User s Guide NBC 2005, Structural Commentaries (Part 4 of Division B)
|
|
- Roxanne Rice
- 5 years ago
- Views:
Transcription
1 Ue Guide NBC 2005, Stutual Commentaie (Pat 4 of Diviion B) Eata Iued by the Canadian Commiion on Building and Fie Code The table that follow lit eata that apply to the Ue Guide NBC 2005, Stutual Commentaie (Pat 4 of Diviion B). The eata ae oetion that have been identified; they ae povided to failitate the ue of the Stutual Commentaie. Cetain page fom the Ue Guide have been updated fo you onveniene; they ae povided following the table. Contat you loal authoity having juidition to find out if thee eata apply in you povine o teitoy. Poviion Commentay G Figue G-8 Commentay I Figue I-2, I-3 and I-4 Eatum The eond Figue Note wa oeted to ead a follow: (2) If b i le than 3S /γ, in m, then the effet of the obtution on the now loading an be ignoed. The following text wa added at the end of the Figue title: (Repodued with the pemiion of the National Capital Commiion NCC/CCN) Date of Iue Figue I-5 The following text wa added at the end of the Figue title: (Repodued with the pemiion of The Heliopte Company In., Toonto, Canada, 2003) Paagaph 22 The equation in the eond entene of the example at the end of the paagaph wa oeted to ead: δ = 5 x 10-5 m 3 /N Figue I-7 Thi Figue wa eplaed with the one on the following page: -1-
2 Figue I-7 Extenal peak ompoite peue-gut oeffiient, CpCg, fo pimay tutual ation aiing fom wind load ating imultaneouly on all ufae -2-
3 Poviion Commentay I (ontinued) Eatum Date of Iue Figue I-11 Thi Figue wa eplaed with the following one: α 7 < α 45 H efeene height, h α 7 < α 27 h oof with ovehang oof without ovehang gable and hip oof 7 < α gable oof 27 < α CpCg C o o o CpCg o o o Aea, m 2 Aea, m 2 EG00924C -3-
4 Poviion Commentay J Eatum Date of Iue Figue J-7 Thi Figue wa eplaed with the following one: Paagaph 205 The following text wa deleted fom the lat entene: the ue of apaity deign piniple fo dutile tutue i peified in the CSA mateial tandad fo onete (CSA A23.3 [49] ), teel (CAN/CSA-S16 [61] ), maony (CSA S304.1 [78] ), and wood (CAN/CSA-O86 [47] ); Refeene Commentay K The tandad deignation in efeene numbe [42] wa oeted to ead CAN/CSA-S6-00 Paagaph 10 The efeene to Figue K-3 wa oeted to ead Figue K-1 Commentay L Paagaph 27 The wod load in the title and in the fit entene wa hanged to effet -4-
5 Commentay I Load ae A: wind geneally pependiula to idge H (8) 3E 4 2 4E 2E H oof lope 1 B 1E Refeene height (h) (5) y (6) wind dietion ange Roof lope 0 to to Building ufae 1 1E 2 2E 3 3E 4 4E Load ae B: wind geneally paallel to idge 3E E 4E 2E oof lope 1 5 1E 5E y (6) Z (7) wind dietion ange Roof lope 0 to 90 Building ufae 1 1E 2 2E 3 3E 4 4E 5 5E 6 6E EG00920B Figue I-7 Extenal peak ompoite peue-gut oeffiient, C p C g, fo pimay tutual ation aiing fom wind load ating imultaneouly on all ufae Ue Guide NBC 2005 Stutual Commentaie (Pat 4 of Diviion B) (Updated page ) I-13
6
7 Commentay I α 7 < α 45 H efeene height, h α 7 < α 27 h oof with ovehang oof without ovehang gable and hip oof 7 < α gable oof 27 < α CpCg C o o o CpCg o o o Aea, m 2 Aea, m 2 EG00924C Figue I-11 Extenal peak ompoite peue-gut oeffiient, C p C g, on ingle-pan gabled and hipped oof with a lope of 7 o geate fo the deign of tutual omponent and ladding Note to Figue I-11: (1) Coeffiient fo ovehung oof have the pefix o and efe to the ame oof aea a efeed to by the oeponding ymbol without a pefix. They inlude ontibution fom both uppe and lowe ufae. [24][44] (2) The abia aea in the gaph i the deign tibutay aea within the peified one. (3) End-one width i the lee of 10% of the leat hoiontal dimenion and 40% of height, H, but not le than 4% of the leat hoiontal dimenion o 1 m. (4) Combination of exteio and inteio peue mut be evaluated to obtain the mot evee loading. (5) Poitive oeffiient denote foe towad the ufae, wheea negative oeffiient denote foe away fom the ufae. Eah tutual element mut be deigned to withtand the foe of both ign. (6) Fo hipped oof with 7 < α 27, edge/idge tip and peue-gut oeffiient fo idge of gabled oof apply along eah hip. [45] Ue Guide NBC 2005 Stutual Commentaie (Pat 4 of Diviion B) (Updated page ) I-17
8
9 Commentay J a t 4H Soil ρ, β T 1 = H V, V a 0 ρ, V Rok EG00991B Figue J-7 Elati laye on elati half-pae Nonlinea Site Amplifiation 67. Unde tong haking, the epone of the oil will be nonlinea. The hea modulu and damping ae tain dependent and theefoe the lage tain, aoiated with tong haking, edue the effetive hea moduli and ineae the damping. The hea tength of the oil alo put a limitation on the magnitude of the ufae aeleation beaue the eimi wave annot geneate hea tee geate than the mobilied heaing eitane of the oil. Field evidene how that the nonlinea behaviou of oil aue the gound motion amplifiation fato to be dependent on the intenity of haking. 68. In Figue J-8, Idi [31] ha onveniently ummaied the nonlinea elationhip between peak aeleation on oft oil ite and thoe on aoiated bedok ite. The median uve i baed on data eoded in Mexio City duing the 1985 Mihoaan eathquake and on tong motion data fom the 1989 Loma Pieta eathquake. The pat of the median uve fo peak ok aeleation geate than 0.2g i baed on 1-D ite epone analye uing the SHAKE ompute pogam (Shnabel et al. [32] ). The uve ugget that, on aveage, the bedok aeleation ae amplified in oft oil until the peak ok aeleation eah about 0.4g. The highe amplifiation atio between ok and oil ite, in the ange of 1.5 4, ae aoiated with ok aeleation level of le than 0.10g, when the epone i loe to being elati. The ineaed nonlineaity of oft oil epone at the highe aeleation edue the amplifiation atio beaue of the ineae in hyteeti damping and the edution in effetive hea moduli. J-18 (Updated page ) Ue Guide NBC 2005 Stutual Commentaie (Pat 4 of Diviion B)
Circular Motion Problem Solving
iula Motion Poblem Soling Aeleation o a hange in eloity i aued by a net foe: Newton nd Law An objet aeleate when eithe the magnitude o the dietion of the eloity hange We aw in the lat unit that an objet
More informationNon-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 informationExperiment 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 informationThen the number of elements of S of weight n is exactly the number of compositions of n into k parts.
Geneating Function In a geneal combinatoial poblem, we have a univee S of object, and we want to count the numbe of object with a cetain popety. Fo example, if S i the et of all gaph, we might want to
More informationTheory. Single Soil Layer. ProShake User s Manual
PoShake Ue Manual Theoy PoShake ue a fequency domain appoach to olve the gound epone poblem. In imple tem, the input motion i epeented a the um of a eie of ine wave of diffeent amplitude, fequencie, and
More informationSAMPLE 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 informationHow can you find the dimensions of a square or a circle when you are given its area? When you multiply a number by itself, you square the number.
7. Finding Squae Root How can you find the dimenion of a quae o a cicle when you ae given it aea? When you multiply a numbe by itelf, you quae the numbe. Symbol fo quaing i the exponent. = = 6 quaed i
More informationChapter 15 Slope Stability
Page 15 1 Chapte 15 Slope Stability 1. The oil lope faile in the fom of a lide by tanlation i called (a) fall. (b) topple. (c) pead. (d) flow. 2. The facto of afety of a lope i defined a the atio of (a)
More informationAutodesk Robot Structural Analysis Professional - Verification Manual for Italian Codes
Autodesk Robot Stutual Analysis Pofessional VERIFICATIO MAUAL FOR ITALIA CODES Mah 2014 ITRODUCTIO... 1 COCRETE... 2 1. DM 9/1/96 RC COLUMS... 3 VERIFICATIO EXAMPLE 1 - COLUM SUBJECTED TO AXIAL LOAD AD
More informationParticle dynamics class, SMS 618, (Emmanuel Boss 11/19/2003) Van Rijn s TRANSPOR lab: computation of sediment transport in current and wave direction.
Patile dynami la SMS 618 (Emmanuel Bo 11/19/003 Van Rijn TRANSPOR lab: omputation of ediment tanpot in uent and ave dietion Handout: Appendix A in van Rijn 1993 Piniple of ediment tanpot in ive etuaie
More informationFrom 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 informationAdaptive LQ Cascade Control of a Tubular Chemical Reactor
MATEC Web of Confeene 7, () DOI:./ mateonf/ 7 CSCC Adaptive LQ Caade Contol of a Tubula Chemial Reato Dotal Pet, Vladimí obal and Jii Vojteek Toma ata Univeity in Zlin, Faulty of Applied Infomati, Nad
More informationPeriod #8: Axial Load/Deformation in Indeterminate Members
ENGR:75 Meh. Def. odie Period #8: ial oad/deformation in Indeterminate Member. Review We are onidering aial member in tenion or ompreion in the linear, elati regime of behavior. Thu the magnitude of aial
More informationmatschek (ccm2548) Ch17-h3 chiu (57890) 1
matshek m2548) Ch17-h3 hiu 5789) 1 This pint-out should have 16 questions. Multiple-hoie questions may ontinue on the next olumn o page find all hoies efoe answeing. 1 1. points A student said, The eleti
More informationTRAVELING WAVES. Chapter Simple Wave Motion. Waves in which the disturbance is parallel to the direction of propagation are called the
Chapte 15 RAVELING WAVES 15.1 Simple Wave Motion Wave in which the ditubance i pependicula to the diection of popagation ae called the tanvee wave. Wave in which the ditubance i paallel to the diection
More informationUltrasonic Measurement Models for Imaging with Phased Arrays
Ultaoni Meauement Model fo Imaging with Phaed Aay Lete W. Shme J. ab Bady J. Engle ab Alexande Sedov and Xiongbing Li d a Cente fo NDE Iowa State Univeity Ame IA 50011 USA b Dept. of Aeopae Eng. Iowa State
More informationAVS 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 informationChapter 19 Webassign Help Problems
Chapte 9 Webaign Help Poblem 4 5 6 7 8 9 0 Poblem 4: The pictue fo thi poblem i a bit mileading. They eally jut give you the pictue fo Pat b. So let fix that. Hee i the pictue fo Pat (a): Pat (a) imply
More informationP1.2 w = 1.35g k +1.5q k = = 4.35kN/m 2 M = wl 2 /8 = /8 = 34.8kN.m V = wl /2 = /2 = 17.4kN
Chapter Solution P. w = 5 0. 0. =.5k/m (or.5/) US load =.5 g k +.5 q k =.5k/m = / =.5 / =.k.m (d) V = / =.5 / =.k P. w =.5g k +.5q k =.5 +.5 =.5k/m = / =.5 / =.k.m V = / =.5 / = 7.k 5 5( ) 000 0,0005000.
More informationRed 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 informationTime 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 informationF g. = G mm. m 1. = 7.0 kg m 2. = 5.5 kg r = 0.60 m G = N m 2 kg 2 = = N
Chapte answes Heinemann Physics 4e Section. Woked example: Ty youself.. GRAVITATIONAL ATTRACTION BETWEEN SMALL OBJECTS Two bowling balls ae sitting next to each othe on a shelf so that the centes of the
More informationIn 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 informationProceedings of Clima 2007 WellBeing Indoors
Poeeing of Clima 2007 WellBeing Inoo Deivation an analyi of the outoo Wet Bulb Globe Tempeatue inex (WBGT) with a human themal engineeing appoah Pat 2. Popetie of the WBGT fomula fo outoo onition with
More informationSection 25 Describing Rotational Motion
Section 25 Decibing Rotational Motion What do object do and wh do the do it? We have a ve thoough eplanation in tem of kinematic, foce, eneg and momentum. Thi include Newton thee law of motion and two
More informationDESIGN OF QUIET PERMANENT MAGNET SYNCHRONOUS ELECTRICAL MOTORS BY OPTIMUM SKEW ANGLE
DESIGN OF QUIET PERMANENT MAGNET SYNCHRONOUS ELECTRICAL MOTORS BY OPTIMUM SKEW ANGLE Jean Le Beneai and Quentin Souon EOMYS ENGINEERING 121 ue de Chanzy, 59260 Lille Hellemme, Fane www.eomy.om email: jean.lebeneai@eomy.om
More information4) Magnetic confinement of plasma
4) Magneti onfineent of plasa Due to the shielding in the plasa, thee is alost no ontol with eleti fields. A ontol is possible with agneti fields, as patiles ae bound to the field lines. This is alled
More informationDetermine 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 informationPHYS 1441 Section 002. Lecture #3
PHYS 1441 Section 00 Chapte 1 Lectue #3 Wednesday, Sept. 6, 017 Coulomb s Law The Electic Field & Field Lines Electic Fields and Conductos Motion of a Chaged Paticle in an Electic Field Electic Dipoles
More informationImproved Research on the Transformer-Inductor Simulation Model of Magnetics
Jounal of Eletoni Reeah and Appliation OPEN Impoved Reeah on the Tanfome-Induto Simulation Model of Magneti Jiang Liyuan, Liu Baoyuan, Zhang Li Beijing Jiaotong Univeity Haibin College, Hebei 0600, China
More informationTest 2 phy a) How is the velocity of a particle defined? b) What is an inertial reference frame? c) Describe friction.
Tet phy 40 1. a) How i the velocity of a paticle defined? b) What i an inetial efeence fae? c) Decibe fiction. phyic dealt otly with falling bodie. d) Copae the acceleation of a paticle in efeence fae
More informationExtra 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 informationGeneralized Vapor Pressure Prediction Consistent with Cubic Equations of State
Genealized Vapo Pessue Pedition Consistent with Cubi Equations of State Laua L. Petasky and Mihael J. Misovih, Hope College, Holland, MI Intodution Equations of state may be used to alulate pue omponent
More informationStatic Electric Fields. Coulomb s Law Ε = 4πε. Gauss s Law. Electric Potential. Electrical Properties of Materials. Dielectrics. Capacitance E.
Coulomb Law Ε Gau Law Electic Potential E Electical Popetie of Mateial Conducto J σe ielectic Capacitance Rˆ V q 4πε R ρ v 2 Static Electic Field εe E.1 Intoduction Example: Electic field due to a chage
More informationKhmelnik S.I. Mathematical Model of Dust Whirl
Khmelnik S.I. Mathematial Model of Dust Whil Abstat The question of the soue of enegy in a dust whil is onsideed. Atmosphei onditions annot be the sole soue of enegy, as suh dust whils exist on Mas, whee
More informationElementary Statistics and Inference. Elementary Statistics and Inference. 11. Regression (cont.) 22S:025 or 7P:025. Lecture 14.
Elementay tatistics and Infeence :05 o 7P:05 Lectue 14 1 Elementay tatistics and Infeence :05 o 7P:05 Chapte 10 (cont.) D. Two Regession Lines uppose two vaiables, and ae obtained on 100 students, with
More informationVISUAL PHYSICS ONLINE EQUATION MINDMAPS
VISUAL PHYSICS ONLIN QUATION MINDMAPS quation ae eential pat of phyi, without them, we an t tat to explain ou phyial wold and make pedition. An equation tell a toy a olletion of a few ymbol ontain a wealth
More informationTo determine the biasing conditions needed to obtain a specific gain each stage must be considered.
PHYSIS 56 Experiment 9: ommon Emitter Amplifier A. Introdution A ommon-emitter oltage amplifier will be tudied in thi experiment. You will inetigate the fator that ontrol the midfrequeny gain and the low-and
More informationSolutions Practice Test PHYS 211 Exam 2
Solution Pactice Tet PHYS 11 Exam 1A We can plit thi poblem up into two pat, each one dealing with a epaate axi. Fo both the x- and y- axe, we have two foce (one given, one unknown) and we get the following
More informationone primary direction in which heat transfers (generally the smallest dimension) simple model good representation for solving engineering problems
CHAPTER 3: One-Dimenional Steady-State Conduction one pimay diection in which heat tanfe (geneally the mallet dimenion) imple model good epeentation fo olving engineeing poblem 3. Plane Wall 3.. hot fluid
More informationStress, 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 information1. Show that the volume of the solid shown can be represented by the polynomial 6x x.
7.3 Dividing Polynomials by Monomials Focus on Afte this lesson, you will be able to divide a polynomial by a monomial Mateials algeba tiles When you ae buying a fish tank, the size of the tank depends
More informationExample 1. Centripetal Acceleration. Example 1 - Step 2 (Sum of Vector Components) Example 1 Step 1 (Free Body Diagram) Example
014-11-18 Centipetal Aeleation 13 Exaple with full olution Exaple 1 A 1500 kg a i oing on a flat oad and negotiate a ue whoe adiu i 35. If the oeffiient of tati fition between the tie and the oad i 0.5,
More informationMATERIAL SPREADING AND COMPACTION IN POWDER-BASED SOLID FREEFORM FABRICATION METHODS: MATHEMATICAL MODELING
MATERIAL SPREADING AND COMPACTION IN POWDER-BASED SOLID FREEFORM FABRICATION METHODS: MATHEMATICAL MODELING Yae Shanjani and Ehan Toyekani Depatment of Mechanical and Mechatonic Engineeing, Univeity of
More informationIon-sound waves (electrostatic low frequency waves)
OTHER TYPES of WAVES Ion-sound waves (eletostati low fequeny waves) ae longitudinal waves simila lassial sound in gas s kt k M B plasma sound is slow fo eletons, but fast fo ions Eleton density is in eah
More informationSupplementary 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, the tangent line is an approximation of the curve (and easier to deal with than the curve).
114 Tangent Planes and Linea Appoimations Back in-dimensions, what was the equation of the tangent line of f ( ) at point (, ) f ( )? (, ) ( )( ) = f Linea Appoimation (Tangent Line Appoimation) of f at
More informationEstimation and Confidence Intervals: Additional Topics
Chapte 8 Etimation and Confidence Inteval: Additional Topic Thi chapte imply follow the method in Chapte 7 fo foming confidence inteval The text i a bit dioganized hee o hopefully we can implify Etimation:
More informationGravity. David Barwacz 7778 Thornapple Bayou SE, Grand Rapids, MI David Barwacz 12/03/2003
avity David Bawacz 7778 Thonapple Bayou, and Rapid, MI 495 David Bawacz /3/3 http://membe.titon.net/daveb Uing the concept dicued in the peceding pape ( http://membe.titon.net/daveb ), I will now deive
More informationRecitation 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 informationV V The circumflex (^) tells us this is a unit vector
Vecto Vecto have Diection and Magnitude Mike ailey mjb@c.oegontate.edu Magnitude: V V V V x y z vecto.pptx Vecto Can lo e Defined a the oitional Diffeence etween Two oint 3 Unit Vecto have a Magnitude
More informationPrecision Spectrophotometry
Peciion Spectophotomety Pupoe The pinciple of peciion pectophotomety ae illutated in thi expeiment by the detemination of chomium (III). ppaatu Spectophotomete (B&L Spec 20 D) Cuvette (minimum 2) Pipet:
More informationTutorial 5 Drive dynamics & control
UNIVERSITY OF NEW SOUTH WALES Electic Dive Sytem School o Electical Engineeing & Telecommunication ELEC463 Electic Dive Sytem Tutoial 5 Dive dynamic & contol. The ollowing paamete ae known o two high peomance
More informationINTRODUCTION. 2. Vectors in Physics 1
INTRODUCTION Vectos ae used in physics to extend the study of motion fom one dimension to two dimensions Vectos ae indispensable when a physical quantity has a diection associated with it As an example,
More informationInference for A One Way Factorial Experiment. By Ed Stanek and Elaine Puleo
Infeence fo A One Way Factoial Expeiment By Ed Stanek and Elaine Puleo. Intoduction We develop etimating equation fo Facto Level mean in a completely andomized one way factoial expeiment. Thi development
More informationRelativity for Global Navigation Satellite Systems
Relativity fo Global Navigation Satellite Systems Notes by Anna Heffenan based on the Living eviews atile, Relativity in the Global Positioning Systems, Neil Ashby, Living Rev. Relativity 6, (003),1 whih
More informationPractice. Understanding Concepts. Answers J 2. (a) J (b) 2% m/s. Gravitation and Celestial Mechanics 287
Pactice Undestanding Concepts 1. Detemine the gavitational potential enegy of the Eath Moon system, given that the aveage distance between thei centes is 3.84 10 5 km, and the mass of the Moon is 0.0123
More informationINFLUENCE OF GROUND INHOMOGENEITY ON WIND INDUCED GROUND VIBRATIONS. Abstract
INFLUENCE OF GROUND INHOMOGENEITY ON WIND INDUCED GROUND VIBRATIONS Mohammad Mohammadi, National Cente fo Physical Acoustics, Univesity of Mississippi, MS Caig J. Hicey, National Cente fo Physical Acoustics,
More informationThe Analysis of the Influence of the Independent Suspension on the Comfort for a Mine Truck
16 3 d Intenational Confeence on Vehicle, Mechanical and Electical Engineeing (ICVMEE 16 ISBN: 978-1-6595-37- The Analyi of the Influence of the Independent Supenion on the Comfot fo a Mine Tuck JINGMING
More informationEncapsulation theory: radial encapsulation. Edmund Kirwan *
Encapsulation theoy: adial encapsulation. Edmund Kiwan * www.edmundkiwan.com Abstact This pape intoduces the concept of adial encapsulation, wheeby dependencies ae constained to act fom subsets towads
More informationImpulse and Momentum
Impule and Momentum 1. A ca poee 20,000 unit of momentum. What would be the ca' new momentum if... A. it elocity wee doubled. B. it elocity wee tipled. C. it ma wee doubled (by adding moe paenge and a
More informationA Bijective Approach to the Permutational Power of a Priority Queue
A Bijective Appoach to the Pemutational Powe of a Pioity Queue Ia M. Gessel Kuang-Yeh Wang Depatment of Mathematics Bandeis Univesity Waltham, MA 02254-9110 Abstact A pioity queue tansfoms an input pemutation
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
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 information3.6 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 informationPHYS Summer Professor Caillault Homework Solutions. Chapter 5
PHYS 1111 - Summe 2007 - Pofesso Caillault Homewok Solutions Chapte 5 7. Pictue the Poblem: The ball is acceleated hoizontally fom est to 98 mi/h ove a distance of 1.7 m. Stategy: Use equation 2-12 to
More information17.1 Electric Potential Energy. Equipotential Lines. PE = energy associated with an arrangement of objects that exert forces on each other
Electic Potential Enegy, PE Units: Joules Electic Potential, Units: olts 17.1 Electic Potential Enegy Electic foce is a consevative foce and so we can assign an electic potential enegy (PE) to the system
More informationKunming, , R.P. China. Kunming, , R.P. China. *Corresponding author: Jianing He
Applied Mechanics and Mateials Online: 2014-04-28 ISSN: 1662-7482, Vol. 540, pp 92-95 doi:10.4028/www.scientific.net/amm.540.92 2014 Tans Tech Publications, Switzeland Reseach on Involute Gea Undecutting
More informationOnline Mathematics Competition Wednesday, November 30, 2016
Math@Mac Online Mathematics Competition Wednesday, Novembe 0, 206 SOLUTIONS. Suppose that a bag contains the nine lettes of the wod OXOMOXO. If you take one lette out of the bag at a time and line them
More informationPROBLEM SET #1 SOLUTIONS by Robert A. DiStasio Jr.
POBLM S # SOLUIONS by obet A. DiStasio J. Q. he Bon-Oppenheime appoximation is the standad way of appoximating the gound state of a molecula system. Wite down the conditions that detemine the tonic and
More informationMarkscheme May 2017 Calculus Higher level Paper 3
M7/5/MATHL/HP3/ENG/TZ0/SE/M Makscheme May 07 Calculus Highe level Pape 3 pages M7/5/MATHL/HP3/ENG/TZ0/SE/M This makscheme is the popety of the Intenational Baccalaueate and must not be epoduced o distibuted
More information1 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 informationThe CENTRE for EDUCATION in MATHEMATICS and COMPUTING cemc.uwaterloo.ca Galois Contest. Wednesday, April 12, 2017
The ENTRE fo EDUATIN in MATHEMATIS and MPUTING cemc.uwateloo.ca 2017 Galois ontest Wednesday, Apil 12, 2017 (in Noth Ameica and South Ameica) Thusday, Apil 13, 2017 (outside of Noth Ameica and South Ameica)
More informationΔt The textbook chooses to say that the average velocity is
1-D Motion Basic I Definitions: One dimensional motion (staight line) is a special case of motion whee all but one vecto component is zeo We will aange ou coodinate axis so that the x-axis lies along the
More information(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 informationTo Feel a Force Chapter 7 Static equilibrium - torque and friction
To eel a oce Chapte 7 Chapte 7: Static fiction, toque and static equilibium A. Review of foce vectos Between the eath and a small mass, gavitational foces of equal magnitude and opposite diection act on
More informationAn 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 informationAnswers 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 informationRoof Support 1. Stand-Up Time (RMR):
Roof Suppot 1 Enty Design is a complex polem. 1. One can use a Roof Classification System. o one can use Beam Fomulas Stand-Up Time (RMR): Maximum Unsuppoted Span (Q): Accoding to the Q system, the maximum
More informationPhases of Matter. Since liquids and gases are able to flow, they are called fluids. Compressible? Able to Flow? shape?
Fluids Chapte 3 Lectue Sequence. Pessue (Sections -3). Mechanical Popeties (Sections 5, and 7) 3. Gauge Pessue (Sections 4, and 6) 4. Moving Fluids (Sections 8-0) Pessue Phases of Matte Phase Retains its
More informationPsychometric 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 informationPhys-272 Lecture 18. Mutual Inductance Self-Inductance R-L Circuits
Phys-7 ectue 8 Mutual nductance Self-nductance - Cicuits Mutual nductance f we have a constant cuent i in coil, a constant magnetic field is ceated and this poduces a constant magnetic flux in coil. Since
More informationUNIT # 08 CURRENT ELECTRICITY
XS UNT # 8 UNT LTTY. j uent density n hage density j nev d v d j v d n e, n n n v d n n : v n n d. j nev d n j n e 9. Node-6\:\ata\\Kota\J-dvanced\SMP\Phy\Solution\Unit-7 & 8\-uent lecticity.p65 d nev
More information7.2.1 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 information6.641 Electromagnetic Fields, Forces, and Motion Spring 2005
MIT OpenouseWae http://ocw.mit.edu 6.641 Electomagnetic Fields, Foces, and Motion Sping 2005 Fo infomation about citing these mateials o ou Tems of Use, visit: http://ocw.mit.edu/tems. 6.641 Electomagnetic
More informationChapter 4. Sampling of Continuous-Time Signals
Chapte 4 Sampling of Continuous-Time Signals 1 Intodution Disete-time signals most ommonly ou as epesentations of sampled ontinuous-time signals. Unde easonable onstaints, a ontinuous-time signal an be
More informationEM-2. 1 Coulomb s law, electric field, potential field, superposition q. Electric field of a point charge (1)
EM- Coulomb s law, electic field, potential field, supeposition q ' Electic field of a point chage ( ') E( ) kq, whee k / 4 () ' Foce of q on a test chage e at position is ee( ) Electic potential O kq
More informationCOMPARING 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 informationElectromagnetism Physics 15b
lectomagnetism Physics 15b Lectue #20 Dielectics lectic Dipoles Pucell 10.1 10.6 What We Did Last Time Plane wave solutions of Maxwell s equations = 0 sin(k ωt) B = B 0 sin(k ωt) ω = kc, 0 = B, 0 ˆk =
More informationEF 152 Exam #1, Spring, 2011 Page 1 of 5
E 15 Exam #1, Sping, 011 Page 1 of 5 Name: Section: Guidelines: Assume 3 significant figues fo all given numbes unless othewise stated Show all of you wok no wok, no cedit Wite you final answe in the box
More informationPDF Created with deskpdf PDF Writer - Trial ::
A APPENDIX D TRIGONOMETRY Licensed to: jsamuels@bmcc.cun.edu PDF Ceated with deskpdf PDF Wite - Tial :: http://www.docudesk.com D T i g o n o m e t FIGURE a A n g l e s Angles can be measued in degees
More informationOBSTACLE DETECTION USING RING BEAM SYSTEM
OBSTACLE DETECTION USING RING BEAM SYSTEM M. Hiaki, K. Takamasu and S. Ozono Depatment of Peision Engineeing, The Univesity of Tokyo 7-3-1 Hongo, Bunkyo-ku, Tokyo, Japan Abstat: In this pape, we popose
More informationNumerical Modeling in Biomedical Systems
Numeial Modeling in Biomedial Systems BME 15:35 Letue 7 9/6/17 Nonlinea Systems Dunn Chapte 5 Nonlinea equations Root finding Baketing methods Open methods Gaphial Bisetion False Position Newton s method
More informationAlgebra-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 informationMass 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 informationWater flows through the voids in a soil which are interconnected. This flow may be called seepage, since the velocities are very small.
Wate movement Wate flows though the voids in a soil which ae inteconnected. This flow may be called seepage, since the velocities ae vey small. Wate flows fom a highe enegy to a lowe enegy and behaves
More informationγ from B D(Kπ)K and B D(KX)K, X=3π or ππ 0
fom and X, X= o 0 Jim Libby, Andew Powell and Guy Wilkinon Univeity of Oxfod 8th Januay 007 Gamma meeting 1 Outline The AS technique to meaue Uing o 0 : intoducing the coheence facto Meauing the coheence
More informationF-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 information11.2 Stability. A gain element is an active device. One potential problem with every active circuit is its stability
5/7/2007 11_2 tability 1/2 112 tability eading Aignment: pp 542-548 A gain element i an active device One potential problem with every active circuit i it tability HO: TABIITY Jim tile The Univ of Kana
More information2 Governing Equations
2 Govening Equations This chapte develops the govening equations of motion fo a homogeneous isotopic elastic solid, using the linea thee-dimensional theoy of elasticity in cylindical coodinates. At fist,
More informationBetween any two masses, there exists a mutual attractive force.
YEAR 12 PHYSICS: GRAVITATION PAST EXAM QUESTIONS Name: QUESTION 1 (1995 EXAM) (a) State Newton s Univesal Law of Gavitation in wods Between any two masses, thee exists a mutual attactive foce. This foce
More information