ACCELEROGRAPH RECORDINGS OF THE M USA EARTHQUAKE 16 SEPTEMBER, 1972
|
|
- Cynthia Hudson
- 5 years ago
- Views:
Transcription
1 115 ACCELEROGRAPH RECORDINGS OF THE M USA EARTHQUAKE 16 SEPTEMBER, 1972 B.Gauir SUMMARY On 16 September, 1972 at UT an earthquake f magnitude ML 5.0 ccurred in sutheast Papua within abut 20 km f a prpsed dam site n the Musa River. The earthquake triggered tw accelergraphs, Musa A and Musa B, ne at the crest and ne at the base f the dam site. The peak grund acceleratins recrded by the accelergraphs were 1.85 m/s^ and 0.39 m/s^ respectively; the peak grund velcities were 87 mm/s and 2.0 mm/s; and the crrespnding mean perids f the grund mtin were abut 0.23 and 0.04 s. The difference in the nature f the accelergrams is attributed t the difference in the gelgical and tpgraphical settings f the accelergraph sites. The upper site has an elevatin f 406 m and cnsists f abut 60 m f weathered sediments verlying fresh ultramafics. The lwer site has an elevatin f 112 m and cnsists f an utcrp f the ultramafic cmplex. 1. INTRODUCTION In June, 1972 the Bureau f Mineral Resurces, Gelgy and Gephysics (BMP), installed 2 accelergraphs (hereafter called "Musa A" and "Musa B"), 600 m apart, ne n weathered sediments n the crest f ne f the abutments and ne n hard ultramafic rck at the base, f a prpsed dam. site n the Musa River in sutheast Papua (Fig. 1). At abut UT n 16 September, 1972 an earthquake f magnitude ML 5.0 ccurred within 20 km f the dam site and triggered the accelergraphs. Despite the clseness f the accelergraphs, the accelergrams differ in bth acceleratin amplitude and perid (Figs. 2 and 3). The triggerings were significant insfar as this was the first time in Papua New Guinea that tw strng-mtin instruments recrded simultaneusly n nearby hard and sft rck sites. 2. GROUND MOTION AT THE ACCELEROGRAPH SITES Table 1 lists the maximum grund acceleratin and velcities in the vertical, nrth-suth, and east-west directins; and the perids f grund mtin at the times f maximum acceleratin. Fig. 2 shws the three cmpnents f bth accelergrams and Fig. 3 is a digitized representatin f bth grund acceleratin and velcity at the Musa A site. 2 Acceleratins greater than 0.3 m/s ( g where g is the acceleratin wing t gravity) were recrded fr abut 11 secnds by the Musa A accelergraph. Acceleratins greater than abut 0.15 m/s^ were recrded fr a duratin f * Department f Minerals and Energy, Prt Mresby Gephysics Observatry, Papua New Guinea. abut 5.5 secnds at the Musa B site. 3. ACCELEROGRAPH SITES Figure 4 shws bth accelergraph-site prfiles dwn t bedrck and includes seismic shear wave velcity, density and thickness f each layer. This data was acquired frm seismic wrk (Bishp et al, in prep.) and drilling (Macias, 1971) in the vicinity f the accelergraph sites. The bedrck which utcrps at the Musa B site is an ultramafic cmplex (seismic shear wave velcity near surface f abut 2500 m/s and density 2.8 x 10 3 kg/m 3 and is als fund 60 m beneath a deeply weathered sedimentary pile at the Musa A site. The 2.5 sec S-P time n bth accelergrams suggests that the earthquake hypcentre was abut 19 km frm the dam site which is much greater than the distance separating the tw accelergraphs (0.6km). Therefre the prpagatin path t the tp f the ultramafics at bth sites culd be cnsidered t be identical and cnsequently the differences between recrded grund mtin at the tw sites is attributed t near surface features f the sites alne. 4. THEORETICAL MODEL TO ACCOUNT FOR ACCELERATION AMPLIFICATION IN LAYERED SYSTEMS Madera (1970) utlined a theretical methd t predict the fundamental perid f the seismic waves and the amplificatin f seismic acceleratin in sil prfiles abve bedrck. He btained gd agreement between cmputed and measured values. The principle is that resnance f seismic waves is set up in the layered system abve bedrck, which amplifies the incming signal. Because it is a resnance effect, the dminating perid recrded n the accelergram shuld be related t the fundamental perid f the layered mdel. On applicatin f Madera's (1970) methd t the prfile with parameters shwn in Fig. BULLETIN OF THE NEW ZEALAND NATIONAL SOCIETY FOR EARTHQUAKE ENGINEERING, VOL.9 N0.2. JUNE 1976
2 a fundamental perid f abut 0.26 s was cmputed fr the Musa A site. This value cmpares reasnably well with the measured mean Musa A accelergram perid f 0.23 s at the time f peak acceleratin (Table 1). Because the prpagatin paths thrugh the ultramafics are cnsidered t be identical, it is reasnable t assume that the input signal at the tp f the ultramaf ics beneath Musa A is the same as that registered at Musa B. Therefre Madera's (1970) mdel culd be used t estimate the peak acceleratin amplificatin at Musa A directly with respect t Musa B. When this was carried cut an amplificatin rati f 2 was btained. When extreme estimates f layer density and internal damping were substituted, the maximum pssible amplificatin rati attainable was 2.7, which is still significantly less than the measured acceleratin rati f 4.5. Hence Madera T s (1970) mdel des nt fully accunt fr the amplificatin f acceleratin which tk place at the Musa A site. 5. TOPOGRAPHICAL FACTOR Davis & West (1973) have bserved the effects f tpgraphy n grund mtin at statin sites carefully selected s that the nly difference between them was tpgraphy. Their results indicate that the amunt f amplificatin and the perids at which it ccurs vary with the size f the muntain, and are prbably a functin f the relatin between the wavelengths f the incming seismic signal and the dimensins f the muntain. The suggested causative mechanism fr this amplificatin is resnance f the muntain set up by shear waves when the wavelength f these waves are f the same rder as the dimensins f the muntain. Musa A and B sites are lcated respectively near the crest and base f a 400 m high muntain. Assuming a shear wave velcity f 3.5 km/s and using a perid f 0.25 s (crrespnding rughly t the perid at peak acceleratin) a wavelength f abut 900 m is btained, which is abut half the width f the muntain. Using the results btained by Davis & West (1973) fr a muntain f similar size (Mt. Butler, Nevada), it was fund that the average amplificatin rati f grund mtin at the crest relative t the base was abut 2.5. nt yet been analysed but it is anticipated that this amplificatin is again due t the cmbinatin f the weathered sedimentary pile and the tpgraphy at the Ynki site. 7. CONCLUSIONS 1. An earthquake f magnitude ML 5.0 triggered the tw accelergraphs at the Musa River dam site n 16 September, The maximum acceleratin recrded by the Musa A accelergraph at the crest f the dam was 1.85 m/s 2 at a perid f 0.23 s. An acceleratin in excess f 0.3 m/s 2 was sustained at the site fr abut 11 s. The maximum acceleratin recrded by the Musa B accelergraph at the base f the dam site was 0.39 m/s 2 at a perid f 0.04 s. An acceleratin in excess f 0.3 m/s 2 was sustained fr abut 2 secnds. 2. The 2.5 s S-P time interval n the accelergrams indicates that the separatin between the earthquake hypcentre and the dam site was abut 19 km. 3. It is suggested that the 4.5:1 rati f amplitude f grund acceleratin which ccurred at the Musa A site relative t that f the Musa B site can be explained by the cmbined effect f the lithlgy and tpgraphy. 8. REFERENCES Bishp, I. D., Pllck, E. J. and Pettifer, G. R. (in prep.), "Musa River hydrelectric-scheme seismic survey, P.N.G., 1970", Bur. Miner. Resur. Aust. Rec. (unpubl.). Davis, L. L., and West, L. R. (1973), "Observed effects f tpgraphy n grund mtin", Bull. seism. Sc. Amer. 63, Macias, L. F. (1971), "Gelgy f the Musa Grge dam site area. Eastern Papua", Gelgical Survey f Papua New Guinea Nte n Investigatin, Madera, G. A. (1970), "Fundamental perid and amplificatin f peak acceleratin in layered systems", Dept. Civ. Eng., Massachusetts Inst, f Tech. Rpt. N. R69-15, Sils Publ. N Hence the ttal amplificatin rati f the grund mtin at Musa A relative t Musa B when the cmbined effect f lithlgical and tpgraphical factrs are taken int accunt has been theretically estimated at abut 5, which is in reasnable agreement with the measured rati f abut YONKI DAMSITE ACCELEROGRAMS On 20 September, 1974 in the eastern highlands f Papua New Guinea, an amplificatin factr f maximum grund acceleratin amplitude f abut 8 was registered between a weathered sedimentary accelergraph site (Ynki) and a hard rck site (Intake) abut 1 km apart. Preliminary maximum recrded acceleratin and perid at the Ynki site were 2.3m sec 2 and 0.17 sees respectively, and at the Intake site were 0.28m sec" 2 and 0.09 sees respectively. Recrds have
3 117 TAELE 1. SUMMARY OF GROUND MOTION AT MUSA GORGE 16 SEPTEMBER/ 1972 Cmpnent Max. accel. Max. velcity Perid (s) m/s 2 mm/s P wave S wave MUSA A Z NS EW Vectr Resultant Mean 0.23 MUSA B Z NS EW Vectr Resultant Mean 0.04
4 FIGURE 1: LOCALITY OF MUSA RIVER 00
5 t Secnds L 0 cm VERTICAL SCALE (apprx) HORIZONTAL COMPONENTS: 1cm = 1.7ms -2 VERTICAL COMPONENTS: lcm* 1.1ms -a. FIGURE 2 : COPIES OF MUSA RIVER ACCELEROGRAMS
6 ACCELERATION cm/s 2 VELOCITY cm/s ACCELERATION VELOCITY ACCELERATION cm/s 2 VELOCITY cm/s GV C DO c z Q H O z cn DO m«>h *T O m s C m > > m 3D O > x
7 121 FIGURE 4: THE MUSA PROFILES Depth MUSA A MUSA B (m) ~ ~ Cs = 171 m/s Y = 2.2 x 10 3 kg/m 3 Cs = 285 m/s y = 2.5 x 10 3 kg/m 3 in 6 CD lh " ' <D ^ Cs = 456 m/s t * Y = 2.25 x 10 kg/iri 24 Cs = 1311 m/s 61 Y = 2.35 x 10 3 kg/m 3 Cs = 2565 m/s u Cs = 2280 m/s H Y = 2.8 x 10 3 kg/m 3 y = 2.8 x 10 3 kg/m 3 n 4J Ntatin Cs = seismic shear v/ave velcity Y = density Nte (1) Density values are estimates supplied by Macias (pers. cmm.) wh examined the drill cres. (2) The Musa A accelergraph site is 300 m abve the Musa B site.
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 informationPhys101 First Major-131 Zero Version Coordinator: Dr. A. A. Naqvi Wednesday, September 25, 2013 Page: 1
Phys11 First Majr-11 Zer Versin Crdinatr: Dr. A. A. Naqvi Wednesday, September 5, 1 Page: 1 Q1. Cnsider tw unifrm slid spheres A and B made f the same material and having radii r A and r B, respectively.
More informationSPH3U1 Lesson 06 Kinematics
PROJECTILE MOTION LEARNING GOALS Students will: Describe the mtin f an bject thrwn at arbitrary angles thrugh the air. Describe the hrizntal and vertical mtins f a prjectile. Slve prjectile mtin prblems.
More informationPhysics 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 informationPhys101 Final Code: 1 Term: 132 Wednesday, May 21, 2014 Page: 1
Phys101 Final Cde: 1 Term: 1 Wednesday, May 1, 014 Page: 1 Q1. A car accelerates at.0 m/s alng a straight rad. It passes tw marks that are 0 m apart at times t = 4.0 s and t = 5.0 s. Find the car s velcity
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 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 informationControl of Strong Motion by the Upper 30 Meters
Bulletin f the Seismlgical Sciety f America, Vl. 86, N. 6, pp. 1749-1759, December 1996 Cntrl f Strng Mtin by the Upper 3 Meters by Jhn G. Andersn, Yajie Lee, Yuehua Zeng, and Steven Day Abstract Lcal
More information1.2.1 Vectors. 1 P age. Examples What is the reference vector angle for a vector that points 50 degrees east of south?
1.2.1 Vectrs Definitins Vectrs are represented n paper by arrws directin = magnitude = Examples f vectrs: Examples What is the reference vectr angle fr a vectr that pints 50 degrees east f suth? What is
More informationFlipping Physics Lecture Notes: Simple Harmonic Motion Introduction via a Horizontal Mass-Spring System
Flipping Physics Lecture Ntes: Simple Harmnic Mtin Intrductin via a Hrizntal Mass-Spring System A Hrizntal Mass-Spring System is where a mass is attached t a spring, riented hrizntally, and then placed
More informationAircraft 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 informationSections 15.1 to 15.12, 16.1 and 16.2 of the textbook (Robbins-Miller) cover the materials required for this topic.
Tpic : AC Fundamentals, Sinusidal Wavefrm, and Phasrs Sectins 5. t 5., 6. and 6. f the textbk (Rbbins-Miller) cver the materials required fr this tpic.. Wavefrms in electrical systems are current r vltage
More information1. Introduction. Lab 4 - Geophysics 424, October 29, One-dimensional Interpretation of Magnetotelluric Data
Lab 4 - Gephysics 424, Octber 29, 2018 One-dimensinal Interpretatin f Magnettelluric Data Lab reprt is due by 5 p.m. Nvember 5, 2018 All late reprts require a valid reasn t be accepted. Include answers
More informationFlipping Physics Lecture Notes: Simple Harmonic Motion Introduction via a Horizontal Mass-Spring System
Flipping Physics Lecture Ntes: Simple Harmnic Mtin Intrductin via a Hrizntal Mass-Spring System A Hrizntal Mass-Spring System is where a mass is attached t a spring, riented hrizntally, and then placed
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 informationChapter 2. Kinematics in One Dimension. Kinematics deals with the concepts that are needed to describe motion.
Chapter Kinematics in One Dimensin Kinematics deals with the cncepts that are needed t describe mtin. Dynamics deals with the effect that frces have n mtin. Tgether, kinematics and dynamics frm the branch
More informationATTENUATION OF STRONG GROUND MOTION IN SHALLOW EARTHQUAKES
3 th Wrld Cnference n Earthquake Engineering Vancuver, B.C., Canada August -6, 4 Paper N. 66 ATTENUATION OF STRONG GROUND MOTION IN SHALLOW EARTHQUAKES Símn ÓLAFSSON, Ragnar SIGBJÖRNSSON SUMMARY In this
More informationmaking triangle (ie same reference angle) ). This is a standard form that will allow us all to have the X= y=
Intrductin t Vectrs I 21 Intrductin t Vectrs I 22 I. Determine the hrizntal and vertical cmpnents f the resultant vectr by cunting n the grid. X= y= J. Draw a mangle with hrizntal and vertical cmpnents
More informationQ x = cos 1 30 = 53.1 South
Crdinatr: Dr. G. Khattak Thursday, August 0, 01 Page 1 Q1. A particle mves in ne dimensin such that its psitin x(t) as a functin f time t is given by x(t) =.0 + 7 t t, where t is in secnds and x(t) is
More informationInterference 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 informationAnalysis of Curved Bridges Crossing Fault Rupture Zones
Analysis f Curved Bridges Crssing Fault Rupture Znes R.K.Gel, B.Qu & O.Rdriguez Dept. f Civil and Envirnmental Engineering, Califrnia Plytechnic State University, San Luis Obisp, CA 93407, USA SUMMARY:
More informationThree charges, all with a charge of 10 C are situated as shown (each grid line is separated by 1 meter).
Three charges, all with a charge f 0 are situated as shwn (each grid line is separated by meter). ) What is the net wrk needed t assemble this charge distributin? a) +0.5 J b) +0.8 J c) 0 J d) -0.8 J e)
More informationBulletin of the Seismological Society of America
Bulletin f the Seismlgical Sciety f America Vl. 81 December 1991 N. 6 ESTIMATION OF GROUND MOTION AT DEEP-SOIL SITES IN EASTERN NORTH AMERICA BY DAVID M. BOORE AND WILLIAM B. JOYNER ABSTRACT The stchastic
More informationBeneficial effect of soil-structure interaction to structural response derived from two building arrays in New Zealand
Zha, J. (008) Beneficial effect f il-tructure interactin t tructural repne derived frm tw building array in New Zealand Prc. 18 th NZGS Getechnical Sympium n Sil-Structure Interactin. Ed. CY Chin, Auckland
More information1 Course Notes in Introductory Physics Jeffrey Seguritan
Intrductin & Kinematics I Intrductin Quickie Cncepts Units SI is standard system f units used t measure physical quantities. Base units that we use: meter (m) is standard unit f length kilgram (kg) is
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 informationCLASS XI SET A PHYSICS
PHYSIS. If the acceleratin f wedge in the shwn arrangement is a twards left then at this instant acceleratin f the blck wuld be, (assume all surfaces t be frictinless) a () ( cs )a () a () cs a If the
More information13. PO TREATMENT OF DEPT (DISTORTIONLESS ENHANCEMENT POLARIZATION TRANSFER)
94 Prduct Operatr Treatment 3. PO TREATMENT OF DEPT (DISTORTIONLESS ENHANCEMENT POLARIZATION TRANSFER) DEPT is a ne-dimensinal sequence used as a tl fr unambiguus identificatin f the CH, CH, and CH 3 peaks
More informationSodium D-line doublet. Lectures 5-6: Magnetic dipole moments. Orbital magnetic dipole moments. Orbital magnetic dipole moments
Lectures 5-6: Magnetic diple mments Sdium D-line dublet Orbital diple mments. Orbital precessin. Grtrian diagram fr dublet states f neutral sdium shwing permitted transitins, including Na D-line transitin
More information2. Precipitation Chemistry Data
STIMATING TH ATMSPHRIC INT A WATRSH INPUT F PLLUTANTS PRRY J. SAMSN epartment f Atmspheric and ceanic Science, University f Michigan, Ann Arbr, All 4819-2143, U.S.A. (Received June 2, 1986; revised March
More informationBulletin of the Seismological Society of America, Vol. 72, No. 6, pp , December 1982
Bulletin f the Seismlgical Sciety f America, Vl. 72, N. 6, pp. 1843-1865, December 1982 ANALYSIS OF THE GROUND ACCELERATIONS RADIATED BY THE 1980 LIVERMORE VALLEY EARTHQUAKES FOR DIRECTIVITY AND DYNAMIC
More informationFigure 1a. A planar mechanism.
ME 5 - Machine Design I Fall Semester 0 Name f Student Lab Sectin Number EXAM. OPEN BOOK AND CLOSED NOTES. Mnday, September rd, 0 Write n ne side nly f the paper prvided fr yur slutins. Where necessary,
More informationStudy 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 informationThermodynamics 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 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 informationCHAPTER 6 WORK AND ENERGY
CHAPTER 6 WORK AND ENERGY CONCEPTUAL QUESTIONS 16. REASONING AND SOLUTION A trapeze artist, starting rm rest, swings dwnward n the bar, lets g at the bttm the swing, and alls reely t the net. An assistant,
More informationRay tracing equations in transversely isotropic media Cosmin Macesanu and Faruq Akbar, Seimax Technologies, Inc.
Ray tracing equatins in transversely istrpic media Csmin Macesanu and Faruq Akbar, Seimax Technlgies, Inc. SUMMARY We discuss a simple, cmpact apprach t deriving ray tracing equatins in transversely istrpic
More informationDetermining the Accuracy of Modal Parameter Estimation Methods
Determining the Accuracy f Mdal Parameter Estimatin Methds by Michael Lee Ph.D., P.E. & Mar Richardsn Ph.D. Structural Measurement Systems Milpitas, CA Abstract The mst cmmn type f mdal testing system
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 information~'- ~I I \~ APPlIED TECHNOlOGY COUNCll
! ATe a Prceedings f SEMNAR N SESMC SLATN, PASSVE ENERGY DSSPATN, AND ACTVE CNTRL VlUME :, l {-. "f.f;m,- ~'- ~ \~ APPlED TECHNlGY CUNCll Funded by Natinal Center lr Earthquake Engineering Research Natinal
More informationBuilding to Transformations on Coordinate Axis Grade 5: Geometry Graph points on the coordinate plane to solve real-world and mathematical problems.
Building t Transfrmatins n Crdinate Axis Grade 5: Gemetry Graph pints n the crdinate plane t slve real-wrld and mathematical prblems. 5.G.1. Use a pair f perpendicular number lines, called axes, t define
More informationDrought 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 informationExaminer: 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 information5 th grade Common Core Standards
5 th grade Cmmn Cre Standards In Grade 5, instructinal time shuld fcus n three critical areas: (1) develping fluency with additin and subtractin f fractins, and develping understanding f the multiplicatin
More informationChapter 23 Electromagnetic Waves Lecture 14
Chapter 23 Electrmagnetic Waves Lecture 14 23.1 The Discvery f Electrmagnetic Waves 23.2 Prperties f Electrmagnetic Waves 23.3 Electrmagnetic Waves Carry Energy and Mmentum 23.4 Types f Electrmagnetic
More informationEarthquake locations using single-station deep borehole recordings: Implications for microseismicity on the San Andreas fault in southern California
JOURNAL OF GEOPHYSCAL RESEARCH, VOL. 100, NO. B12, PAGES 24,003-24,014, DECEMBER 10, 1995 Earthquake lcatins using single-statin deep brehle recrdings: mplicatins fr micrseismicity n the San Andreas fault
More informationPOLARISATION VISUAL PHYSICS ONLINE. View video on polarisation of light
VISUAL PHYSICS ONLINE MODULE 7 NATURE OF LIGHT POLARISATION View vide n plarisatin f light While all the experimental evidence s far that supprts the wave nature f light, nne f it tells us whether light
More informationo Land and water both are heated by solar radiation, but land
Benchmark: SC.D.l.4.1 The student knws hw climatic patterns n Earth result frm an interplay f many factrs (Earth's tpgraphy, its rtatin'tn its axis, slar radiatin, the transfer f heat energy where the
More informationEvaluation of the outdoor thermal environment in redevelopment buildings in front of Osaka Station based on observations
Academic Article Jurnal f Heat Island Institute Internatinal Vl. 9-2 (2014) Evaluatin f the utdr thermal envirnment in redevelpment buildings in frnt f Osaka Statin based n bservatins Kentar Ayama *1 Sae
More informationWeathering. Title: Chemical and Mechanical Weathering. Grade Level: Subject/Content: Earth and Space Science
Weathering Title: Chemical and Mechanical Weathering Grade Level: 9-12 Subject/Cntent: Earth and Space Science Summary f Lessn: Students will test hw chemical and mechanical weathering can affect a rck
More informationYeu-Sheng Paul Shiue, Ph.D 薛宇盛 Professor and Chair Mechanical Engineering Department Christian Brothers University 650 East Parkway South Memphis, TN
Yeu-Sheng Paul Shiue, Ph.D 薛宇盛 Prfessr and Chair Mechanical Engineering Department Christian Brthers University 650 East Parkway Suth Memphis, TN 38104 Office: (901) 321-3424 Rm: N-110 Fax : (901) 321-3402
More informationPHYSICS Unit 3 Trial Examination
STAV Publishing Pty Ltd 005 PHYSICS Unit 3 Trial Examinatin SOLUTIONS BOOK Published by STAV Publishing Pty Ltd. STAV Huse, 5 Munr Street, Cburg VIC 3058 Australia. Phne: 6 + 3 9385 3999 Fax: 6 + 3 9386
More information39th International Physics Olympiad - Hanoi - Vietnam Theoretical Problem No. 1 /Solution. Solution
39th Internatinal Physics Olympiad - Hani - Vietnam - 8 Theretical Prblem N. /Slutin Slutin. The structure f the mrtar.. Calculating the distance TG The vlume f water in the bucket is V = = 3 3 3 cm m.
More informationAssume 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 informationMethods for Determination of Mean Speckle Size in Simulated Speckle Pattern
0.478/msr-04-004 MEASUREMENT SCENCE REVEW, Vlume 4, N. 3, 04 Methds fr Determinatin f Mean Speckle Size in Simulated Speckle Pattern. Hamarvá, P. Šmíd, P. Hrváth, M. Hrabvský nstitute f Physics f the Academy
More information14. Which shows the direction of the centripetal force acting on a mass spun in a vertical circle?
Physics 0 Public Exam Questins Unit 1: Circular Mtin NAME: August 009---------------------------------------------------------------------------------------------------------------------- 1. Which describes
More informationAuthor(s) OKANO, Kennosuke; HIRANO, Isamu.
Title Seismic Attenuatin in Relatin t Vicinity f Kyt Authr(s) OKANO, Kennsuke; HIRANO, Isamu Citatin Bulletin f the Disaster Preventin 22(2): 97-11 Issue Date 1973-2 URL http://hdl.handle.net/2433/124823
More information14. Which shows the direction of the centripetal force acting on a mass spun in a vertical circle?
Physics 3204 Public Exam Questins Unit 1: Circular Mtin NAME: August 2009---------------------------------------------------------------------------------------------------------------------- 12. Which
More informationLHS 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 informationDavid HORN and Irit OPHER. School of Physics and Astronomy. Raymond and Beverly Sackler Faculty of Exact Sciences
Cmplex Dynamics f Neurnal Threshlds David HORN and Irit OPHER Schl f Physics and Astrnmy Raymnd and Beverly Sackler Faculty f Exact Sciences Tel Aviv University, Tel Aviv 69978, Israel hrn@neurn.tau.ac.il
More informationA Simple Set of Test Matrices for Eigenvalue Programs*
Simple Set f Test Matrices fr Eigenvalue Prgrams* By C. W. Gear** bstract. Sets f simple matrices f rder N are given, tgether with all f their eigenvalues and right eigenvectrs, and simple rules fr generating
More informationROUNDING ERRORS IN BEAM-TRACKING CALCULATIONS
Particle Acceleratrs, 1986, Vl. 19, pp. 99-105 0031-2460/86/1904-0099/$15.00/0 1986 Grdn and Breach, Science Publishers, S.A. Printed in the United States f America ROUNDING ERRORS IN BEAM-TRACKING CALCULATIONS
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 informationSNOW AND AVALANCHES FORECASTING OVER THE ANDES MOUNTAlNS. Jose A. Vergara* Departamento de Geoflsica, Universidad de Chile
SNOW AND AVALANCHES FORECASTNG OVER THE ANDES MOUNTAlNS Jse A. Vergara* Departament de Geflsica, Universidad de Chile Rene len, Camins y Nieve, ANDNA-CODElCO, CHLE ABSTRACT: During the last three years
More informationPhysics 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 informationSUPPLEMENTARY MATERIAL GaGa: a simple and flexible hierarchical model for microarray data analysis
SUPPLEMENTARY MATERIAL GaGa: a simple and flexible hierarchical mdel fr micrarray data analysis David Rssell Department f Bistatistics M.D. Andersn Cancer Center, Hustn, TX 77030, USA rsselldavid@gmail.cm
More informationComputational 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 informationIntroduction: A Generalized approach for computing the trajectories associated with the Newtonian N Body Problem
A Generalized apprach fr cmputing the trajectries assciated with the Newtnian N Bdy Prblem AbuBar Mehmd, Syed Umer Abbas Shah and Ghulam Shabbir Faculty f Engineering Sciences, GIK Institute f Engineering
More informationNonlinear Soil Response in the Vicinity of the Van Norman Complex Following the 1994 Northridge, California, Earthquake
Bulletin f the Seismlgical Sciety f America, 89, 5, pp. 1214-1231, ctber 1999 Nnlinear Sil Respnse in the Vicinity f the Van Nrman Cmplex Fllwing the 1994 Nrthridge, Califrnia, Earthquake by Givanna Cultrera,
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 informationMAJOR 40,000m GOLD EXPLORATION DRILLING PROGRAM COMMENCES
2 Nvember 2016 MAJOR 40,000m GOLD EXPLORATION DRILLING PROGRAM COMMENCES Highlights A majr explratin drilling prgram has cmmenced n the Tampia Gld Prject t scpe the extent f the knwn gld resurce thrugh
More informationLCAO APPROXIMATIONS OF ORGANIC Pi MO SYSTEMS The allyl system (cation, anion or radical).
Principles f Organic Chemistry lecture 5, page LCAO APPROIMATIONS OF ORGANIC Pi MO SYSTEMS The allyl system (catin, anin r radical).. Draw mlecule and set up determinant. 2 3 0 3 C C 2 = 0 C 2 3 0 = -
More informationChapter 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 informationSTUDIECENTRUM T.N.O. VOOR SCHEEPSBOUW EN NAVIGATIE AFDELING MACHINEBOUW - DROOGBAK la - AMSTERDAM
REPORT N. 31 M APRIL 1960 STUDIECENTRUM T.N.O. VOOR SCHEEPSBOUW EN NAVIGATIE AFDELING MACHINEBOUW - DROOGBAK la - AMSTERDAM NETHERLANDS RESEARCH CENTRE T.N.O. FOR SHIPBUILDING AND NAVIGATION ENGINEERING
More information( ) + θ θ. ω rotation rate. θ g geographic latitude - - θ geocentric latitude - - Reference Earth Model - WGS84 (Copyright 2002, David T.
1 Reference Earth Mdel - WGS84 (Cpyright, David T. Sandwell) ω spherid c θ θ g a parameter descriptin frmula value/unit GM e (WGS84) 3.9864418 x 1 14 m 3 s M e mass f earth - 5.98 x 1 4 kg G gravitatinal
More informationES201 - 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 informationANALYSIS OF THE PACOIMA DAM ACCELEROGRAM--SAN FERNANDO, CALIFORNIA, EARTHQUAKE OF 1971 B~ 5/I. D. TRIFUNAC AND D. E. HUDSON
Bulletin f the Seismlgical Sciety f America. Vl. 61, N. 5, pp. 1393-1141. Octber, 1971 ANALYSIS OF THE PACOIMA DAM ACCELEROGRAM--SAN FERNANDO, CALIFORNIA, EARTHQUAKE OF 1971 B~ 5/I. D. TRIFUNAC AND D.
More informationWork, Energy, and Power
rk, Energy, and Pwer Physics 1 There are many different TYPES f Energy. Energy is expressed in JOULES (J 419J 4.19 1 calrie Energy can be expressed mre specifically by using the term ORK( rk The Scalar
More informationEXAM #1 PHYSICAL SCIENCE 103 Spring, 2016
OBJECTIVES 1. Ft Pressure EXAM #1 PHYSICAL SCIENCE 103 Spring, 2016 Determine the surface area f an bject. Given the weight and surface area, calculate the pressure. 2. Measuring Vlume & Mass Prvided a
More informationLab 11 LRC Circuits, Damped Forced Harmonic Motion
Physics 6 ab ab 11 ircuits, Damped Frced Harmnic Mtin What Yu Need T Knw: The Physics OK this is basically a recap f what yu ve dne s far with circuits and circuits. Nw we get t put everything tgether
More informationGeneral Chemistry II, Unit I: Study Guide (part I)
1 General Chemistry II, Unit I: Study Guide (part I) CDS Chapter 14: Physical Prperties f Gases Observatin 1: Pressure- Vlume Measurements n Gases The spring f air is measured as pressure, defined as the
More information( ) 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 informationLecture 13: Electrochemical Equilibria
3.012 Fundamentals f Materials Science Fall 2005 Lecture 13: 10.21.05 Electrchemical Equilibria Tday: LAST TIME...2 An example calculatin...3 THE ELECTROCHEMICAL POTENTIAL...4 Electrstatic energy cntributins
More information^YawataR&D Laboratory, Nippon Steel Corporation, Tobata, Kitakyushu, Japan
Detectin f fatigue crack initiatin frm a ntch under a randm lad C. Makabe," S. Nishida^C. Urashima,' H. Kaneshir* "Department f Mechanical Systems Engineering, University f the Ryukyus, Nishihara, kinawa,
More informationBootstrap Method > # Purpose: understand how bootstrap method works > obs=c(11.96, 5.03, 67.40, 16.07, 31.50, 7.73, 11.10, 22.38) > n=length(obs) >
Btstrap Methd > # Purpse: understand hw btstrap methd wrks > bs=c(11.96, 5.03, 67.40, 16.07, 31.50, 7.73, 11.10, 22.38) > n=length(bs) > mean(bs) [1] 21.64625 > # estimate f lambda > lambda = 1/mean(bs);
More information5.4 Measurement Sampling Rates for Daily Maximum and Minimum Temperatures
5.4 Measurement Sampling Rates fr Daily Maximum and Minimum Temperatures 1 1 2 X. Lin, K. G. Hubbard, and C. B. Baker University f Nebraska, Lincln, Nebraska 2 Natinal Climatic Data Center 1 1. INTRODUCTION
More information(s6 ~lj t') >~.'c;. .. ' ' 9adanki ( N, E)',- !2!!!m'!!.y~ation-6fhorizont~~cb' in the ~()wert.~2qq~~hereover --:!"
t (s6 ~lj t') \ >""\., ~hysia Indian Jurnal f 11adi&Sp8Ce V~3.February 1994,pp. ~::4().,I\' :!",,,. 'I\.J \ '0f"'~ r't t ~.'c;. ~~ \,!2!!!m'!!.y~atin6fhriznt~~cb' in the ~()wert.~2qq~~herever.. '
More informationTHE SEPARATION OF ALUNITE IN ALUNITIC KAOLIN BY SELECTIVE FLOCCULATION
Clays and Clay Minerals, Vl. 23, pp. 468 472. Pergamn Press 1975. Printed in Great Britain THE SEPARATON OF ALUNTE N ALUNTC KAOLN BY SELECTVE FLOCCULATON C. USTAER and. Gi)RGEY Metallurgical Department,
More informationSubject description processes
Subject representatin 6.1.2. Subject descriptin prcesses Overview Fur majr prcesses r areas f practice fr representing subjects are classificatin, subject catalging, indexing, and abstracting. The prcesses
More informationEEO 401 Digital Signal Processing Prof. Mark Fowler
EEO 401 Digital Signal Prcessing Prf. Mark Fwler Intrductin Nte Set #1 ading Assignment: Ch. 1 f Prakis & Manlakis 1/13 Mdern systems generally DSP Scenari get a cntinuus-time signal frm a sensr a cnt.-time
More informationVortex Dynamics at the Transition to the Normal State in YBa 2 Cu 3 O 7-δ Films
Vrtex Dynamics at the Transitin t the Nrmal State in YBa 2 Cu 3 O 7- Films P.Bernstein a), J.F.Hamet a), M.T.Gnzález b,*) and M.Ruibal Acuña b) a) CRISMAT-ENSICAEN (UMR-CNRS 6508) F14050 Caen cedex 4,
More informationPower Flow in Electromagnetic Waves. The time-dependent power flow density of an electromagnetic wave is given by the instantaneous Poynting vector
Pwer Flw in Electrmagnetic Waves Electrmagnetic Fields The time-dependent pwer flw density f an electrmagnetic wave is given by the instantaneus Pynting vectr P t E t H t ( ) = ( ) ( ) Fr time-varying
More informationEarthquake accelerograms and attenuation of seismic waves at Oolong, New South Wales
3 BMR Jurnal f Australian Gelgy &: Gephysics 5 198 3-7 arthquake accelergrams and attenuatin f seismic waves at Olng New Suth Wales Rn S Smith & A J Mcwin The first Australian earthquake accelergrams were
More informationPreparation 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 informationarxiv:hep-ph/ v1 2 Jun 1995
WIS-95//May-PH The rati F n /F p frm the analysis f data using a new scaling variable S. A. Gurvitz arxiv:hep-ph/95063v1 Jun 1995 Department f Particle Physics, Weizmann Institute f Science, Rehvt 76100,
More informationRevision: August 19, E Main Suite D Pullman, WA (509) Voice and Fax
.7.4: Direct frequency dmain circuit analysis Revisin: August 9, 00 5 E Main Suite D Pullman, WA 9963 (509) 334 6306 ice and Fax Overview n chapter.7., we determined the steadystate respnse f electrical
More informationEmpirical Analysis of Strong Ground Motion from the 1992 Landers, California, Earthquake
Bulletin f the Seismlgical Sciety f America, Vl. 84, N. 3, pp. 573-588, June 1994 Empirical Analysis f Strng Grund Mtin frm the 1992 Landers, Califrnia, Earthquake by K. W. Campbell and Y. Bzrgnia Abstract
More informationSeries and Parallel Resonances
Series and Parallel esnances Series esnance Cnsider the series circuit shwn in the frequency dmain. The input impedance is Z Vs jl jl I jc C H s esnance ccurs when the imaginary part f the transfer functin
More information