6.2. orbits. Satellites and Space Stations

Size: px
Start display at page:

Download "6.2. orbits. Satellites and Space Stations"

Transcription

1 obits RADARSAT-1 and RADARSAT-2 ae Eath-obsevation satellites designed and commissioned by the Canadian Space Agency. These eyes in the skies pee down fom obit, captuing images and data that help scientists monito envionmental changes and the planet s natual esouces. Examples of satellite monitoing include detecting oil spills, tacking ice movements, identifying ships at sea, and monitoing natual disastes. Figue 1 shows an image of RADARSAT Figue 1 RADARSAT-2 uses sophisticated micowave-based ada to collect images of Eath day and night, even though cloud cove. Satellites and Space Stations A satellite is an object o a body that evolves aound anothe body that usually has much moe mass than the satellite. Fo example, the planets ae natual satellites evolving aound the Sun. Planetay moons, including Eath s moon, ae natual satellites, too. Atificial satellites, on the othe hand, ae human-made objects that obit Eath o othe bodies in the sola system. CAREER LINK RADARSAT-1 and RADARSAT-2 ae examples of atificial satellites. Anothe wellknown example of atificial satellites is the netwok of 24 satellites that make up the Global Positioning System (GPS). By coodinating seveal signals at once, as shown in Figue 2, the system can locate an object on Eath s suface to within 15 m of its actual position. satellite an object o a body that evolves aound anothe body due to gavitational attaction atificial satellite an object that has been intentionally placed by humans into obit aound Eath o anothe body; efeed to as atifi cial to distinguish fom natual satellites such as the Moon S 1 S 1 S 2 S 1 S 2 S 3 (a) (b) (c) Figue 2 GPS satellites can detemine the location of an object, in this case a boat. (a) The data fom one satellite will show that the location is somewhee along the cicumfeence of a cicle. (b) Two satellites consulted simultaneously will efi ne the location to one of two intesection spots. (c) With thee satellites consulted simultaneously, the intesection of thee cicles will give the location of the boat to within 15 m of its actual position. 6.2 Obits 297

2 space station a spacecaft in which people live and wok Figue 3 The Intenational Space Station is an obiting spacecaft in which astonauts live and wok in space. The boat shown in Figue 2 on the pevious page has a compute-contolled GPS eceive that detects signals fom thee satellites simultaneously. The system calculates distances based on signal speeds and tansmission times. A single satellite can identify the boat s location somewhee along the cicumfeence of a cicle. Two simultaneous satellite signals can pinpoint the location at one of two intesecting spots whee two cicles intesect. With a thid satellite and theefoe thee intesecting cicles the boat s location can be pinpointed. This is efeed to as tiangulation. Anothe example of an atificial satellite in Eath obit is a space station, a spacecaft in which people live and wok. An example is the Intenational Space Station (ISS), shown in Figue 3. The ISS is a pemanent obiting laboatoy that suppots many diffeent eseach pojects. In the pocess, scientists ae also able to study human esponses to space tavel and zeo gavity o, moe accuately, micogavity: times the value of g. A micogavity envionment is pesent when any object is in fee fall. So when you dive fom a dive towe into a swimming pool, you ae in micogavity until you hit the wate. Similaly, astonauts aboad the ISS ae in a constant state of fee fall and ae thus in a micogavity envionment. It is impotant to note the diffeence between micogavity and the gavitational field stength, since the value of g at the altitude of the ISS is appoximately 8.7 N/kg. Clealy, thee is still a significant gavitational foce at that altitude and it is incoect to say that the astonauts ae in zeo gavity. A gavitational foce of appoximately zeo would only occu if you wee extemely fa away fom any mass. The knowledge gained fom eseach by obiting space stations enables scientists to design spacecaft that can safely tanspot people though space and pefom expeiments in micogavity envionments. These micogavity expeiments can lead to beakthoughs in medicine and chemisty. CAREER LINK Mini Investigation Exploing Gavity and Obits Mini Investigation Skills: Pefoming, Obseving, Analyzing, Communicating In this investigation, you will use a simulation to ceate and exploe diffeent configuations of obiting bodies. Move the planets, moons, o the Sun to see how the obital paths change. Change the sizes of the objects and the distances between them. Exploe the vaiations that occu as the foce of gavity is changed o when gavity is emoved fom the model. Equipment and Mateials: compute with Intenet access 1. Go to the Nelson Science website. 2. Load the suppoting softwae, if necessay. 3. Select the option to view the Sun, Eath, and Moon and the options to show Gavity Foce and the Path. 4. Play the simulation and allow Eath to complete one full evolution aound the Sun. 5. Pause the simulation. 6. Using the slide ba, incease the size of the Sun and stat the simulation again. Obseve the motion of Eath and the Moon aound the Sun fo one full evolution. 7. Pause the simulation again. Retun the Sun to its oiginal size and then incease the size of Eath. 8. Stat the simulation again and obseve Eath s evolution. A. What happens to the obit of Eath when you incease the size of the Sun? T/I A B. What happens to the Moon when you incease the size of the Sun? What happens when you incease the size of Eath? T/I A C. What happens to Eath s obit when you incease the size of Eath? T/I A D. The MESSENGER pobe mentioned at the beginning of this chapte made use of seveal gavity assists to each Mecuy without using too much of its own enegy. This method is also known as a gavitational slingshot. It woks by using the gavity of a celestial body to acceleate, slow down, o ediect the path of a spacecaft. Gavity assists can save fuel, time, and expense. Ty to design a system of obiting elements within the simulation that demonstates this effect. K/U T/I C A WEB LINK 298 Chapte 6 Gavitational Fields

3 Satellites in Cicula Obits When Newton developed the idea of univesal gavitation, he also theoized that the same foce that pulls objects to Eath also keeps the Moon in its obit. One diffeence, of couse, is that the Moon does not hit Eath s suface. The Moon obits Eath at a distance fom Eath s cente called the obital adius. The obit of the Moon about Eath is anothe example of centipetal motion, which you studied in Chapte 3. The foce of gavity on the Moon due to Eath is a centipetal foce that pulls the Moon towad Eath s cente. As the Moon obits Eath, the Moon has velocity pependicula to the adius vecto. Without gavity, the Moon would fly off in a staight line. Without its obital velocity, howeve, the foce of gavity would pull the Moon staight to Eath s suface. The obital motion of the Moon depends on both the centipetal foce due to gavity and the Moon s obital velocity. The Moon s obit, simila to the obits of the planets aound the Sun, is actually elliptical. We can closely appoximate the obits, howeve, by assuming that they ae cicula. This appoximation is useful fo most poblem-solving puposes. To analyze the motion of a satellite in unifom cicula motion, combine Newton s law of univesal gavitation with the mathematical expession descibing centipetal acceleation. Using the univesal law of gavitation fom Section 6.1, we can say that the gavitational field stength of Eath with mass m E at the location of a satellite at height above Eath s cente is obital adius the distance between the cente of a satellite and the cente of its paent body g 5 Gm E 2 Recall fom Chapte 3 that the fomula fo centipetal acceleation based on the obiting object s speed v is a c 5 v 2 Fo a satellite in a cicula obit, the gavitational foce povides the centipetal foce. Combining the above two equations gives a c 5 g v 2 5 Gm E 2 Unit TASK BOOKMARK You can apply what you have leaned about obits and satellites to the Unit Task on page 422. Solving fo the speed of the satellite and using only the positive squae oot gives v 5 Å Gm E This equation holds fo an obiting body in a cental gavitational field. If a satellite obits aound any othe lage body with mass m, we can eplace the mass of Eath in this equation and genealize it to v 5 Å Gm This equation indicates that the speed of a satellite depends on its obital adius and is independent of the satellite s own mass. Fo a satellite to maintain an obit of adius, its speed v must be constant. 6.2 Obits 299

4 geosynchonous obit the obit aound Eath of an object with an obital speed matching the ate of Eath s otation; the peiod of such an obit is exactly one Eath day A communications satellite in geosynchonous obit that is, a satellite obiting Eath with a speed matching that of Eath s own otation is an example of an atificial satellite with a constant obital adius (Figue 4). The obital peiod, epesented by the symbol T, is the time it takes an object to complete one obit aound anothe object. A geosynchonous satellite s obital speed leads to an obital peiod that exactly matches Eath s otational peiod. To an obseve on Eath, the satellite will appea to tavel though the same point in the sky evey 24 h. A geostationay obit is a type of geosynchonous obit in which the satellite obits diectly ove the equato. To an obseve on Eath, a geostationay satellite will appea to emain fixed in the same point in the sky at all times. CAREER LINK adius foce of gavity Figue 4 A satellite with a geosynchonous obit tavels at the same speed as Eath s otation. Its obital peiod is one Eath day. In the following Tutoial you will exploe how you can use the equation fo obital speed in poblem solving. obit Tutoial 1 Solving Poblems Relating to Cicula Obits The Sample Poblems in this Tutoial show how to detemine the popeties of an object in a cicula obit within a gavitational field aound a lage object. Sample Poblem 1: Calculating the Speed and Obital Peiod of a Satellite The Intenational Space Station (ISS) obits Eath at an altitude of about 350 km above Eath s suface. (a) Detemine the speed needed by the ISS to maintain its obit. (b) Detemine the obital peiod of the ISS in minutes. Solution (a) Given: G N m 2 /kg 2 ; m E kg; E m; h ISS km m Requied: v Gm E Analysis: v 5 ; 5 Å E 1 h ISS m Solution: v 5 Å Gm E kg # m # m 2 s kg2 kg 2 5 ï m v m/s 1two exta digits caied2 Statement: The ISS equies a speed of m/s to maintain its obit. 300 Chapte 6 Gavitational Fields

5 (b) Given: v m/s; m Requied: T Analysis: The distance tavelled in one peiod is 2p. The obital peiod, T, is the time it takes fo the space station to tavel this distance, so it is the distance divided by the speed, T 5 2p. v Solution: T 5 2p v 5 2p m m 3 1 min 60 s 3 s T 5 92 min Statement: The ISS has an obital peiod of 92 min. Sample Poblem 2: Calculating the Speeds of Planets aound the Sun Detemine the speeds of Venus and Eath as they obit the Sun. The Sun s mass is kg. Venus has an obital adius of m, and Eath has an obital adius of m. Given: G N m 2 /kg 2 ; m S kg; V m; E m Requied: v V ; v E Gm Analysis: v 5 Å Solution: Gm S v V 5 Å V kg # m # m 2 s kg2 kg 2 5 ï m v V m/s Gm S v E 5 Å E kg # m # m 2 s kg2 kg 2 5 ï m v E m/s Statement: Venus obits the Sun at a speed of m/s, and Eath obits the Sun at a speed of m/s. 6.2 Obits 301

6 Pactice 1. Astonomes have detemined that a black hole sits at the cente of galaxy M87 (Figue 5). Obsevations show matte at a distance of m fom the black hole and tavelling at speeds of m/s. Calculate the mass of the black hole, assuming the matte being obseved moves in a cicula obit aound it. T/I A [ans: kg] Figue 5 Investigation Design a Sola System (page 309) With what you have leaned about obits and the movement of planetay bodies, you ae eady to take the next step. This investigation will give you an oppotunity to ceate you own sola system with a sun, seveal planets, and moons. 2. Mas obits the Sun in a nealy cicula obit of adius m. The mass of Mas is kg. Mas expeiences a gavitational foce fom the Sun of magnitude N. Calculate the speed of Mas and the peiod of evolution fo Mas in tems of Eath yeas. T/I A [ans: m/s; 1.90 Eath yeas] 3. Calculate the speed of a satellite in a cicula obit km above Eath s suface. Detemine the obital peiod of the satellite to two signifi cant digits. T/I A [ans: m/s; 97 min] 4. Satellites can obit the Moon vey close to the Moon s suface because the Moon has no atmosphee to slow the satellite though ai esistance. Detemine the speed of a satellite that obits the Moon just 25 m above the suface. (Hint: Refe to Appendix B fo adius and mass data fo the Moon.) T/I A [ans: m/s] eseach This Space Junk Skills: Reseaching, Analyzing, Communicating Space junk is debis fom atifi cial objects obiting Eath. It is just one example of how benefi cial technology can have unwanted envionmental effects. In this activity, you will eseach space junk and discove how an obiting body can go fom being a functioning satellite to being space junk. 1. Reseach the mechanisms that satellites have to maintain speed and obital adius. 2. Reseach methods of dealing with diffeent foms of space junk. 3. Exploe one stoy of space junk that catches you inteest. A. Review this chapte s fomulas petaining to the elationship between obital speed and obital adius. Descibe effects that could make a satellite slow down in its obit and slip into a lowe obit. C A SKILLS HANDBOOK A4.1 B. Descibe what happens when a satellite difts so low that it entes Eath s atmosphee. C A C. Ae thee any ways to avoid ceating space junk? T/I C D. Ae thee any effective ways to get id of existing space junk? C A E. Compose an to a fiend descibing what space junk is. Include the inteesting example you eseached in Step 3. C WEB LINK 302 Chapte 6 Gavitational Fields

7 6.2 Review Summay Satellites can be natual, such as moons aound planets, o atificial, such as the RADARSAT satellites and the Intenational Space Station. The speed, v, of a satellite in unifom cicula motion aound a cental body depends on the mass of the cental body, m, and the adius of the obit, : v 5 Å Gm Fo a given obital adius, a satellite in cicula obit has a constant speed. Questions 1. What is the diffeence between natual and atificial satellites? Give an example of each. K/U 2. Explain what micogavity is. K/U 3. Explain in you own wods how GPS satellites wok. K/U 4. (a) What is a geosynchonous obit? (b) How does a satellite in geosynchonous obit appea to an obseve on Eath? (c) How does a satellite in geostationay obit appea to an obseve on Eath? K/U C 5. Calculate the obital adius of a satellite in geosynchonous obit. K/U T/I A 6. Neptune obits the Sun in Eath yeas in an appoximately cicula obit at a adius of km. T/I A (a) Detemine the obital speed of Neptune. (b) Detemine the mass of the Sun. 7. Satun makes one complete obit of the Sun evey 29 Eath yeas with a speed of 9.69 km/s. Calculate the adius of the obit of Satun. Assume a cicula obit. T/I A 8. The egion of the sola system between Mas and Jupite, called the Asteoid Belt, contains many asteoids that obit the Sun. Conside an asteoid in a cicula obit of adius m. T/I A (a) Calculate the speed of the asteoid aound the Sun. (b) Calculate the peiod of the obit in yeas. 9. In ecent yeas, astonomes have discoveed that a numbe of neaby stas have planets of thei own, called exoplanets. A newly discoveed exoplanet obits a sta with ou Sun s mass ( kg) in a cicula obit with an obital adius of m. What is the obital speed of the exoplanet in kilometes pe hou? T/I A 10. The obital adius of one exoplanet is m, with a peiod of 1100 Eath days. Calculate the mass of the sta aound which the exoplanet evolves. T/I A 11. Phobos (Figue 6), one of Mas s moons, has an elliptical obit aound Mas with an obital adius that vaies between 9200 km and 9500 km. Calculate the obital peiod of Phobos in Eath days, assuming a cicula obit of adius m. The mass of Mas is kg. T/I A Figue Detemine the speed of a satellite, in kilometes pe hou, that is in a geosynchonous obit about Eath. (Hint: Use the equation fo the speed of an object in cicula motion and equate that to the speed of a satellite in obit aound a cental body. Reaange the equation to solve fo the adius. Use the adius to calculate the speed.) K/U T/I A 13. (a) Calculate the obital speeds of the planets Mecuy, Venus, Eath, and Mas using the sola system data in Appendix B. (b) What can you conclude about the speed of the planets in obit fathe fom the Sun? T/I A 14. Scientists wish to place a geosynchonous satellite nea a moon at an altitude of 410 km. The mass of the moon is kg and it has a adius of m. Calculate the velocity and the peiod of the satellite. T/I A 6.2 Obits 303

FXA 2008. Candidates should be able to : Describe how a mass creates a gravitational field in the space around it.

FXA 2008. Candidates should be able to : Describe how a mass creates a gravitational field in the space around it. Candidates should be able to : Descibe how a mass ceates a gavitational field in the space aound it. Define gavitational field stength as foce pe unit mass. Define and use the peiod of an object descibing

More information

Episode 401: Newton s law of universal gravitation

Episode 401: Newton s law of universal gravitation Episode 401: Newton s law of univesal gavitation This episode intoduces Newton s law of univesal gavitation fo point masses, and fo spheical masses, and gets students pactising calculations of the foce

More information

Determining solar characteristics using planetary data

Determining solar characteristics using planetary data Detemining sola chaacteistics using planetay data Intoduction The Sun is a G type main sequence sta at the cente of the Sola System aound which the planets, including ou Eath, obit. In this inestigation

More information

2 r2 θ = r2 t. (3.59) The equal area law is the statement that the term in parentheses,

2 r2 θ = r2 t. (3.59) The equal area law is the statement that the term in parentheses, 3.4. KEPLER S LAWS 145 3.4 Keple s laws You ae familia with the idea that one can solve some mechanics poblems using only consevation of enegy and (linea) momentum. Thus, some of what we see as objects

More information

PHYSICS 111 HOMEWORK SOLUTION #13. May 1, 2013

PHYSICS 111 HOMEWORK SOLUTION #13. May 1, 2013 PHYSICS 111 HOMEWORK SOLUTION #13 May 1, 2013 0.1 In intoductoy physics laboatoies, a typical Cavendish balance fo measuing the gavitational constant G uses lead sphees with masses of 2.10 kg and 21.0

More information

Gravitation. AP Physics C

Gravitation. AP Physics C Gavitation AP Physics C Newton s Law of Gavitation What causes YOU to be pulled down? THE EARTH.o moe specifically the EARTH S MASS. Anything that has MASS has a gavitational pull towads it. F α Mm g What

More information

The Role of Gravity in Orbital Motion

The Role of Gravity in Orbital Motion ! The Role of Gavity in Obital Motion Pat of: Inquiy Science with Datmouth Developed by: Chistophe Caoll, Depatment of Physics & Astonomy, Datmouth College Adapted fom: How Gavity Affects Obits (Ohio State

More information

Experiment 6: Centripetal Force

Experiment 6: Centripetal Force Name Section Date Intoduction Expeiment 6: Centipetal oce This expeiment is concened with the foce necessay to keep an object moving in a constant cicula path. Accoding to Newton s fist law of motion thee

More information

Physics 235 Chapter 5. Chapter 5 Gravitation

Physics 235 Chapter 5. Chapter 5 Gravitation Chapte 5 Gavitation In this Chapte we will eview the popeties of the gavitational foce. The gavitational foce has been discussed in geat detail in you intoductoy physics couses, and we will pimaily focus

More information

Physics HSC Course Stage 6. Space. Part 1: Earth s gravitational field

Physics HSC Course Stage 6. Space. Part 1: Earth s gravitational field Physics HSC Couse Stage 6 Space Pat 1: Eath s gavitational field Contents Intoduction... Weight... 4 The value of g... 7 Measuing g...8 Vaiations in g...11 Calculating g and W...13 You weight on othe

More information

(a) The centripetal acceleration of a point on the equator of the Earth is given by v2. The velocity of the earth can be found by taking the ratio of

(a) The centripetal acceleration of a point on the equator of the Earth is given by v2. The velocity of the earth can be found by taking the ratio of Homewok VI Ch. 7 - Poblems 15, 19, 22, 25, 35, 43, 51. Poblem 15 (a) The centipetal acceleation of a point on the equato of the Eath is given by v2. The velocity of the eath can be found by taking the

More information

Gravitational Mechanics of the Mars-Phobos System: Comparing Methods of Orbital Dynamics Modeling for Exploratory Mission Planning

Gravitational Mechanics of the Mars-Phobos System: Comparing Methods of Orbital Dynamics Modeling for Exploratory Mission Planning Gavitational Mechanics of the Mas-Phobos System: Compaing Methods of Obital Dynamics Modeling fo Exploatoy Mission Planning Alfedo C. Itualde The Pennsylvania State Univesity, Univesity Pak, PA, 6802 This

More information

7 Circular Motion. 7-1 Centripetal Acceleration and Force. Period, Frequency, and Speed. Vocabulary

7 Circular Motion. 7-1 Centripetal Acceleration and Force. Period, Frequency, and Speed. Vocabulary 7 Cicula Motion 7-1 Centipetal Acceleation and Foce Peiod, Fequency, and Speed Vocabulay Vocabulay Peiod: he time it takes fo one full otation o evolution of an object. Fequency: he numbe of otations o

More information

2. Orbital dynamics and tides

2. Orbital dynamics and tides 2. Obital dynamics and tides 2.1 The two-body poblem This efes to the mutual gavitational inteaction of two bodies. An exact mathematical solution is possible and staightfowad. In the case that one body

More information

F G r. Don't confuse G with g: "Big G" and "little g" are totally different things.

F G r. Don't confuse G with g: Big G and little g are totally different things. G-1 Gavity Newton's Univesal Law of Gavitation (fist stated by Newton): any two masses m 1 and m exet an attactive gavitational foce on each othe accoding to m m G 1 This applies to all masses, not just

More information

12. Rolling, Torque, and Angular Momentum

12. Rolling, Torque, and Angular Momentum 12. olling, Toque, and Angula Momentum 1 olling Motion: A motion that is a combination of otational and tanslational motion, e.g. a wheel olling down the oad. Will only conside olling with out slipping.

More information

Voltage ( = Electric Potential )

Voltage ( = Electric Potential ) V-1 Voltage ( = Electic Potential ) An electic chage altes the space aound it. Thoughout the space aound evey chage is a vecto thing called the electic field. Also filling the space aound evey chage is

More information

1240 ev nm 2.5 ev. (4) r 2 or mv 2 = ke2

1240 ev nm 2.5 ev. (4) r 2 or mv 2 = ke2 Chapte 5 Example The helium atom has 2 electonic enegy levels: E 3p = 23.1 ev and E 2s = 20.6 ev whee the gound state is E = 0. If an electon makes a tansition fom 3p to 2s, what is the wavelength of the

More information

Magnetic Field and Magnetic Forces. Young and Freedman Chapter 27

Magnetic Field and Magnetic Forces. Young and Freedman Chapter 27 Magnetic Field and Magnetic Foces Young and Feedman Chapte 27 Intoduction Reiew - electic fields 1) A chage (o collection of chages) poduces an electic field in the space aound it. 2) The electic field

More information

Voltage ( = Electric Potential )

Voltage ( = Electric Potential ) V-1 of 9 Voltage ( = lectic Potential ) An electic chage altes the space aound it. Thoughout the space aound evey chage is a vecto thing called the electic field. Also filling the space aound evey chage

More information

Gravitation and Kepler s Laws Newton s Law of Universal Gravitation in vectorial. Gm 1 m 2. r 2

Gravitation and Kepler s Laws Newton s Law of Universal Gravitation in vectorial. Gm 1 m 2. r 2 F Gm Gavitation and Keple s Laws Newton s Law of Univesal Gavitation in vectoial fom: F 12 21 Gm 1 m 2 12 2 ˆ 12 whee the hat (ˆ) denotes a unit vecto as usual. Gavity obeys the supeposition pinciple,

More information

Vector Calculus: Are you ready? Vectors in 2D and 3D Space: Review

Vector Calculus: Are you ready? Vectors in 2D and 3D Space: Review Vecto Calculus: Ae you eady? Vectos in D and 3D Space: Review Pupose: Make cetain that you can define, and use in context, vecto tems, concepts and fomulas listed below: Section 7.-7. find the vecto defined

More information

Figure 2. So it is very likely that the Babylonians attributed 60 units to each side of the hexagon. Its resulting perimeter would then be 360!

Figure 2. So it is very likely that the Babylonians attributed 60 units to each side of the hexagon. Its resulting perimeter would then be 360! 1. What ae angles? Last time, we looked at how the Geeks intepeted measument of lengths. Howeve, as fascinated as they wee with geomety, thee was a shape that was much moe enticing than any othe : the

More information

Exam 3: Equation Summary

Exam 3: Equation Summary MASSACHUSETTS INSTITUTE OF TECHNOLOGY Depatment of Physics Physics 8.1 TEAL Fall Tem 4 Momentum: p = mv, F t = p, Fext ave t= t f t= Exam 3: Equation Summay total = Impulse: I F( t ) = p Toque: τ = S S,P

More information

est using the formula I = Prt, where I is the interest earned, P is the principal, r is the interest rate, and t is the time in years.

est using the formula I = Prt, where I is the interest earned, P is the principal, r is the interest rate, and t is the time in years. 9.2 Inteest Objectives 1. Undestand the simple inteest fomula. 2. Use the compound inteest fomula to find futue value. 3. Solve the compound inteest fomula fo diffeent unknowns, such as the pesent value,

More information

Gravity. A. Law of Gravity. Gravity. Physics: Mechanics. A. The Law of Gravity. Dr. Bill Pezzaglia. B. Gravitational Field. C.

Gravity. A. Law of Gravity. Gravity. Physics: Mechanics. A. The Law of Gravity. Dr. Bill Pezzaglia. B. Gravitational Field. C. Physics: Mechanics 1 Gavity D. Bill Pezzaglia A. The Law of Gavity Gavity B. Gavitational Field C. Tides Updated: 01Jul09 A. Law of Gavity 3 1a. Invese Squae Law 4 1. Invese Squae Law. Newton s 4 th law

More information

PY1052 Problem Set 8 Autumn 2004 Solutions

PY1052 Problem Set 8 Autumn 2004 Solutions PY052 Poblem Set 8 Autumn 2004 Solutions H h () A solid ball stats fom est at the uppe end of the tack shown and olls without slipping until it olls off the ight-hand end. If H 6.0 m and h 2.0 m, what

More information

Lab #7: Energy Conservation

Lab #7: Energy Conservation Lab #7: Enegy Consevation Photo by Kallin http://www.bungeezone.com/pics/kallin.shtml Reading Assignment: Chapte 7 Sections 1,, 3, 5, 6 Chapte 8 Sections 1-4 Intoduction: Pehaps one of the most unusual

More information

The force between electric charges. Comparing gravity and the interaction between charges. Coulomb s Law. Forces between two charges

The force between electric charges. Comparing gravity and the interaction between charges. Coulomb s Law. Forces between two charges The foce between electic chages Coulomb s Law Two chaged objects, of chage q and Q, sepaated by a distance, exet a foce on one anothe. The magnitude of this foce is given by: kqq Coulomb s Law: F whee

More information

AP Physics Electromagnetic Wrap Up

AP Physics Electromagnetic Wrap Up AP Physics Electomagnetic Wap Up Hee ae the gloious equations fo this wondeful section. F qsin This is the equation fo the magnetic foce acting on a moing chaged paticle in a magnetic field. The angle

More information

Chapter 3 Savings, Present Value and Ricardian Equivalence

Chapter 3 Savings, Present Value and Ricardian Equivalence Chapte 3 Savings, Pesent Value and Ricadian Equivalence Chapte Oveview In the pevious chapte we studied the decision of households to supply hous to the labo maket. This decision was a static decision,

More information

Analytical Proof of Newton's Force Laws

Analytical Proof of Newton's Force Laws Analytical Poof of Newton s Foce Laws Page 1 1 Intouction Analytical Poof of Newton's Foce Laws Many stuents intuitively assume that Newton's inetial an gavitational foce laws, F = ma an Mm F = G, ae tue

More information

VISCOSITY OF BIO-DIESEL FUELS

VISCOSITY OF BIO-DIESEL FUELS VISCOSITY OF BIO-DIESEL FUELS One of the key assumptions fo ideal gases is that the motion of a given paticle is independent of any othe paticles in the system. With this assumption in place, one can use

More information

Spirotechnics! September 7, 2011. Amanda Zeringue, Michael Spannuth and Amanda Zeringue Dierential Geometry Project

Spirotechnics! September 7, 2011. Amanda Zeringue, Michael Spannuth and Amanda Zeringue Dierential Geometry Project Spiotechnics! Septembe 7, 2011 Amanda Zeingue, Michael Spannuth and Amanda Zeingue Dieential Geomety Poject 1 The Beginning The geneal consensus of ou goup began with one thought: Spiogaphs ae awesome.

More information

Chapter 17 The Kepler Problem: Planetary Mechanics and the Bohr Atom

Chapter 17 The Kepler Problem: Planetary Mechanics and the Bohr Atom Chapte 7 The Keple Poblem: Planetay Mechanics and the Boh Atom Keple s Laws: Each planet moves in an ellipse with the sun at one focus. The adius vecto fom the sun to a planet sweeps out equal aeas in

More information

SAMPLE CHAPTERS UNESCO EOLSS THE MOTION OF CELESTIAL BODIES. Kaare Aksnes Institute of Theoretical Astrophysics University of Oslo

SAMPLE CHAPTERS UNESCO EOLSS THE MOTION OF CELESTIAL BODIES. Kaare Aksnes Institute of Theoretical Astrophysics University of Oslo THE MOTION OF CELESTIAL BODIES Kaae Aksnes Institute of Theoetical Astophysics Univesity of Oslo Keywods: celestial mechanics, two-body obits, thee-body obits, petubations, tides, non-gavitational foces,

More information

Epdf Sulf petroleum, Eflecti and Eeflecti

Epdf Sulf petroleum, Eflecti and Eeflecti ANALYSIS OF GLOBAL WARMING MITIGATION BY WHITE REFLECTING SURFACES Fedeico Rossi, Andea Nicolini Univesity of Peugia, CIRIAF Via G.Duanti 67 0615 Peugia, Italy T: +9-075-585846; F: +9-075-5848470; E: fossi@unipg.it

More information

Structure and evolution of circumstellar disks during the early phase of accretion from a parent cloud

Structure and evolution of circumstellar disks during the early phase of accretion from a parent cloud Cente fo Tubulence Reseach Annual Reseach Biefs 2001 209 Stuctue and evolution of cicumstella disks duing the ealy phase of accetion fom a paent cloud By Olusola C. Idowu 1. Motivation and Backgound The

More information

Experiment MF Magnetic Force

Experiment MF Magnetic Force Expeiment MF Magnetic Foce Intoduction The magnetic foce on a cuent-caying conducto is basic to evey electic moto -- tuning the hands of electic watches and clocks, tanspoting tape in Walkmans, stating

More information

Magnetic Bearing with Radial Magnetized Permanent Magnets

Magnetic Bearing with Radial Magnetized Permanent Magnets Wold Applied Sciences Jounal 23 (4): 495-499, 2013 ISSN 1818-4952 IDOSI Publications, 2013 DOI: 10.5829/idosi.wasj.2013.23.04.23080 Magnetic eaing with Radial Magnetized Pemanent Magnets Vyacheslav Evgenevich

More information

Chapter 4: Fluid Kinematics

Chapter 4: Fluid Kinematics Oveview Fluid kinematics deals with the motion of fluids without consideing the foces and moments which ceate the motion. Items discussed in this Chapte. Mateial deivative and its elationship to Lagangian

More information

The Binomial Distribution

The Binomial Distribution The Binomial Distibution A. It would be vey tedious if, evey time we had a slightly diffeent poblem, we had to detemine the pobability distibutions fom scatch. Luckily, thee ae enough similaities between

More information

Lecture 16: Color and Intensity. and he made him a coat of many colours. Genesis 37:3

Lecture 16: Color and Intensity. and he made him a coat of many colours. Genesis 37:3 Lectue 16: Colo and Intensity and he made him a coat of many colous. Genesis 37:3 1. Intoduction To display a pictue using Compute Gaphics, we need to compute the colo and intensity of the light at each

More information

Software Engineering and Development

Software Engineering and Development I T H E A 67 Softwae Engineeing and Development SOFTWARE DEVELOPMENT PROCESS DYNAMICS MODELING AS STATE MACHINE Leonid Lyubchyk, Vasyl Soloshchuk Abstact: Softwae development pocess modeling is gaining

More information

Chapter 30: Magnetic Fields Due to Currents

Chapter 30: Magnetic Fields Due to Currents d Chapte 3: Magnetic Field Due to Cuent A moving electic chage ceate a magnetic field. One of the moe pactical way of geneating a lage magnetic field (.1-1 T) i to ue a lage cuent flowing though a wie.

More information

Thank you for participating in Teach It First!

Thank you for participating in Teach It First! Thank you fo paticipating in Teach It Fist! This Teach It Fist Kit contains a Common Coe Suppot Coach, Foundational Mathematics teache lesson followed by the coesponding student lesson. We ae confident

More information

Displacement, Velocity And Acceleration

Displacement, Velocity And Acceleration Displacement, Velocity And Acceleation Vectos and Scalas Position Vectos Displacement Speed and Velocity Acceleation Complete Motion Diagams Outline Scala vs. Vecto Scalas vs. vectos Scala : a eal numbe,

More information

Coordinate Systems L. M. Kalnins, March 2009

Coordinate Systems L. M. Kalnins, March 2009 Coodinate Sstems L. M. Kalnins, Mach 2009 Pupose of a Coodinate Sstem The pupose of a coodinate sstem is to uniquel detemine the position of an object o data point in space. B space we ma liteall mean

More information

Charges, Coulomb s Law, and Electric Fields

Charges, Coulomb s Law, and Electric Fields Q&E -1 Chages, Coulomb s Law, and Electic ields Some expeimental facts: Expeimental fact 1: Electic chage comes in two types, which we call (+) and ( ). An atom consists of a heavy (+) chaged nucleus suounded

More information

Problem Set # 9 Solutions

Problem Set # 9 Solutions Poblem Set # 9 Solutions Chapte 12 #2 a. The invention of the new high-speed chip inceases investment demand, which shifts the cuve out. That is, at evey inteest ate, fims want to invest moe. The incease

More information

Gauss Law. Physics 231 Lecture 2-1

Gauss Law. Physics 231 Lecture 2-1 Gauss Law Physics 31 Lectue -1 lectic Field Lines The numbe of field lines, also known as lines of foce, ae elated to stength of the electic field Moe appopiately it is the numbe of field lines cossing

More information

SELF-INDUCTANCE AND INDUCTORS

SELF-INDUCTANCE AND INDUCTORS MISN-0-144 SELF-INDUCTANCE AND INDUCTORS SELF-INDUCTANCE AND INDUCTORS by Pete Signell Michigan State Univesity 1. Intoduction.............................................. 1 A 2. Self-Inductance L.........................................

More information

The Electric Potential, Electric Potential Energy and Energy Conservation. V = U/q 0. V = U/q 0 = -W/q 0 1V [Volt] =1 Nm/C

The Electric Potential, Electric Potential Energy and Energy Conservation. V = U/q 0. V = U/q 0 = -W/q 0 1V [Volt] =1 Nm/C Geneal Physics - PH Winte 6 Bjoen Seipel The Electic Potential, Electic Potential Enegy and Enegy Consevation Electic Potential Enegy U is the enegy of a chaged object in an extenal electic field (Unit

More information

Financing Terms in the EOQ Model

Financing Terms in the EOQ Model Financing Tems in the EOQ Model Habone W. Stuat, J. Columbia Business School New Yok, NY 1007 hws7@columbia.edu August 6, 004 1 Intoduction This note discusses two tems that ae often omitted fom the standad

More information

UNIT CIRCLE TRIGONOMETRY

UNIT CIRCLE TRIGONOMETRY UNIT CIRCLE TRIGONOMETRY The Unit Cicle is the cicle centeed at the oigin with adius unit (hence, the unit cicle. The equation of this cicle is + =. A diagam of the unit cicle is shown below: + = - - -

More information

AN IMPLEMENTATION OF BINARY AND FLOATING POINT CHROMOSOME REPRESENTATION IN GENETIC ALGORITHM

AN IMPLEMENTATION OF BINARY AND FLOATING POINT CHROMOSOME REPRESENTATION IN GENETIC ALGORITHM AN IMPLEMENTATION OF BINARY AND FLOATING POINT CHROMOSOME REPRESENTATION IN GENETIC ALGORITHM Main Golub Faculty of Electical Engineeing and Computing, Univesity of Zageb Depatment of Electonics, Micoelectonics,

More information

The LCOE is defined as the energy price ($ per unit of energy output) for which the Net Present Value of the investment is zero.

The LCOE is defined as the energy price ($ per unit of energy output) for which the Net Present Value of the investment is zero. Poject Decision Metics: Levelized Cost of Enegy (LCOE) Let s etun to ou wind powe and natual gas powe plant example fom ealie in this lesson. Suppose that both powe plants wee selling electicity into the

More information

Solution Derivations for Capa #8

Solution Derivations for Capa #8 Solution Deivations fo Capa #8 1) A ass spectoete applies a voltage of 2.00 kv to acceleate a singly chaged ion (+e). A 0.400 T field then bends the ion into a cicula path of adius 0.305. What is the ass

More information

An Introduction to Omega

An Introduction to Omega An Intoduction to Omega Con Keating and William F. Shadwick These distibutions have the same mean and vaiance. Ae you indiffeent to thei isk-ewad chaacteistics? The Finance Development Cente 2002 1 Fom

More information

Multiple choice questions [60 points]

Multiple choice questions [60 points] 1 Multiple choice questions [60 points] Answe all o the ollowing questions. Read each question caeully. Fill the coect bubble on you scanton sheet. Each question has exactly one coect answe. All questions

More information

ON THE (Q, R) POLICY IN PRODUCTION-INVENTORY SYSTEMS

ON THE (Q, R) POLICY IN PRODUCTION-INVENTORY SYSTEMS ON THE R POLICY IN PRODUCTION-INVENTORY SYSTEMS Saifallah Benjaafa and Joon-Seok Kim Depatment of Mechanical Engineeing Univesity of Minnesota Minneapolis MN 55455 Abstact We conside a poduction-inventoy

More information

CRRC-1 Method #1: Standard Practice for Measuring Solar Reflectance of a Flat, Opaque, and Heterogeneous Surface Using a Portable Solar Reflectometer

CRRC-1 Method #1: Standard Practice for Measuring Solar Reflectance of a Flat, Opaque, and Heterogeneous Surface Using a Portable Solar Reflectometer CRRC- Method #: Standad Pactice fo Measuing Sola Reflectance of a Flat, Opaque, and Heteogeneous Suface Using a Potable Sola Reflectomete Scope This standad pactice coves a technique fo estimating the

More information

STUDENT RESPONSE TO ANNUITY FORMULA DERIVATION

STUDENT RESPONSE TO ANNUITY FORMULA DERIVATION Page 1 STUDENT RESPONSE TO ANNUITY FORMULA DERIVATION C. Alan Blaylock, Hendeson State Univesity ABSTRACT This pape pesents an intuitive appoach to deiving annuity fomulas fo classoom use and attempts

More information

Converting knowledge Into Practice

Converting knowledge Into Practice Conveting knowledge Into Pactice Boke Nightmae srs Tend Ride By Vladimi Ribakov Ceato of Pips Caie 20 of June 2010 2 0 1 0 C o p y i g h t s V l a d i m i R i b a k o v 1 Disclaime and Risk Wanings Tading

More information

Solutions for Physics 1301 Course Review (Problems 10 through 18)

Solutions for Physics 1301 Course Review (Problems 10 through 18) Solutions fo Physics 1301 Couse Review (Poblems 10 though 18) 10) a) When the bicycle wheel comes into contact with the step, thee ae fou foces acting on it at that moment: its own weight, Mg ; the nomal

More information

Chapter 22. Outside a uniformly charged sphere, the field looks like that of a point charge at the center of the sphere.

Chapter 22. Outside a uniformly charged sphere, the field looks like that of a point charge at the center of the sphere. Chapte.3 What is the magnitude of a point chage whose electic field 5 cm away has the magnitude of.n/c. E E 5.56 1 11 C.5 An atom of plutonium-39 has a nuclea adius of 6.64 fm and atomic numbe Z94. Assuming

More information

The Gravity Field of the Earth - Part 1 (Copyright 2002, David T. Sandwell)

The Gravity Field of the Earth - Part 1 (Copyright 2002, David T. Sandwell) 1 The Gavity Field of the Eath - Pat 1 (Copyight 00, David T. Sandwell) This chapte coves physical geodesy - the shape of the Eath and its gavity field. This is just electostatic theoy applied to the Eath.

More information

TORQUE AND ANGULAR MOMENTUM IN CIRCULAR MOTION

TORQUE AND ANGULAR MOMENTUM IN CIRCULAR MOTION MISN-0-34 TORQUE AND ANGULAR MOMENTUM IN CIRCULAR MOTION shaft TORQUE AND ANGULAR MOMENTUM IN CIRCULAR MOTION by Kiby Mogan, Chalotte, Michigan 1. Intoduction..............................................

More information

Introduction to Fluid Mechanics

Introduction to Fluid Mechanics Chapte 1 1 1.6. Solved Examples Example 1.1 Dimensions and Units A body weighs 1 Ibf when exposed to a standad eath gavity g = 3.174 ft/s. (a) What is its mass in kg? (b) What will the weight of this body

More information

Ilona V. Tregub, ScD., Professor

Ilona V. Tregub, ScD., Professor Investment Potfolio Fomation fo the Pension Fund of Russia Ilona V. egub, ScD., Pofesso Mathematical Modeling of Economic Pocesses Depatment he Financial Univesity unde the Govenment of the Russian Fedeation

More information

Mechanics 1: Work, Power and Kinetic Energy

Mechanics 1: Work, Power and Kinetic Energy Mechanics 1: Wok, Powe and Kinetic Eneg We fist intoduce the ideas of wok and powe. The notion of wok can be viewed as the bidge between Newton s second law, and eneg (which we have et to define and discuss).

More information

Define What Type of Trader Are you?

Define What Type of Trader Are you? Define What Type of Tade Ae you? Boke Nightmae srs Tend Ride By Vladimi Ribakov Ceato of Pips Caie 20 of June 2010 1 Disclaime and Risk Wanings Tading any financial maket involves isk. The content of this

More information

Problems of the 2 nd and 9 th International Physics Olympiads (Budapest, Hungary, 1968 and 1976)

Problems of the 2 nd and 9 th International Physics Olympiads (Budapest, Hungary, 1968 and 1976) Poblems of the nd and 9 th Intenational Physics Olympiads (Budapest Hungay 968 and 976) Péte Vankó Institute of Physics Budapest Univesity of Technology and Economics Budapest Hungay Abstact Afte a shot

More information

Chapte 3 Is Gavitation A Results Of Asymmetic Coulomb Chage Inteactions? Jounal of Undegaduate Reseach èjurè Univesity of Utah è1992è, Vol. 3, No. 1, pp. 56í61. Jeæey F. Gold Depatment of Physics, Depatment

More information

Forces & Magnetic Dipoles. r r τ = μ B r

Forces & Magnetic Dipoles. r r τ = μ B r Foces & Magnetic Dipoles x θ F θ F. = AI τ = U = Fist electic moto invented by Faaday, 1821 Wie with cuent flow (in cup of Hg) otates aound a a magnet Faaday s moto Wie with cuent otates aound a Pemanent

More information

Do Vibrations Make Sound?

Do Vibrations Make Sound? Do Vibations Make Sound? Gade 1: Sound Pobe Aligned with National Standads oveview Students will lean about sound and vibations. This activity will allow students to see and hea how vibations do in fact

More information

Deflection of Electrons by Electric and Magnetic Fields

Deflection of Electrons by Electric and Magnetic Fields Physics 233 Expeiment 42 Deflection of Electons by Electic and Magnetic Fields Refeences Loain, P. and D.R. Coson, Electomagnetism, Pinciples and Applications, 2nd ed., W.H. Feeman, 199. Intoduction An

More information

Multiple choice questions [70 points]

Multiple choice questions [70 points] Multiple choice questions [70 points] Answe all of the following questions. Read each question caefull. Fill the coect bubble on ou scanton sheet. Each question has exactl one coect answe. All questions

More information

The transport performance evaluation system building of logistics enterprises

The transport performance evaluation system building of logistics enterprises Jounal of Industial Engineeing and Management JIEM, 213 6(4): 194-114 Online ISSN: 213-953 Pint ISSN: 213-8423 http://dx.doi.og/1.3926/jiem.784 The tanspot pefomance evaluation system building of logistics

More information

Questions & Answers Chapter 10 Software Reliability Prediction, Allocation and Demonstration Testing

Questions & Answers Chapter 10 Software Reliability Prediction, Allocation and Demonstration Testing M13914 Questions & Answes Chapte 10 Softwae Reliability Pediction, Allocation and Demonstation Testing 1. Homewok: How to deive the fomula of failue ate estimate. λ = χ α,+ t When the failue times follow

More information

Mechanics 1: Motion in a Central Force Field

Mechanics 1: Motion in a Central Force Field Mechanics : Motion in a Cental Foce Field We now stud the popeties of a paticle of (constant) ass oving in a paticula tpe of foce field, a cental foce field. Cental foces ae ve ipotant in phsics and engineeing.

More information

Carter-Penrose diagrams and black holes

Carter-Penrose diagrams and black holes Cate-Penose diagams and black holes Ewa Felinska The basic intoduction to the method of building Penose diagams has been pesented, stating with obtaining a Penose diagam fom Minkowski space. An example

More information

Concept and Experiences on using a Wiki-based System for Software-related Seminar Papers

Concept and Experiences on using a Wiki-based System for Software-related Seminar Papers Concept and Expeiences on using a Wiki-based System fo Softwae-elated Semina Papes Dominik Fanke and Stefan Kowalewski RWTH Aachen Univesity, 52074 Aachen, Gemany, {fanke, kowalewski}@embedded.wth-aachen.de,

More information

Physics Core Topic 9.2 Space

Physics Core Topic 9.2 Space Physics 9. Space Syllabus Notes Physics Coe Topic 9. Space Summay of Contextual Outline Scientists daw on othe aeas of science to deelop iable spacecaft Launch, e enty and landing ae dangeous Huge foces

More information

CHAPTER 5 GRAVITATIONAL FIELD AND POTENTIAL

CHAPTER 5 GRAVITATIONAL FIELD AND POTENTIAL CHATER 5 GRAVITATIONAL FIELD AND OTENTIAL 5. Intoduction. This chapte deals with the calculation of gavitational fields and potentials in the vicinity of vaious shapes and sizes of massive bodies. The

More information

Lesson 7 Gauss s Law and Electric Fields

Lesson 7 Gauss s Law and Electric Fields Lesson 7 Gauss s Law and Electic Fields Lawence B. Rees 7. You may make a single copy of this document fo pesonal use without witten pemission. 7. Intoduction While it is impotant to gain a solid conceptual

More information

Database Management Systems

Database Management Systems Contents Database Management Systems (COP 5725) D. Makus Schneide Depatment of Compute & Infomation Science & Engineeing (CISE) Database Systems Reseach & Development Cente Couse Syllabus 1 Sping 2012

More information

Open Economies. Chapter 32. A Macroeconomic Theory of the Open Economy. Basic Assumptions of a Macroeconomic Model of an Open Economy

Open Economies. Chapter 32. A Macroeconomic Theory of the Open Economy. Basic Assumptions of a Macroeconomic Model of an Open Economy Chapte 32. A Macoeconomic Theoy of the Open Economy Open Economies An open economy is one that inteacts feely with othe economies aound the wold. slide 0 slide 1 Key Macoeconomic Vaiables in an Open Economy

More information

Skills Needed for Success in Calculus 1

Skills Needed for Success in Calculus 1 Skills Needed fo Success in Calculus Thee is much appehension fom students taking Calculus. It seems that fo man people, "Calculus" is snonmous with "difficult." Howeve, an teache of Calculus will tell

More information

Quantity Formula Meaning of variables. 5 C 1 32 F 5 degrees Fahrenheit, 1 bh A 5 area, b 5 base, h 5 height. P 5 2l 1 2w

Quantity Formula Meaning of variables. 5 C 1 32 F 5 degrees Fahrenheit, 1 bh A 5 area, b 5 base, h 5 height. P 5 2l 1 2w 1.4 Rewite Fomulas and Equations Befoe You solved equations. Now You will ewite and evaluate fomulas and equations. Why? So you can apply geometic fomulas, as in Ex. 36. Key Vocabulay fomula solve fo a

More information

Comparing Availability of Various Rack Power Redundancy Configurations

Comparing Availability of Various Rack Power Redundancy Configurations Compaing Availability of Vaious Rack Powe Redundancy Configuations White Pape 48 Revision by Victo Avela > Executive summay Tansfe switches and dual-path powe distibution to IT equipment ae used to enhance

More information

Gravitation and Kepler s Laws

Gravitation and Kepler s Laws 3 Gavitation and Keple s Laws In this chapte we will ecall the law of univesal gavitation and will then deive the esult that a spheically symmetic object acts gavitationally like a point mass at its cente

More information

Valuation of Floating Rate Bonds 1

Valuation of Floating Rate Bonds 1 Valuation of Floating Rate onds 1 Joge uz Lopez us 316: Deivative Secuities his note explains how to value plain vanilla floating ate bonds. he pupose of this note is to link the concepts that you leaned

More information

Chapter 4: Fluid Kinematics

Chapter 4: Fluid Kinematics 4-1 Lagangian g and Euleian Desciptions 4-2 Fundamentals of Flow Visualization 4-3 Kinematic Desciption 4-4 Reynolds Tanspot Theoem (RTT) 4-1 Lagangian and Euleian Desciptions (1) Lagangian desciption

More information

Comparing Availability of Various Rack Power Redundancy Configurations

Comparing Availability of Various Rack Power Redundancy Configurations Compaing Availability of Vaious Rack Powe Redundancy Configuations By Victo Avela White Pape #48 Executive Summay Tansfe switches and dual-path powe distibution to IT equipment ae used to enhance the availability

More information

DYNAMICS AND STRUCTURAL LOADING IN WIND TURBINES

DYNAMICS AND STRUCTURAL LOADING IN WIND TURBINES DYNAMIS AND STRUTURAL LOADING IN WIND TURBINES M. Ragheb 12/30/2008 INTRODUTION The loading egimes to which wind tubines ae subject to ae extemely complex equiing special attention in thei design, opeation

More information

Semipartial (Part) and Partial Correlation

Semipartial (Part) and Partial Correlation Semipatial (Pat) and Patial Coelation his discussion boows heavily fom Applied Multiple egession/coelation Analysis fo the Behavioal Sciences, by Jacob and Paticia Cohen (975 edition; thee is also an updated

More information

CHAPTER 9 THE TWO BODY PROBLEM IN TWO DIMENSIONS

CHAPTER 9 THE TWO BODY PROBLEM IN TWO DIMENSIONS 9. Intoduction CHAPTER 9 THE TWO BODY PROBLEM IN TWO DIMENSIONS In this chapte we show how Keple s laws can be deived fom Newton s laws of motion and gavitation, and consevation of angula momentum, and

More information

TECHNICAL DATA. JIS (Japanese Industrial Standard) Screw Thread. Specifications

TECHNICAL DATA. JIS (Japanese Industrial Standard) Screw Thread. Specifications JIS (Japanese Industial Standad) Scew Thead Specifications TECNICAL DATA Note: Although these specifications ae based on JIS they also apply to and DIN s. Some comments added by Mayland Metics Coutesy

More information

PAN STABILITY TESTING OF DC CIRCUITS USING VARIATIONAL METHODS XVIII - SPETO - 1995. pod patronatem. Summary

PAN STABILITY TESTING OF DC CIRCUITS USING VARIATIONAL METHODS XVIII - SPETO - 1995. pod patronatem. Summary PCE SEMINIUM Z PODSTW ELEKTOTECHNIKI I TEOII OBWODÓW 8 - TH SEMIN ON FUNDMENTLS OF ELECTOTECHNICS ND CICUIT THEOY ZDENĚK BIOLEK SPŠE OŽNO P.., CZECH EPUBLIC DLIBO BIOLEK MILITY CDEMY, BNO, CZECH EPUBLIC

More information