Technical Note

Size: px
Start display at page:

Download "Technical Note"

Transcription

1 ES7I Call N. CcpK H. 7 / Technical Nte Cntinuus Cverage f the Nrth Plar Regin with Only Tw Cmmunicatins Satellites J. U. Beusch 4 September 1969 Lincln Labratry MASSACHUSETTS INSTITUTE OF TECHNOLOGY Lexingtn, Massachusetts 0km

2 This dcument has been apprved fr public release its distributin is unlimited.

3 MASSACHUSETTS INSTITUTE OF TECHNOLOGY LINCOLN LABORATORY CONTINUOUS COVERAGE OF THE NORTH POLAR REGION WITH ONLY TWO COMMUNICATIONS SATELLITES /. U. BEUSCH Grup 67 TECHNICAL NOTE SEPTEMBER 1969 This dcument has been apprved fr public release and sale; its distributin is unlimited. LEXINGTON MASSACHUSETTS

4 The wrk reprted in this dcument was perfrmed at Lincln Labratry, a center fr research perated by Massachusetts Institute f Technlgy. The wrk was spnsred by the Department f the Navy under Air Frce Cntract AF 19(628)-S167. This reprt may be reprduced t satisfy needs f U.S. Gvernment agencies. n

5 ABSTRACT The prblem f prviding cntinuus cverage f the nrth plar regin with a small number f cmmunicatins satellites is cnsidered. The system described requires nly tw satellites t prvide bth this cverage and cverage f a cnsiderable fractin f the nrthern hemisphere. Tw rbit planes with 6. 4 inclinatin, high eccentricity and ~24 hur perids are emplyed. The regins f the earth frm which a satellite is cntinuusly visible frm terminals with varius minimum elevatin angles are shwn. The regins in which mutual visibility f a satellite by tw terminals is guaranteed are shwn. A few cmments cncerning satellite design fr this rbit are included. Accepted fr the Air Frce Franklin C. Hudsn Chief, Lincln Labratry Office in

6 Cntinuus Cverage f the Nrth Plar Regin with Only Tw Cmmunicatins Satellites I. Intrductin Cntinuus cverage f the nrth plar regin is desirable, and in sme cases mandatry, fr many satellite cmmunicatins systems. Synchrnus, equatrial satellites prvide cverage t nly lw and mderate latitudes. Satellites in inclined circular rbits can prvide plar cverage but cnsiderably mre than tw satellites are required.* Cnsider the prblem f prviding cntinuus nrth plar cverage using a small number f satellites. It is clear that a single satellite in earth rbit cannt prvide this cverage. T prvide this cverage by keeping a single satellite hvering cnstantly ver the nrthern hemisphere by firing jets n the satellite wuld be prhibitively expensive. In the next sectin we describe a system f nly tw satellites which prvides this cverage and als prvides cntinuus cverage dwn t mderate latitudes f a wide strip f the earth near an arbitrarily selected lngitude. These tw satellites can augment the cverage f synchrnus equatrial satellites r can be used by terminals which perate in an area which includes bth the nrth plar regin and a strip f the earth near a particular lngitude. An example f the latter case is military frces which are deplyed in the plar regin and must cmmunicate with a base lcated in the cntinental United States (CONUS). The system described has the further advantage that, whenever the earth casts its shadw n the slar array f a satellite, the terminals are using the ther satellite. Thus the cmmunicatins transmitter need nt be used during slar eclipse s nly a small strage battery need be included in each satellite. II. Selectin f the Satellite Orbits In synthesizing a system t prvide cntinuus nrth plar cverage with nly tw satellites, ne must cnsider elliptical rbits since circular rbits cannt achieve this bjective. A highly elliptical rbit with its apgee in the nrthern hemisphere is attractive since a satellite spends cnsiderably mre time near its apgee than its perigee. * The advantage f these rbits wuld be that cverage f the suth plar regin wuld als be prvided in thse cases in which it is desired.

7 In general, such an rbit is unstable in the sense that the apgee will nt remain ver the nrthern hemisphere due t perturbatins caused by the nn-sphericity f the earth. The angular velcity with which the apgee rtates in the rbit plane is prprtinal t 2 5 cs i - 1 where i is the rbit inclinatin, i.e., the angle between the equatrial and rbital planes (Ref. 1). When i = 6.4, apgee rtatin is zer s this inclinatin has been chsen. If tw satellites are placed in the same rbit plane phased such that when ne is at apgee the ther is at perigee, cntinuus nrth plar cverage can be prvided if the apgee height is sufficiently large. When cntinuus cverage f a wide strip f the earth dwn t mderate latitudes near an arbitrarily selected lngitude is als required, tw satellites in the same rbit plane n lnger suffice. This cverage can be prvided if each satellite reaches apgee nly when it is ver the selected lngitude. Figure 1 shws the simplest way f achieving this. Bth rbit planes intersect the equatrial plane in the same line, the line f ndes. Relative t the line f ndes the earth rtates with a perid T «24 hr. The rbital perid f the satellites is als T and they are phased s that ne reaches apgee every T/2 hr. The directin f rtatin f the satellites are chsen s that they fllw the rtatin f the selected lngitude when they are near apgee. If a particular set f terminals can pint antennas tward ne satellite in a particular directin at time t, they can pint tward the ther satellite in the same directin at time t + T/2. This symmetry is use- ful in the cverage analysis f the next sectin. It shuld be nted that T is slightly less than 24 hurs s the satellites reach a particular pint in rbit at slightly different times each day. T insure negligible atmspheric drag the perigee altitude is apprximately 700 km. The effects f drift f perigee altitude is discussed in Sectin VII. A semi-majr axis f earth radii and an eccentricity f prvide an rbital perid f hurs. This is the perid f rtatin f the earth relative t the line f ndes.* As shwn in Fig. 1, the inclinatin f bth rbital planes is 6.4, the ascending ndes are separated by 180 and the argument f perigee is 270. tthe Mlniya satellites use this inclinatin fr high latitude cverage. * Relative t the vernal equinx the earth rtates at a rate f per day. The line f ndes rtates at a rate f per day because f perturbatins f the rbit due t the earth's equatrial bulge. Thus, the earth rtates at per day relative t the line f ndes, i.e., requires 2. 9 hurs t rtate 60.

8 III. Regin f Cntinuus Visibility The earth's equatrial plane and the line f ndes determine an rthgnal crdinate system; the crdinates are the line f ndes, a line perpendicular t the equatrial plane and a line in the equatrial plane perpendicular t the ther lines. Cnsidering the effects f the secnd harmnic f the earth's gravitatinal field, bth rbit planes are statinary in this crdinate system. Sme higher rder effects including perturbatins due t the sun and mn must be canceled by adjusting the rbit with thrusters in the satellite. Fuel requirements fr these adjustments are fairly small. We assume these adjustments are made. Since the rbital perids and the perids f rtatin f the earth in this crdinate system are equal, the cverage f the satellites during a single perid is repeated exactly in all subsequent perids. Because f the symmetry described in the previus sectin, cverage prvided by ne satellite during ne half-rbit is repeated exactly by the ther satellite in the next half-rbit. Therefre, if a terminal with a particular lcatin and minimum elevatin angle can pint its antenna tward ne satellite fr a half-rbit (~12 hurs) it can always pint tward ne f the satellites, i.e., has cntinuus satellite visibility. Furthermre, if ne satellite is simultaneusly visible frm tw terminals fr a half-rbit, ne f the satellites is always visible frm bth terminals. In Fig. 2, cntinuus visibility cnturs fr terminals with minimum elevatin angles f 0, 5,10, 20 and 0 degrees are shwn. A terminal with a particular minimum elevatin angle lcated n the crrespnding cntur can pint tward ne satellite fr ~12 hurs and thus has cntinuus satellite visibility. A terminal lcated nrth f this cntur als has cntinuus satellite visibility. The cnturs can be mved east r west n the map by changing the lngitude f the ascending ndes f the rbits. IV. Regins f Cntinuus Mutual Visibility A terminal lcated n the cnturs f Figs., 4, and 5 crrespnding t its minimum elevatin angle can pint tward each satellite fr 14, and 21 hurs per rbital perid, respectively. These cnturs prvide mutual visibility infrmatin in the fllwing way. Cnsider the rbit plane f Fig. 6. The satellite is visible frm terminals A and B fr time intervals f length T. and r R. The satellite is visible frm bth terminals fr time T. R and visible frm neither fr time r. R. Frm Fig. 6,

9 r A + T B- T AB +1 Ai = T ~ 24hr - where T is the rbital perid. Fr cntinuus mutual visibility we require T. R 5 12 hr. s we require r T +T T + T 12 hr A B * T AB nr - ^ + ^.7+12-^. It can be shwn fr the nrthern hemisphere lcatins f interest, TTT > 1 hr. s if T. + r R 5 5 hr., T. R 12 hr. and cntinuus mutual visibility is prvided. Cnsider tw terminals with'particular minimum elevatin angles. If each is lcated n r nrth f the crrespnding hr. cntur f Fig. 4, cntinuus mutual visibility is prvided. If ne is lcated nrth f the crrespnding cntur f Fig. and the ther nrth f the crrespnding cntur f Fig. 5, cntinuus mutual visibility is prvided. As with Fig. 2, the cnturs f Figs., 4, and 5 can be mved east r west n the map. An existing cmputer prgram was emplyed t btain the cnturs. Because f the frm f the prgram, results were cmputed fr particular terminal lcatins and were quantized t 1/ hr. Cnturs were drawn between these particular terminal lcatins using straight lines. T the extent f the quantizatin and f the departure f the straight lines frm smth curves, the results are apprximate. V. Examples In Fig. 7 we shw cverage prvided by tw satellites t terminals with lw (0 r 5 ) minimum elevatin angles. A terminal lcated in the cntinental United States (CONUS) abve the 21 hr. line has cntinuus mutual visibility with all terminals (e.g., aircraft) lcated abve the 14 hr. line. Mst f the nrthern hemisphere is abve the 14 hr. line. In Fig. 8 cverage is shwn prvided by three satellites, tw in 6. 4 inclined rbits and ne in synchrnus equatrial rbit. Assume there are tw 5 elevatin

10 terminals lcated in CONUS as shwn. The terminal in Califrnia has cntinuus mutual visibility with shipbrne terminals lcated inside the curved cnturs in the Pacific and limited t elevatin angles greater than 20 r 0. The terminal in Maine has cntinuus mutual visibility with shipbrne terminals lcated in the Mediterranean Sea, and the Nrth Atlantic, Nrth Pacific and Arctic Oceans. VI. Satellite Design Cnsideratins Relative t the earth's equatrial plane the rbit planes f bth satellites are inclined by Relative t the earth's rbit plane (ecliptic) the inclinatin varies frm 40 t 87. As seen frm the satellite the sun can be lcated in any directin in the ecliptic plane and the earth can be lcated in any directin in the rbit plane. Thus if slar panels n the satellite are sun-riented, an earth-riented antenna must be able t pint in almst all directins relative t the plane f the slar panel. This is nt true f equatrial satellites because their rbit plane is inclined nly 2 relative t the ecliptic. An attractive way t cnfigure the satellite is shwn in Fig. 9. A mmentum wheel r cntrl mment gyr is munted n the slar panels. The wheel spins at a bias speed abut an axis nrmal t the plane f the panels. The wheel axis always pints tward the sun s the angular mmentum vectr must be rtated nce per year by appyling external trque with thrusters. Once per rbit the spacecraft rtates abut the wheel axis and the satellite bdy scillates ±180 abut the slar array shaft. A flexible cable transfers pwer and cntrl signals frm the slar panels t the bdy. Attitude cntrl is accmplished by rienting the antennas tward the earth with earth sensrs while using sun sensrs t rient the slar array. With this cnfiguratin, antennas remain earth riented but they rtate abut an axis frm the satellite t the center f the earth. During the useful part f the satellite's rbit the angle subtended by the earth varies frm ~40 t 9. 5 s use f variable beamwidth antennas wuld be desirable. At X-band (~8 GHz) a reasnable design is t include 4 r 5 antennas, with prgressively narrwer beams, and electrnically switch between them as the satellite traverses its rbit. The antenna apertures wuld vary frm t 12 inches. If a lwer frequency, e.g., UHF (00 MHz), transpnder is included, prviding a variable beamwidth antenna ver the wide variatin f satellite altitude is a mre difficult prblem due t the large aperture invlved.

11 Thermal design f the satellite bdy is smewhat simpler than fr a synchrnus equatrial rbit satellite because the sun is always in the plane which is perpendicular t the slar array shaft. Launch int the rbits frm Cape Kennedy culd be accmplished by initial launch int a 52 inclined 180 km (100 nautical miles) parking rbit, nn-cplanar transfer t 6. 4 inclinatin and 700 km (80 nm) rbit and finally cplanar transfer t the highly elliptical rbit. A launch vehicle wuld have slightly mre paylad capability fr this rbit than fr synchrnus equatrial rbit. VII. Stability f the Orbits The inclinatin f the rbits relative t the ecliptic varies frm 40 t 87. One f the effects f the secnd harmnics f the luni-slar disturbing functins (Ref. 2) is t cause the perigee height t vary in an irregular but predictable manner. This effect has been examined in Ref. 2 and the authrs have develped cmputer prgrams t btain quantitative results. When a satellite is launched int an rbit such that the perigee height initially decreases, the initial value must be large enugh t insure that, befre this height reaches a value s small that atmspheric drag is encuntered, either it passes thrugh its minimum and begins increasing r the satellite lifetime requirement is fulfilled. Thus, perigee height may be a few hundred kilmeters higher than the 700 km assumed in the cverage analysis. Increasing the perigee height by as much as several thusand kilmeters prduces nly a small change in the cverage if the rbital perid is nt changed. It may be desirable t increase perigee height t avid expsure t radiatin in the Van Allen belts. Fr this rbit, dppler shift due t the velcity f a satellite relative t a terminal is quite high. Depending n the psitin f the satellite in rbit, dppler shift can vary frm 0 t ±200 khz when the satellite frequency is 8 GHz. Lincln Experimental Terminal Number 1 demnstrated the feasibility f predicting, acquiring and tracking dppler shifts f this magnitude several years ag.

12 REFERENCES I.I. Shapir, H.M. Jnes, and C.W. Perkins, "Orbital Prperties f the West Frd Diple Belt," Prceedings f the IEEE, Vl. 52, 5, p. 472 (May 1964). G.E. Ck and D. W. Sctt, "Lifetimes f Satellites in Large-Eccentricity Orbits, " Planetary Space Science, Vl. 15, p , Pergamn Press Ltd. ACKNOWLEDGMENT The valuable cntributin f Ferenc Nagy, Jr. wh made results frm his cmputer prgrams available is greatly appreciated.

13 LINE OF NODES Fig. 1. The earth, the satellites and their rbital planes.

14 i in V 0) *-> in I > H I u 8 c a u C I u tu H be

15 a X) ^H CO ' H E t O s C u CD > cfl - CO >H a O m <-> bi vw 0 6 CQ 1-1 M c O M a a O U 0 U VM 0 t i CO 5 a c H en 1 <U h CO U CD bi 6 -<»* UH * 10

16 I 9»00l-9-(M Hi CO > a t-> e CO O.5 u CD > xs CO U O +-> c u ItH X! i-l CD % O ^^ CO a c u h b 11

17 XI»H in -.-H > - i D M n a w O = C ^ M C a cu > ed Xi w n 0 CO 4-J c 0 CJ.-1 U-H ^-i 5 c/ )H u c O J-J a d u u C O <4-l O 0) 5. i ft eg a c [/) i 1 h.5 p 1-1 I/O 0) M 5 --H ^ PH > 12

18 [ AB Fig. 6. Satellite rbit plane. 1

19 CO V 5 CO g u > CO (H 9 O g u H a XI i CN O 10 H =i P u H 9 I In MH 0 O c x; «ti 1 _c a en VH "C m q h. I-I 4-1 bi>-5 14

20 c S.5 a th 0) fcj 4-J H ^H i-h H eg CD. i 4-1 U Cfi '0 O 5 4-J 0 ^ S 0) & CO f-h O XJ C fh O CO > 1 & 2 en 0) c 0 b O c 7 C O u U c 7) OJ *J 00 ^H < bjd i-t.-1 OS tin en 15

21 =7\ SATELLITE BODY SOLAR ARRAY Fig. 9. Satellite cnfiguratin. 16

22 UNCLASSIFIED Security Classificatin DOCUMENT CONTROL DATA - R&D (Security classificatin f title, bdy f abstract and indexing anntatin must be entered when the verall reprt is classified) I. ORIGINATING ACTIVITY (Crprate authr) Lincln Labratry, M.I.T.. REPORT TITLE 2a. REPORT SECURITY CLASSIFICATION Unclassified 26. GROUP Nne Cntinuus Cverage f the Nrth Plar Regin With Only Tw Cmmunicatins Satellites 4. DESCRIPTIVE NOTES (Type f reprt and inclusive dates) Technical Nte 5. AUTHOR(S) (Last name, first name, initial) Beusch, Jhn U. 8. REPORT DATE 4 September a. CONTRACT OR GRANT NO. AF 19(628)-5167 b. PROJECT NO. 1508A 10. AVAILABILITY/LIMITATION NOTICES 7a. TOTAL NO. OF PAGES 22 9a. ORIGINATOR'S REPORT NUMBER(S) Technical Nte b. NO. OF REFS 96. OTHER REPORT NOISI (Any ther numbers that may be assigned this reprt) ESD-TR This dcument has been apprved fr public release and sale; its distributin is unlimited. 11. SUPPLEMENTARY NOTES 12. SPONSORING MILITARY ACTIVITY Nne Department f the Navy 1. ABSTRACT The prblem f prviding cntinuus cverage f the nrth plar regin with a small number f cmmunicatins satellites is cnsidered. The system described requires nly tw satellites t prvide bth this cverage and cverage f a cnsiderable fractin f the nrthern hemisphere. Tw rbit planes with 6.4 inclinatin, high eccentricity and ~24 hur perids are emplyed. The regins f the earth frm which a satellite is cntinuusly visible frm terminals with varius minimum elevatin angles are shwn. The regins in which mutual visibility f a satellite by tw terminals is guaranteed are shwn. A few cmments cncerning satellite design fr this rbit are included. 14. KEY WORDS nrth plar cverage cmmunicatins satellites satellites satellite rbits 17 UNCLASSIFIED Security Classificatin

ASTRODYNAMICS. o o o. Early Space Exploration. Kepler's Laws. Nicolaus Copernicus ( ) Placed Sun at center of solar system

ASTRODYNAMICS. o o o. Early Space Exploration. Kepler's Laws. Nicolaus Copernicus ( ) Placed Sun at center of solar system ASTRODYNAMICS Early Space Explratin Niclaus Cpernicus (1473-1543) Placed Sun at center f slar system Shwed Earth rtates n its axis nce a day Thught planets rbit in unifrm circles (wrng!) Jhannes Kepler

More information

and the Doppler frequency rate f R , can be related to the coefficients of this polynomial. The relationships are:

and the Doppler frequency rate f R , can be related to the coefficients of this polynomial. The relationships are: Algrithm fr Estimating R and R - (David Sandwell, SIO, August 4, 2006) Azimith cmpressin invlves the alignment f successive eches t be fcused n a pint target Let s be the slw time alng the satellite track

More information

Chapter 1 Notes Using Geography Skills

Chapter 1 Notes Using Geography Skills Chapter 1 Ntes Using Gegraphy Skills Sectin 1: Thinking Like a Gegrapher Gegraphy is used t interpret the past, understand the present, and plan fr the future. Gegraphy is the study f the Earth. It is

More information

CESAR Science Case The differential rotation of the Sun and its Chromosphere. Introduction. Material that is necessary during the laboratory

CESAR Science Case The differential rotation of the Sun and its Chromosphere. Introduction. Material that is necessary during the laboratory Teacher s guide CESAR Science Case The differential rtatin f the Sun and its Chrmsphere Material that is necessary during the labratry CESAR Astrnmical wrd list CESAR Bklet CESAR Frmula sheet CESAR Student

More information

A Polarimetric Survey of Radio Frequency Interference in C- and X-Bands in the Continental United States using WindSat Radiometry

A Polarimetric Survey of Radio Frequency Interference in C- and X-Bands in the Continental United States using WindSat Radiometry A Plarimetric Survey f Radi Frequency Interference in C- and X-Bands in the Cntinental United States using WindSat Radimetry Steven W. Ellingsn Octber, Cntents Intrductin WindSat Methdlgy Analysis f RFI

More information

Flipping Physics Lecture Notes: Simple Harmonic Motion Introduction via a Horizontal Mass-Spring System

Flipping 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 information

Technical Note

Technical Note CO &< S8 i CO PJ < '! t-i H i M Q H U3 CO w w ESD-TR-68-188 ESD RECORD COPY RETURN TO SCIENTIFIC & TECHNICAL INFORMATION DIVISION (ESTi), BUILDING 1211 ESD ACCESSION LIST ESTI Call N. AL 61616 Cpy N. f

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

Flipping Physics Lecture Notes: Simple Harmonic Motion Introduction via a Horizontal Mass-Spring System

Flipping 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 information

AP Statistics Notes Unit Two: The Normal Distributions

AP Statistics Notes Unit Two: The Normal Distributions AP Statistics Ntes Unit Tw: The Nrmal Distributins Syllabus Objectives: 1.5 The student will summarize distributins f data measuring the psitin using quartiles, percentiles, and standardized scres (z-scres).

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

Chapter 9 Vector Differential Calculus, Grad, Div, Curl

Chapter 9 Vector Differential Calculus, Grad, Div, Curl Chapter 9 Vectr Differential Calculus, Grad, Div, Curl 9.1 Vectrs in 2-Space and 3-Space 9.2 Inner Prduct (Dt Prduct) 9.3 Vectr Prduct (Crss Prduct, Outer Prduct) 9.4 Vectr and Scalar Functins and Fields

More information

the results to larger systems due to prop'erties of the projection algorithm. First, the number of hidden nodes must

the results to larger systems due to prop'erties of the projection algorithm. First, the number of hidden nodes must M.E. Aggune, M.J. Dambrg, M.A. El-Sharkawi, R.J. Marks II and L.E. Atlas, "Dynamic and static security assessment f pwer systems using artificial neural netwrks", Prceedings f the NSF Wrkshp n Applicatins

More information

Phys101 Final Code: 1 Term: 132 Wednesday, May 21, 2014 Page: 1

Phys101 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 information

Sections 15.1 to 15.12, 16.1 and 16.2 of the textbook (Robbins-Miller) cover the materials required for this topic.

Sections 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 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

CHAPTER 3 INEQUALITIES. Copyright -The Institute of Chartered Accountants of India

CHAPTER 3 INEQUALITIES. Copyright -The Institute of Chartered Accountants of India CHAPTER 3 INEQUALITIES Cpyright -The Institute f Chartered Accuntants f India INEQUALITIES LEARNING OBJECTIVES One f the widely used decisin making prblems, nwadays, is t decide n the ptimal mix f scarce

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

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

Bootstrap 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) >

Bootstrap 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 information

Journal of Molecular EvOlution by Springer-Verlag. 1979

Journal of Molecular EvOlution by Springer-Verlag. 1979 0022-28447900140057~ 01.60 J. Ml. Evl. 14, 57--64 (1979) Jurnal f Mlecular EvOlutin by Springer-Verlag. 1979 Slar Radiatin Incident n the Martian Surface W.R. Kuhn and S.K. Atreya Department f Atmspheric

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

NGSS High School Physics Domain Model

NGSS High School Physics Domain Model NGSS High Schl Physics Dmain Mdel Mtin and Stability: Frces and Interactins HS-PS2-1: Students will be able t analyze data t supprt the claim that Newtn s secnd law f mtin describes the mathematical relatinship

More information

On Boussinesq's problem

On Boussinesq's problem Internatinal Jurnal f Engineering Science 39 (2001) 317±322 www.elsevier.cm/lcate/ijengsci On Bussinesq's prblem A.P.S. Selvadurai * Department f Civil Engineering and Applied Mechanics, McGill University,

More information

Yeu-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 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 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

14. Which shows the direction of the centripetal force acting on a mass spun in a vertical circle?

14. 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 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

14. Which shows the direction of the centripetal force acting on a mass spun in a vertical circle?

14. 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 information

The Sputtering Problem James A Glackin, James V. Matheson

The Sputtering Problem James A Glackin, James V. Matheson The Sputtering Prblem James A Glackin, James V. Mathesn I prpse t cnsider first the varius elements f the subject, next its varius parts r sectins, and finally the whle in its internal structure. In ther

More information

Q x = cos 1 30 = 53.1 South

Q 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 information

I. Analytical Potential and Field of a Uniform Rod. V E d. The definition of electric potential difference is

I. Analytical Potential and Field of a Uniform Rod. V E d. The definition of electric potential difference is Length L>>a,b,c Phys 232 Lab 4 Ch 17 Electric Ptential Difference Materials: whitebards & pens, cmputers with VPythn, pwer supply & cables, multimeter, crkbard, thumbtacks, individual prbes and jined prbes,

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

Figure 1a. A planar mechanism.

Figure 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 information

Astro 102 Lab #2. 1) Learning the user interface and setting up your home location

Astro 102 Lab #2. 1) Learning the user interface and setting up your home location Name: Astr 102 Lab #2 Lab bjectives 1) Learn hw t use the Stellarium planetarium prgram by becming familiar with the user interface and cnfiguring the planetarium t yur present lcatin n Earth 2) Learn

More information

Sodium D-line doublet. Lectures 5-6: Magnetic dipole moments. Orbital magnetic dipole moments. Orbital magnetic dipole moments

Sodium 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 information

UNIT 6 DETERMINATION OF FLASH AND FIRE POINT OF A LUBRICATING OIL BY OPEN CUP AND CLOSED CUP METHODS

UNIT 6 DETERMINATION OF FLASH AND FIRE POINT OF A LUBRICATING OIL BY OPEN CUP AND CLOSED CUP METHODS UNIT 6 DETERMINATION OF FLASH AND FIRE POINT OF A LUBRICATING OIL BY OPEN CUP AND CLOSED CUP METHODS Determinatin f Flash and Fire Pint f a Cup and Clsed Cup Structure 6. Intrductin Objectives 6. Experiment

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

Building to Transformations on Coordinate Axis Grade 5: Geometry Graph points on the coordinate plane to solve real-world and mathematical problems.

Building 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 information

Space Shuttle Ascent Mass vs. Time

Space Shuttle Ascent Mass vs. Time Space Shuttle Ascent Mass vs. Time Backgrund This prblem is part f a series that applies algebraic principles in NASA s human spaceflight. The Space Shuttle Missin Cntrl Center (MCC) and the Internatinal

More information

1 The limitations of Hartree Fock approximation

1 The limitations of Hartree Fock approximation Chapter: Pst-Hartree Fck Methds - I The limitatins f Hartree Fck apprximatin The n electrn single determinant Hartree Fck wave functin is the variatinal best amng all pssible n electrn single determinants

More information

Q1. In figure 1, Q = 60 µc, q = 20 µc, a = 3.0 m, and b = 4.0 m. Calculate the total electric force on q due to the other 2 charges.

Q1. In figure 1, Q = 60 µc, q = 20 µc, a = 3.0 m, and b = 4.0 m. Calculate the total electric force on q due to the other 2 charges. Phys10 Secnd Majr-08 Zer Versin Crdinatr: Dr. I. M. Nasser Saturday, May 3, 009 Page: 1 Q1. In figure 1, Q = 60 µc, q = 0 µc, a = 3.0 m, and b = 4.0 m. Calculate the ttal electric frce n q due t the ther

More information

Forward-Integration Riccati-Based Feedback Control for Spacecraft Rendezvous Maneuvers on Elliptic Orbits

Forward-Integration Riccati-Based Feedback Control for Spacecraft Rendezvous Maneuvers on Elliptic Orbits 5st IEEE Cnference n Decisin and Cntrl December -3,. Maui, Hawaii, USA Frward-Integratin Riccati-Based Feedback Cntrl fr Spacecraft Rendezvus Maneuvers n Elliptic Avishai Weiss, Ilya Klmanvsky, Mrgan Baldwin,

More information

Uncertainties in TRP Measurements Due to Finite Range Lengths

Uncertainties in TRP Measurements Due to Finite Range Lengths Uncertainties in TRP Measurements Due t Finite Range Lengths James D Huff Carl W Sirles The Hwland Cmpany, Inc 4540 Atwater Curt, Suite 107 Bufrd, Gergia 30518 Abstract Ttal Radiated Pwer (TRP) and Ttal

More information

(s6 ~lj t') >~.'c;. .. ' ' 9adanki ( N, E)',- !2!!!m'!!.y~ation-6fhorizont~~cb' in the ~()wert.~2qq~~hereover --:!"

(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 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

Introduction: A Generalized approach for computing the trajectories associated with the Newtonian N Body Problem

Introduction: 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 information

3D FE Modeling Simulation of Cold Rotary Forging with Double Symmetry Rolls X. H. Han 1, a, L. Hua 1, b, Y. M. Zhao 1, c

3D FE Modeling Simulation of Cold Rotary Forging with Double Symmetry Rolls X. H. Han 1, a, L. Hua 1, b, Y. M. Zhao 1, c Materials Science Frum Online: 2009-08-31 ISSN: 1662-9752, Vls. 628-629, pp 623-628 di:10.4028/www.scientific.net/msf.628-629.623 2009 Trans Tech Publicatins, Switzerland 3D FE Mdeling Simulatin f Cld

More information

5.4 Measurement Sampling Rates for Daily Maximum and Minimum Temperatures

5.4 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

THERMAL TEST LEVELS & DURATIONS

THERMAL TEST LEVELS & DURATIONS PREFERRED RELIABILITY PAGE 1 OF 7 PRACTICES PRACTICE NO. PT-TE-144 Practice: 1 Perfrm thermal dwell test n prtflight hardware ver the temperature range f +75 C/-2 C (applied at the thermal cntrl/munting

More information

A study on GPS PDOP and its impact on position error

A study on GPS PDOP and its impact on position error IndianJurnalfRadi& SpacePhysics V1.26,April1997,pp. 107-111 A study n GPS and its impact n psitin errr P Banerjee,AnindyaBse& B SMathur TimeandFrequencySectin,NatinalPhysicalLabratry,NewDelhi110012 Received19June

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

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

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

Synchronous Motor V-Curves

Synchronous Motor V-Curves Synchrnus Mtr V-Curves 1 Synchrnus Mtr V-Curves Intrductin Synchrnus mtrs are used in applicatins such as textile mills where cnstant speed peratin is critical. Mst small synchrnus mtrs cntain squirrel

More information

Physics 2B Chapter 23 Notes - Faraday s Law & Inductors Spring 2018

Physics 2B Chapter 23 Notes - Faraday s Law & Inductors Spring 2018 Michael Faraday lived in the Lndn area frm 1791 t 1867. He was 29 years ld when Hand Oersted, in 1820, accidentally discvered that electric current creates magnetic field. Thrugh empirical bservatin and

More information

SPH3U1 Lesson 06 Kinematics

SPH3U1 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 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

CS 477/677 Analysis of Algorithms Fall 2007 Dr. George Bebis Course Project Due Date: 11/29/2007

CS 477/677 Analysis of Algorithms Fall 2007 Dr. George Bebis Course Project Due Date: 11/29/2007 CS 477/677 Analysis f Algrithms Fall 2007 Dr. Gerge Bebis Curse Prject Due Date: 11/29/2007 Part1: Cmparisn f Srting Algrithms (70% f the prject grade) The bjective f the first part f the assignment is

More information

THE FLUXOID QUANTUM AND ELECTROGRAVITATIONAL DYNAMICS. Chapter 8. This work extends chapter 6 titled, "Field Mass Generation and Control", while

THE FLUXOID QUANTUM AND ELECTROGRAVITATIONAL DYNAMICS. Chapter 8. This work extends chapter 6 titled, Field Mass Generation and Control, while 133 THE FLUXOID QUANTUM AND ELECTROGRAVITATIONAL DYNAMICS Chapter 8 This wrk extends chapter 6 titled, "Field Mass Generatin and Cntrl", while als develping a new cnceptual apprach t mass-field vehicle

More information

ECEN 4872/5827 Lecture Notes

ECEN 4872/5827 Lecture Notes ECEN 4872/5827 Lecture Ntes Lecture #5 Objectives fr lecture #5: 1. Analysis f precisin current reference 2. Appraches fr evaluating tlerances 3. Temperature Cefficients evaluatin technique 4. Fundamentals

More information

Three 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 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 information

PHYSICAL PROPERTIES OF SEA WATER - TEMPERATURE AND SALINITY

PHYSICAL PROPERTIES OF SEA WATER - TEMPERATURE AND SALINITY NAME PHYSICAL PROPERTIES OF SEA WATER - TEMPERATURE AND SALINITY I. Sea water temperatures The distributin f surface temperatures fr the majr ceans is shwn in Figure 1. The istherms (lines f equal temperature)

More information

( ) + θ θ. ω rotation rate. θ g geographic latitude - - θ geocentric latitude - - Reference Earth Model - WGS84 (Copyright 2002, David T.

( ) + 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 information

Plan o o. I(t) Divide problem into sub-problems Modify schematic and coordinate system (if needed) Write general equations

Plan o o. I(t) Divide problem into sub-problems Modify schematic and coordinate system (if needed) Write general equations STAPLE Physics 201 Name Final Exam May 14, 2013 This is a clsed bk examinatin but during the exam yu may refer t a 5 x7 nte card with wrds f wisdm yu have written n it. There is extra scratch paper available.

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

COASTAL ENGINEERING Chapter 2

COASTAL ENGINEERING Chapter 2 CASTAL ENGINEERING Chapter 2 GENERALIZED WAVE DIFFRACTIN DIAGRAMS J. W. Jhnsn Assciate Prfessr f Mechanical Engineering University f Califrnia Berkeley, Califrnia INTRDUCTIN Wave diffractin is the phenmenn

More information

Supporting information

Supporting information Electrnic Supplementary Material (ESI) fr Physical Chemistry Chemical Physics This jurnal is The wner Scieties 01 ydrgen perxide electrchemistry n platinum: twards understanding the xygen reductin reactin

More information

Chem 115 POGIL Worksheet - Week 12 Molecular Shapes

Chem 115 POGIL Worksheet - Week 12 Molecular Shapes Chem 115 POGIL Wrksheet - Week 12 Mlecular Shapes Why? Cntrary t the impressin that Lewis structures may give, many mlecules have threedimensinal gemetries. These mlecular shapes are very imprtant t understanding

More information

DATING LUNAR SURFACE FEATURES BY USING CRATER FREQUENCIES* T. J. Kreiter

DATING LUNAR SURFACE FEATURES BY USING CRATER FREQUENCIES* T. J. Kreiter DATING LUNAR SURFACE FEATURES BY USING CRATER FREQUENCIES* T. J. Kreiter Divisin f Space Sciences Jet Prpulsin Labratry Califrnia Institute f Technlgy INTRODUCTION Several theries have been advanced relating

More information

Chapter 23 Electromagnetic Waves Lecture 14

Chapter 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 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

Measurement of Radial Loss and Lifetime. of Microwave Plasma in the Octupo1e. J. C. Sprott PLP 165. Plasma Studies. University of Wisconsin DEC 1967

Measurement of Radial Loss and Lifetime. of Microwave Plasma in the Octupo1e. J. C. Sprott PLP 165. Plasma Studies. University of Wisconsin DEC 1967 Measurement f Radial Lss and Lifetime f Micrwave Plasma in the Octup1e J. C. Sprtt PLP 165 Plasma Studies University f Wiscnsin DEC 1967 1 The number f particles in the tridal ctuple was measured as a

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

Module 4: General Formulation of Electric Circuit Theory

Module 4: General Formulation of Electric Circuit Theory Mdule 4: General Frmulatin f Electric Circuit Thery 4. General Frmulatin f Electric Circuit Thery All electrmagnetic phenmena are described at a fundamental level by Maxwell's equatins and the assciated

More information

Kinematic transformation of mechanical behavior Neville Hogan

Kinematic transformation of mechanical behavior Neville Hogan inematic transfrmatin f mechanical behavir Neville Hgan Generalized crdinates are fundamental If we assume that a linkage may accurately be described as a cllectin f linked rigid bdies, their generalized

More information

1.2.1 Vectors. 1 P age. Examples What is the reference vector angle for a vector that points 50 degrees east of south?

1.2.1 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 information

Introduction to Spacetime Geometry

Introduction to Spacetime Geometry Intrductin t Spacetime Gemetry Let s start with a review f a basic feature f Euclidean gemetry, the Pythagrean therem. In a twdimensinal crdinate system we can relate the length f a line segment t the

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

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

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

(2) Even if such a value of k was possible, the neutrons multiply

(2) Even if such a value of k was possible, the neutrons multiply CHANGE OF REACTOR Nuclear Thery - Curse 227 POWER WTH REACTVTY CHANGE n this lessn, we will cnsider hw neutrn density, neutrn flux and reactr pwer change when the multiplicatin factr, k, r the reactivity,

More information

Heat Management Methodology for Successful UV Processing on Heat Sensitive Substrates

Heat Management Methodology for Successful UV Processing on Heat Sensitive Substrates Heat Management Methdlgy fr Successful UV Prcessing n Heat Sensitive Substrates Juliet Midlik Prime UV Systems Abstract: Nw in 2005, UV systems pssess heat management cntrls that fine tune the exthermic

More information

CHAPTER 4 DIAGNOSTICS FOR INFLUENTIAL OBSERVATIONS

CHAPTER 4 DIAGNOSTICS FOR INFLUENTIAL OBSERVATIONS CHAPTER 4 DIAGNOSTICS FOR INFLUENTIAL OBSERVATIONS 1 Influential bservatins are bservatins whse presence in the data can have a distrting effect n the parameter estimates and pssibly the entire analysis,

More information

THERMAL-VACUUM VERSUS THERMAL- ATMOSPHERIC TESTS OF ELECTRONIC ASSEMBLIES

THERMAL-VACUUM VERSUS THERMAL- ATMOSPHERIC TESTS OF ELECTRONIC ASSEMBLIES PREFERRED RELIABILITY PAGE 1 OF 5 PRACTICES PRACTICE NO. PT-TE-1409 THERMAL-VACUUM VERSUS THERMAL- ATMOSPHERIC Practice: Perfrm all thermal envirnmental tests n electrnic spaceflight hardware in a flight-like

More information

Fall 2013 Physics 172 Recitation 3 Momentum and Springs

Fall 2013 Physics 172 Recitation 3 Momentum and Springs Fall 03 Physics 7 Recitatin 3 Mmentum and Springs Purpse: The purpse f this recitatin is t give yu experience wrking with mmentum and the mmentum update frmula. Readings: Chapter.3-.5 Learning Objectives:.3.

More information

BASD HIGH SCHOOL FORMAL LAB REPORT

BASD HIGH SCHOOL FORMAL LAB REPORT BASD HIGH SCHOOL FORMAL LAB REPORT *WARNING: After an explanatin f what t include in each sectin, there is an example f hw the sectin might lk using a sample experiment Keep in mind, the sample lab used

More information

Activity Guide Loops and Random Numbers

Activity Guide Loops and Random Numbers Unit 3 Lessn 7 Name(s) Perid Date Activity Guide Lps and Randm Numbers CS Cntent Lps are a relatively straightfrward idea in prgramming - yu want a certain chunk f cde t run repeatedly - but it takes a

More information

Physics 321 Solutions for Final Exam

Physics 321 Solutions for Final Exam Page f 8 Physics 3 Slutins fr inal Exa ) A sall blb f clay with ass is drpped fr a height h abve a thin rd f length L and ass M which can pivt frictinlessly abut its center. The initial situatin is shwn

More information

RN52-STK2 Starter Kit

RN52-STK2 Starter Kit The RN52-STK2 Starter Kit has everything yu need t kick-start yur prject and is a great tl fr develpers: Prf f cncept prttypes as well as final cmmercial slutins. fr educatinal use: Natural sciences curses

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

Determining the Accuracy of Modal Parameter Estimation Methods

Determining 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 information

February 28, 2013 COMMENTS ON DIFFUSION, DIFFUSIVITY AND DERIVATION OF HYPERBOLIC EQUATIONS DESCRIBING THE DIFFUSION PHENOMENA

February 28, 2013 COMMENTS ON DIFFUSION, DIFFUSIVITY AND DERIVATION OF HYPERBOLIC EQUATIONS DESCRIBING THE DIFFUSION PHENOMENA February 28, 2013 COMMENTS ON DIFFUSION, DIFFUSIVITY AND DERIVATION OF HYPERBOLIC EQUATIONS DESCRIBING THE DIFFUSION PHENOMENA Mental Experiment regarding 1D randm walk Cnsider a cntainer f gas in thermal

More information

ELECTRON CYCLOTRON HEATING OF AN ANISOTROPIC PLASMA. December 4, PLP No. 322

ELECTRON CYCLOTRON HEATING OF AN ANISOTROPIC PLASMA. December 4, PLP No. 322 ELECTRON CYCLOTRON HEATING OF AN ANISOTROPIC PLASMA by J. C. SPROTT December 4, 1969 PLP N. 3 These PLP Reprts are infrmal and preliminary and as such may cntain errrs nt yet eliminated. They are fr private

More information

ROUNDING ERRORS IN BEAM-TRACKING CALCULATIONS

ROUNDING 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 information

Chapter 31: Galaxies and the Universe

Chapter 31: Galaxies and the Universe Chapter 31: Galaxies and the Universe Sectin 1: The Milky Way Galaxy Objectives 1. Determine the size and shape f the Milky Way, as well as Earth s lcatin within it. 2. Describe hw the Milky Way frmed.

More information

Using GPS with Students High Tech Hide & Seek!

Using GPS with Students High Tech Hide & Seek! Using GPS with Students High Tech Hide & Seek! Intrductin: As we cntinue int the twenty-first century, we are cntinuusly being challenged by new technlgies. As teachers, we try t use technlgy effectively

More information

Chemistry 20 Lesson 11 Electronegativity, Polarity and Shapes

Chemistry 20 Lesson 11 Electronegativity, Polarity and Shapes Chemistry 20 Lessn 11 Electrnegativity, Plarity and Shapes In ur previus wrk we learned why atms frm cvalent bnds and hw t draw the resulting rganizatin f atms. In this lessn we will learn (a) hw the cmbinatin

More information