8.4. Motion of Charged Particles in Magnetic Fields

Size: px
Start display at page:

Download "8.4. Motion of Charged Particles in Magnetic Fields"

Transcription

1 Motion of Chaged Paticles in Magnetic Fields Atos and olecules ae paticles that ae the building blocks of ou uniese. How do scientists study the natue of these sall paticles? The ass spectoete shown in Figue 1 is an instuent scientists use to study atos and olecules. Mass spectoetes ae used to define the eleental coposition of a saple o olecule, to deteine asses of paticles, and to eeal the cheical stuctues of olecules. 8.4 Figue 1 A scientist insets a saple into a ass spectoete. How does a ass spectoete wok? Iagine a billiad table with a billiad ball olling acoss the table fo you left to you ight. If you hit the ball with a sideways foce, the ball will oe away fo you. Now suppose a bowling ball olls acoss the table in the sae diection. If you apply the sae sideways foce on the bowling ball, it will also oe away fo you but not as fa. The asses of the billiad ball and bowling ball deteine the distance they will be deflected by the foce. If you know the aount of foce, the speeds of the balls, and the cue of thei paths, you can calculate the ass of each ball. The less deflection thee is, the heaie the ball ust be. In a siila way, a ass spectoete uses a agnetic field to deflect electically chaged paticles. Atos ae coneted into ions and then acceleated into a finely focused bea. Diffeent ions ae then deflected by the agnetic field by diffeent aounts, depending on the ass of the ion and its chage. Lighte ions ae deflected oe than heaie ones. Ions with oe positie chages ae deflected oe than ions with fewe positie chages. Only soe ions ake it all the way though the achine to the ion detecto, whee they ae detected electically. If you ay the agnetic field, diffeent types of ions will each the detecto. Scientists use the ass spectoete to identify unknown copounds, to deteine the stuctue of a copound, and to undestand the isotopic akeup of olecula eleents. The ass spectoete has applications in the edical field, the food industy, genetics, cabon dating, foensics, and space exploation. CAREER LINK NEL 8.4 Motion of Chaged Paticles in Magnetic Fields 397

2 Chages and Unifo Cicula Motion To undestand how a ass spectoete woks, we fist need to undestand how a diectional foce affects the otion of an object in this case, a chaged paticle. Conside the diection of a agnetic foce F > M and how this foce affects the otion of a chaged paticle. We know F M q sin u. Fo siplicity, we assue the agnetic field, >, is unifo, so the agnitude and diection of > ae the sae eeywhee. Figue 2(a) shows a chaged paticle, 1q, oing at elocity > paallel to the diection of >. In this case, the angle u between > and > is zeo. The facto sin u in F M q sin u is then zeo, so the agnetic foce in this case is also zeo. If a chaged paticle has a elocity paallel to >, the agnetic foce on the paticle is zeo. Figue 2(b) shows a chaged paticle oing pependicula to >. Now we hae u 908, and sin u 1. The agnitude of the agnetic foce is thus F M q, and the foce is pependicula to the elocity. F M q q (a) (b) Figue 2 (a) When the elocity of a chaged paticle is paallel to the agnetic field >, the agnetic foce on the paticle is zeo. (b) When > akes a ight angle with > (u 908), the chaged paticle oes in a cicle that lies in a plane pependicula to >. Recall that when a paticle expeiences a foce of constant agnitude pependicula to its elocity, the esult is cicula otion, as shown in Figue 2(b). Hence, if a chaged paticle is oing pependicula to a unifo agnetic field, the paticle will oe in a cicle. This cicle lies in the plane pependicula to the field lines. The adius of the cicle can be deteined fo Newton s second law and centipetal acceleation. Recall that fo a paticle to oe in a cicle of adius, thee ust be a foce of agnitude 2 diected towad the cente of the cicle. Hee, the foce poducing cicula otion is the agnetic foce, so we hae F M 2 The agnetic foce is pependicula to the elocity and sin 908 1, so we can inset F M q: q 2 Soling fo gies q Now calculate the alue of fo an electon that has a speed of /s oing in a agnetic field of stength T. Inseting these alues into the equation q and using 1 T 1 kg, we get C# s q kg2 a s b kg C2 a C # b s Chapte 8 Magnetic Fields NEL

3 This calculation shows that we can deteine the adius of a paticle s deflection if we know the ass of the paticle, its elocity, its chage, and the stength of the agnetic field though which it oes. Tutoial 1 Soling Pobles Related to Chaged Paticles in Cicula Motion in Magnetic Fields Saple Poble 1: An Electon in a Magnetic Field An electon stats fo est. A hoizontally diected electic field acceleates the electon though a potential diffeence of 37 V. The electon then leaes the electic field and oes into a agnetic field. The agnetic field stength is 0.26 T, diected into the page (Figue 3), and the ass of the electon is kg. Figue 3 y (a) Deteine the speed of the electon at the oent it entes the agnetic field. (b) Deteine the agnitude and diection of the agnetic foce on the electon. (c) Deteine the adius of the electon s cicula path. Solution (a) Gien: DV 37 V; e kg; q C Requied: i Analysis: The decease in the electon s electic potential enegy equals the incease in its kinetic enegy, -DE E DE k, whee 2DE E qdv and E k The speed of the electon befoe it entes the electic J field is zeo. Theefoe, DE k E kf. Use 1 V 1 C kg# and 2 1 J 1. s 2 Solution: 2DE E DE k qdv 1 2 i 2 i Å 2qDV Å C2 137 V kg kg # C2 a37 C # b s 2 ã kg i /s 1two exta digits caied2 Stateent: The initial speed of the electon at the oent it entes the agnetic field is /s. (b) Gien: 0.26 T; q C; u 908; i /s Requied: F M and its diection Analysis: Use F M q sin u to deteine the agnitude of the foce. Then use the ight-hand ule to deteine the diection. The agnetic foce will be the opposite of this diection because the chage is negatie. Solution: F M q sin u C2 a kg 6 b a0.26 s C # b 1 sin 9082 s F M N Apply the ight-hand ule fo an electic chage oing though a agnetic field: point the finges of you ight hand in the diection of the extenal agnetic field, into the page. Point you ight thub in the diection that the chage is oing, to the ight. You pal points in the diection of the agnetic foce fo a positie chage, up the page. The chage is negatie, so the agnetic foce is down the page. Stateent: The agnitude of the agnetic foce on the electon is N down the page. (c) Gien: e kg; 0.26 T; q C; /s Requied: Analysis: The only foce acting on the electon is the agnetic foce. This foce is pependicula to the electon s elocity, causing it to oe in unifo cicula otion. The agnetic foce is the centipetal foce, F c 2. Solution: F M F c q 2 1because sin q kg2 a s b C2 a0.26 kg C # b s Stateent: The adius of the electon s cicula path is NEL 8.4 Motion of Chaged Paticles in Magnetic Fields 399

4 Saple Poble 2: The Mass Spectoete: Identifying Paticles A eseache using a ass spectoete obsees a paticle taelling at /s in a cicula path of adius 8.2 c. The spectoete s agnetic field is pependicula to the paticle s path and has a agnitude of 0.41 T. (a) Calculate the ass-to-chage atio of the paticle. (In 1910, Robet Millikan accuately deteined the chage caied by an electon. His finding allowed eseaches to calculate the ass of chaged paticles using the ass-to-chage atio.) (b) Identify the paticle using Table 1. Table 1 Isotope (kg) q (C) Solution (a) Gien: /s; 8.2 c ; u 908; 0.41 T q (kg/c) hydogen deuteiu titiu Requied: q Analysis: The only foce acting on the electon is the agnetic foce, F M q sin u. This foce is pependicula to the electon s elocity, causing it to oe in unifo cicula otion. The agnetic foce is the centipetal foce, F c 2. Solution: F M F c q 2 q 1because sin a0.41 kg C# s b s q kg/c Stateent: The ass-to-chage atio of the paticle is kg/c. (b) Accoding to Table 1, the paticle is the isotope deuteiu. Saple Poble 3: The Mass Spectoete: Sepaating Isotopes A eseache uses a ass spectoete in a cabon dating expeient (Figue 4). The incoing ions ae a ixtue of 12 C 1 and 14 C 1, and they hae speed /s. The stength of the agnetic field is 0.10 T. The ass of the electon is kg. The ass of the poton and the ass of the neuton ae both kg. The eseache fist positions the ion detecto to deteine the alue of fo 12 C 1 and then oes it to deteine the alue of fo 14 C 1. How fa ust the detecto oe between detecting 12 C 1 and 14 C 1? incoing ions q ion detecto Figue 4 Gien: q C; e kg; p n kg; /s; 0.10 T Requied: Dd Analysis: Use the ass of the poton and the ass of the neuton to deteine the ass of each isotope. Then use the equation fo the adius of cuatue fo a paticle deflected in a agnetic field,. The detecto will hae to oe a q distance equal to twice the diffeence between the two adii. Solution: Deteine the ass of each isotope. C12 6 p 1 6 n 1 e kg kg kg2 C kg 1two exta digits caied2 C14 6 p 1 8 n 1 e kg kg kg2 C kg 1two exta digits caied2 Calculate the adius of cuatue of each paticle. C12 C12 q kg2 a s b C2 a0.10 kg C # b s C two exta digits caied2 400 Chapte 8 Magnetic Fields NEL

5 C14 C14 q kg2 a s b C2 a0.10 kg C # s b C two exta digits caied2 Calculate how fa the detecto ust oe. Dd 21 C14 2 C Dd 0.04 Stateent: The ion detecto ust oe a distance equal to the diffeence in the diaetes of the cicula tajectoies, so it ust oe a distance of Pactice 1. A heliu 21 ion with chage C and ass kg entes a unifo 2.4 T agnetic fi eld at a elocity of /s, at ight angles to the fi eld. Calculate the adius of the ion s path. T/i [ans: 0.13 ] 2. A poton with ass kg oes in a plane pependicula to a unifo 1. T agnetic fi eld in a cicle of adius 8.0 c. Calculate the poton s speed. T/i [ans: /s] 3. Conside a ass spectoete used to sepaate the two isotopes hydogen and deuteiu. The isotope hydogen has a poton, and deuteiu has a poton and a neuton. Assue both ions hae a 11 chage and they ente the agnetic fi eld egion with a speed of /s. Calculate the agnitude of the agnetic fi eld that is equied to gie a detecto placeent diffeence of 1. as easued fo the initial enty point into the spectoete copaed to when the ions leae the spectoete. T/i A [ans: 8.4 T] 4. The ainbidge-type ass spectoete uses a elocity selecto to select only those ions with the pope elocity. The selecto has two chaged paallel plates to ceate an electic fi eld pointing up, and coppe coils to ceate a agnetic fi eld. Positie ions pass though the selecto, with elocity diected to the ight (Figue ). T/i A (a) In which diection should the agnetic fi eld point in ode to balance the electic foce against the agnetic foce? (b) If the electic field has agnitude e, the agnetic field has agnitude, and the ion has chage q, deteine the pope elocity fo the ions to pass though the selecto without defl ection. (c) Pedict the paths of ions that hae too geat, and too sall, a elocity. Justify you answes. e Figue Mini inestigation Siulating a Mass Spectoete Mini inestigation Skills: Pefoing, Obseing, Analyzing, Counicating Equipent and Mateials: eye potection; 0 c wooden o plastic ap; ba agnet; 2 sall steel ball beaings of diffeent asses Wea closed-toed shoes fo this actiity. 1. Set up the ap at appoxiately a 48 angle. 2. Place the ba agnet on the leel suface at the ap s base. One pole of the agnet should be facing the botto of the ap. 3. Put on you eye potection. Roll a steel ball beaing down the ap, but not diectly at the agnet. SKILLS HANDOOK A Obsee the path of the ball.. Daw its tajectoy on a piece of pape. 6. Repeat Steps 3 to using a ball beaing with a diffeent ass. 7. Daw the new tajectoy next to the fi st one and note any diffeences. A. Copae this actiity to the function of a ass spectoete. How is it siila? K/U C. How is this actiity diffeent fo the function of a ass spectoete? K/U C NEL 8.4 Motion of Chaged Paticles in Magnetic Fields 401

6 Eath s Magnetic Field Chaged paticles taelling paallel to a agnetic field do not expeience a agnetic foce and continue oing along the field diection. Chaged paticles taelling pependicula to a agnetic field expeience a foce that keeps the oing in a cicula path. Chaged paticles with elocity coponents that ae both paallel and pependicula to a agnetic field expeience a cobination of these effects. The esult is a spial path that esebles the shape of a coil of wie. The paticle taels with a looping otion along the diection of the field (Figue 6). z q y x Figue 7 Eath s agnetic field deflects chaged paticles fo outside the atosphee. The paticles tael in spial paths along the field lines towad the agnetic poles. Figue 6 When the elocity of a chaged paticle has non-zeo coponents paallel and pependicula to the agnetic field, the paticle will oe along a spial path. Chaged paticles enteing Eath s agnetic field ae deflected in this way. Since they ae chaged paticles with a coponent of the elocity pependicula to the agnetic field, they will spial along the field lines towad the agnetic poles. This otion esults in a concentation of chaged paticles at Eath s noth and south agnetic poles (Figue 7). Collisions between the chaged paticles and atos in the atosphee elease light that causes the glow of the auoa boealis in the nothen heisphee and the auoa austalis in the southen heisphee (Figue 8). Eath s agnetic field Figue 8 The auoa austalis. The glow of the auoas occus when chaged paticles spial along Eath s agnetic field lines and collide with olecules in the atosphee aboe the pola egions. inne Van Allen belt oute Van Allen belt Figue 9 The Van Allen belts ae egions of chaged paticles and adiation tapped by Eath s agnetic field. At high altitudes in Eath s agnetic field ae zones of highly enegetic chaged paticles called the Van Allen adiation belts (Figue 9). Jaes A. Van Allen, an Aeican physicist, discoeed the tooidal (doughnut-shaped) zones of intense adiation while studying data fo a satellite he built in 198. Van Allen was able to show that chaged paticles fo cosic ays wee tapped in Eath s agnetic field. Most intense oe the equato, the Van Allen belts ae alost absent oe Eath s poles and consist of an inne egion and an oute egion. The oute Van Allen belt contains chaged paticles fo the atosphee and the Sun, ostly ions fo the sola wind. The inne Van Allen belt is a ing of highly enegetic potons. The concentation of chaged paticles and adiation can easily daage electonic equipent, so eseaches poga the paths and tajectoies of satellites and spacecaft to aoid the belts. 402 Chapte 8 Magnetic Fields NEL

7 Field Theoy We associate the te foce with a physical action of one object on anothe. When we talk about the foce of a bat against a baseball, ou inds use a concept of contact between the objects, which tansits the foce. To deelop a oe accuate concept of foce, we need to talk about it in tes of fields. We know that all objects ae ade of atos inteacting without actually touching each othe. Thee ae spatial gaps between the atos in a bat and a baseball, so the idea that the bat akes contact with the ball is deceptie. In eality, electoagnetic foces affect the inteacting atos in each object. How do we ceate an undestanding of the gaitational, electic, and agnetic foces? We need a scientific odel that descibes diffeent types of foces that exist at diffeent points in space, and field theoy does that. Field theoy is a scientific odel that descibes foces in tes of entities, called fields, that exist at eey point in space. The geneal idea of fields links diffeent kinds of foces once thought of as sepaate. Field theoy states that if an object expeiences a specific type of foce oe a continuous ange of positions in an aea, then a field exists in that aea. Field theoy can be applied in explaining the inute inteactions of subatoic paticles as well as descibing otions of galaxies thoughout the uniese. Studying gaitational, electic, and agnetic foces has eealed diffeences and siilaities between these foces and thei espectie fields. The electic and agnetic fields hae a stonge effect on the otion of subatoic paticles, such as potons and electons, but the gaitational field has a stonge effect on lage objects, such as planets, galaxies, and clustes of galaxies (Figue 10). field theoy a scientific odel that descibes foces in tes of entities that exist at eey point in space Figue 10 Gaity contols the collision of two clustes of galaxies, while electicity and agnetis affect the elease of adiation duing the collision. (Colous hae been added to the iage to enhance the isual epesentation.) The electic and gaitational foces eseble each othe in that the foce on an object depends on the location of the object. The agnetic foce, howee, depends on a chaged object s otion. The diection of electic and gaitational foces points fo the object towad the chage o ass souce. The diection of the agnetic foce depends on the otion of chaged paticles with espect to the agnetic field. Despite these siilaities and diffeences, field theoy states that electic and agnetic fields ae oe closely elated to one anothe than they ae to the gaitational field. In fact, the electic and agnetic fields ae thought to be diffeent aspects of a single field, the electoagnetic field. They ae used in conjunction with one anothe in a ultitude of innoatie technologies anging fo paticle acceleatos to atificial heats. NEL 8.4 Motion of Chaged Paticles in Magnetic Fields 403

8 8.4 Reiew Suay If a chaged paticle oes in a unifo agnetic field so that its initial elocity is paallel to the field, it will not expeience a agnetic foce. If it oes so that its initial elocity is pependicula to the field, it will oe in a cicula path in a plane pependicula to the agnetic field. If a chaged paticle oes in a unifo agnetic field with a elocity that is neithe paallel no pependicula to the field, it will oe in a spial path along the field lines. The adius of the cicula path a chaged paticle takes in a unifo agnetic field can be deteined fo Newton s second law and centipetal acceleation and is gien by, whee is the ass of the paticle, q q is its chage, is its speed, and is the agnitude of the agnetic field. Chaged paticles enteing Eath s agnetic field ae deflected and spial along the field lines towad the agnetic poles. This otion esults in a concentation of chaged paticles at Eath s noth and south agnetic poles. Field theoy states that if an object expeiences a specific type of foce oe a continuous ange of positions in an aea, then a field exists in that aea. Questions 1. Explain how a ass spectoete woks. Include a sketch as pat of you answe. K/U C 2. Conside a ass spectoete used to sepaate the two isotopes of uaniu, 238 U 31 ( kg) and 23 U 31 ( kg). Assue the ions ente the agnetic field egion of stength 9. T with identical speeds and leae the spectoete with a sepaation of 2.2 (as easued fo the enty point) afte copleting a half-cicle tun. Calculate the initial speed of the ions. T/I 3. An electon oes in a cicula path pependicula to a agnetic field of agnitude T. The kinetic enegy of the electon is J. Calculate the adius of the electon s path. Refe to Appendix fo the ass of the electon. T/I 4. A paticle caies a chage of C. When it oes with elocity /s [E 48 N], a unifo agnetic field exets a foce diectly upwad. When the paticle oes with a elocity of /s diectly upwad, thee is a foce of N [W] exeted on it. What ae the agnitude and diection of the agnetic field? T/I. An electon, afte being acceleated though a potential diffeence of V, entes a unifo agnetic field of T pependicula to its diection of otion. Calculate the adius of the path descibed by the electon. T/I 6. A elocity selecto is a deice that can choose the elocity of a chaged paticle oing though a egion in which the electic field is pependicula to the agnetic field, and with both fields pependicula to the initial elocity of the paticle (Figue 11). To ake the chaged paticle tael staight though the paallel plates, the downwad deflection due to the electic field ust equal the upwad deflection due to the agnetic field. Suppose you want to design a elocity selecto that will allow potons to pass though, undeflected, only if they hae a speed of /s. T/I A e i P elocity selecto Figue 11 (a) The agnetic field is 0.00 T. Calculate the electic field you need. (b) What is the adius of the path the poton takes to get to point P? Refe to Appendix fo the ass of the poton. 404 Chapte 8 Magnetic Fields NEL

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

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

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

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

10. Collisions. Before During After

10. Collisions. Before During After 10. Collisions Use conseation of momentum and enegy and the cente of mass to undestand collisions between two objects. Duing a collision, two o moe objects exet a foce on one anothe fo a shot time: -F(t)

More information

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

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

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

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

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

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

(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

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

Worked Examples. v max =?

Worked Examples. v max =? Exaple iction + Unifo Cicula Motion Cicula Hill A ca i diing oe a ei-cicula hill of adiu. What i the fatet the ca can die oe the top of the hill without it tie lifting off of the gound? ax? (1) Copehend

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

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

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

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

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

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

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

Pearson Physics Level 30 Unit VI Forces and Fields: Chapter 10 Solutions

Pearson Physics Level 30 Unit VI Forces and Fields: Chapter 10 Solutions Peason Physics Level 30 Unit VI Foces and Fields: hapte 10 Solutions Student Book page 518 oncept heck 1. It is easie fo ebonite to eove electons fo fu than fo silk.. Ebonite acquies a negative chage when

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

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

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

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

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

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

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

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

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

Phys 2101 Gabriela González. cos. sin. sin

Phys 2101 Gabriela González. cos. sin. sin 1 Phys 101 Gabiela González a m t t ma ma m m T α φ ω φ sin cos α τ α φ τ sin m m α τ I We know all of that aleady!! 3 The figue shows the massive shield doo at a neuton test facility at Lawence Livemoe

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

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

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

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

9.5 Amortization. Objectives

9.5 Amortization. Objectives 9.5 Aotization Objectives 1. Calculate the payent to pay off an aotized loan. 2. Constuct an aotization schedule. 3. Find the pesent value of an annuity. 4. Calculate the unpaid balance on a loan. Congatulations!

More information

NUCLEAR MAGNETIC RESONANCE

NUCLEAR MAGNETIC RESONANCE 19 Jul 04 NMR.1 NUCLEAR MAGNETIC RESONANCE In this expeiment the phenomenon of nuclea magnetic esonance will be used as the basis fo a method to accuately measue magnetic field stength, and to study magnetic

More information

Chapter 2. Electrostatics

Chapter 2. Electrostatics Chapte. Electostatics.. The Electostatic Field To calculate the foce exeted by some electic chages,,, 3,... (the souce chages) on anothe chage Q (the test chage) we can use the pinciple of supeposition.

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

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

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

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

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

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

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

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

(d) False. The orbital period of a planet is independent of the planet s mass.

(d) False. The orbital period of a planet is independent of the planet s mass. Chapte Gaity Conceptual Pobles [SS] ue o false: (a) o Keple s law of equal aeas to be alid, the foce of aity ust ay inesely with the squae of the distance between a ien planet and the Sun. (b) he planet

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

A r. (Can you see that this just gives the formula we had above?)

A r. (Can you see that this just gives the formula we had above?) 24-1 (SJP, Phys 1120) lectic flux, and Gauss' law Finding the lectic field due to a bunch of chages is KY! Once you know, you know the foce on any chage you put down - you can pedict (o contol) motion

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

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

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

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

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

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

Strength Analysis and Optimization Design about the key parts of the Robot

Strength Analysis and Optimization Design about the key parts of the Robot Intenational Jounal of Reseach in Engineeing and Science (IJRES) ISSN (Online): 2320-9364, ISSN (Pint): 2320-9356 www.ijes.og Volume 3 Issue 3 ǁ Mach 2015 ǁ PP.25-29 Stength Analysis and Optimization Design

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

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

Model Question Paper Mathematics Class XII

Model Question Paper Mathematics Class XII Model Question Pape Mathematics Class XII Time Allowed : 3 hous Maks: 100 Ma: Geneal Instuctions (i) The question pape consists of thee pats A, B and C. Each question of each pat is compulsoy. (ii) Pat

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

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

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

Chapter 19: Electric Charges, Forces, and Fields ( ) ( 6 )( 6

Chapter 19: Electric Charges, Forces, and Fields ( ) ( 6 )( 6 Chapte 9 lectic Chages, Foces, an Fiels 6 9. One in a million (0 ) ogen molecules in a containe has lost an electon. We assume that the lost electons have been emove fom the gas altogethe. Fin the numbe

More information

and that of the outgoing water is mv f

and that of the outgoing water is mv f Week 6 hoework IMPORTANT NOTE ABOUT WEBASSIGN: In the WebAssign ersions of these probles, arious details hae been changed, so that the answers will coe out differently. The ethod to find the solution is

More information

Fluids Lecture 15 Notes

Fluids Lecture 15 Notes Fluids Lectue 15 Notes 1. Unifom flow, Souces, Sinks, Doublets Reading: Andeson 3.9 3.12 Unifom Flow Definition A unifom flow consists of a velocit field whee V = uî + vĵ is a constant. In 2-D, this velocit

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

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

Electrostatic properties of conductors and dielectrics

Electrostatic properties of conductors and dielectrics Unit Electostatic popeties of conductos and dielectics. Intoduction. Dielectic beaking. onducto in electostatic equilibium..3 Gound connection.4 Phenomena of electostatic influence. Electostatic shields.5

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

Uniform Rectilinear Motion

Uniform Rectilinear Motion Engineeing Mechanics : Dynamics Unifom Rectilinea Motion Fo paticle in unifom ectilinea motion, the acceleation is zeo and the elocity is constant. d d t constant t t 11-1 Engineeing Mechanics : Dynamics

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

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

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

Chapter 13 Fluids. Use the definition of density to express the mass of the gold sphere: The mass of the copper sphere is given by:

Chapter 13 Fluids. Use the definition of density to express the mass of the gold sphere: The mass of the copper sphere is given by: Chapte Fluid 5 One phee i ade of gold and ha a adiu and anothe phee i ade of coppe and ha a adiu. f the phee have equal a, hat i the atio of the adii, /? ictue the oble We can ue the definition of denity

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

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

Moment and couple. In 3-D, because the determination of the distance can be tedious, a vector approach becomes advantageous. r r

Moment and couple. In 3-D, because the determination of the distance can be tedious, a vector approach becomes advantageous. r r Moment and couple In 3-D, because the detemination of the distance can be tedious, a vecto appoach becomes advantageous. o k j i M k j i M o ) ( ) ( ) ( + + M o M + + + + M M + O A Moment about an abita

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

4a 4ab b 4 2 4 2 5 5 16 40 25. 5.6 10 6 (count number of places from first non-zero digit to

4a 4ab b 4 2 4 2 5 5 16 40 25. 5.6 10 6 (count number of places from first non-zero digit to . Simplify: 0 4 ( 8) 0 64 ( 8) 0 ( 8) = (Ode of opeations fom left to ight: Paenthesis, Exponents, Multiplication, Division, Addition Subtaction). Simplify: (a 4) + (a ) (a+) = a 4 + a 0 a = a 7. Evaluate

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

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

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

Lesson 8 Ampère s Law and Differential Operators

Lesson 8 Ampère s Law and Differential Operators Lesson 8 Ampèe s Law and Diffeential Opeatos Lawence Rees 7 You ma make a single cop of this document fo pesonal use without witten pemission 8 Intoduction Thee ae significant diffeences between the electic

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

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

Lab M4: The Torsional Pendulum and Moment of Inertia

Lab M4: The Torsional Pendulum and Moment of Inertia M4.1 Lab M4: The Tosional Pendulum and Moment of netia ntoduction A tosional pendulum, o tosional oscillato, consists of a disk-like mass suspended fom a thin od o wie. When the mass is twisted about the

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

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

PY106 Class13. Permanent Magnets. Magnetic Fields and Forces on Moving Charges. Interactions between magnetic north and south poles.

PY106 Class13. Permanent Magnets. Magnetic Fields and Forces on Moving Charges. Interactions between magnetic north and south poles. Permanent Magnets Magnetic ields and orces on Moing Charges 1 We encounter magnetic fields frequently in daily life from those due to a permanent magnet. Each permanent magnet has a north pole and a south

More information

Newton s Law of Universal Gravitation and the Scale Principle

Newton s Law of Universal Gravitation and the Scale Principle Newton s Law of Univesal avitation and the ale iniple RODOLO A. RINO July 0 Eletonis Enginee Degee fo the National Univesity of Ma del lata - Agentina (odolfo_fino@yahoo.o.a) Ealie this yea I wote a pape

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

GAUSS S LAW APPLIED TO CYLINDRICAL AND PLANAR CHARGE DISTRIBUTIONS ` E MISN-0-133. CHARGE DISTRIBUTIONS by Peter Signell, Michigan State University

GAUSS S LAW APPLIED TO CYLINDRICAL AND PLANAR CHARGE DISTRIBUTIONS ` E MISN-0-133. CHARGE DISTRIBUTIONS by Peter Signell, Michigan State University MISN-0-133 GAUSS S LAW APPLIED TO CYLINDRICAL AND PLANAR CHARGE DISTRIBUTIONS GAUSS S LAW APPLIED TO CYLINDRICAL AND PLANAR CHARGE DISTRIBUTIONS by Pete Signell, Michigan State Univesity 1. Intoduction..............................................

More information

Graphs of Equations. A coordinate system is a way to graphically show the relationship between 2 quantities.

Graphs of Equations. A coordinate system is a way to graphically show the relationship between 2 quantities. Gaphs of Equations CHAT Pe-Calculus A coodinate sstem is a wa to gaphicall show the elationship between quantities. Definition: A solution of an equation in two vaiables and is an odeed pai (a, b) such

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

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

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

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