BED FORM DEFORMATION DUE TO UPSTREAM GROUP PILES

Size: px
Start display at page:

Download "BED FORM DEFORMATION DUE TO UPSTREAM GROUP PILES"

Transcription

1 BED FORM DEFORMATION DUE TO UPSTREAM GROUP PILES TAE HOON YOON Prfessr Emeritus Deartment f Civil Engineering Hanyang University, Seul, Krea taehyn@htmail.cm Abstract Defrmatin f be frms by assing thrugh a gru f vertical iles installe ustream in an en channel was examine exerimentally. With Frue number the heights an lengths f unes are increase an the steeness f unes ecreases. The heights f iles were fun t have negligible imact n the variatin f be frms. The ile iameter is a significant factr that causes the reuctin in the imensins f unes. Increase in number f iles er unit area efine as a ile ensity brings abut the ecrease in the size f une as much as 60%. Hwever, there exists an uer limit f the ile ensity beyn which the efrmatin f une becmes ineenent f the ensity. The steeness f unes becmes steeer with increase f the ensity. The efrme be frms resume their riginal states at a istance wnstream X/L 6 frm the en f ile zne.. Intructin Deening n the flw arameters an seiment rerties, an alluvial stream may unerg ifferent be frms. Fr the lwer regime f a subcritical flw, the stream be can exhibit riles an unes with the water surface being arximately flat. Kenney(1969) argue that the ccurrence f be frms is ue t (1) the result f an rerly attern f scur an esitin, (2) the instability henmenn an (3) the flw arameters an seiment rerties. Yalin(1977) inte ut that the unes are cause by a iscntinuity(rige) f a lane initial be, which inuces an alternatin in velcity rfile thrugh isturbance f turbulence structure an in cnsequence the velcity alternatin is resulte in the ecrease f seiment transrt, the grwth f accretin must take lace, an the variatin f be level by the Exner equatin must be accmanie. Base n the afrementine reasnings, any hysical aitin t a flw, which causes an alternatin in the flw structure an in the alluvial stream be features, will bring abut change in seiment transrt. Such change will lea t either increase r ecrease the magnitues f be frm gemetries such as the imensins f unes. Placing iles n the stream be may be ne f the aitins resulting in the alteratin, ssibly reuctin, f the imensins f unes. In alluvial streams, when the trughs f unes ass hyraulic structures, substantial art f their funatin may be exse t flw an it may enanger the safety f structures. Therefre, fr rer management, maintenance an safe esign f hyraulic structures, it is very 1

2 imrtant t evel measures t reuce the magnitues f unes r antiunes assing hyraulic structures r eliminate them entirely if ssible. The bjective f this aer is t examine hw the imensins f unes are affecte by assing thrugh a gru f iles with ifferent cmbinatin f ile installatin n the be in an en channel. Exeriments Exeriments were cnucte in a recirculating tilting flume that is 20m lng, 0.9m wie an 0.4m ee. Unifrm be seiments with a meian article iameter f 0.45mm were lace with the eth f 10cm in the flume be. The iles were sitine at the central regin f the flume with ifferent cmbinatin f ile iameter, istance amng iles an ile ensity. Fig.1 shws the efinitin sketch f exerimental setu. The evelment uratin f san waves varies frm 20min t 20hr eening n the value f τ / τ c (Yalin 1979). Hwever, each exeriment was run fr a uratin f 4 hur since the exeriments were aime t fin hw the alternatin f unes take laces. Fig. 1 Definitin sketch f exerimental setu Fig. 2 Layut f ile installatin The heights an lengths f unes were measure by a int gage an a ruler. At each run mre than ten measurements were mae an their imensins were average. Mst f exeriments were erfrme uner cnitins f flw eth f y = 13cm an flw velcity f u = 0.6m/s. The sitining f iles was rather arbitrary, i.e. the lngituinal istance an transverse sacing between iles were set as 52cm an 20cm, resectively as shwn in Fig. 2. The lngituinal istance f 52cm is the average length f unes at y = 13cm an u = 0.6m/s. Thrughut the exeriments the ile zne was a rectangular f 156cm in the irectin f flw an 60cm in the transverse irectin. 2

3 Table 1. Flw cnitins an average imensins f unes Flw eth (cm) Velcity (m/s) Fr Av height (cm) Av length (cm) Table 2. Prerties f iles Diameter (mm) Height ( h /y 0 ) Density (cm 2 /cm 2 ) x10 3 Dunes A une is ne f tyical be frms with shae that has an ustream face with a gentle, graually varying sl an an abrut wnstream face with a cnstant sle, which is arximately equal t the tangent f the rese angle f be material. Dunes fun in a subcritical flw regin f F r = (Mercer 1971) are nt statinary but they mve in the irectin f flw. The imensins f the be frms are eenent n the rerties f the flw, flui an be material. Yalin(1964) shwe a linear relatin f L = 5 y an Hin(1969) rerte a similar relatin f L = 7 y. Allen(1963) resente the fllwing relatinshi frm the bserve ata. lg y = lg H (1) lg H = lg L (2) in which L is the length f a san wave r une an H is the height f a une. Frue numbers f the flw that inuce the unes in this stuy fall in the range f 0.18 an 0.62(Table 1), which agrees with the finings by Gswami(1967). As can be seen in Fig. 3 the heights an lengths f unes are nte t be eenent n Frue number fr a given flw eth Fr 4.174Fr H/ y =0.0407e, L/ y = e (3a,b) where Fr is the Frue number ( u / gy ). The ltte ata f the heights versus lengths shwn in Fig.4 might be sai t agree t Allen s relatinshi f Eq.2 if it stans fr large riles, an the steeness f unes 3

4 Fig. 3 Increase f une imensins with Frue number Fig.4 Plt f heights versus lengths f unes fr ifferent velcities has the value f 1/14, whereas Yalin(1964, 1977) shwe H/L=1/30 1/5. The steeness was fun t be a functin f Frue number fr a given flw eth. In this articular case it can be efine in terms f Frue number Fr as 0.289Fr H/L = e (4) Effects f Piles n Dimensins f Dunes Effect f ile height : As shwn in Fig. 5, the effect f ile height at the ensity f iles f 1.47/1000 is negligible n bth heights an lengths f unes regarless f the iameter f ile. Meanwhile, the flw in an en channel are influence significantly by the height f vegetatin zne lace ustream(yn et al. 2004). The effect f vegetatin height n the velcity rfile leas t the reuctin in the scuring eth arun a ier with ifferent vegetatin height. The abve facts call fr further research fr the effect f ile height n the be frms with higher ensity f iles. Frm Fig. 5 it is nte that the variatin f heights an lengths f unes with ifferent ile height is negligible. Effect f ile iameter: Fig. 6 shws the variatin f the heights an lengths f unes in the wnstream regin f the ile zne f X 0-1.0m r X/L 0-2.0, where X starts at the wnstream en f the ile zne. It is nte that the heights an lengths f unes ecrease with increase f ile iameter an the reuctins amunt t 24% an 40% f the riginal sizes at D / y =1.0. Base n the limite ata in Fig.6, the imensins f unes wnstream regin f the ile zne can be reicte as 4

5 H H = ( D 2 ), y u L L u D = ( ) y 2 (5a,b) u=0.6m/s y 0 =13cm H av =4.26cm L av =52.73cm 0.2 wnstream 0-1m H/H av wnstream 0-1m L/L av D / y 0 Fig. 5 Effect f ile height n height Fig. 6 Effect f ile iameter n an length f unes imensins f unes Effect f ile ensity: The ensity f iles is efine as the rati f areas f ile gru an ile zne. Fr the sitins f iles within the ile zne, three rw f iles are lace in the transverse irectin an in the lngituinal irectin the number iles were varie in the range f tw t ten iles resulting in ensities ranging frm δ = 0.97/1000 t 4.93/1000. Fig. 7 Effect f ile ensity n Fig. 8 Effect f ile ensity n height f unes length f unes 5

6 The facts nte in Figs. 7 an 8 are that the effect f ile ensity is significant in the reuctin f the imensins f unes an there exists a limiting ensity f iles f ρ =3.45/1000 beyn which the imensins f unes are cease t ecrease. The steeness f une was fun t increase with the increase f ile ensity an the imensins f unes are reuce with the ensity f iles. Alternatin f unes in wnstream regin f ile zne: Figs.9 an 10 shw the variatins f the heights an lengths f unes in the wnstream regin f the ile zne an they inicate that the reuce heights an lengths f unes ue t assing thrugh Fig. 9 Heights f unes with istance wnstream Fig. 10 Lengths f unes with istance wnstream frm ile zne fr ifferent ile iameters frm ile zne fr ifferent iameters the ile zne increase with istance in wnstream irectin frm the ile zne, i.e. the reuce heights an lengths f unes are recvering graually t their riginal imensins befre entering the ile zne. At the istance f X=3m r X/L 6 wnstream frm the ile zne the reuce heights an lengths f unes resume arximately 90% f their riginal imensins Estimatin f alternatin f unes ue t assing thrugh ile zne: Uner the limite cnitins f be seiment 50 = 0.45mm, D/ y 108, an 0.97/1000 ρ 4.93/1000, the altere heights an lengths f unes after assing thrugh the gru f ile lace ustream may be estimate in terms f flw eth y, ile iameter D, ile ensity ρ an Frue number Fr as D H = { ( ) 6.19 ρ } e 3.89Fr y (6) y ρ 0 0 6

7 D = { ( ) ρ } (7) 4.17 Fr L e y ρ 0 y0 where H an L are the height an length f unes in the wnstream regin after assing the ile zne. Cnclusins The efrmatin f unes by assing a gru f iles in an en channel was investigate exerimentally an the finings are summarize. The imensins f unes are an increasing functin f Frue number in a subcritical flw regin, an ver a wie range f the length f unes a cnstant steeness revails an the steeness can be estimate in terms f Frue number. At a lwer ensity f iles such as ρ =1.47/1000, the effect f ile height is negligible an it nees further stuy at higher ensity f iles if the significant effect f vegetatin is cnsiere. With increase f ile iameter, reuctin in the heights an lengths f unes amunts t 24% an 40%, resectively at D / y = The imensins f unes are reuce significantly with the ensity f iles but there exists an uer limit f ρ =3.45/1000 abve which the unes cease t ecrease further. The reuce unes in their size in the wnstream regin f the ile zne resume their riginal magnitue graually as they mve wnstream an at X/L 0.6 they reach 90% f the riginal size. Equatins were erive t be able t reict the heights an lengths f unes in terms f arameters f flw an iles at a given rerties f be material. References Allen, J. R. L.(1963). Asymmetrical rile marks an the rigin f water-lai csets f crss-strata, Liverl an Manchester Gelgical Jurnal, 3, Gswami, A. C.(1967). Gemetric stuy f riles an unes, M.S. Thesis, Det. f Civil Engineering, Clra State University, Frt Cllins, Clra. Hin, M.(1969). Equilibrium range sectre f san waves frme by running water, J. Flui Mechanics, 34(3), Kenney, J. F.(1969). The frmatin f seiment riles, unes, an antiunes, Annual Review f Flui Mechanics, W. R. Sears, E., vl. 1, Annual Reviews, Inc., Pal Alt, Calif., Mercer, A. G.(1971). Analytically etermine be-frm shae, J. f Engineering Mech., ASCE, 97(1), Yalin, M. S.(1964). Gemetrical rerties f san waves, J. f Hyraul. Div., ASCE, 90(5), Yalin, M. S.(1977). Mechanics f Seiment Transrt, 2 n Eitin, Pergamn Press, New Yrk. 7

8 Yalin, M. S. an Karahan, E. (1979). Steeness f seimentary unes, J. f Hyraul. Div., ASCE, 105(4), Yn, T. H., Kim, Y. D., an Kim, S. T.(2004). Effects f a vegetatin zne n flw an scur arun a wnstream brige ier, J. f Krean Sc. f Civil Engineers, Water Engineering, 23(6B),

Energy considerations Energy considerations

Energy considerations Energy considerations Energy cnsieratins 99.0.8 DRFT. Energy cnsieratins The wrk reuire t assemble tw charges, an is fun by first bringing frm infinity t its esire psitin (which reuires n wrk) an then bringing frm infinity

More information

Key words: Hydraulic jump, Theoretical modeling, Stilling basin, Non-prismatic basins, Expanding channels, Negative steps

Key words: Hydraulic jump, Theoretical modeling, Stilling basin, Non-prismatic basins, Expanding channels, Negative steps Prc. f th Int. River Engineering Cnf., 8-0 Jan 00, Shahi-Chamran Univ., Ahvaz, Iran (CD ROM) Theretical meling f free hyraulic jumps at negative step in raial stilling basins Abelazim M. Negm, G.M. Abel-Aal,

More information

LATERAL DISPLACEMENT RESPONSE OF PILES INSTALLED IN NEAR SURFACE IMPROVED COARSE-GRAINED SOILS

LATERAL DISPLACEMENT RESPONSE OF PILES INSTALLED IN NEAR SURFACE IMPROVED COARSE-GRAINED SOILS ateral Displacement Respnse f Piles Installe in near Surface Imprve Carse-Graine Sils IGC 9, Guntur, INDIA ATERA DISPACEMENT RESPONSE OF PIES INSTAED IN NEAR SURFACE IMPROVED COARSE-GRAINED SOIS V. Pamavathi

More information

STUDENT NAME: STUDENT id #: WORK ONLY 5 QUESTIONS

STUDENT NAME: STUDENT id #: WORK ONLY 5 QUESTIONS GENERAL PHYSICS PH -A (MIROV) Exam 3 (03/31/15) STUDENT NAME: STUDENT i #: ------------------------------------------------------------------------------------------------------------------------------------------

More information

Physical Nature of the Covalent Bond Appendix H + H > H 2 ( ) ( )

Physical Nature of the Covalent Bond Appendix H + H > H 2 ( ) ( ) Physical Nature f the Cvalent Bn Appeni his stuy f the nature f the H cvalent bn frms a mlecular rbital as a linear cmbinatin f scale hyrgenic rbitals, LCAO-MO. he quantum mechanical integrals necessary

More information

In Flow Performance Relationship - IPR Curves

In Flow Performance Relationship - IPR Curves In Flw Perfrmance Relatinshi - IPR Curves The Inflw Perfrmance Relatinshi (IPR) fr a well is the relatinshi between the flw rate f the well and the flwing ressure f the well. In single hase flw this is

More information

Study Group Report: Plate-fin Heat Exchangers: AEA Technology

Study Group Report: Plate-fin Heat Exchangers: AEA Technology Study Grup Reprt: Plate-fin Heat Exchangers: AEA Technlgy The prblem under study cncerned the apparent discrepancy between a series f experiments using a plate fin heat exchanger and the classical thery

More information

Experiment #4 Gauss s Law Prelab Hints

Experiment #4 Gauss s Law Prelab Hints Eperiment #4 Gauss s Law Prela Hints This la an prela will make etensive use f Ptentials an Gauss s Law, an using calculus t recast the electric fiel in terms f ptential The intent f this is t prvie sme

More information

Cairo University Faculty of Engineering. Outline

Cairo University Faculty of Engineering. Outline Outline. Definitins. Parameters 3. Cmressibility f Chesinless Sils (Sand and Gravel) 4. Cmressibility f Chesive Sil 5. The edmeter Test fr Cmressin Measurements 6. Swelling f Clay 7. Cllasibility f Sand

More information

Key words Shock waves. Dusty gas. Solid particles. Shock jump relations. Mach number

Key words Shock waves. Dusty gas. Solid particles. Shock jump relations. Mach number Shck jum relatins fr a dusty gas atmshere Shck jum relatins fr a dusty gas atmshere R. K. Anand Deartment f Physics, University f Allahabad, Allahabad-00, India E-mail: anand.rajkumar@rediffmail.cm Abstract

More information

WYSE Academic Challenge Sectional Physics 2007 Solution Set

WYSE Academic Challenge Sectional Physics 2007 Solution Set WYSE caemic Challenge Sectinal Physics 7 Slutin Set. Crrect answer: E. Energy has imensins f frce times istance. Since respnse e. has imensins f frce ivie by istance, it clearly es nt represent energy.

More information

convection coefficient. The different property values of water at 20 C are given by: u W/m K, h=8062 W/m K

convection coefficient. The different property values of water at 20 C are given by: u W/m K, h=8062 W/m K Practice rblems fr Cnvective Heat Transfer 1. Water at 0 C flws ver a flat late 1m 1m at 10 C with a free stream velcity f 4 m/s. Determine the thickness f bndary layers, lcal and average vale f drag cefficient

More information

Differentiation Applications 1: Related Rates

Differentiation Applications 1: Related Rates Differentiatin Applicatins 1: Related Rates 151 Differentiatin Applicatins 1: Related Rates Mdel 1: Sliding Ladder 10 ladder y 10 ladder 10 ladder A 10 ft ladder is leaning against a wall when the bttm

More information

Projection Moiré Profilometry using Liquid Crystal Digital Gratings

Projection Moiré Profilometry using Liquid Crystal Digital Gratings 0th IMEKO TC4 ymsium n Braunschweig, GERMAY, 20, etember 2-4 Prjectin Miré Prfilmetry using iquid Crystal Digital Gratings Fumi Kbayashi, Center fr Otical Research and Educatin, Utsunmiya University; Yukitshi

More information

Physics 212. Lecture 12. Today's Concept: Magnetic Force on moving charges. Physics 212 Lecture 12, Slide 1

Physics 212. Lecture 12. Today's Concept: Magnetic Force on moving charges. Physics 212 Lecture 12, Slide 1 Physics 1 Lecture 1 Tday's Cncept: Magnetic Frce n mving charges F qv Physics 1 Lecture 1, Slide 1 Music Wh is the Artist? A) The Meters ) The Neville rthers C) Trmbne Shrty D) Michael Franti E) Radiatrs

More information

Physics 2010 Motion with Constant Acceleration Experiment 1

Physics 2010 Motion with Constant Acceleration Experiment 1 . Physics 00 Mtin with Cnstant Acceleratin Experiment In this lab, we will study the mtin f a glider as it accelerates dwnhill n a tilted air track. The glider is supprted ver the air track by a cushin

More information

Capacitance. Applications of Electric Potential. Capacitors in Kodak Cameras 3/17/2014. AP Physics B

Capacitance. Applications of Electric Potential. Capacitors in Kodak Cameras 3/17/2014. AP Physics B 3/7/04 apacitance P Physics B pplicatins f Electric Ptential Is there any way we can use a set f plates with an electric fiel? YES! We can make what is calle a Parallel Plate apacitr an Stre harges between

More information

Proceedings of the 11 th International Conference on Nanochannels, Microchannels, and Minichannels ICNMM2013 June 16-19, 2013, Sapporo, JAPAN

Proceedings of the 11 th International Conference on Nanochannels, Microchannels, and Minichannels ICNMM2013 June 16-19, 2013, Sapporo, JAPAN Prceeings the th Internatinal Cnerence n Nanchannels, Micrchannels, an Minichannels ICNMM3 June 6-9, 3, Sar, JAPAN ICNMM3-7378 HERMAL PERFORMANCE OF OSCILLAING HEA PIPES WIH NANOFLUID: A HEOREICAL SUDY

More information

" E ds = 0 becomes " E ds = 0 # d$ B. ! Not only charges produce E-field. ! a changing B-field also produces an E-field.

 E ds = 0 becomes  E ds = 0 # d$ B. ! Not only charges produce E-field. ! a changing B-field also produces an E-field. Faraay s aw & EM waves This ecture Displacement currents Mawell s equatins EM Waves MTE2 results Sme peple that ha the alternate will have a minr grae change talk t me after lecture Ave= 72/15 = 68% Frm

More information

SUPPLEMENTARY INFORMATION

SUPPLEMENTARY INFORMATION SUPPLEENTARY INFORATION i: 10.1038/nmat In situ NR Observatin f the Frmatin f etalli thium irstrutures in thium Batteries Rangeet Bhattaharyya a, Baris Key a, Hailng Chen a, Aam S. Best b, Anthny F. Hllenkam

More information

Chapter 16. Capacitance. Capacitance, cont. Parallel-Plate Capacitor, Example 1/20/2011. Electric Energy and Capacitance

Chapter 16. Capacitance. Capacitance, cont. Parallel-Plate Capacitor, Example 1/20/2011. Electric Energy and Capacitance summary C = ε A / d = πε L / ln( b / a ) ab C = 4πε 4πε a b a b >> a Chapter 16 Electric Energy and Capacitance Capacitance Q=CV Parallel plates, caxial cables, Earth Series and parallel 1 1 1 = + +..

More information

ENGI 4430 Parametric Vector Functions Page 2-01

ENGI 4430 Parametric Vector Functions Page 2-01 ENGI 4430 Parametric Vectr Functins Page -01. Parametric Vectr Functins (cntinued) Any nn-zer vectr r can be decmpsed int its magnitude r and its directin: r rrˆ, where r r 0 Tangent Vectr: dx dy dz dr

More information

Solar Characteristics

Solar Characteristics Slar Characteristics 8/8/03 1:55 Slar Characteristics Much f the structure f this sectin is base upn Chapter 7 f [Rahman 1999]. Here yu will be intruce t the characteristics f the energy we receive frm

More information

GAUSS' LAW E. A. surface

GAUSS' LAW E. A. surface Prf. Dr. I. M. A. Nasser GAUSS' LAW 08.11.017 GAUSS' LAW Intrductin: The electric field f a given charge distributin can in principle be calculated using Culmb's law. The examples discussed in electric

More information

Introduction to Three-phase Circuits. Balanced 3-phase systems Unbalanced 3-phase systems

Introduction to Three-phase Circuits. Balanced 3-phase systems Unbalanced 3-phase systems Intrductin t Three-hase Circuits Balanced 3-hase systems Unbalanced 3-hase systems 1 Intrductin t 3-hase systems Single-hase tw-wire system: Single surce cnnected t a lad using tw-wire system Single-hase

More information

A THREE-DIMENSIONAL STUDY OF THE MOTION OF A DROP IN PLANE POISEUILLE FLOW AT FINITE REYNOLDS NUMBERS *

A THREE-DIMENSIONAL STUDY OF THE MOTION OF A DROP IN PLANE POISEUILLE FLOW AT FINITE REYNOLDS NUMBERS * Iranian Jurnal f Science & Technlgy, Transactin B: Engineering, Vl. 34, N. B2, pp 179-196 Printe in The Islamic Republic f Iran, 2010 Shiraz University A THREE-DIMENSIONAL STUDY OF THE MOTION OF A DROP

More information

Computational modeling techniques

Computational modeling techniques Cmputatinal mdeling techniques Lecture 2: Mdeling change. In Petre Department f IT, Åb Akademi http://users.ab.fi/ipetre/cmpmd/ Cntent f the lecture Basic paradigm f mdeling change Examples Linear dynamical

More information

Section 5.8 Notes Page Exponential Growth and Decay Models; Newton s Law

Section 5.8 Notes Page Exponential Growth and Decay Models; Newton s Law Sectin 5.8 Ntes Page 1 5.8 Expnential Grwth and Decay Mdels; Newtn s Law There are many applicatins t expnential functins that we will fcus n in this sectin. First let s lk at the expnential mdel. Expnential

More information

Interference is when two (or more) sets of waves meet and combine to produce a new pattern.

Interference is when two (or more) sets of waves meet and combine to produce a new pattern. Interference Interference is when tw (r mre) sets f waves meet and cmbine t prduce a new pattern. This pattern can vary depending n the riginal wave directin, wavelength, amplitude, etc. The tw mst extreme

More information

Determination of ionic product constant of water (K w ) Handout 2014

Determination of ionic product constant of water (K w ) Handout 2014 Determinatin f inic rduct cnstant f water (K w ) andut 2014 Determinatin f inic rduct cnstant f water (Kw) frm equilibrium tential measurement f a hydrgen electrde Overview In this exeriment we use an

More information

MAGNETIC FIELDS CURRENT & RESISTANCE

MAGNETIC FIELDS CURRENT & RESISTANCE Fiels an Waves I Spring 005 MAGNETIC FIELDS CURRENT & RESISTANCE Name Slutin Sectin Typs Crrecte Multiple Chice 1. (8 Pts). (8 Pts) 3. (8 Pts) 4. (8 Pts) 5. (8 Pts) Ntes: 1. In the multiple chice questins,

More information

Low Speed Current Bearing Anti-force Waves

Low Speed Current Bearing Anti-force Waves Jurnal f the Arkansas Acaemy f Science Vlume 68 Article 13 014 Lw Spee Current Bearing Anti-frce Waves M. Hemmati Arkansas Tech University, mhemmati@atu.eu W. P. Chils Arkansas Tech University H. Shjaei

More information

Assume that the water in the nozzle is accelerated at a rate such that the frictional effect can be neglected.

Assume that the water in the nozzle is accelerated at a rate such that the frictional effect can be neglected. 1 HW #3: Cnservatin f Linear Mmentum, Cnservatin f Energy, Cnservatin f Angular Mmentum and Turbmachines, Bernulli s Equatin, Dimensinal Analysis, and Pipe Flws Prblem 1. Cnservatins f Mass and Linear

More information

Compressibility Effects

Compressibility Effects Definitin f Cmpressibility All real substances are cmpressible t sme greater r lesser extent; that is, when yu squeeze r press n them, their density will change The amunt by which a substance can be cmpressed

More information

Part a: Writing the nodal equations and solving for v o gives the magnitude and phase response: tan ( 0.25 )

Part a: Writing the nodal equations and solving for v o gives the magnitude and phase response: tan ( 0.25 ) + - Hmewrk 0 Slutin ) In the circuit belw: a. Find the magnitude and phase respnse. b. What kind f filter is it? c. At what frequency is the respnse 0.707 if the generatr has a ltage f? d. What is the

More information

Characteristics of premixed flame in microcombustors with different diameters

Characteristics of premixed flame in microcombustors with different diameters Applie Thermal Engineering 25 (25) 271 281 www.elsevier.cm/lcate/apthermeng Characteristics f premixe flame in micrcmbustrs with ifferent iameters Z.W. Li a, *, S.K Chu a, C. Shu a, H. Xue b, W.M. Yang

More information

Computational modeling techniques

Computational modeling techniques Cmputatinal mdeling techniques Lecture 4: Mdel checing fr ODE mdels In Petre Department f IT, Åb Aademi http://www.users.ab.fi/ipetre/cmpmd/ Cntent Stichimetric matrix Calculating the mass cnservatin relatins

More information

Drought damaged area

Drought damaged area ESTIMATE OF THE AMOUNT OF GRAVEL CO~TENT IN THE SOIL BY A I R B O'RN EMS S D A T A Y. GOMI, H. YAMAMOTO, AND S. SATO ASIA AIR SURVEY CO., l d. KANAGAWA,JAPAN S.ISHIGURO HOKKAIDO TOKACHI UBPREFECTRAl OffICE

More information

Equilibrium of Stress

Equilibrium 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 information

Chapter 4. Unsteady State Conduction

Chapter 4. Unsteady State Conduction Chapter 4 Unsteady State Cnductin Chapter 5 Steady State Cnductin Chee 318 1 4-1 Intrductin ransient Cnductin Many heat transfer prblems are time dependent Changes in perating cnditins in a system cause

More information

Preparation work for A2 Mathematics [2017]

Preparation work for A2 Mathematics [2017] Preparatin wrk fr A2 Mathematics [2017] The wrk studied in Y12 after the return frm study leave is frm the Cre 3 mdule f the A2 Mathematics curse. This wrk will nly be reviewed during Year 13, it will

More information

L a) Calculate the maximum allowable midspan deflection (w o ) critical under which the beam will slide off its support.

L a) Calculate the maximum allowable midspan deflection (w o ) critical under which the beam will slide off its support. ecture 6 Mderately arge Deflectin Thery f Beams Prblem 6-1: Part A: The department f Highways and Public Wrks f the state f Califrnia is in the prcess f imprving the design f bridge verpasses t meet earthquake

More information

2-D Momentum Conservation

2-D Momentum Conservation -D Mmentum Cnseratin Saleback Cllege Physics Department Purpse: T cnirm that linear mmentum is cnsere in tw-imensinal cllisins. T shw that kinetic energy is nearly cnsere in tw-imensinal near-elastic cllisins.

More information

( ) kt. Solution. From kinetic theory (visualized in Figure 1Q9-1), 1 2 rms = 2. = 1368 m/s

( ) kt. Solution. From kinetic theory (visualized in Figure 1Q9-1), 1 2 rms = 2. = 1368 m/s .9 Kinetic Mlecular Thery Calculate the effective (rms) speeds f the He and Ne atms in the He-Ne gas laser tube at rm temperature (300 K). Slutin T find the rt mean square velcity (v rms ) f He atms at

More information

, which yields. where z1. and z2

, which yields. where z1. and z2 The Gaussian r Nrmal PDF, Page 1 The Gaussian r Nrmal Prbability Density Functin Authr: Jhn M Cimbala, Penn State University Latest revisin: 11 September 13 The Gaussian r Nrmal Prbability Density Functin

More information

https://goo.gl/eaqvfo SUMMER REV: Half-Life DUE DATE: JULY 2 nd

https://goo.gl/eaqvfo SUMMER REV: Half-Life DUE DATE: JULY 2 nd NAME: DUE DATE: JULY 2 nd AP Chemistry SUMMER REV: Half-Life Why? Every radiistpe has a characteristic rate f decay measured by its half-life. Half-lives can be as shrt as a fractin f a secnd r as lng

More information

Soil Layer Deformation Model During Wide Raised Bed's Construction

Soil Layer Deformation Model During Wide Raised Bed's Construction Australian Jurnal f Basic an Applie Sciences, 7(0): 030, 03 ISSN 99878 Sil Layer Defrmatin Mel During Wie Raise Be's Cnstructin Ismail, Z. Erahim an Nahe K. Ismail Agric. Eng. Dept., Fac. f Agric. Mansura

More information

Department of Economics, University of California, Davis Ecn 200C Micro Theory Professor Giacomo Bonanno. Insurance Markets

Department of Economics, University of California, Davis Ecn 200C Micro Theory Professor Giacomo Bonanno. Insurance Markets Department f Ecnmics, University f alifrnia, Davis Ecn 200 Micr Thery Prfessr Giacm Bnann Insurance Markets nsider an individual wh has an initial wealth f. ith sme prbability p he faces a lss f x (0

More information

Optimization of frequency quantization. VN Tibabishev. Keywords: optimization, sampling frequency, the substitution frequencies.

Optimization of frequency quantization. VN Tibabishev. Keywords: optimization, sampling frequency, the substitution frequencies. UDC 519.21 Otimizatin f frequency quantizatin VN Tibabishev Asvt51@nard.ru We btain the functinal defining the rice and quality f samle readings f the generalized velcities. It is shwn that the timal samling

More information

Aircraft Performance - Drag

Aircraft Performance - Drag Aircraft Perfrmance - Drag Classificatin f Drag Ntes: Drag Frce and Drag Cefficient Drag is the enemy f flight and its cst. One f the primary functins f aerdynamicists and aircraft designers is t reduce

More information

Surface and Contact Stress

Surface and Contact Stress Surface and Cntact Stress The cncept f the frce is fundamental t mechanics and many imprtant prblems can be cast in terms f frces nly, fr example the prblems cnsidered in Chapter. Hwever, mre sphisticated

More information

Lecture 5: Equilibrium and Oscillations

Lecture 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 information

"NEET / AIIMS " SOLUTION (6) Avail Video Lectures of Experienced Faculty.

NEET / AIIMS  SOLUTION (6) Avail Video Lectures of Experienced Faculty. 07 NEET EXAMINATION SOLUTION (6) Avail Vide Lectures f Exerienced Faculty Page Sl. The lean exressin which satisfies the utut f this lgic gate is C = A., Whichindicates fr AND gate. We can see, utut C

More information

LHS Mathematics Department Honors Pre-Calculus Final Exam 2002 Answers

LHS Mathematics Department Honors Pre-Calculus Final Exam 2002 Answers LHS Mathematics Department Hnrs Pre-alculus Final Eam nswers Part Shrt Prblems The table at the right gives the ppulatin f Massachusetts ver the past several decades Using an epnential mdel, predict the

More information

Material Balance Equations

Material Balance Equations TG450 Reservir Recvery Techniques 07 T illustrate the simlest ssible mdel e can have f analysis f reservir behavi, e ill start ith derivatin f s-called. This tye f mdel excludes fluid fl inside the reservir,

More information

Chapter 2 GAUSS LAW Recommended Problems:

Chapter 2 GAUSS LAW Recommended Problems: Chapter GAUSS LAW Recmmended Prblems: 1,4,5,6,7,9,11,13,15,18,19,1,7,9,31,35,37,39,41,43,45,47,49,51,55,57,61,6,69. LCTRIC FLUX lectric flux is a measure f the number f electric filed lines penetrating

More information

Q1. A) 48 m/s B) 17 m/s C) 22 m/s D) 66 m/s E) 53 m/s. Ans: = 84.0 Q2.

Q1. A) 48 m/s B) 17 m/s C) 22 m/s D) 66 m/s E) 53 m/s. Ans: = 84.0 Q2. Phys10 Final-133 Zer Versin Crdinatr: A.A.Naqvi Wednesday, August 13, 014 Page: 1 Q1. A string, f length 0.75 m and fixed at bth ends, is vibrating in its fundamental mde. The maximum transverse speed

More information

Examiner: Dr. Mohamed Elsharnoby Time: 180 min. Attempt all the following questions Solve the following five questions, and assume any missing data

Examiner: Dr. Mohamed Elsharnoby Time: 180 min. Attempt all the following questions Solve the following five questions, and assume any missing data Benha University Cllege f Engineering at Banha Department f Mechanical Eng. First Year Mechanical Subject : Fluid Mechanics M111 Date:4/5/016 Questins Fr Final Crrective Examinatin Examiner: Dr. Mhamed

More information

TOPPER SAMPLE PAPER 2 Class XII- Physics

TOPPER SAMPLE PAPER 2 Class XII- Physics TOPPER SAMPLE PAPER 2 Class XII- Physics Time: Three Hurs Maximum Marks: 70 General Instructins (a) All questins are cmpulsry. (b) There are 30 questins in ttal. Questins 1 t 8 carry ne mark each, questins

More information

Lecture 10 Adiabatic Processes

Lecture 10 Adiabatic Processes ASME231 Atmsheri hermdynamis NC A& State U Deartment f Physis Dr. Yuh-Lang Lin htt://meslab.rg ylin@nat.edu Leture 10 Adiabati Presses (Se.3.5 f Hess) [Classial equatin editr: 0 dq ] Definitin: If a thermdynami

More information

Q1. A string of length L is fixed at both ends. Which one of the following is NOT a possible wavelength for standing waves on this string?

Q1. A string of length L is fixed at both ends. Which one of the following is NOT a possible wavelength for standing waves on this string? Term: 111 Thursday, January 05, 2012 Page: 1 Q1. A string f length L is fixed at bth ends. Which ne f the fllwing is NOT a pssible wavelength fr standing waves n this string? Q2. λ n = 2L n = A) 4L B)

More information

Solution to HW14 Fall-2002

Solution to HW14 Fall-2002 Slutin t HW14 Fall-2002 CJ5 10.CQ.003. REASONING AND SOLUTION Figures 10.11 and 10.14 shw the velcity and the acceleratin, respectively, the shadw a ball that underges unirm circular mtin. The shadw underges

More information

2D Turbulent Jets on Rough and Smooth Boundaries

2D Turbulent Jets on Rough and Smooth Boundaries IOSR Jurnal f Envirnmental Science, Txiclgy and Fd Technlgy (IOSR-JESTFT) e-issn: 39-,p- ISSN: 39-399.Vlume, Issue Ver. I (April. ), PP 7- www.isrjurnals.rg D Turbulent Jets n Rugh and Smth Bundaries Shazy

More information

ANALYSIS OF PNEUMATIC FINE PARTICLE PEENING PROCESS BY USING A HIGH-SPEED-CAMERA

ANALYSIS OF PNEUMATIC FINE PARTICLE PEENING PROCESS BY USING A HIGH-SPEED-CAMERA International Journal of Moern Physics B Vol. 24, Nos. 15 & 16 (21) 347 352 Worl Scientific Publishing Comany DOI: 1.1142/S217979216669 ANALYSIS OF PNEUMATIC FINE PARTICLE PEENING PROCESS BY USING A HIGH-SPEED-CAMERA

More information

On the Commutation Process of Capacitor Commutated Converter (CCC)

On the Commutation Process of Capacitor Commutated Converter (CCC) On the Cmmutatin Prcess f Capacitr Cmmutate Cnverter (CCC Angel J. J. Rezek*; Ariana A. s Sants zir*; Jcéli Suza e Sá** NFE/EE/DET Feeral niversity f tajubá / Electrical Engineering nstitute(* Av. BPS,

More information

Pressure And Entropy Variations Across The Weak Shock Wave Due To Viscosity Effects

Pressure And Entropy Variations Across The Weak Shock Wave Due To Viscosity Effects Pressure And Entrpy Variatins Acrss The Weak Shck Wave Due T Viscsity Effects OSTAFA A. A. AHOUD Department f athematics Faculty f Science Benha University 13518 Benha EGYPT Abstract:-The nnlinear differential

More information

Computational modeling techniques

Computational modeling techniques Cmputatinal mdeling techniques Lecture 11: Mdeling with systems f ODEs In Petre Department f IT, Ab Akademi http://www.users.ab.fi/ipetre/cmpmd/ Mdeling with differential equatins Mdeling strategy Fcus

More information

AP Physics Kinematic Wrap Up

AP 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 information

DEDICATED TO THE MEMORY OF R.J. WEINSHENK 1. INTRODUCTION

DEDICATED TO THE MEMORY OF R.J. WEINSHENK 1. INTRODUCTION CONVOLUTION TRIANGLES FOR GENERALIZED FIBONACCI NUMBERS VERNER E. HOGGATT, JR. San Jse State Cllege, San Jse, Califrnia DEDICATED TO THE MEMORY OF R.J. WEINSHENK. INTRODUCTION The sequence f integers Fj

More information

INVESTIGATION OF B-JUMP NEGATIVE STEP IN RADIAL STILLING BASINS

INVESTIGATION OF B-JUMP NEGATIVE STEP IN RADIAL STILLING BASINS Seventh Internatinal Water Technlgy Cnference Egypt 1-3 April 003 INVESTIGATION OF B-JUMP NEGATIVE STEP IN RADIAL STILLING BASINS A.M. Negm 1, G. M. Abdel-Aal 1, T.M. Owais and A.A. Habib 3 1 Assciate

More information

Section 6-2: Simplex Method: Maximization with Problem Constraints of the Form ~

Section 6-2: Simplex Method: Maximization with Problem Constraints of the Form ~ Sectin 6-2: Simplex Methd: Maximizatin with Prblem Cnstraints f the Frm ~ Nte: This methd was develped by Gerge B. Dantzig in 1947 while n assignment t the U.S. Department f the Air Frce. Definitin: Standard

More information

BASIC DIRECT-CURRENT MEASUREMENTS

BASIC DIRECT-CURRENT MEASUREMENTS Brwn University Physics 0040 Intrductin BASIC DIRECT-CURRENT MEASUREMENTS The measurements described here illustrate the peratin f resistrs and capacitrs in electric circuits, and the use f sme standard

More information

MATHEMATICS Higher Grade - Paper I

MATHEMATICS Higher Grade - Paper I Higher Mathematics - Practice Eaminatin B Please nte the frmat f this practice eaminatin is different frm the current frmat. The paper timings are different and calculatrs can be used thrughut. MATHEMATICS

More information

37 Maxwell s Equations

37 Maxwell s Equations 37 Maxwell s quatins In this chapter, the plan is t summarize much f what we knw abut electricity and magnetism in a manner similar t the way in which James Clerk Maxwell summarized what was knwn abut

More information

Electric Current and Resistance

Electric Current and Resistance Electric Current and Resistance Electric Current Electric current is the rate f flw f charge thrugh sme regin f space The SI unit f current is the ampere (A) 1 A = 1 C / s The symbl fr electric current

More information

2.8 The Derivative as a Function

2.8 The Derivative as a Function SECTION 2.8 THE DERIVATIVEASA FUNCTION D 129 2.8 The Derivative as a Functin 1. It appears that I is an dd functin, s l' will be an even functin- that is, t ' (-a) = l'(a). (a) l'(- 3) ~ 1.5 (b ) 1' (

More information

DINGWALL ACADEMY NATIONAL QUALIFICATIONS. Mathematics Higher Prelim Examination 2010/2011 Paper 1 Assessing Units 1 & 2.

DINGWALL ACADEMY NATIONAL QUALIFICATIONS. Mathematics Higher Prelim Examination 2010/2011 Paper 1 Assessing Units 1 & 2. INGWLL EMY Mathematics Higher Prelim Eaminatin 00/0 Paper ssessing Units & NTIONL QULIFITIONS Time allwed - hur 0 minutes Read carefull alculatrs ma NOT be used in this paper. Sectin - Questins - 0 (0

More information

MODULE 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

MODULE 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 information

Chapter 8. The Steady Magnetic Field 8.1 Biot-Savart Law

Chapter 8. The Steady Magnetic Field 8.1 Biot-Savart Law hapter 8. The teady Magnetic Field 8. Bit-avart Law The surce f steady magnetic field a permanent magnet, a time varying electric field, a direct current. Hayt; /9/009; 8- The magnetic field intensity

More information

Introductory Thoughts

Introductory Thoughts Flw Similarity By using the Buckingham pi therem, we have reduced the number f independent variables frm five t tw If we wish t run a series f wind-tunnel tests fr a given bdy at a given angle f attack,

More information

CHAPTER 8b Static Equilibrium Units

CHAPTER 8b Static Equilibrium Units CHAPTER 8b Static Equilibrium Units The Cnditins fr Equilibrium Slving Statics Prblems Stability and Balance Elasticity; Stress and Strain The Cnditins fr Equilibrium An bject with frces acting n it, but

More information

Thermodynamics Partial Outline of Topics

Thermodynamics Partial Outline of Topics Thermdynamics Partial Outline f Tpics I. The secnd law f thermdynamics addresses the issue f spntaneity and invlves a functin called entrpy (S): If a prcess is spntaneus, then Suniverse > 0 (2 nd Law!)

More information

Higher Mathematics Booklet CONTENTS

Higher Mathematics Booklet CONTENTS Higher Mathematics Bklet CONTENTS Frmula List Item Pages The Straight Line Hmewrk The Straight Line Hmewrk Functins Hmewrk 3 Functins Hmewrk 4 Recurrence Relatins Hmewrk 5 Differentiatin Hmewrk 6 Differentiatin

More information

Phy 213: General Physics III 6/14/2007 Chapter 28 Worksheet 1

Phy 213: General Physics III 6/14/2007 Chapter 28 Worksheet 1 Ph 13: General Phsics III 6/14/007 Chapter 8 Wrksheet 1 Magnetic Fields & Frce 1. A pint charge, q= 510 C and m=110-3 m kg, travels with a velcit f: v = 30 ˆ s i then enters a magnetic field: = 110 T ˆj.

More information

Conjoined. For Two Double Basses. Music by Martin Ritter 2016/17

Conjoined. For Two Double Basses. Music by Martin Ritter 2016/17 Cnjined r Tw Duble Basses Music by Martin Ritter 2016/17 Legend: The tw layers shuld always errm asynchrnusly unless the arts are cnnected by a dtted line r ntes are stemmed acrss bth arts. In these situatins

More information

ES201 - Examination 2 Winter Adams and Richards NAME BOX NUMBER

ES201 - Examination 2 Winter Adams and Richards NAME BOX NUMBER ES201 - Examinatin 2 Winter 2003-2004 Adams and Richards NAME BOX NUMBER Please Circle One : Richards (Perid 4) ES201-01 Adams (Perid 4) ES201-02 Adams (Perid 6) ES201-03 Prblem 1 ( 12 ) Prblem 2 ( 24

More information

READING STATECHART DIAGRAMS

READING STATECHART DIAGRAMS READING STATECHART DIAGRAMS Figure 4.48 A Statechart diagram with events The diagram in Figure 4.48 shws all states that the bject plane can be in during the curse f its life. Furthermre, it shws the pssible

More information

Part One: Heat Changes and Thermochemistry. This aspect of Thermodynamics was dealt with in Chapter 6. (Review)

Part One: Heat Changes and Thermochemistry. This aspect of Thermodynamics was dealt with in Chapter 6. (Review) CHAPTER 18: THERMODYNAMICS AND EQUILIBRIUM Part One: Heat Changes and Thermchemistry This aspect f Thermdynamics was dealt with in Chapter 6. (Review) A. Statement f First Law. (Sectin 18.1) 1. U ttal

More information

CHEM Thermodynamics. Change in Gibbs Free Energy, G. Review. Gibbs Free Energy, G. Review

CHEM Thermodynamics. Change in Gibbs Free Energy, G. Review. Gibbs Free Energy, G. Review Review Accrding t the nd law f Thermdynamics, a prcess is spntaneus if S universe = S system + S surrundings > 0 Even thugh S system

More information

OTHER USES OF THE ICRH COUPL ING CO IL. November 1975

OTHER USES OF THE ICRH COUPL ING CO IL. November 1975 OTHER USES OF THE ICRH COUPL ING CO IL J. C. Sprtt Nvember 1975 -I,," PLP 663 Plasma Studies University f Wiscnsin These PLP Reprts are infrmal and preliminary and as such may cntain errrs nt yet eliminated.

More information

Solution: (a) C 4 1 AI IC 4. (b) IBC 4

Solution: (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 information

NAME TEMPERATURE AND HUMIDITY. I. Introduction

NAME TEMPERATURE AND HUMIDITY. I. Introduction NAME TEMPERATURE AND HUMIDITY I. Intrductin Temperature is the single mst imprtant factr in determining atmspheric cnditins because it greatly influences: 1. The amunt f water vapr in the air 2. The pssibility

More information

Beam Expander Basics: Not All Spots Are Created Equal

Beam Expander Basics: Not All Spots Are Created Equal EARNING UNERSTANING INTROUCING APPYING Beam Expander Basics: Nt All Spts Are Created Equal A P P I C A T I O N N O T E S BEAM EXPANERS A laser beam expander is designed t increase the diameter f a cllimated

More information

NOTE ON APPELL POLYNOMIALS

NOTE ON APPELL POLYNOMIALS NOTE ON APPELL POLYNOMIALS I. M. SHEFFER An interesting characterizatin f Appell plynmials by means f a Stieltjes integral has recently been given by Thrne. 1 We prpse t give a secnd such representatin,

More information

Analysis of the heat transfer in double and triple concentric tube heat exchangers

Analysis of the heat transfer in double and triple concentric tube heat exchangers IOP Cnference Series: Materials Science an Engineering PAPER OPEN ACCESS Analysis f the heat transfer in uble an triple cncentric tube heat exchangers T cite this article: S Rulescu et al 06 IOP Cnf. Ser.:

More information

Homology groups of disks with holes

Homology groups of disks with holes Hmlgy grups f disks with hles THEOREM. Let p 1,, p k } be a sequence f distinct pints in the interir unit disk D n where n 2, and suppse that fr all j the sets E j Int D n are clsed, pairwise disjint subdisks.

More information

Reactor Pressure Vessel Head Loaded by a Corium Slug Impact Confirmation of the Results

Reactor Pressure Vessel Head Loaded by a Corium Slug Impact Confirmation of the Results Reactr Pressure Vessel Hea Lae by a Crium Slug Impact Cnfirmatin f the Results B. Dlensky, B. G11er, T. Jran, R. Krieg, M. Lux, G. Messemer, H. Rieger, M. Sir Frschungszentrum Karlsruhe GmbH, Pstfach 364,

More information

4. Find a, b, and c. 6. Find x and y.

4. Find a, b, and c. 6. Find x and y. Grace Brethren Christian Schl Entering Trig/Analysis: Page f Summer Packet fr Students entering Trig/Analysis Review prblems frm Gemetry: Shw yur wrk!. Twice the cmplement f angle A is 35 less than the

More information

An Introduction to Matrix Algebra

An Introduction to Matrix Algebra Mdern Cntrl Systems, Eleventh Editin, by Richard C Drf and Rbert H. Bish. ISBN: 785. 8 Pearsn Educatin, Inc., Uer Saddle River, NJ. All rights reserved. APPENDIX E An Intrductin t Matrix Algebra E. DEFINITIONS

More information

Lecture 6: Phase Space and Damped Oscillations

Lecture 6: Phase Space and Damped Oscillations Lecture 6: Phase Space and Damped Oscillatins Oscillatins in Multiple Dimensins The preius discussin was fine fr scillatin in a single dimensin In general, thugh, we want t deal with the situatin where:

More information