LINEAR FLOW BAR DIFFUSER
|
|
- Mavis Hopkins
- 5 years ago
- Views:
Transcription
1 INER FO BR IFFUER FB eies PPICION Fl Ba ystems satisfy bth the achitect's and enginee's equiements f ai distibutin system that ill maintain ptimum m ai cnditins hile being incnspicuus t the viee. he KBE Fl Ba linea system is a cntinuus slt system hich alls the ai distibutin hile fully integated the ceiling system and its cmpnents. Jet h ( J is an excellent chice f high bay applicatin peimete znes equiing vetical pjectin, typically installed n alls.igh h ( h Patten cntlle alls ai t be diected t the left ight hizntally as ell as dnad hen installed in a ceiling system, suface effect is maintained, even at educed vlumes t pvide m ai mtin ithut dafts.he igh h ( can be altenated ith the ng h ( Patten cntlle hee it is me dedicated t diect ai hizntally. FEURE NR CONRUCION Fame: -Cnstucted f extuded aluminum ally Fixed Fame (FF ngle end cap is pvided. Please check page 5 f inf. Fame Patitin: - Cnstucted f extuded aluminum ally eflects: - Cnstucted f extuded aluminum ally eflects cl: Black - he fully adjustable deflects all f ai patten t be cntlled fm vetical staight dn t hizntal alng the ceiling. izes: - tandad slt sizes ae, /", ", /", 3". - inimum length f 8. Finish: - tandad finish is hite cl ( Ral 900 f face f the diffuse & black f the deflects. OPION Please check page 3 / extended fame facty emvable(rf, Fameless(F0 & V-shape hidden fame(vf. f me inf. iteed cne f ceiling & all applicatin.(90 angle any special angle. Cuved f ceiling applicatin. Please check page 5 Open end & Flush end ae available. f me inf. BO metal blank-ff. ight hield. Othe cl available upn equest. Plenum bx - insulated nn-insulated. N.B: F cne edge (all a daing shing the aifl shuld be pvided. PGE /5 PP REV:.0 08 ate:30/04/08
2 R B O F R INE ERIE B F INER FO BR IFFUER FB ERIE ON I IURION R IU al h Vetic h ngula h ntal z i h del Vetical h ( igh igh h ( del al h Vetic del ( h h ntal iz izntal h ng Vetical h ng h ( del al h Vetic ngula h la h ngu Vetical h h Jet Jet h (J del Nte: h can be adjusted n site. be can : h Nte del (J e. n sit d ste adju l.cm.k a atin n e t n bei PGE /5 P P REV:.0 08 ate:30/04/08
3 INER FO BR IFFUER FB ERIE IENION N BORER YPE NR OE / extended Fame Facty emvable RF Fixed Fame FF (tandad 43mm (-/6 3 (/ 5.8mm (5/8 V-shape idden Fame VF Only lt Fameless F0 Numbe f lts lt idth 3mm (0." 3mm (0." idth Bde Bde eies J eies eies 5 ( 70 (3/4 (7/8 36 (3/8 38 (/ 95 (33/4 8 (/8 4 (5/8 0 (43/4 35 (3/8 4 (5/8 47 ( 64 (/ 46 (53/4 50 (5/6 55 (3/6 43 (/6 76 (3 7 (63/4 48 (7/8 6 (7/6 5 ( 3 (57/3 * (7/8 36 (3/8 93 (73/5 8 (/8 4 (5/8 47 ( 44 (93/5 35 (3/8 64 (/ 95 (3/5 76 (3 345 (33/5 38 (/ 59mm (-5/6 (5/6 43 (/6 4 (5/8 55 (3/6 48 (7/8 6 (7/6 50 NB:imensins ae in mm (inches. PGE 3/5 P P REV:.0 08 ate:30/04/08
4 INER FO BR IFFUER FB ERIE IENION N BORER YPE CORNER OE Ceiling Cne Face Vie p Vie CORNER O (9/ 50(0/ 0 546(/ 46 (53/4 57(/ (63/4 50(0 / 0 (43/4 546(/ (53/4 7 (63/4 (73/ (3/3 58 (67/3 (43/4 53(03/3 3 (57/3 / 593(37/0 93 (73/5 644(57/0 / 495(9/ / 3 (3/4 470(8/ / ith Fame Famless lt idth O 57(/ 597(3 / (47/0 44 (93/5 9 (83/5 670(67/0 70(03/5 695(77/0 95 (3/5 7(87/0 3 (3/5 345 (33/5 745(97/0 77(307/0 37 (43/5 3 all Cne CORNER O ith Fame 70 (3/4 / 0 (43/4 0 (43/4 46 (53/4 7 (63/4 97 (73/4 / 3 O Famless lt idth / / 3 46 (53/4 7 (63/4 3 (57/3 58 (67/3 93 (73/5 44 (93/5 95 (3/5 345 (33/5 9 (83/5 70(03/5 3 (3/5 37 (43/5 NB:imensins ae in mm (inches. PGE 4/5 P P REV:.0 08 ate:30/04/08
5 IGNEN RIP FC FIE CU his ptin alls the linea slt diffuse t be t size at the jb site. he diffuse is supplied 50mm (6 lnge ith the slt spaces set ba all timming. Field cut uld be specified FB ERIE a cntinuus un f diffuse m layut is equied and hee thee may be a duct lenght vaiatin. Jin stips and Pins ae pvided n all units ve 400mm (96 ith n exta cst. Pviding linea alignment f cntinuus linea slt diffuse, the jin stip slides int the utside & inside channels f the diffuse fame. ypical f all fame types. INER FO BR IFFUER CCEORIE & CONFIGURION iteed Cne pace Patten Cntlle ngle end Cap Flush End Cap BO E BNK-F Blank-ffs ae used t cve inactive sectins f lignment the linea slt diffuse. tip Clip Open end IG IE IG IE ight hield is used t cve nn plenum etu ight hield is used t cve nn plenum sectins f f thethelinea diffuse fm light e etun sectins linea slt slt diffuse fm tin. hipped lse f field cutting and instal light eflectin. hipped lse f field cutting and installatin. B OUNING BRCKE -lignment tips maintain tight jints beteen sectins and pvide alignment f lng cntinuus un CORNER (C - Facty assembled miteed cne sectins ae available ith 90 angle any special angle. -iteed cnes ae pvided ith standad length f 40cm intenal dimensin, the lengths ae pvided upn equest. kbe@kbeintenatinal.cm -- Ref : E PECIFICION RE UBJECE O CNGE IOU NOICE OR OBIGION. 4 -F cne edge (all a daing shing the aifl shuld be pvided. Face Vie p Vie 400 cm all Cne Vaiable CURVE CEIING FB (CU-CE -Facty cuved linea fl ba diffuse manufactued as ac full cicle f vaius adius & numbe f slts. -Cuved linea fl ba ae pvided ithut ai patten. PGE 5/5 P P REV:.0 08 ate:30/04/08
Work, 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 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 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 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 informationSurface and Interface Science Physics 627; Chemistry 542. Lecture 10 March 1, 2013
Suface and Inteface Science Physics 67; Chemisty 54 Lectue 0 Mach, 03 Int t Electnic Ppeties: Wk Functin,Theminic Electn Emissin, Field Emissin Refeences: ) Wduff & Delcha, Pp. 40-4; 46-484 ) Zangwill
More informationGraphs 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 informationGENERAL NOTES FOR THE YODOCK 2001M WITH STEEL RAIL KIT DESIGN NOTES FOR THE YODOCK 2001M WITH STEEL RAIL KIT 1.
GENEAL NOTES FO THE YODOCK 2001M WITH STEEL AIL KIT 1. 2. 3. 4. 5. 6. 7. 8. 9. THE LONGITUDINAL TAFFIC BAIE SYSTEMS PESENTED ON THIS STANDAD DAWING (INDEX) AND THE LABEL YODOCK AE POPIETAY DESIGNS BY YODOCK
More informationGENERAL NOTES FOR THE YODOCK 2001 WITH STEEL RAIL KIT DESIGN NOTES FOR THE YODOCK 2001 WITH STEEL RAIL KIT
GENEAL NOTES FO THE YODOCK 2001 WITH STEEL AIL KIT 1. 2. 3. 4. 5. 6. 7. 8. THE LONGITUDINAL TAFFIC BAIE SYSTEMS PESENTED ON THIS STANDAD DAWING (INDEX) AND THE LABEL YODOCK AE POPIETAY DESIGNS BY THE YODOCK
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 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 informationMuch that has already been said about changes of variable relates to transformations between different coordinate systems.
MULTIPLE INTEGRLS I P Calculus Cooinate Sstems Much that has alea been sai about changes of vaiable elates to tansfomations between iffeent cooinate sstems. The main cooinate sstems use in the solution
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 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 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 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 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 informationPhysics Fall Mechanics, Thermodynamics, Waves, Fluids. Lecture 6: motion in two and three dimensions III. Slide 6-1
Physics 1501 Fall 2008 Mechanics, Themodynamics, Waves, Fluids Lectue 6: motion in two and thee dimensions III Slide 6-1 Recap: elative motion An object moves with velocity v elative to one fame of efeence.
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 information(n 1)n(n + 1)(n + 2) + 1 = (n 1)(n + 2)n(n + 1) + 1 = ( (n 2 + n 1) 1 )( (n 2 + n 1) + 1 ) + 1 = (n 2 + n 1) 2.
Paabola Volume 5, Issue (017) Solutions 151 1540 Q151 Take any fou consecutive whole numbes, multiply them togethe and add 1. Make a conjectue and pove it! The esulting numbe can, fo instance, be expessed
More informationCh 30 - Sources of Magnetic Field! The Biot-Savart Law! = k m. r 2. Example 1! Example 2!
Ch 30 - Souces of Magnetic Field 1.) Example 1 Detemine the magnitude and diection of the magnetic field at the point O in the diagam. (Cuent flows fom top to bottom, adius of cuvatue.) Fo staight segments,
More informationThe study of the motion of a body along a general curve. the unit vector normal to the curve. Clearly, these unit vectors change with time, u ˆ
Section. Cuilinea Motion he study of the motion of a body along a geneal cue. We define u ˆ û the unit ecto at the body, tangential to the cue the unit ecto nomal to the cue Clealy, these unit ectos change
More informationKCET 2015 TEST PAPER WITH ANSWER KEY (HELD ON TUESDAY 12 th MAY, 2015) MATHEMATICS ALLEN Y (0, 14) (4) 14x + 5y ³ 70 y ³ 14and x - y ³ 5 (2) (3) (4)
KET 0 TEST PAPER WITH ANSWER KEY (HELD ON TUESDAY th MAY, 0). If a and b ae the oots of a + b = 0, then a +b is equal to a b () a b a b () a + b Ans:. If the nd and th tems of G.P. ae and esectively, then
More informationPhysics 2212 GH Quiz #2 Solutions Spring 2016
Physics 2212 GH Quiz #2 Solutions Sping 216 I. 17 points) Thee point chages, each caying a chage Q = +6. nc, ae placed on an equilateal tiangle of side length = 3. mm. An additional point chage, caying
More informationUniform Circular Motion
Unifom Cicula Motion Intoduction Ealie we defined acceleation as being the change in velocity with time: a = v t Until now we have only talked about changes in the magnitude of the acceleation: the speeding
More informationPhysics 201 Homework 4
Physics 201 Homewok 4 Jan 30, 2013 1. Thee is a cleve kitchen gadget fo dying lettuce leaves afte you wash them. 19 m/s 2 It consists of a cylindical containe mounted so that it can be otated about its
More informationLecture 8 - Gauss s Law
Lectue 8 - Gauss s Law A Puzzle... Example Calculate the potential enegy, pe ion, fo an infinite 1D ionic cystal with sepaation a; that is, a ow of equally spaced chages of magnitude e and altenating sign.
More informationPhysics 111 Lecture 5 Circular Motion
Physics 111 Lectue 5 Cicula Motion D. Ali ÖVGÜN EMU Physics Depatment www.aovgun.com Multiple Objects q A block of mass m1 on a ough, hoizontal suface is connected to a ball of mass m by a lightweight
More informationInsulated Bearings MEGAOHM TM Series
Fo ew Technology etwok copoation R Insulated eaings MEGAOHM TM Seies Insulated eaings MEGAOHM TM Seies : Offeing Enhanced Safety and Reliability eaings used in electical equipment such as motos and powe
More informationReview Exercise Set 16
Review Execise Set 16 Execise 1: A ectangula plot of famland will be bounded on one side by a ive and on the othe thee sides by a fence. If the fame only has 600 feet of fence, what is the lagest aea that
More informationPhysics 1114: Unit 5 Hand-out Homework (Answers)
Physics 1114: Unit 5 Hand-out Homewok (Answes) Poblem set 1 1. The flywheel on an expeimental bus is otating at 420 RPM (evolutions pe minute). To find (a) the angula velocity in ad/s (adians/second),
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 informationSection 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 informationOLYMON. Produced by the Canadian Mathematical Society and the Department of Mathematics of the University of Toronto. Issue 9:2.
OLYMON Poduced by the Canadian Mathematical Society and the Depatment of Mathematics of the Univesity of Toonto Please send you solution to Pofesso EJ Babeau Depatment of Mathematics Univesity of Toonto
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 informationHandout: IS/LM Model
Econ 32 - IS/L odel Notes Handout: IS/L odel IS Cuve Deivation Figue 4-4 in the textbook explains one deivation of the IS cuve. This deivation uses the Induced Savings Function fom Chapte 3. Hee, I descibe
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 informationSERVICE SECTION. There's Always Something Cooking! Service, Parts, and Schematics For Gas Fryers With Options
SEVICE SECTIN There's Always Something Cooking! Service, Parts, and Schematics For Gas Fryers With ptions Including ptions, Built-In and UFM (Spacefighter) Filter Systems Covering Models 7, 1, 14, 14,
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 informationMath Section 4.2 Radians, Arc Length, and Area of a Sector
Math 1330 - Section 4. Radians, Ac Length, and Aea of a Secto The wod tigonomety comes fom two Geek oots, tigonon, meaning having thee sides, and mete, meaning measue. We have aleady defined the six basic
More informationUniform Circular Motion
Unifom Cicula Motion Have you eve idden on the amusement pak ide shown below? As it spins you feel as though you ae being pessed tightly against the wall. The ide then begins to tilt but you emain glued
More informationPhysics 201, Lecture 6
Physics 201, Lectue 6 Today s Topics q Unifom Cicula Motion (Section 4.4, 4.5) n Cicula Motion n Centipetal Acceleation n Tangential and Centipetal Acceleation q Relatie Motion and Refeence Fame (Sec.
More informationHELLA. Linear slot diffuser. Ordering codes. HELLA - Linear diffuser. Linear Diffusers 1 / 18. Example of the ordering code HELLA B-0-0-AN
Linear Diffusers / 8 HELLA Linear slot diffuser Ordering codes HELLA - Linear diffuser HELLA - Number of slots... Diffuser length L (mm) ) Increment mm... Deflector colour Damper Diffuser construction
More informationx 1 b 1 Consider the midpoint x 0 = 1 2
1 chapte 2 : oot-finding def : Given a function f(), a oot is a numbe satisfying f() = 0. e : f() = 2 3 = ± 3 question : How can we find the oots of a geneal function f()? 2.1 bisection method idea : Find
More information( ) ( ) Review of Force. Review of Force. r = =... Example 1. What is the dot product for F r. Solution: Example 2 ( )
: PHYS 55 (Pat, Topic ) Eample Solutions p. Review of Foce Eample ( ) ( ) What is the dot poduct fo F =,,3 and G = 4,5,6? F G = F G + F G + F G = 4 +... = 3 z z Phs55 -: Foce Fields Review of Foce Eample
More 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 informationCBN 98-1 Developable constant perimeter surfaces: Application to the end design of a tape-wound quadrupole saddle coil
CBN 98-1 Developale constant peimete sufaces: Application to the end design of a tape-wound quadupole saddle coil G. Dugan Laoatoy of Nuclea Studies Conell Univesity Ithaca, NY 14853 1. Intoduction Constant
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 informationMONTE CARLO SIMULATION OF FLUID FLOW
MONTE CARLO SIMULATION OF FLUID FLOW M. Ragheb 3/7/3 INTRODUCTION We conside the situation of Fee Molecula Collisionless and Reflective Flow. Collisionless flows occu in the field of aefied gas dynamics.
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 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 informationtransformation Earth V-curve (meridian) λ Conical projection. u,v curves on the datum surface projected as U,V curves on the projection surface
. CONICAL PROJECTIONS In elementay texts on map pojections, the pojection sufaces ae often descibed as developable sufaces, such as the cylinde (cylindical pojections) and the cone (conical pojections),
More informationRelative motion (Translating axes)
Relative motion (Tanslating axes) Paticle to be studied This topic Moving obseve (Refeence) Fome study Obseve (no motion) bsolute motion Relative motion If motion of the efeence is known, absolute motion
More informationChapter 5. Uniform Circular Motion. a c =v 2 /r
Chapte 5 Unifom Cicula Motion a c =v 2 / Unifom cicula motion: Motion in a cicula path with constant speed s v 1) Speed and peiod Peiod, T: time fo one evolution Speed is elated to peiod: Path fo one evolution:
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 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 informationPolar Coordinates. a) (2; 30 ) b) (5; 120 ) c) (6; 270 ) d) (9; 330 ) e) (4; 45 )
Pola Coodinates We now intoduce anothe method of labelling oints in a lane. We stat by xing a oint in the lane. It is called the ole. A standad choice fo the ole is the oigin (0; 0) fo the Catezian coodinate
More information( )( )( ) ( ) + ( ) ( ) ( )
3.7. Moel: The magnetic fiel is that of a moving chage paticle. Please efe to Figue Ex3.7. Solve: Using the iot-savat law, 7 19 7 ( ) + ( ) qvsinθ 1 T m/a 1.6 1 C. 1 m/s sin135 1. 1 m 1. 1 m 15 = = = 1.13
More informationME 210 Applied Mathematics for Mechanical Engineers
Tangent and Ac Length of a Cuve The tangent to a cuve C at a point A on it is defined as the limiting position of the staight line L though A and B, as B appoaches A along the cuve as illustated in the
More informationDepartment of Physics, Korea University Page 1 of 5
Name: Depatment: Student ID #: Notice ˆ + ( 1) points pe coect (incoect) answe. ˆ No penalty fo an unansweed question. ˆ Fill the blank ( ) with ( ) if the statement is coect (incoect). ˆ : coections to
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 informationSlot diffuser. Type VSD35 2/2.6/B/3. with 35 mm wide slot
2/2.6/B/3 Slot diffuser Type VSD35 with 35 mm wide slot TROX UK Ltd Telephone +44 (0) 1842 754545 Caxton Way Telefax +44 (0) 1842 763051 Thetford e-mail trox@troxuk.co.uk Norfolk IP24 3SQ www.troxuk.co.uk
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 informationMotion along curved path *
OpenStax-CNX module: m14091 1 Motion along cuved path * Sunil Kuma Singh This wok is poduced by OpenStax-CNX and licensed unde the Ceative Commons Attibution License 2.0 We all expeience motion along a
More informationPhysics: Work & Energy Beyond Earth Guided Inquiry
Physics: Wok & Enegy Beyond Eath Guided Inquiy Elliptical Obits Keple s Fist Law states that all planets move in an elliptical path aound the Sun. This concept can be extended to celestial bodies beyond
More 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 informationPLAY OFF 48" FOOSBALL TABLE ASSEM BLY I NSTRU CTI ONS
PLAY OFF 48" FOOSBALL TABLE ASSEM BLY I NSTRU CTI ONS NG1031F THANK Y OU! Th a n k yo u f o r p u r ch a si n g t h i s p r o d u ct. We w o r k a r o u n d t h e cl o ck a n d a r o u n d t h e g l o
More informationCBE Transport Phenomena I Final Exam. December 19, 2013
CBE 30355 Tanspot Phenomena I Final Exam Decembe 9, 203 Closed Books and Notes Poblem. (20 points) Scaling analysis of bounday laye flows. A popula method fo measuing instantaneous wall shea stesses in
More informationRadian 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 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 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 informationElectrostatics (Electric Charges and Field) #2 2010
Electic Field: The concept of electic field explains the action at a distance foce between two chaged paticles. Evey chage poduces a field aound it so that any othe chaged paticle expeiences a foce when
More informationEffect of no-flow boundaries on interference testing. in fractured reservoirs
Effect of no-flo boundaies on intefeence testing in factued esevois T.Aa. Jelmet 1 1 epatement of petoleum engineeing and applied geophysics,, Noegian Univesity of Science and Tecnology, NTNU. Tondheim,
More informationSEE LAST PAGE FOR SOME POTENTIALLY USEFUL FORMULAE AND CONSTANTS
Cicle instucto: Moow o Yethiaj Name: MEMORIL UNIVERSITY OF NEWFOUNDLND DEPRTMENT OF PHYSICS ND PHYSICL OCENOGRPHY Final Eam Phsics 5 Winte 3:-5: pil, INSTRUCTIONS:. Do all SIX (6) questions in section
More information1) Consider an object of a parabolic shape with rotational symmetry z
Umeå Univesitet, Fysik 1 Vitaly Bychkov Pov i teknisk fysik, Fluid Mechanics (Stömningsläa), 01-06-01, kl 9.00-15.00 jälpmedel: Students may use any book including the tetbook Lectues on Fluid Dynamics.
More informationMO-ARML --- September, POWER OF A POINT
M-ML --- Septembe, 208 -- W INT owe of a oint is a set of thee-theoems-in-one about cicles and line segments. * = * 2 = * * = * XISS G 8 8 2 S X H Z 3 6 H 7 T K. = 4 and X < X, find X.. ind HK.. ind TV.
More informationSolution to Problem First, the firm minimizes the cost of the inputs: min wl + rk + sf
Econ 0A Poblem Set 4 Solutions ue in class on Tu 4 Novembe. No late Poblem Sets accepted, so! This Poblem set tests the knoledge that ou accumulated mainl in lectues 5 to 9. Some of the mateial ill onl
More informationRelated Rates - the Basics
Related Rates - the Basics In this section we exploe the way we can use deivatives to find the velocity at which things ae changing ove time. Up to now we have been finding the deivative to compae the
More informationSubject : MATHEMATICS
CCE RF 560 00 KARNATAKA SECONDARY EDUCATION EXAMINATION BOARD, MALLESWARAM, BANGALORE 560 00 05 S. S. L. C. EXAMINATION, MARCH/APRIL, 05 : 06. 04. 05 ] MODEL ANSWERS : 8-E Date : 06. 04. 05 ] CODE NO.
More informationLab #9: The Kinematics & Dynamics of. Circular Motion & Rotational Motion
Reading Assignment: Lab #9: The Kinematics & Dynamics of Cicula Motion & Rotational Motion Chapte 6 Section 4 Chapte 11 Section 1 though Section 5 Intoduction: When discussing motion, it is impotant to
More informationNo. 48. R.E. Woodrow. Mathematics Contest of the British Columbia Colleges written March 8, Senior High School Mathematics Contest
341 THE SKOLIAD CORNER No. 48 R.E. Woodow This issue we give the peliminay ound of the Senio High School Mathematics Contest of the Bitish Columbia Colleges witten Mach 8, 2000. My thanks go to Jim Totten,
More information1 Dark Cloud Hanging over Twentieth Century Physics
We ae Looking fo Moden Newton by Caol He, Bo He, and Jin He http://www.galaxyanatomy.com/ Wuhan FutueSpace Scientific Copoation Limited, Wuhan, Hubei 430074, China E-mail: mathnob@yahoo.com Abstact Newton
More informationH STO RY OF TH E SA NT
O RY OF E N G L R R VER ritten for the entennial of th e Foundin g of t lair oun t y on ay 8 82 Y EEL N E JEN K RP O N! R ENJ F ] jun E 3 1 92! Ph in t ed b y h e t l a i r R ep u b l i c a n O 4 1922
More informationJournal of Solid Mechanics and Materials Engineering
Junal f Slid Mechanics and Mateials Engineeing Vl. 4, N. 8, 21 Themal Stess and Heat Tansfe Cefficient f Ceamics Stalk Having Ptubeance Dipping int Mlten Metal* Na-ki NOD**, Henda**, Wenbin LI**, Yasushi
More informationNUMERICAL EVALUATION ON FLOOR COOLING CAPACITY IN AN AIRPORT AH, Nijmegen, the Netherlands Tianjin, China
ceedings: Building Simulatin 07 NUMEICAL EVALUATION ON FLOO COOLING CAACITY IN AN AIOT 3,3, Bing Yu, J.. uchti and.g. Luscuee Divisin Building Sevices, yal Haskning Gup, stbx 5 6500 AH, Nijmegen, the Nethelands
More information2 Cut the circle along the fold lines to divide the circle into 16 equal wedges. radius. Think About It
Activity 8.7 Finding Aea of Cicles Question How do you find the aea of a cicle using the adius? Mateials compass staightedge scissos Exploe 1 Use a compass to daw a cicle on a piece of pape. Cut the cicle
More informationMovie Review Part One due Tuesday (in class) please print
Movie Review Pat One due Tuesday (in class) please pint Test in class on Fiday. You may stat at 8:30 if you want. (The topic of powe is not on test.) Chaptes 4-6 Main Ideas in Class Today Afte class, you
More informationAir distribution systems. Adjustable induction outlet IN-V...
ir distribution systems djustable induction outlet IN-V... DS E 0. Construction and function Preliminary remarks In addition to its induction outlet with preset discharge direction ), KRNTZ KOMPONENTEN
More informationChap 5. Circular Motion: Gravitation
Chap 5. Cicula Motion: Gavitation Sec. 5.1 - Unifom Cicula Motion A body moves in unifom cicula motion, if the magnitude of the velocity vecto is constant and the diection changes at evey point and is
More informationPhysics 4A Chapter 8: Dynamics II Motion in a Plane
Physics 4A Chapte 8: Dynamics II Motion in a Plane Conceptual Questions and Example Poblems fom Chapte 8 Conceptual Question 8.5 The figue below shows two balls of equal mass moving in vetical cicles.
More informationEcon 201: Problem Set 2 Answers
Econ 0: Poblem Set Anses Instucto: Alexande Sollaci T.A.: Ryan Hughes Winte 08 Question (a) The fixed cost is F C = 4 and the total vaiable costs ae T CV (y) = 4y. (b) To anse this question, let x = (x,...,
More informationUnit 7: Sources of magnetic field
Unit 7: Souces of magnetic field Oested s expeiment. iot and Savat s law. Magnetic field ceated by a cicula loop Ampèe s law (A.L.). Applications of A.L. Magnetic field ceated by a: Staight cuent-caying
More informationWritten as per the revised syllabus prescribed by the Maharashtra State Board of Secondary and Higher Secondary Education, Pune.
Witten as pe e evised syllabus pescibed by e Mahaashta State oad of Seconday and Highe Seconday Education, Pune. Pecise Physics I SD. XII Sci. Salient Featues Concise coveage of syllabus in Question nswe
More information8.7 Circumference and Area
Page 1 of 8 8.7 Cicumfeence and Aea of Cicles Goal Find the cicumfeence and aea of cicles. Key Wods cicle cente adius diamete cicumfeence cental angle secto A cicle is the set of all points in a plane
More informationAir distribution systems. Please note, type code is new, see last page. Floor twist outlets DB-E... for commercial rooms DS 1146 E 02.
Air distributin systems Please nte, type cde is new, see last page. Flr twist utlets DB-E... fr cmmercial rms DS E 0.0/ Flr twist utlets nstructin design Preliminary remarks Air utlets frm KRANTZ KOMPONENTEN
More informationWheel : MC, IC, rc. Pendulum : MB, IB, LB
In the figue, two cables of stiffness connect a wheel of mass M c to gound. The wheel with adius, has mass moment of inetia is I The pendulum, attached to the wheel cente, has mass M and mass moment of
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 informationMomentum is conserved if no external force
Goals: Lectue 13 Chapte 9 v Employ consevation of momentum in 1 D & 2D v Examine foces ove time (aka Impulse) Chapte 10 v Undestand the elationship between motion and enegy Assignments: l HW5, due tomoow
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 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 informationChapter 5. really hard to start the object moving and then, once it starts moving, you don t have to push as hard to keep it moving.
Chapte 5 Fiction When an object is in motion it is usually in contact with a viscous mateial (wate o ai) o some othe suface. So fa, we have assumed that moving objects don t inteact with thei suoundings
More information