Example 11: The man shown in Figure (a) pulls on the cord with a force of 70
|
|
- Virgil Bates
- 5 years ago
- Views:
Transcription
1 Chapte Tw ce System 35.4 α α 100 Rx cs R β β 100 Ry cs R 111 Example 11: The man shwn in igue (a) pulls n the cd with a fce f 70 lb. Repesent this fce actin n the suppt A as Catesian cmpnents and detemine its diectin. Slutin: ind the Catesian pjectins f the : x x ft 1 y y ft 1 z 6 30 z 1 4 ft (1) ( 8) ( 4) 8 ft and the Catesian cmpnents equal: x y z 1 * lb 8 *70 0 lb 8 4 *70 60 lb 8 The cdinate diectin angles ae measued between ( ) and the psitive axes f a lcalized cdinate system with igin placed at A, igue (b). 1 cs 1 α cs 1 β cs 1 γ Univesity f Qadisiyah\aculty f Eng.\Civil Dep 7
2 Chapte Tw ce System Example 1: The fce in igue (a) acts n the hk. Expess it as Catesian cmpnents. Slutin: As Shwn in igue (b), the cdinate f pints A and B ae and A( m, 0, m) 4 B 5sin m, 5cs30 5 B[- m, m, 3 m ] 3 m, 5m 5 ind the Catesian pjectins f the : x x 1 y y z 3 z 1 1m 4 m 3.464m ( 4) S, the Catesian cmpnents f : m x 4 * N y * N z * N Univesity f Qadisiyah\aculty f Eng.\Civil Dep 8
3 Chapte Tw ce System Example 13: Tw fces act n the hk shwn in igue (a). Specify the magnitude f and its cdinate diectin angles f that the esultant fce R acts alng the psitive y-axis and has a magnitude f 800 N. Slutin: T slve this pblem, the esultant f fce R and its tw cmpnents 1 and, will each expessed in Catesian cmpnents. Then, as shwn in igue (a), it is necessay that R 1. The Catesian cmpnents f 1, 1x 1 csα 1 300cs45 1.1N 1y 1 csβ 1 300cs60 150Ν 1z 1 csγ 1 300cs10 150Ν Since R has a magnitude f 800 N and acts in psitive y-diectin, the diectins csines α and γ ae equal 90 while β 0, s the cmpnents Σ x Σ z 0 and Σ y 800. S the cmpnents f, x x -1.1 N y y 650 N z z 150 N The magnitude f is thus, ( 1.1) N and its cdinate diectin angles, 1.1 csα α cs β β Univesity f Qadisiyah\aculty f Eng.\Civil Dep 9
4 Chapte Tw ce System 150 csγ γ Example 14: The f is suppted by cables as shwn in the pht. If the cables exet fces 100 N and AC 10 N n the wall hk at A as shwn in igue (a), detemine the esultant fce acting at A. Expess the esult as Catesian cmpnents. Slutin: ind the Catesian pjectins f the : : x x y y m 0 m z z m ( 4) 5.65 m AC: 4 0 x x 1 y y m m z z m 1 AC ( ) ( ) ( ) 4 ( 4) 6.0 m The cmpnents f esultant fce: x y z ix AC 4 4 *100 * AC iy AC 0 *100 * ix AC And the esultant 151N 40 N ( 4) ( 4) *100 * AC 151N x y z ( 151) 16N.Univesity f Qadisiyah\aculty f Eng.\Civil Dep 30
5 Chapte Tw ce System.Univesity f Qadisiyah\aculty f Eng.\Civil Dep 31
6 Chapte Tw ce System Mment f ce When a fce is applied t a bdy it will pduce a tendency f the bdy t tate abut a pint that is nt n the line f actin f the fce. This tendency t tate is smetimes called a tque, but mst ften it is called the mment f a fce simply mment. The magnitude f the mment is: M d (-8) Whee d is the mment am pependicula distance fm the axis at pint O t the line f actin f the fce. Units f mment magnitude cnsist f fce times distance, i.e., N.m lb.ft. Nte 1: If the fce is applied at an angle θ 90, igue b, then it will be difficult t tun the blt since the mment am d' d sinθ will be smalle than d. Nte : If is applied alng the wench, igue c, its mment am will be ze since the line f actin f will intesect pint O (the z-axis). As a esult, the mment f abut O is als ze and n tuning can ccu The mment M abut O, abut an axis passing thugh O and pependicula t the plane, is a vect quantity since it has a specified magnitude and diectin..univesity f Qadisiyah\aculty f Eng.\Civil Dep 3
7 Chapte Tw ce System Diectin: The diectin f M is defined by its mment axis, which is pependicula t the plane that cntain the fce and its mment am d. The ight-hand ule is used t establish the sense f diectin f M. Accding t this ule, the natue cul f the finges f the ight-hand, as they ae dawn twads the palm, epesent the tendency f tatin caused by the mment. As the actin is pefmed, the thumb f the ight-hand will give the diectin sense f M. Ntice that the mment vect is epesented in thee-diectinally by a cul aund an aw as in igue b. Since in this case the mment will tend t cause a cunteclckwise tatin, the mment vect is actually diected ut f page. If the fce des nt lie in a plane pependicula t the mment axis, it may be eslved int tw cmpnents, ne being paallel t the mment axis and the the lying in a plane pependicula t the axis. The cmpnent f paallel t the efeence axis has n tendency t tate the bdy abut the axis and has n mment with espect t this axis. The mment f the the cmpnent is thus the mment f the fce with espect t the line axis. M d (-9) Resultant mment: tw-dimensinal pblems, whee all the fces lie in the x-y plane the esultant (M R ) abut pint O (the z-axis) can be detemined by finding the algebaic sum f the mments caused by all fces in the system. As a cnventin, we will geneally cnside psitive mment as cunteclckwise since they ae diected alng the psitive z-axis (ut f page). Clckwise mment will be negative. Ding this, the diectinal sense f each mment can be epesented by a plus minus sign..univesity f Qadisiyah\aculty f Eng.\Civil Dep 33
8 Chapte Tw ce System theefe: Using this sign cnventin, the esultant mment in figue belw is (M R ) O d; (M R ) O 1 d 1 - d 3 d 3 If the numeical esult f this sum is psitive scala, (M R ) O will be cunteclckwise mment (ut f page); if the esult is negative, (M R ) O will be clckwise mment (int the page). Pinciple Mments f ces: When detemining the mment f a fce abut a pint, it is ften cnvenient t use the pinciple f mments, als knwn as Vaignn s theem which indicates that: The mment f a fce abut a pint is equal t the sum f the mments f its cmpnents abut that pint. Example 15: each case illustated in igues belw, detemine the mment f the fce abut pint O. Slutin: igue (a) igue (b) igue (c) igue (d) igue (e) M O -(100)() N.m M O -(50)(0.75) N.m M O - (40)(4 cs30 ) -9 9 lb.ft M O (60)(1 sin 45 ) 4.4 lb.ft M O (7)(4-1) 1.0 kn.m.univesity f Qadisiyah\aculty f Eng.\Civil Dep 34
9 Chapte Tw ce System Example 16: Detemine the esultant mment f the fu fces acting n the d shwn in igue abut O. Slutin: M R Σd; M R -50() 60(0) 0(3 sin30 ) -40(4 3 cs30 ) -334 N.m M R 334 N.m Example 17: Detemine the mment f the fce in figue abut O. Slutin I: The mment am d in igue (a) can be fund fm tignmety. Thus, d (3) sin m M O d -(5)(.898) kn.m 14.5 kn.m Since the fce tends t tate bit clckwise abut pint O, the mment is diected int the page. Slutin II: The x and y cmpnents f the fce ae indicated in igue (b). M O x d y y d x -(5 cs45 )(3 sin30 )-(5 sin45 )(3 cs30 ) kn.m 14.5 kn.m Slutin III: The x and y axes can be set paallel and pependicula t the d's axis as shwn in igue (c). Hee x pduces n mment abut pint O since its line f actin passes thugh this pint. Theefe,.Univesity f Qadisiyah\aculty f Eng.\Civil Dep 35
5.1 Moment of a Force Scalar Formation
Outline ment f a Cuple Equivalent System Resultants f a Fce and Cuple System ment f a fce abut a pint axis a measue f the tendency f the fce t cause a bdy t tate abut the pint axis Case 1 Cnside hizntal
More informationENGI 1313 Mechanics I
ENGI 1313 Mechanics I Lectue 05: Catesian Vects Shawn Kenny, Ph.D., P.Eng. ssistant Pfess Faculty f Engineeing and pplied Science Memial Univesity f Newfundland spkenny@eng.mun.ca Chapte Objectives t eview
More informationMagnetism. Chapter 21
1.1 Magnetic Fields Chapte 1 Magnetism The needle f a cmpass is pemanent magnet that has a nth magnetic ple (N) at ne end and a suth magnetic ple (S) at the the. 1.1 Magnetic Fields 1.1 Magnetic Fields
More informationElectric Charge. Electric charge is quantized. Electric charge is conserved
lectstatics lectic Chage lectic chage is uantized Chage cmes in incements f the elementay chage e = ne, whee n is an intege, and e =.6 x 0-9 C lectic chage is cnseved Chage (electns) can be mved fm ne
More informationSolution: (a) C 4 1 AI IC 4. (b) IBC 4
C A C C R A C R C R C sin 9 sin. A cuent f is maintaine in a single cicula lp f cicumfeence C. A magnetic fiel f is iecte paallel t the plane f the lp. (a) Calculate the magnetic mment f the lp. (b) What
More informationChapter 4 Motion in Two and Three Dimensions
Chapte 4 Mtin in Tw and Thee Dimensins In this chapte we will cntinue t stud the mtin f bjects withut the estictin we put in chapte t me aln a staiht line. Instead we will cnside mtin in a plane (tw dimensinal
More informationA) N B) 0.0 N C) N D) N E) N
Cdinat: H Bahluli Sunday, Nvembe, 015 Page: 1 Q1. Five identical pint chages each with chage =10 nc ae lcated at the cnes f a egula hexagn, as shwn in Figue 1. Find the magnitude f the net electic fce
More informationChapter 5 Trigonometric Functions
Chapte 5 Tignmetic Functins Sectin 5.2 Tignmetic Functins 5-5. Angles Basic Teminlgy Degee Measue Standad Psitin Cteminal Angles Key Tems: vetex f an angle, initial side, teminal side, psitive angle, negative
More informationMEM202 Engineering Mechanics Statics Course Web site:
0 Engineeing Mechanics - Statics 0 Engineeing Mechanics Statics Cuse Web site: www.pages.dexel.edu/~cac54 COUSE DESCIPTION This cuse cves intemediate static mechanics, an extensin f the fundamental cncepts
More informationCHAPTER 24 GAUSS LAW
CHAPTR 4 GAUSS LAW LCTRIC FLUX lectic flux is a measue f the numbe f electic filed lines penetating sme suface in a diectin pependicula t that suface. Φ = A = A csθ with θ is the angle between the and
More information1. Show that if the angular momentum of a boby is determined with respect to an arbitrary point A, then. r r r. H r A can be expressed by H r r r r
1. Shw that if the angula entu f a bb is deteined with espect t an abita pint, then H can be epessed b H = ρ / v + H. This equies substituting ρ = ρ + ρ / int H = ρ d v + ρ ( ω ρ ) d and epanding, nte
More informationWork, Energy, and Power. AP Physics C
k, Eneg, and Pwe AP Phsics C Thee ae man diffeent TYPES f Eneg. Eneg is expessed in JOULES (J) 4.19 J = 1 calie Eneg can be expessed me specificall b using the tem ORK() k = The Scala Dt Pduct between
More informationIntroduction. Electrostatics
UNIVESITY OF TECHNOLOGY, SYDNEY FACULTY OF ENGINEEING 4853 Electmechanical Systems Electstatics Tpics t cve:. Culmb's Law 5. Mateial Ppeties. Electic Field Stength 6. Gauss' Theem 3. Electic Ptential 7.
More informationAnnouncements Candidates Visiting Next Monday 11 12:20 Class 4pm Research Talk Opportunity to learn a little about what physicists do
Wed., /11 Thus., /1 Fi., /13 Mn., /16 Tues., /17 Wed., /18 Thus., /19 Fi., / 17.7-9 Magnetic Field F Distibutins Lab 5: Bit-Savat B fields f mving chages (n quiz) 17.1-11 Pemanent Magnets 18.1-3 Mic. View
More informationSummary chapter 4. Electric field s can distort charge distributions in atoms and molecules by stretching and rotating:
Summa chapte 4. In chapte 4 dielectics ae discussed. In thse mateials the electns ae nded t the atms mlecules and cannt am fee thugh the mateial: the electns in insulats ae n a tight leash and all the
More informationWYSE Academic Challenge Sectional Mathematics 2006 Solution Set
WYSE Academic Challenge Sectinal 006 Slutin Set. Cect answe: e. mph is 76 feet pe minute, and 4 mph is 35 feet pe minute. The tip up the hill takes 600/76, 3.4 minutes, and the tip dwn takes 600/35,.70
More informationPhys 332 Electricity & Magnetism Day 3. Note: I should have recommended reading section 1.5 (delta function) as well. rˆ rˆ
Phs 33 lecticit & Magnetism Da 3 Mn. 9/9 Wed. 9/ Thus 9/ Fi. 9/3 (C.-.5,.8). &.5;..-.. Gauss & Div, T Numeical Quadatue (C.-.5,.8)..3 Using Gauss (C.-.5,.8)..3-.. Using Gauss HW quipment Bing in ppt s
More information5/20/2011. HITT An electron moves from point i to point f, in the direction of a uniform electric field. During this displacement:
5/0/011 Chapte 5 In the last lectue: CapacitanceII we calculated the capacitance C f a system f tw islated cnducts. We als calculated the capacitance f sme simple gemeties. In this chapte we will cve the
More informationA) (0.46 î ) N B) (0.17 î ) N
Phys10 Secnd Maj-14 Ze Vesin Cdinat: xyz Thusday, Apil 3, 015 Page: 1 Q1. Thee chages, 1 = =.0 μc and Q = 4.0 μc, ae fixed in thei places as shwn in Figue 1. Find the net electstatic fce n Q due t 1 and.
More informationElectromagnetic Waves
Chapte 3 lectmagnetic Waves 3.1 Maxwell s quatins and ectmagnetic Waves A. Gauss s Law: # clsed suface aea " da Q enc lectic fields may be geneated by electic chages. lectic field lines stat at psitive
More informationThe Gradient and Applications This unit is based on Sections 9.5 and 9.6, Chapter 9. All assigned readings and exercises are from the textbook
The Gadient and Applicatins This unit is based n Sectins 9.5 and 9.6 Chapte 9. All assigned eadings and eecises ae fm the tetbk Objectives: Make cetain that u can define and use in cntet the tems cncepts
More informationCHAPTER GAUSS'S LAW
lutins--ch 14 (Gauss's Law CHAPTE 14 -- GAU' LAW 141 This pblem is ticky An electic field line that flws int, then ut f the cap (see Figue I pduces a negative flux when enteing and an equal psitive flux
More informationME 3600 Control Systems Frequency Domain Analysis
ME 3600 Cntl Systems Fequency Dmain Analysis The fequency espnse f a system is defined as the steady-state espnse f the system t a sinusidal (hamnic) input. F linea systems, the esulting utput is itself
More informationA) 100 K B) 150 K C) 200 K D) 250 K E) 350 K
Phys10 Secnd Maj-09 Ze Vesin Cdinat: k Wednesday, May 05, 010 Page: 1 Q1. A ht bject and a cld bject ae placed in themal cntact and the cmbinatin is islated. They tansfe enegy until they each a final equilibium
More informationMarch 15. Induction and Inductance Chapter 31
Mach 15 Inductin and Inductance Chapte 31 > Fces due t B fields Lentz fce τ On a mving chage F B On a cuent F il B Cuent caying cil feels a tque = µ B Review > Cuents geneate B field Bit-Savat law = qv
More informationELECTRIC & MAGNETIC FIELDS I (STATIC FIELDS) ELC 205A
LCTRIC & MAGNTIC FILDS I (STATIC FILDS) LC 05A D. Hanna A. Kils Assciate Pfess lectnics & Cmmnicatins ngineeing Depatment Faclty f ngineeing Cai Univesity Fall 0 f Static lecticity lectic & Magnetic Fields
More informationELECTROMAGNETIC INDUCTION PREVIOUS EAMCET BITS
P P Methd EECTOMAGNETIC INDUCTION PEVIOUS EAMCET BITS [ENGINEEING PAPE]. A cnduct d f length tates with angula speed ω in a unifm magnetic field f inductin B which is pependicula t its mtin. The induced
More informationLecture #2 : Impedance matching for narrowband block
Lectue # : Ipedance atching f nawband blck ichad Chi-Hsi Li Telephne : 817-788-848 (UA) Cellula phne: 13917441363 (C) Eail : chihsili@yah.c.cn 1. Ipedance atching indiffeent f bandwidth ne pat atching
More informationCHAPTER 25 ELECTRIC POTENTIAL
CHPTE 5 ELECTIC POTENTIL Potential Diffeence and Electic Potential Conside a chaged paticle of chage in a egion of an electic field E. This filed exets an electic foce on the paticle given by F=E. When
More informationPhy 213: General Physics III
Phy 1: Geneal Physics III Chapte : Gauss Law Lectue Ntes E Electic Flux 1. Cnside a electic field passing thugh a flat egin in space w/ aea=a. The aea vect ( A ) with a magnitude f A and is diected nmal
More informationOBJECTIVE To investigate the parallel connection of R, L, and C. 1 Electricity & Electronics Constructor EEC470
Assignment 7 Paallel Resnance OBJECTIVE T investigate the paallel cnnectin f R,, and C. EQUIPMENT REQUIRED Qty Appaatus 1 Electicity & Electnics Cnstuct EEC470 1 Basic Electicity and Electnics Kit EEC471-1
More informationChapter 4 Motion in Two and Three Dimensions
Chpte 4 Mtin in Tw nd Thee Dimensins In this chpte we will cntinue t stud the mtin f bjects withut the estictin we put in chpte t me ln stiht line. Insted we will cnside mtin in plne (tw dimensinl mtin)
More informationn Power transmission, X rays, lightning protection n Solid-state Electronics: resistors, capacitors, FET n Computer peripherals: touch pads, LCD, CRT
.. Cu-Pl, INE 45- Electmagnetics I Electstatic fields anda Cu-Pl, Ph.. INE 45 ch 4 ECE UPM Maagüe, P me applicatins n Pwe tansmissin, X as, lightning ptectin n lid-state Electnics: esists, capacits, FET
More informationStrees Analysis in Elastic Half Space Due To a Thermoelastic Strain
IOSR Junal f Mathematics (IOSRJM) ISSN: 78-578 Vlume, Issue (July-Aug 0), PP 46-54 Stees Analysis in Elastic Half Space Due T a Themelastic Stain Aya Ahmad Depatment f Mathematics NIT Patna Biha India
More informationVECTOR MECHANICS FOR ENGINEERS: STATICS
4 Equilibium CHAPTER VECTOR MECHANICS FOR ENGINEERS: STATICS Fedinand P. Bee E. Russell Johnston, J. of Rigid Bodies Lectue Notes: J. Walt Ole Texas Tech Univesity Contents Intoduction Fee-Body Diagam
More informationFri. 10/23 (C14) Linear Dielectrics (read rest at your discretion) Mon. (C 17) , E to B; Lorentz Force Law: fields
Fi. 0/23 (C4) 4.4. Linea ielectics (ead est at yu discetin) Mn. (C 7) 2..-..2, 2.3. t B; 5..-..2 Lentz Fce Law: fields Wed. and fces Thus. (C 7) 5..3 Lentz Fce Law: cuents Fi. (C 7) 5.2 Bit-Savat Law HW6
More informationDonnishJournals
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 informationOutline. Steady Heat Transfer with Conduction and Convection. Review Steady, 1-D, Review Heat Generation. Review Heat Generation II
Steady Heat ansfe ebuay, 7 Steady Heat ansfe wit Cnductin and Cnvectin ay Caett Mecanical Engineeing 375 Heat ansfe ebuay, 7 Outline eview last lectue Equivalent cicuit analyses eview basic cncept pplicatin
More informationPhysics Tutorial V1 2D Vectors
Physics Tutoial V1 2D Vectos 1 Resolving Vectos & Addition of Vectos A vecto quantity has both magnitude and diection. Thee ae two ways commonly used to mathematically descibe a vecto. y (a) The pola fom:,
More informationCS579 - Homework 2. Tu Phan. March 10, 2004
I! CS579 - Hmewk 2 Tu Phan Mach 10, 2004 1 Review 11 Planning Pblem and Plans The planning pblem we ae cnsideing is a 3-tuple descibed in the language whse syntax is given in the bk, whee is the initial
More informationChapter 4. Energy and Potential
Chpte 4. Enegy nd Ptentil Hyt; 0/5/009; 4-4. Enegy Expended in Mving Pint Chge in n Electic Field The electic field intensity is defined s the fce n unit test chge. The fce exeted y the electic field n
More informationCh. 3: Inverse Kinematics Ch. 4: Velocity Kinematics. The Interventional Centre
Ch. : Invee Kinemati Ch. : Velity Kinemati The Inteventinal Cente eap: kinemati eupling Apppiate f ytem that have an am a wit Suh that the wit jint ae ae aligne at a pint F uh ytem, we an plit the invee
More informationChapter 15. ELECTRIC POTENTIALS and ENERGY CONSIDERATIONS
Ch. 15--Elect. Pt. and Enegy Cns. Chapte 15 ELECTRIC POTENTIALS and ENERGY CONSIDERATIONS A.) Enegy Cnsideatins and the Abslute Electical Ptential: 1.) Cnside the fllwing scenai: A single, fixed, pint
More informationLecture 4. Electric Potential
Lectue 4 Electic Ptentil In this lectue yu will len: Electic Scl Ptentil Lplce s n Pissn s Eutin Ptentil f Sme Simple Chge Distibutins ECE 0 Fll 006 Fhn Rn Cnell Univesity Cnsevtive Ittinl Fiels Ittinl
More informationMODULE 1. e x + c. [You can t separate a demominator, but you can divide a single denominator into each numerator term] a + b a(a + b)+1 = a + b
. REVIEW OF SOME BASIC ALGEBRA MODULE () Slving Equatins Yu shuld be able t slve fr x: a + b = c a d + e x + c and get x = e(ba +) b(c a) d(ba +) c Cmmn mistakes and strategies:. a b + c a b + a c, but
More informationElectric potential energy Electrostatic force does work on a particle : Potential energy (: i initial state f : final state):
Electc ptental enegy Electstatc fce des wk n a patcle : v v v v W = F s = E s. Ptental enegy (: ntal state f : fnal state): Δ U = U U = W. f ΔU Electc ptental : Δ : ptental enegy pe unt chag e. J ( Jule)
More informationVectors. Chapter. Introduction of Vector. Types of Vector. Vectors 1
Vect 1 Chapte 0 Vect Intductin f Vect Phical quantitie haing magnitude, diectin and being la f ect algeba ae called ect. Eample : Diplacement, elcit, acceleatin, mmentum, fce, impule, eight, thut, tque,
More informationLecture 5: Equilibrium and Oscillations
Lecture 5: Equilibrium and Oscillatins Energy and Mtin Last time, we fund that fr a system with energy cnserved, v = ± E U m ( ) ( ) One result we see immediately is that there is n slutin fr velcity if
More informationFaculty of Engineering and Department of Physics Engineering Physics 131 Midterm Examination February 27, 2006; 7:00 pm 8:30 pm
Faculty f Engineering and Department f Physics Engineering Physics 131 Midterm Examinatin February 27, 2006; 7:00 pm 8:30 pm N ntes r textbks allwed. Frmula sheet is n the last page (may be remved). Calculatrs
More informationworking 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 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 informationElectric Fields and Electric Forces
Cpyight, iley 006 (Cutnell & Jhnsn 9. Ptential Enegy Chapte 9 mgh mgh GPE GPE Electic Fields and Electic Fces 9. Ptential Enegy 9. Ptential Enegy 9. The Electic Ptential Diffeence 9. The Electic Ptential
More informationENGI 1313 Mechanics I
ENGI 1313 Mechanics I Lecture 11: 2D and 3D Particle Equilibrium Shawn Kenny, Ph.D., P.Eng. Assistant Prfessr aculty f Engineering and Applied Science Memrial University f Newfundland spkenny@engr.mun.ca
More informationCombustion Chamber. (0.1 MPa)
ME 354 Tutial #10 Winte 001 Reacting Mixtues Pblem 1: Detemine the mle actins the pducts cmbustin when ctane, C 8 18, is buned with 00% theetical ai. Als, detemine the dew-pint tempeatue the pducts i the
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 informationPhysics 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 informationto point uphill and to be equal to its maximum value, in which case f s, max = μsfn
Chapte 6 16. (a) In this situation, we take f s to point uphill and to be equal to its maximum value, in which case f s, max = μsf applies, whee μ s = 0.5. pplying ewton s second law to the block of mass
More informationMAGNETIC FIELD INTRODUCTION
MAGNETIC FIELD INTRODUCTION It was found when a magnet suspended fom its cente, it tends to line itself up in a noth-south diection (the compass needle). The noth end is called the Noth Pole (N-pole),
More informationQualifying Examination Electricity and Magnetism Solutions January 12, 2006
1 Qualifying Examination Electicity and Magnetism Solutions Januay 12, 2006 PROBLEM EA. a. Fist, we conside a unit length of cylinde to find the elationship between the total chage pe unit length λ and
More information. Using our polar coordinate conversions, we could write a
504 Chapte 8 Section 8.4.5 Dot Poduct Now that we can add, sutact, and scale vectos, you might e wondeing whethe we can multiply vectos. It tuns out thee ae two diffeent ways to multiply vectos, one which
More informationSection 4.2 Radians, Arc Length, and Area of a Sector
Sectin 4.2 Radian, Ac Length, and Aea f a Sect An angle i fmed by tw ay that have a cmmn endpint (vetex). One ay i the initial ide and the the i the teminal ide. We typically will daw angle in the cdinate
More informationVIII. Further Aspects of Edge Diffraction
VIII. Futhe Aspects f Edge Diffactin Othe Diffactin Cefficients Oblique Incidence Spheical Wave Diffactin by an Edge Path Gain Diffactin by Tw Edges Numeical Examples Septembe 3 3 by H.L. Betni Othe Diffactin
More informationPhysics 2B Chapter 22 Notes - Magnetic Field Spring 2018
Physics B Chapte Notes - Magnetic Field Sping 018 Magnetic Field fom a Long Staight Cuent-Caying Wie In Chapte 11 we looked at Isaac Newton s Law of Gavitation, which established that a gavitational field
More informatione.g: If A = i 2 j + k then find A. A = Ax 2 + Ay 2 + Az 2 = ( 2) = 6
MOTION IN A PLANE 1. Scala Quantities Physical quantities that have only magnitude and no diection ae called scala quantities o scalas. e.g. Mass, time, speed etc. 2. Vecto Quantities Physical quantities
More informationKinetics of Particles. Chapter 3
Kinetics f Particles Chapter 3 1 Kinetics f Particles It is the study f the relatins existing between the frces acting n bdy, the mass f the bdy, and the mtin f the bdy. It is the study f the relatin between
More informationConsider the simple circuit of Figure 1 in which a load impedance of r is connected to a voltage source. The no load voltage of r
1 Intductin t Pe Unit Calculatins Cnside the simple cicuit f Figue 1 in which a lad impedance f L 60 + j70 Ω 9. 49 Ω is cnnected t a vltage suce. The n lad vltage f the suce is E 1000 0. The intenal esistance
More informationCAUTION: Do not install damaged parts!!!
Yu satisfactin is imptant t us, please let us help! If yu have any questins cncens duing the installatin, u suppt epesentatives ae available t assist yu. Please call: 1-877-769-3765 Live Chat at www.aptseies.cm
More informationTEAL Physics and Mathematics Documentation
Vesin. 7/7/008 TAL Phsics and Mathematics cumentatin Jhn Belche, Stanislaw Olbet, and Nman eb IN PF FORMAT THIS OCUMNT HAS BOOKMARKS FOR NAVIGATION CLICK ON TH LFT BOOKMARK TAB IN TH PF RAR Vesin., Jul
More informationAP Physics Kinematic Wrap Up
AP Physics Kinematic Wrap Up S what d yu need t knw abut this mtin in tw-dimensin stuff t get a gd scre n the ld AP Physics Test? First ff, here are the equatins that yu ll have t wrk with: v v at x x
More informationMODULE 5a and 5b (Stewart, Sections 12.2, 12.3) INTRO: In MATH 1114 vectors were written either as rows (a1, a2,..., an) or as columns a 1 a. ...
MODULE 5a and 5b (Stewat, Sections 2.2, 2.3) INTRO: In MATH 4 vectos wee witten eithe as ows (a, a2,..., an) o as columns a a 2... a n and the set of all such vectos of fixed length n was called the vecto
More information( ) ( )( ) ˆ. Homework #8. Chapter 27 Magnetic Fields II.
Homewok #8. hapte 7 Magnetic ields. 6 Eplain how ou would modif Gauss s law if scientists discoveed that single, isolated magnetic poles actuall eisted. Detemine the oncept Gauss law fo magnetism now eads
More informationExample
hapte Exaple.6-3. ---------------------------------------------------------------------------------- 5 A single hllw fibe is placed within a vey lage glass tube. he hllw fibe is 0 c in length and has a
More informationCAUTION: Do not install damaged parts!!!
Yu satisfactin is imptant t us, please let us help! If yu have any questins cncens duing the installatin, u suppt epesentatives ae available t assist yu. Please call: 1-877-769-3765 Live Chat at www.aptseies.cm
More informationMagnetic Fields Due to Currents
PH -C Fall 1 Magnetic Fields Due to Cuents Lectue 14 Chapte 9 (Halliday/esnick/Walke, Fundamentals of Physics 8 th edition) 1 Chapte 9 Magnetic Fields Due to Cuents In this chapte we will exploe the elationship
More informationAnalytical Solution to Diffusion-Advection Equation in Spherical Coordinate Based on the Fundamental Bloch NMR Flow Equations
Intenatinal Junal f heetical and athematical Phsics 5, 5(5: 4-44 OI:.593/j.ijtmp.555.7 Analtical Slutin t iffusin-advectin Equatin in Spheical Cdinate Based n the Fundamental Blch N Flw Equatins anladi
More informationUNIT 1 COPLANAR AND NON-COPLANAR FORCES
UNIT 1 COPLANA AND NON-COPLANA FOCES Cplanar and Nn-Cplanar Frces Structure 1.1 Intrductin Objectives 1. System f Frces 1.3 Cplanar Frce 1.3.1 Law f Parallelgram f Frces 1.3. Law f Plygn f Frces 1.3.3
More informationEquilibrium of Stress
Equilibrium f Stress Cnsider tw perpendicular planes passing thrugh a pint p. The stress cmpnents acting n these planes are as shwn in ig. 3.4.1a. These stresses are usuall shwn tgether acting n a small
More informationSchool of Chemical & Biological Engineering, Konkuk University
Schl f Cheical & Bilgical Engineeing, Knkuk Univesity Lectue 7 Ch. 2 The Fist Law Thecheisty Pf. Y-Sep Min Physical Cheisty I, Sping 2008 Ch. 2-2 The study f the enegy tansfeed as heat duing the cuse f
More informationPhysics Spring 2012 Announcements: Mar 07, 2012
Physics 00 - Sping 01 Announcements: Ma 07, 01 HW#6 due date has been extended to the moning of Wed. Ma 1. Test # (i. Ma ) will cove only chaptes 0 and 1 All of chapte will be coveed in Test #4!!! Test
More informationChapter 5 Force and Motion
Chapte 5 Foce and Motion In chaptes 2 and 4 we have studied kinematics i.e. descibed the motion of objects using paametes such as the position vecto, velocity and acceleation without any insights as to
More informationPhysics for Scientists and Engineers
Phsics 111 Sections 003 and 005 Instucto: Pof. Haimin Wang E-mail: haimin@flae.njit.edu Phone: 973-596-5781 Office: 460 Tienan Hall Homepage: http://sola.njit.edu/~haimin Office Hou: 2:30 to 3:50 Monda
More informationCambridge Assessment International Education Cambridge Ordinary Level. Published
Cambridge Assessment Internatinal Educatin Cambridge Ordinary Level ADDITIONAL MATHEMATICS 4037/1 Paper 1 Octber/Nvember 017 MARK SCHEME Maximum Mark: 80 Published This mark scheme is published as an aid
More informationPHYS 110B - HW #7 Spring 2004, Solutions by David Pace Any referenced equations are from Griffiths Problem statements are paraphrased
PHYS 0B - HW #7 Sping 2004, Solutions by David Pace Any efeenced euations ae fom Giffiths Poblem statements ae paaphased. Poblem 0.3 fom Giffiths A point chage,, moves in a loop of adius a. At time t 0
More informationExample 1. A robot has a mass of 60 kg. How much does that robot weigh sitting on the earth at sea level? Given: m. Find: Relationships: W
Eample 1 rbt has a mass f 60 kg. Hw much des that rbt weigh sitting n the earth at sea level? Given: m Rbt = 60 kg ind: Rbt Relatinships: Slutin: Rbt =589 N = mg, g = 9.81 m/s Rbt = mrbt g = 60 9. 81 =
More informationPhysics 235 Chapter 5. Chapter 5 Gravitation
Chapte 5 Gavitation In this Chapte we will eview the popeties of the gavitational foce. The gavitational foce has been discussed in geat detail in you intoductoy physics couses, and we will pimaily focus
More informationVector d is a linear vector function of vector d when the following relationships hold:
Appendix 4 Dyadic Analysis DEFINITION ecto d is a linea vecto function of vecto d when the following elationships hold: d x = a xxd x + a xy d y + a xz d z d y = a yxd x + a yy d y + a yz d z d z = a zxd
More informationChapter 5 Force and Motion
Chapte 5 Foce and Motion In Chaptes 2 and 4 we have studied kinematics, i.e., we descibed the motion of objects using paametes such as the position vecto, velocity, and acceleation without any insights
More informationVectors, Vector Calculus, and Coordinate Systems
Apil 5, 997 A Quick Intoduction to Vectos, Vecto Calculus, and Coodinate Systems David A. Randall Depatment of Atmospheic Science Coloado State Univesity Fot Collins, Coloado 80523. Scalas and vectos Any
More informationJ. N. R E DDY ENERGY PRINCIPLES AND VARIATIONAL METHODS APPLIED MECHANICS
J. N. E DDY ENEGY PINCIPLES AND VAIATIONAL METHODS IN APPLIED MECHANICS T H I D E DI T IO N JN eddy - 1 MEEN 618: ENEGY AND VAIATIONAL METHODS A EVIEW OF VECTOS AND TENSOS ead: Chapte 2 CONTENTS Physical
More informationP-2: The screw eye is subjected to two forces, ԦF 1 and ԦF 2. Determine the magnitude and direction of the resultant force.
P-1: ԦA=Ԧi +Ԧj -5k and B =Ԧi - 7Ԧj -6k. Detemine;?????? - A B B A A B B A B A B A 7 P-: The scew ee is subjected to two foces, Ԧ 1 and Ԧ. Detemine the magnitude and diection of the esultant foce. P-: The
More informationMAGNETIC FIELDS & UNIFORM PLANE WAVES
MAGNETIC FIELDS & UNIFORM PLANE WAVES Nme Sectin Multiple Chice 1. (8 Pts). (8 Pts) 3. (8 Pts) 4. (8 Pts) 5. (8 Pts) Ntes: 1. In the multiple chice questins, ech questin my hve me thn ne cect nswe; cicle
More informationPhysics 111. Exam #1. January 26, 2018
Physics xam # Januay 6, 08 ame Please ead and fllw these instuctins caefully: Read all pblems caefully befe attempting t slve them. Yu wk must be legible, and the ganizatin clea. Yu must shw all wk, including
More informationCHAPTER 1. Learning Objectives
CHTE sitin and Orientatin Definitins and Transfrmatins Marcel H. ng Jr., ug 26 Learning Objectives Describe psitin and rientatin f rigid bdies relative t each ther Mathematically represent relative psitin
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 information1 PreCalculus AP Unit G Rotational Trig (MCR) Name:
1 PreCalculus AP Unit G Rtatinal Trig (MCR) Name: Big idea In this unit yu will extend yur knwledge f SOH CAH TOA t wrk with btuse and reflex angles. This extensin will invlve the unit circle which will
More informationTrigonometric Ratios Unit 5 Tentative TEST date
1 U n i t 5 11U Date: Name: Trignmetric Ratis Unit 5 Tentative TEST date Big idea/learning Gals In this unit yu will extend yur knwledge f SOH CAH TOA t wrk with btuse and reflex angles. This extensin
More informationChapter 3 Kinematics in Two Dimensions; Vectors
Chapter 3 Kinematics in Tw Dimensins; Vectrs Vectrs and Scalars Additin f Vectrs Graphical Methds (One and Tw- Dimensin) Multiplicatin f a Vectr b a Scalar Subtractin f Vectrs Graphical Methds Adding Vectrs
More informationAIR FORCE RESEARCH LABORATORY
AIR FORC RSARCH LABORATORY The xtinctin Theem as an xample f Reseach Vistas in Mathematical Optics Mach Richad A. Albanese Infmatin Opeatins and Applied Mathematics Human ffectiveness Diectate Bks City-Base
More informationr 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