 page 1 of 8. Lab 5. Magnetism

Physics 2020, Spring 2005 Lab 5 page 1 of 8. Lab 5. Magnetism Physics 2020, Sping 2005 Lab 5 page 1 of 8 Lab 5. Magnetism PART I: INTRODUCTION TO MAGNETS This week we will begin wok with magnets and the foces that they poduce. By now you ae an expet on setting up

More information

COLLAPSING WALLS THEOREM

COLLAPSING WALLS THEOREM COLLAPSING WALLS THEOREM IGOR PAK AND ROM PINCHASI Abstact. Let P R 3 be a pyamid with the base a convex polygon Q. We show that when othe faces ae collapsed (otated aound the edges onto the plane spanned

More information

The geometric construction of Ewald sphere and Bragg condition:

The geometric construction of Ewald sphere and Bragg condition: The geometic constuction of Ewald sphee and Bagg condition: The constuction of Ewald sphee must be done such that the Bagg condition is satisfied. This can be done as follows: i) Daw a wave vecto k in

More information

effective pinhole, p=(0,c)

effective pinhole, p=(0,c) Appeaed in the Poeedings of the 6th Intenational Confeene on Compute Vision, Bombay, Januay 1998. A Theoy of Catadiopti Image Fomation Simon Bake and Shee K. Naya Depatment of Compute Siene Columbia Univesity

More information

Non-Ideal Gas Behavior P.V.T Relationships for Liquid and Solid:

Non-Ideal Gas Behavior P.V.T Relationships for Liquid and Solid: hemodynamis Non-Ideal Gas Behavio.. Relationships fo Liquid and Solid: An equation of state may be solved fo any one of the thee quantities, o as a funtion of the othe two. If is onsideed a funtion of

More information

Force between two parallel current wires and Newton s. third law

Force between two parallel current wires and Newton s. third law Foce between two paallel cuent wies and Newton s thid law Yannan Yang (Shanghai Jinjuan Infomation Science and Technology Co., Ltd.) Abstact: In this pape, the essence of the inteaction between two paallel

More information

11.2 Proving Figures are Similar Using Transformations

11.2 Proving Figures are Similar Using Transformations Name lass ate 11. Poving igues ae Simila Using Tansfomations ssential Question: How can similait tansfomations be used to show two figues ae simila? esouce ocke ploe onfiming Similait similait tansfomation

More information

Dissolution of Solid Particles in Liquids: A Shrinking Core Model

Dissolution of Solid Particles in Liquids: A Shrinking Core Model Wold Aademy of Siene, Engineeing and Tehnology 5 9 Dissolution of Solid Patiles in Liquids: A Shining oe Model Wei-Lun Hsu, Mon-Jyh Lin, and Jyh-Ping Hsu Astat The dissolution of spheial patiles in liquids

More information

Dynamic Visualization of Complex Integrals with Cabri II Plus

Dynamic Visualization of Complex Integrals with Cabri II Plus Dynamic Visualiation of omplex Integals with abi II Plus Sae MIKI Kawai-juu, IES Japan Email: sand_pictue@hotmailcom Abstact: Dynamic visualiation helps us undestand the concepts of mathematics This pape

More information

1 Fundamental Solutions to the Wave Equation

1 Fundamental Solutions to the Wave Equation 1 Fundamental Solutions to the Wave Equation Physial insight in the sound geneation mehanism an be gained by onsideing simple analytial solutions to the wave equation. One example is to onside aousti adiation

More information

e sin cos i sin sin j cos k [2 POINTS] (c) Hence, determine expressions for sin sin i sin cos j sin e

e sin cos i sin sin j cos k [2 POINTS] (c) Hence, determine expressions for sin sin i sin cos j sin e EN: Continuum Mehanis Homewok : Kinematis Due : noon Fiday Febuay 4th Shool of Engineeing Bown Univesity. To analyze the defomation of a onial membane, it is poposed to use a two-dimensional onial-pola

More information

Position Error Estimation of a Laser Illuminated Object

Position Error Estimation of a Laser Illuminated Object SCIENTIFIC PUBLICATIONS OF THE STATE UNIVERSITY OF NOVI PAZAR SER. A: APPL. MATH. INFORM. AND MECH. vol. 3, 1 (2011, 59-69 Position Eo Estimation of a Lase Illuminated Object Ž. P. Babaić Abstact: Position

More information

A NEW VARIABLE STIFFNESS SPRING USING A PRESTRESSED MECHANISM

A NEW VARIABLE STIFFNESS SPRING USING A PRESTRESSED MECHANISM Poceedings of the ASME 2010 Intenational Design Engineeing Technical Confeences & Computes and Infomation in Engineeing Confeence IDETC/CIE 2010 August 15-18, 2010, Monteal, Quebec, Canada DETC2010-28496

More information

A Comment on Increasing Returns and Spatial. Unemployment Disparities

A Comment on Increasing Returns and Spatial. Unemployment Disparities The Society fo conomic Studies The nivesity of Kitakyushu Woking Pape Seies No.06-5 (accepted in Mach, 07) A Comment on Inceasing Retuns and Spatial nemployment Dispaities Jumpei Tanaka ** The nivesity

More information

7.2.1 Basic relations for Torsion of Circular Members

7.2.1 Basic relations for Torsion of Circular Members Section 7. 7. osion In this section, the geomety to be consideed is that of a long slende cicula ba and the load is one which twists the ba. Such poblems ae impotant in the analysis of twisting components,

More information

Investigation of the Centrifugal Force Effect to a Revolving Vane (RV) Machine

Investigation of the Centrifugal Force Effect to a Revolving Vane (RV) Machine Pudue Univesity Pudue e-pubs Intenational Compesso Engineeing Confeene Shool of Mehanial Engineeing 01 Investigation of the Centifugal oe Effet to a Revolving Vane (RV) Mahine Alison Subiantoo alis0004@ntu.edu.sg

More information

COMPUTATIONS OF ELECTROMAGNETIC FIELDS RADIATED FROM COMPLEX LIGHTNING CHANNELS

COMPUTATIONS OF ELECTROMAGNETIC FIELDS RADIATED FROM COMPLEX LIGHTNING CHANNELS Pogess In Electomagnetics Reseach, PIER 73, 93 105, 2007 COMPUTATIONS OF ELECTROMAGNETIC FIELDS RADIATED FROM COMPLEX LIGHTNING CHANNELS T.-X. Song, Y.-H. Liu, and J.-M. Xiong School of Mechanical Engineeing

More information

THEORETICAL AND EXPERIMENTAL STUDY ON DROPWISE CONDENSATION IN PLATE HEAT EXCHANGERS

THEORETICAL AND EXPERIMENTAL STUDY ON DROPWISE CONDENSATION IN PLATE HEAT EXCHANGERS Abstat THEORETICAL AND EXPERIMENTAL STUDY ON DROPWISE CONDENSATION IN PLATE HEAT EXCHANGERS V. Bendt, S. Zunft and H. Mülle-Steinhagen Geman Aeospae Cente (DLR), Stuttgat, Gemany This pape desibes the

More information

Discrete-Time Immersion and Invariance Adaptive Control of a Slider-crank Mechanism

Discrete-Time Immersion and Invariance Adaptive Control of a Slider-crank Mechanism Pepints of the 9th Wold Congess he Intenational Fedeation of Automati Contol Cape own South Afia August -9 0 Disete-ime Immesion and Invaiane Adaptive Contol of a Slide-an Mehanism Yapa Yalçın Dept of

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

Correspondence Analysis & Related Methods

Correspondence Analysis & Related Methods Coespondene Analysis & Related Methods Oveview of CA and basi geometi onepts espondents, all eades of a etain newspape, osstabulated aoding to thei eduation goup and level of eading of the newspape Mihael

More information

REVIEW Polar Coordinates and Equations

REVIEW Polar Coordinates and Equations REVIEW 9.1-9.4 Pola Coodinates and Equations You ae familia with plotting with a ectangula coodinate system. We ae going to look at a new coodinate system called the pola coodinate system. The cente of

More information

What Form of Gravitation Ensures Weakened Kepler s Third Law?

What Form of Gravitation Ensures Weakened Kepler s Third Law? Bulletin of Aichi Univ. of Education, 6(Natual Sciences, pp. - 6, Mach, 03 What Fom of Gavitation Ensues Weakened Keple s Thid Law? Kenzi ODANI Depatment of Mathematics Education, Aichi Univesity of Education,

More information

Eddy Currents and Magnetic Calibrations in LDX using a Copper Plasma. D.P. Boyle, PPPL M.E. Mauel, D.T. Garnier, Columbia J.

Eddy Currents and Magnetic Calibrations in LDX using a Copper Plasma. D.P. Boyle, PPPL M.E. Mauel, D.T. Garnier, Columbia J. Eddy Cuents and Magneti Calibations in LDX using a Coppe Plasma D.P. Boyle PPPL M.E. Mauel D.T. Ganie Columbia J. Kesne MIT PSFC Coppe Plasma Oveview LDX Magnetis Goals Calibate magneti diagnostis positions

More information

A near-perfect invisibility cloak constructed with homogeneous materials

A near-perfect invisibility cloak constructed with homogeneous materials A nea-pefet invisibility loak onstuted with homogeneous mateials Wei Li, Jianguo Guan, * Zhigang Sun, Wei Wang, and Qingjie Zhang 1 State Key Lab of Advaned Tehnology fo Mateials Synthesis and Poessing,

More information

AVS fiziks. Institute for NET/JRF, GATE, IIT-JAM, JEST, TIFR and GRE in PHYSICAL SCIENCES

AVS fiziks. Institute for NET/JRF, GATE, IIT-JAM, JEST, TIFR and GRE in PHYSICAL SCIENCES ELECTROMAGNETIC THEORY SOLUTIONS GATE- Q. An insulating sphee of adius a aies a hage density a os ; a. The leading ode tem fo the eleti field at a distane d, fa away fom the hage distibution, is popotional

More information

Electromagnetic Noise Source Approximation for Finite- Difference Time-Domain Modeling Using Near-Field Scanning and Particle Swarm Optimization

Electromagnetic Noise Source Approximation for Finite- Difference Time-Domain Modeling Using Near-Field Scanning and Particle Swarm Optimization Eletomagneti Noise Soue Appoximation fo Finite- Diffeene Time-Domain Modeling Using Nea-Field Sanning and Patile Swam Optimization Autho Siven, Ian, Lu, Junwei, Lewis, Andew Published 2010 Jounal Title

More information

KOEBE DOMAINS FOR THE CLASSES OF FUNCTIONS WITH RANGES INCLUDED IN GIVEN SETS

KOEBE DOMAINS FOR THE CLASSES OF FUNCTIONS WITH RANGES INCLUDED IN GIVEN SETS Jounal of Applied Analysis Vol. 14, No. 1 2008), pp. 43 52 KOEBE DOMAINS FOR THE CLASSES OF FUNCTIONS WITH RANGES INCLUDED IN GIVEN SETS L. KOCZAN and P. ZAPRAWA Received Mach 12, 2007 and, in evised fom,

More information

The Radii of Baryons

The Radii of Baryons Jounal Heading Yea; Vol. (No.): page ange DOI: 0.592/j.xxx.xxxxxxxx.xx The Radii of Bayons Maio Evealdo de Souza Depatmento de Físia, Univesidade Fedeal de Segipe, São Cistovão, 4900-000, Bazil Astat Consideing

More information

Mathematisch-Naturwissenschaftliche Fakultät I Humboldt-Universität zu Berlin Institut für Physik Physikalisches Grundpraktikum.

Mathematisch-Naturwissenschaftliche Fakultät I Humboldt-Universität zu Berlin Institut für Physik Physikalisches Grundpraktikum. Mathematisch-Natuwissenschaftliche Fakultät I Humboldt-Univesität zu Belin Institut fü Physik Physikalisches Gundpaktikum Vesuchspotokoll Polaisation duch Reflexion (O11) duchgefüht am 10.11.2009 mit Vesuchspatne

More information

Psychometric Methods: Theory into Practice Larry R. Price

Psychometric Methods: Theory into Practice Larry R. Price ERRATA Psychometic Methods: Theoy into Pactice Lay R. Pice Eos wee made in Equations 3.5a and 3.5b, Figue 3., equations and text on pages 76 80, and Table 9.1. Vesions of the elevant pages that include

More information

QUALITATIVE AND QUANTITATIVE ANALYSIS OF MUSCLE POWER

QUALITATIVE AND QUANTITATIVE ANALYSIS OF MUSCLE POWER QUALITATIVE AND QUANTITATIVE ANALYSIS OF MUSCLE POWER Jey N. Baham Anand B. Shetty Mechanical Kinesiology Laboatoy Depatment of Kinesiology Univesity of Nothen Coloado Geeley, Coloado Muscle powe is one

More information

Answers to Coursebook questions Chapter 2.11

Answers to Coursebook questions Chapter 2.11 Answes to Couseook questions Chapte 11 1 he net foe on the satellite is F = G Mm and this plays the ole of the entipetal foe on the satellite, ie mv mv Equating the two gives π Fo iula motion we have that

More information

On the integration of the equations of hydrodynamics

On the integration of the equations of hydrodynamics Uebe die Integation de hydodynamischen Gleichungen J f eine u angew Math 56 (859) -0 On the integation of the equations of hydodynamics (By A Clebsch at Calsuhe) Tanslated by D H Delphenich In a pevious

More information

3.6 Applied Optimization

3.6 Applied Optimization .6 Applied Optimization Section.6 Notes Page In this section we will be looking at wod poblems whee it asks us to maimize o minimize something. Fo all the poblems in this section you will be taking the

More information

IMPLEMENTATION OF MUR S ABSORBING BOUNDARIES WITH PERIODIC STRUCTURES TO SPEED UP THE DESIGN PROCESS USING FINITE-DIFFERENCE TIME-DOMAIN METHOD

IMPLEMENTATION OF MUR S ABSORBING BOUNDARIES WITH PERIODIC STRUCTURES TO SPEED UP THE DESIGN PROCESS USING FINITE-DIFFERENCE TIME-DOMAIN METHOD Pogess In Eletomagnetis Reseah, PIER 58, 101 114, 006 IMPLEMENTATION OF MUR S ABSORBING BOUNDARIES WITH PERIODIC STRUCTURES TO SPEED UP THE DESIGN PROCESS USING FINITE-DIFFERENCE TIME-DOMAIN METHOD G.

More information

LIST OF EQUIPMENT SET UP AND PROCEDURE 3B SCIENTIFIC PHYSICS EXPERIMENT

LIST OF EQUIPMENT SET UP AND PROCEDURE 3B SCIENTIFIC PHYSICS EXPERIMENT UE104005 (3) T J D D: Tosional coefficient of coil spings The means that the peiod of oscillation T will be geate when the moment of inetia J is lage. Fom equation (3) it is possible to obtain a fomula

More information

Question 1: The dipole

Question 1: The dipole Septembe, 08 Conell Univesity, Depatment of Physics PHYS 337, Advance E&M, HW #, due: 9/5/08, :5 AM Question : The dipole Conside a system as discussed in class and shown in Fig.. in Heald & Maion.. Wite

More information

The Research of AQI Index Changing Regularity Mainly in Tianjin Ziyu Guo

The Research of AQI Index Changing Regularity Mainly in Tianjin Ziyu Guo nd Intenational Confeene on Eduation Tehnology, Management and Humanities Siene (ETMHS 06 The Reseah of AQI Index Changing Regulaity Mainly in Tianjin Ziyu Guo Shool of Institute of Eletial and Eletoni

More information

Geometry of the homogeneous and isotropic spaces

Geometry of the homogeneous and isotropic spaces Geomety of the homogeneous and isotopic spaces H. Sonoda Septembe 2000; last evised Octobe 2009 Abstact We summaize the aspects of the geomety of the homogeneous and isotopic spaces which ae most elevant

More information

PHYS 110B - HW #7 Fall 2005, Solutions by David Pace Equations referenced as Eq. # are from Griffiths Problem statements are paraphrased

PHYS 110B - HW #7 Fall 2005, Solutions by David Pace Equations referenced as Eq. # are from Griffiths Problem statements are paraphrased PHYS B - HW #7 Fall 5, Solutions by David Pae Equations efeened as Eq. # ae fom Giffiths Poblem statements ae paaphased [.] Poblem.4 fom Giffiths Show that Eq..4, V, t an be witten as Eq..44, V, t q t

More information

On Rotating Frames and the Relativistic Contraction of the Radius (The Rotating Disc)

On Rotating Frames and the Relativistic Contraction of the Radius (The Rotating Disc) On Rotating Fames and the Relativisti Contation of the Radius (The Rotating Dis) Pantelis M. Pehlivanides Atlanti IKE, Athens 57, Geee ppexl@teemail.g Abstat The elativisti poblem of the otating dis o

More information

Mass- and light-horizons, black holes' radii, the Schwartzschild metric and the Kerr metric

Mass- and light-horizons, black holes' radii, the Schwartzschild metric and the Kerr metric 006-010 Thiey De Mees Mass- and light-hoizons, blak holes' adii, the Shwatzshild meti and the Ke meti mpoved alulus. (using gavitomagnetism) T. De Mees - thieydm@pandoa.be Abstat Blak holes geneally ae

More information

Fresnel Diffraction. monchromatic light source

Fresnel Diffraction. monchromatic light source Fesnel Diffaction Equipment Helium-Neon lase (632.8 nm) on 2 axis tanslation stage, Concave lens (focal length 3.80 cm) mounted on slide holde, iis mounted on slide holde, m optical bench, micoscope slide

More information

Radian and Degree Measure

Radian and Degree Measure CHAT Pe-Calculus Radian and Degee Measue *Tigonomety comes fom the Geek wod meaning measuement of tiangles. It pimaily dealt with angles and tiangles as it petained to navigation, astonomy, and suveying.

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

Graphs of Sine and Cosine Functions

Graphs of Sine and Cosine Functions Gaphs of Sine and Cosine Functions In pevious sections, we defined the tigonometic o cicula functions in tems of the movement of a point aound the cicumfeence of a unit cicle, o the angle fomed by the

More information

Suppose you have a bank account that earns interest at rate r, and you have made an initial deposit of X 0

Suppose you have a bank account that earns interest at rate r, and you have made an initial deposit of X 0 IOECONOMIC MODEL OF A FISHERY (ontinued) Dynami Maximum Eonomi Yield In ou deivation of maximum eonomi yield (MEY) we examined a system at equilibium and ou analysis made no distintion between pofits in

More information

Liquid gas interface under hydrostatic pressure

Liquid gas interface under hydrostatic pressure Advances in Fluid Mechanics IX 5 Liquid gas inteface unde hydostatic pessue A. Gajewski Bialystok Univesity of Technology, Faculty of Civil Engineeing and Envionmental Engineeing, Depatment of Heat Engineeing,

More information

4. Some Applications of first order linear differential

4. Some Applications of first order linear differential August 30, 2011 4-1 4. Some Applications of fist ode linea diffeential Equations The modeling poblem Thee ae seveal steps equied fo modeling scientific phenomena 1. Data collection (expeimentation) Given

More information

Designing a Sine-Coil for Measurement of Plasma Displacements in IR-T1 Tokamak

Designing a Sine-Coil for Measurement of Plasma Displacements in IR-T1 Tokamak Designing a Sine-Coil fo Measuement of Plasma Displacements in IR-T Tokamak Pejman Khoshid, M. Razavi, M. Ghoanneviss, M. Molaii, A. TalebiTahe, R. Avin, S. Mohammadi and A. NikMohammadi Dept. of Physics,

More information

Ultrafast effects in 3D Metamaterials

Ultrafast effects in 3D Metamaterials Ultafast effects in 3D Metamateials Nkoni Katte,2 and Philip G.Evans 3 Electical Engineeing Wilbefoce Univesity, 2 Sensos Laboatoy Wight State Univesity and 3 Oak idge National Laboatoy *Coesponding autho:

More information

radians). Figure 2.1 Figure 2.2 (a) quadrant I angle (b) quadrant II angle is in standard position Terminal side Terminal side Terminal side

radians). Figure 2.1 Figure 2.2 (a) quadrant I angle (b) quadrant II angle is in standard position Terminal side Terminal side Terminal side . TRIGONOMETRIC FUNCTIONS OF GENERAL ANGLES In ode to etend the definitions of the si tigonometic functions to geneal angles, we shall make use of the following ideas: In a Catesian coodinate sstem, an

More information

3D Modelling of Temperature Dependent Power Distribution During Microwave Annealing of Doped c-si

3D Modelling of Temperature Dependent Power Distribution During Microwave Annealing of Doped c-si IOSR Jounal of Eletial and Eletonis Engineeing (IOSR-JEEE) e-issn: 2278-1676,p-ISSN: 2320-3331, Volume 9, Issue 1 Ve. V (Feb. 2014), PP 46-51 3D Modelling of Tempeatue Dependent Powe Distibution Duing

More information

INTEGRATION OF THE SELF-ORGANIZING MAP AND NEURAL GAS WITH MULTIDIMENSIONAL SCALING

INTEGRATION OF THE SELF-ORGANIZING MAP AND NEURAL GAS WITH MULTIDIMENSIONAL SCALING ISSN 39 4X INFORMATION TECHNOLOGY AND CONTROL, 0, Vol.40, No. INTEGRATION OF THE SELF-ORGANIZING MAP AND NEURAL GAS WITH MULTIDIMENSIONAL SCALING Olga Kuasova, Alma Molytė Vilnius Univesity, Institute

More information

9.1 POLAR COORDINATES

9.1 POLAR COORDINATES 9. Pola Coodinates Contempoay Calculus 9. POLAR COORDINATES The ectangula coodinate system is immensely useful, but it is not the only way to assign an addess to a point in the plane and sometimes it is

More information

In electrostatics, the electric field E and its sources (charges) are related by Gauss s law: Surface

In electrostatics, the electric field E and its sources (charges) are related by Gauss s law: Surface Ampee s law n eletostatis, the eleti field E and its soues (hages) ae elated by Gauss s law: EdA i 4πQenl Sufae Why useful? When symmety applies, E an be easily omputed Similaly, in magnetism the magneti

More information

EFFECTS OF FRINGING FIELDS ON SINGLE PARTICLE DYNAMICS. M. Bassetti and C. Biscari INFN-LNF, CP 13, Frascati (RM), Italy

EFFECTS OF FRINGING FIELDS ON SINGLE PARTICLE DYNAMICS. M. Bassetti and C. Biscari INFN-LNF, CP 13, Frascati (RM), Italy Fascati Physics Seies Vol. X (998), pp. 47-54 4 th Advanced ICFA Beam Dynamics Wokshop, Fascati, Oct. -5, 997 EFFECTS OF FRININ FIELDS ON SINLE PARTICLE DYNAMICS M. Bassetti and C. Biscai INFN-LNF, CP

More information

DARK MATTER AND THE DYNAMICS OF GALAXIES: A NEWTONIAN APPROACH 1. INTRODUCTION

DARK MATTER AND THE DYNAMICS OF GALAXIES: A NEWTONIAN APPROACH 1. INTRODUCTION DARK MATTER AND THE DYNAMICS OF GALAXIES: A NEWTONIAN APPROACH Mugu B. RĂUŢ Coesponding autho: Mugu RĂUŢ, E-mail: m_b_aut@yahoo.om Abstat In this pape I popose a oetion to the well-known Newtonian gavitational

More information

Investigation of Magnitude and Phase Errors in Waveguide Samples for the Nicolson-Ross-Weir Permittivity Technique

Investigation of Magnitude and Phase Errors in Waveguide Samples for the Nicolson-Ross-Weir Permittivity Technique Univesity of New Hampshie Univesity of New Hampshie Sholas' Repositoy Maste's Theses and Capstones Student Sholaship Winte 016 Investigation of Magnitude and Phase Eos in Waveguide Samples fo the Niolson-Ross-Wei

More information

Mass Transfer (Stoffaustausch)

Mass Transfer (Stoffaustausch) Mass Tansfe (Stoffaustaush) Examination 3. August 3 Name: Legi-N.: Edition Diffusion by E. L. Cussle: none nd 3 d Test Duation: minutes The following mateials ae not pemitted at you table and have to be

More information

Phys 201A. Homework 5 Solutions

Phys 201A. Homework 5 Solutions Phys 201A Homewok 5 Solutions 3. In each of the thee cases, you can find the changes in the velocity vectos by adding the second vecto to the additive invese of the fist and dawing the esultant, and by

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

THE DETERMINATION OF THE EFFICIENCY OF OPTICAL FIBRE SENSORS

THE DETERMINATION OF THE EFFICIENCY OF OPTICAL FIBRE SENSORS Jounal of Optoelectonics and Advanced Mateials Vol. 3, No. 1, Mach 001, p. 65-74 THE DETERMINATION OF THE EFFICIENCY OF OPTICAL FIBRE SENSORS M. A. Chita, S. Anghel a, I. Ioga-Siman a, I. Vlad b Electonics

More information

Σk=1. g r 3/2 z. 2 3-z. g 3 ( 3/2 ) g r 2. = 1 r = 0. () z = ( a ) + Σ. c n () a = ( a) 3-z -a. 3-z. z - + Σ. z 3, 5, 7, z ! = !

Σk=1. g r 3/2 z. 2 3-z. g 3 ( 3/2 ) g r 2. = 1 r = 0. () z = ( a ) + Σ. c n () a = ( a) 3-z -a. 3-z. z - + Σ. z 3, 5, 7, z ! = ! 09 Maclauin Seies of Completed Riemann Zeta 9. Maclauin Seies of Lemma 9.. ( Maclauin seies of gamma function ) When is the gamma function, n is the polygamma function and B n,kf, f, ae Bell polynomials,

More information

MASSACHUSETTS INSTITUTE OF TECHNOLOGY Physics Department. Problem Set 10 Solutions. r s

MASSACHUSETTS INSTITUTE OF TECHNOLOGY Physics Department. Problem Set 10 Solutions. r s MASSACHUSETTS INSTITUTE OF TECHNOLOGY Physics Depatment Physics 8.033 Decembe 5, 003 Poblem Set 10 Solutions Poblem 1 M s y x test paticle The figue above depicts the geomety of the poblem. The position

More information

FORMATION FLYING DYNAMICS OF MICRO- SATELLITES NEAR EQUATORIAL LOW ORBITS UNDER THE INFLUENCE OF J2 AND J3

FORMATION FLYING DYNAMICS OF MICRO- SATELLITES NEAR EQUATORIAL LOW ORBITS UNDER THE INFLUENCE OF J2 AND J3 IAA-AAS-DyCoSS-14-08-09 FORMATION FLYING DYNAMICS OF MICRO- SATELLITES NEAR EQUATORIAL LOW ORBITS UNDER THE INFLUENCE OF J AND J Haijono Djojodihadjo 1 The pesent wok assess the effet of the Eath s oblateness

More information

Aspects of Modelling: Examples from Consideration of Unusual Movements. in Crash Simulation

Aspects of Modelling: Examples from Consideration of Unusual Movements. in Crash Simulation Examples fom Consideation of Unusual Movements Univ.-Pof. D.-Ing. Matin Meywek Depatment of Automotive and Powe Tain Engineeing Helmut-Schmidt-Univesity Univesity of the Fedeal Amed Foces, Hambug 1/17

More information

Solving Some Definite Integrals Using Parseval s Theorem

Solving Some Definite Integrals Using Parseval s Theorem Ameican Jounal of Numeical Analysis 4 Vol. No. 6-64 Available online at http://pubs.sciepub.com/ajna///5 Science and Education Publishing DOI:.69/ajna---5 Solving Some Definite Integals Using Paseval s

More information

Section 8.2 Polar Coordinates

Section 8.2 Polar Coordinates Section 8. Pola Coodinates 467 Section 8. Pola Coodinates The coodinate system we ae most familia with is called the Catesian coodinate system, a ectangula plane divided into fou quadants by the hoizontal

More information

Supporting Information. and NaCl at the Air/Aqueous Interface revealed by Heterodyne Detected. Phase-Sensitive Sum Frequency

Supporting Information. and NaCl at the Air/Aqueous Interface revealed by Heterodyne Detected. Phase-Sensitive Sum Frequency Suppoting Infomation lectic Field Revesal of Na SO 4, (NH 4 ) SO 4, and Na CO 3 elative to CaCl and NaCl at the Ai/Aqueous Inteface evealed by Heteodyne Detected Phase-Sensitive Sum Fequency Wei Hua, Aaon

More information

DonnishJournals

DonnishJournals DonnishJounals 041-1189 Donnish Jounal of Educational Reseach and Reviews. Vol 1(1) pp. 01-017 Novembe, 014. http:///dje Copyight 014 Donnish Jounals Oiginal Reseach Pape Vecto Analysis Using MAXIMA Savaş

More information

Conservation of Angular Momentum

Conservation of Angular Momentum 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 0 1 1 1 1 1 1 1 Consevation of Angula Momentum Pupose: To investigate consevation of angula momentum by diectly measuing the moment of inetia and angula velocities

More information

Assessment of the impact of calculation methodologies on defect determinations in manufacturing

Assessment of the impact of calculation methodologies on defect determinations in manufacturing iginal Aticle HME Poceedings of IDMME - Vitual Concept 2010 Bodeaux, Fance, ctobe 20 22, 2010 Assessment of the impact of calculation ologies on defect deteminations in manufactuing Bui-Minh H. 1, Segent

More information