7.2. Coulomb s Law. The Electric Force

Size: px
Start display at page:

Download "7.2. Coulomb s Law. The Electric Force"

Transcription

1 Coulomb s aw Recall that chaged objects attact some objects and epel othes at a distance, without making any contact with those objects Electic foce,, o the foce acting between two chaged objects, is somewhat simila to gavity Both ae non-contact foces Simila to the foce of gavity, the electic foce becomes weake as the distance,, between the chaged objects inceases (Figue 1) Electic foce becomes stonge as the amount of chage on eithe object inceases, in the same way that the foce of gavity becomes stonge with an incease in mass of eithe object In this section, you will lean moe about how the electic foce depends on chage and distance You will also lean how to solve poblems elated to the electic foce 7 electic foce ( ) a foce with magnitude and diection that acts between two chaged paticles (a) 1 4 F 1 E 4 (b) Figue 1 The electic foce of epulsion between two identical chages deceases as the sepaation inceases The Electic Foce If you dop a tennis ball, the foce of gavity is esponsible fo its fall The tennis ball will take appoimately 1 s to fall fom a height of m How long do you think the tennis ball will take to stop as it hits the gound? It will take a lot less time to stop than it took to fall What foce is esponsible fo making the tennis ball stop? The electic foce of epulsion between the potons in the tennis ball and the potons in the gound stop it This electic foce must be significantly stonge than gavity Conside two chaged objects so tiny that you can model them as point paticles These objects have chages and and ae sepaated by a distance (Figue ) The magnitude of the electic foce between and is epessed by the euation Figue The electic foce between two point chages and is given by Coulomb s law k This euation epesents Coulomb s law Coulomb s aw The foce between two point chages is invesely popotional to the suae of the distance between the chages and diectly popotional to the poduct of the chages The constant k, which is sometimes called Coulomb s constant, has the value k N# m /C Do not confuse this constant k with the sping constant in Hooke s law Most physicists use the same symbol fo both The diection of the electic foce on each of the chages is along the line that connects the two chages, as illustated in Figue fo the case of two like chages As mentioned ealie, this foce is epulsive fo two chages with the same type of chage Stictly speaking, the value of in the euation fo Coulomb s law applies only to two point chages Howeve, it is a good appoimation wheneve the sizes of the paticles ae much smalle than thei distance of sepaation Coulomb s constant (k) the popotionality constant in Coulomb s law; k N# m /C NE 7 Coulomb s aw 37

2 Investigation 71 Coulomb s aw (page 366) Now that you have leaned how to calculate the electic foce between two chages with a given sepaation, pefom Investigation 71 to detemine how electic foce vaies with distance and 1 You will use this infomation with two diffeent chage values to detemine Coulomb s law Coulomb s law has seveal impotant popeties: You have aleady seen that the electic foce is epulsive fo like chages and attactive fo unlike chages Mathematically, this popety esults fom the poduct in the numeato of the Coulomb s law euation The magnitude of the electic foce,, is always positive In physics, it is convenient to use a negative sign to show diection Including the negative sign of a negatively chaged object would imply a diection You neve include the sign of the chage when solving poblems elated to Coulomb s law The electic foce is invesely popotional to the suae of the distance between the two paticles The magnitude of the electic foce is the magnitude of the foce eeted on each of the paticles That is, a foce of magnitude is eeted on chage by chage, and a foce of eual magnitude and opposite diection is eeted on by This paiing of eual but opposite foces is descibed by Newton s thid law, the action eaction pinciple Using the euation fo Coulomb s law, we can show that electic foces can be etemely lage Suppose you have two boes of electons, each with a total chage of T C sepaated by a distance of 10 m Fo simplicity, assume that each bo is so small that it can be modelled as a point paticle The magnitude of the total electic foce is k a N # m N C b C C 110 m This is an etemely lage foce, all fom just two small containes of electons Note that the negative sign fo chage was not included Why, then, does the electic foce not dominate eveyday life? The fact is that it is essentially impossible to obtain a bo containing only electons Recall foalie science studies that a neutal atom contains eual numbes of electons and potons If ou two point-like boes had contained eual numbes of electons and potons, thei total chages, T, would have been zeo, and so would the foce calculated using Coulomb s law Odinay matte consists of eual, o nealy eual, numbes of electons and potons The total chage is theefoe eithe zeo o vey close to zeo At the atomic and molecula scales, howeve, it is common to have the positive and negative chages (nuclei and electons) sepaated by a small distance In this case, the electic foce is not zeo, and these electic foces hold matte togethe Compaing Coulomb s aw and Univesal Gavitation The euation fo Coulomb s law may seem familia to you, even though you have only just leaned it This is because it is simila to the univesal law of gavitation, which you leaned in Chapte 6 Both of these laws descibe the foce between two objects In addition, both depend on cetain popeties of the objects involved Fo gavitation, this popety is mass Fo the electic foce, this popety is electic chage Both mass and chage can be consideed to be concentated at a cental point If you think of the mass o chage as a solid sphee, you can teat this same mass o chage as if it wee a point at the cente of that sphee Anothe similaity between the two laws is that both the gavitational foce and the electic foce decease as the distance between the two inteacting objects inceases If the distance between the objects is geat (compaed to the size of eithe object), the actual size and shape of the objects involved become mathematically ielevant The theoetical mass and chage at the cente point of each object ae then used in calculations 38 Chapte 7 Electic Fields NE

3 Although thee ae similaities between electic and gavitational foces, thee ae also impotant diffeences Gavitational foces ae always attactive The diection of electic foces depends on the types of chage: unlike chages attact, and like chages epel Also, the magnitude of the electic foce is much geate than the magnitude of the gavitational foce ove the same distance The Supeposition Pinciple So fa, you have leaned about the electic foce between two point paticles Now conside how to use Coulomb s law with moe than two chages Suppose you have thee paticles One paticle has a chage of The second paticle has a chage of and is a distance fom the fist paticle, as shown in Figue 3 What is the electic foce on a thid chage,, placed midway between these two chages? Solve this poblem by fist using Coulomb s law to calculate the foce eeted by chage on Then use Coulomb s law a second time to calculate the foce eeted by the chage on The total foce on euals the vecto sum of these two sepaate contibutions This combining of two foces is an eample of the supeposition pinciple The supeposition pinciple says that the total foce acting on is the sum, o supeposition, of the individual foces eeted on by all the othe chages in the poblem Remembe that foce is a vecto, so be caeful to add these foces as vectos This means that, fo chages not on a staight line, the solution euies some tigonomety involving tiangles o the use of vecto components When all chages lie in a staight line, the supeposition pinciple simplifies so that you can add o subtact the vaious individual foces to o fom one anothe to obtain the esultant, o net, foce As shown in Figue 3, the sepaation between and is Coulomb s law fo this pai of chages is theefoe FE1 Figue 3 The total foce on euals the sum of the foces fom chages and supeposition pinciple the esultant, o net, vecto acting at a given point euals the sum of the individual vectos fom all souces, each calculated at the given point k Using the coodinate system in Figue 3, this coesponds to a foce on by in the positive -diection because like chages epel So, is the component of the foce along the positive -ais The chages line up along the -ais, so the component of the foce along the y-ais is zeo Now conside the foce on by the chage in a simila way The sepaation of the chages is again, so, using the euation fo Coulomb s law, you get k 1 k Fom Figue 3 you can see that this coesponds to the foce on by in the negative -diection, again because like chages epel This is because the electic foce acts along the line connecting the two chages, which in this case is the -ais Fo this eason, the component of the foce along the y-ais is again zeo So, the foce eeted by on is in the negative -diection, o to the left The total foce on is the sum of the two electic foces, and Be caeful to take diection into account fo the calculation In this case, the sign of each foce indicates its diection F > E net F > E 1 1 F > E 1 k k F > E net k The negative sign means that, fo the positive poduct, the foce eeted on is along the negative -diection NE 7 Coulomb s aw 39

4 Tutoial 1 Using Coulomb s aw This Tutoial shows how to use Coulomb s law to solve chage distibution poblems in both one and two dimensions Sample Poblem 1: Applying Coulomb s aw in One Dimension An ealy model of the hydogen atom depicted the electon evolving aound the poton, much like Eath evolving aound the Sun The poton and electon both have mass, so they eet a gavitational foce upon each othe They also have chage, so they eet an electic foce on each othe (a) The distance between the electon and the poton in a hydogen atom is m, the chage of each is C, the mass of the electon is kg, and the mass of the poton is kg Calculate the atio of the electic foce to the gavitational foce F g (b) Detemine the acceleations of the electon caused by both the electic foce and the gavitational foce Solution (a) Given: m; C; kg; m p kg; k Nm /C ; G Nm /kg Reuied: F g Analysis: Use Coulomb s law to calculate, and use the euation fo univesal gavitation to calculate F g F g Gm p and F E k e p, whee e p Fom these esults, calculate F g Solution: k e p a N # m C b C m N 1two eta digits caied The euation fo Coulomb s law is moe accuately epesented by 0F > E 0 k Hee, the vetical bas suounding the electic foce vecto, 0F > E0, epesent the magnitude of the electic foce, and the vetical bas suounding the chages and, and, epesent the absolute values of the electic chages This epesentation is moe accuate because the magnitude of the electic foce is a stictly positive uantity If you just use the euation k, you will get a negative value fo the magnitude of the electic foce when one of the chages is negative The absolute value bas keep the values of the chages positive Howeve, many people find the moe accuate vesion of the euation cumbesome and confusing and pefe to use k This is what we will do when solving poblems Always emembe to dop the negative signs on chages when using this euation The following Tutoial will give you some pactice in solving poblems using Coulomb s law F g Gm p a N # m 11 kg b kg kg m F g N 1two eta digits caied N F g N F g Statement: The electic foce between the electon and the poton of a hydogen atom is times the gavitational foce F g between these same paticles (b) Given: kg; F g N; N Reuied: a E ; a g Analysis: Use the euation fo electic foce to calculate a E using and ikewise, use the euation fo gavitational foce to calculate a g using the values of F g and a E and a g F g Use 1 N 1 kg# m/s Solution: a E kg # m s kg a E m/s 330 Chapte 7 Electic Fields NE

5 a g F g kg # m s kg a g m/s Statement: The acceleation of the electon caused by the electic foce of the poton is m/s, and the acceleation of the electon caused by the gavitational foce is m/s Sample Poblem : Detemining Electostatic Euilibium Two chages, C and C, ae sepaated by a distance,, of 400 m A thid chage, C, is placed somewhee between and, as shown in Figue 4, whee the net foce eeted on 3 by the othe two chages is zeo Detemine the location of 3 3 Figue 4 Given: 400 m; C; C; C; k Nm /C Reuied:, the location of 3 Analysis: Use the supeposition pinciple, and use the euation fo Coulomb s law to calculate the foces eeted on 3 by and eeted on 3 by The foce euations ae k 3 and F E k 3 1 Since the net foce on 3 is zeo, 0, o Solution: k 3 k 3 1 Divide both sides of the euation by the common tems k and 3, and then simplify Substitute the values fo,, and into the euation, noting that is in metes with thee significant digits Solve fo C C C a C C b o Distance is always a positive uantity, so 1 Statement: The location of 3, such that the electic foces fom and cancel, is 100 m, o 100 m to the ight of Sample Poblem 3: Applying Coulomb s aw in Two Dimensions Two point paticles have eual but opposite chages of 1 and The paticles ae aanged as shown in Figue Suppose a chage is placed on the -ais as shown C, C, and the distance between 1 and is 80 m measued vetically along the y-ais Calculate the magnitude and the diection of the net electic foce on Given: C; C; C; k Nm /C Reuied: net electic foce on Analysis: As shown in Figue, thee ae symmetical ight tiangles above and below the -ais, so we can use the Pythagoean theoem to calculate (the distance sepaating 1 and ) Then use to calculate the electic foce between 1 and and that between and Use tigonomety to calculate the hoizontal and vetical components of these two foces to detemine the magnitude and diection of the net electic foce Use Coulomb s law to calculate the foce between the chages 40 m 40 m y 30 m Figue NE 7 Coulomb s aw 331

6 Solution: Fist, calculate the magnitudes of the electic foces along the hoizontal and vetical diections Both of the foces along the -ais act on the left side of the chage, so the net hoizontal foce is the sum of the two hoizontal foce components Use the Pythagoean theoem to calculate, the distance between 1 and, and that between and "140 m m 0 m Calculate the foce of 1 on, k a N # m 9 b C C C 10 m N 1two eta digits caied The foce between a positive chage and anothe positive chage is epulsion, so this foce is diected towad along the line connecting 1 and Calculate the foce of on, Since the magnitude of is the same as that of 1, the magnitude of is the same as that of N 1two eta digits caied The foce between a negative chage and a positive chage is attaction, so this foce is diected away fom along the line connecting and Now calculate the -component of, 1 et u be the angle that makes with the -ais 1 cos u 1 cos u N a 30 m 0 m b N 1two eta digits caied is diected towad, so 1 is diected towad along the positive -diection By symmety, the -component of,, must have the same magnitude as the -component of and is diected away fom along the negative -diection N 1two eta digits caied Detemine the vecto sum of the two hoizontal foce components F > E net F > E 1 1 F > E N N F > E net 0 N Thee is no net foce on along the -diection Now calculate the y-component of, y1 y1 sin u y1 sin u N a 40 m 0 m b y N 1two eta digits caied is diected towad fom 1, so y1 is diected towad downwad Since, the y-component of, y, has the same magnitude as the y-component of, y1 y y1 y N 1two eta digits caied is diected away fom fom, so y is also diected downwad Detemine the vecto sum of the two vetical foce components Choose upwad as positive, so downwad is negative F > Ey net F > Ey 1 1 F > Ey N N F > Ey net N Statement: The net electic foce acting on is N [down] Pactice 1 Detemine the magnitude of the electic foce between two chages of C and C that ae sepaated by a distance of 00 m T/I [ans: N] Two paticles of chage and (with positive) ae located as shown in Figue 6 A thid chage 3 is placed on the -ais to the left of The total electic foce on 3 is zeo The chages ae sepaated by 1000 m Detemine whee 3 must be located K/U T/I [ans: 414 m [left of ]] 1000 m Figue 6 3 Thee point chages ae placed at the following points on the -ais: 10 mc at 0, 30 mc at 400 cm, and 0 mc at 100 cm Detemine the foce on the 30 mc chage T/I [ans: 0 N towad the negative -diection, o 0 N [left]] 33 Chapte 7 Electic Fields NE

7 7 Review Summay Accoding to Coulomb s law, the foce between two point chages is diectly popotional to the poduct of the chages and invesely popotional to the suae of the distance between the chages, given as k Coulomb s constant, k, is eual to N m /C Coulomb s law applies to point chages and to chages that can be concentated euivalently in points located at the cente, when the sizes of the chages ae much smalle than thei distance of sepaation Thee ae similaities between the electic foce and the gavitational foce The supeposition pinciple states that the total foce acting on a chage is the vecto sum, o supeposition, of the individual foces eeted on by all the othe chages in the poblem Questions 1 Two chaged objects have a epulsive foce of 0080 N The distance sepaating the two objects is tipled Detemine the new foce T/I Two chaged objects have an attactive foce of 0080 N Suppose that the chage of one of the objects is tipled and the distance sepaating the objects is tipled Calculate the new foce T/I 3 Detemine the magnitude of the electic foce between two electons sepaated by a distance of 010 nm (appoimately the diamete of an atom) K/U T/I 4 Two point chages ae sepaated by a distance Detemine the facto by which the electic foce between them changes when the sepaation is educed by a facto of 10 K/U T/I Detemine the distance of sepaation euied fo two 100 µc chages to be positioned so that the epulsive foce between them is euivalent to the weight (on Eath) of a 100 kg mass T/I 6 Conside an electon and a poton sepaated by a distance of 10 nm K/U T/I (a) Calculate the magnitude of the gavitational foce between them (b) Calculate the magnitude of the electic foce between them (c) Eplain how the atio of these gavitational and electic foces would change if the distance wee inceased to 10 m 7 Paticles of chage and 3 ae placed on the -ais at 40 and 0, espectively A thid paticle of chage is placed on the -ais, and the total electic foce on this paticle is zeo Detemine the position of the paticle K/U T/I 8 Two chages of C and C ae placed at a sepaation of 10 cm Detemine whee a thid chage should be placed on the line connecting the two chages so that it epeiences no net foce due to these two chages K/U T/I A 9 Thee chages with C ae located as shown in Figue 7, with cm Detemine the magnitude and diection of the total electic foce on each paticle listed below T/I Figue 7 y (a) the chage at the bottom (b) the chage on the ight (c) an electon placed at the oigin 10 Two pith balls, each with a mass of 00 g, ae attached to non-conducting theads and suspended fom the same point on the ceiling Each thead has a length of 100 m The balls ae then given an identical chage, which causes them to sepaate At the point that the electic and gavitational foces balance, the theads ae sepaated by an angle of 300 Calculate the chage on each pith ball K/U A NE 7 Coulomb s aw 333

AP Physics - Coulomb's Law

AP Physics - Coulomb's Law AP Physics - oulomb's Law We ve leaned that electons have a minus one chage and potons have a positive one chage. This plus and minus one business doesn t wok vey well when we go in and ty to do the old

More information

The Millikan Experiment: Determining the Elementary Charge

The Millikan Experiment: Determining the Elementary Charge LAB EXERCISE 7.5.1 7.5 The Elementay Chage (p. 374) Can you think of a method that could be used to suggest that an elementay chage exists? Figue 1 Robet Millikan (1868 1953) m + q V b The Millikan Expeiment:

More information

Physics 107 TUTORIAL ASSIGNMENT #8

Physics 107 TUTORIAL ASSIGNMENT #8 Physics 07 TUTORIAL ASSIGNMENT #8 Cutnell & Johnson, 7 th edition Chapte 8: Poblems 5,, 3, 39, 76 Chapte 9: Poblems 9, 0, 4, 5, 6 Chapte 8 5 Inteactive Solution 8.5 povides a model fo solving this type

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

Objects usually are charged up through the transfer of electrons from one object to the other.

Objects usually are charged up through the transfer of electrons from one object to the other. 1 Pat 1: Electic Foce 1.1: Review of Vectos Review you vectos! You should know how to convet fom pola fom to component fom and vice vesa add and subtact vectos multiply vectos by scalas Find the esultant

More information

Electric Forces: Coulomb s Law

Electric Forces: Coulomb s Law Electic Foces: Coulomb s Law All the matte aound you contains chaged paticles, and it is the electic foces between these chaged paticles that detemine the stength of the mateials and the popeties of the

More information

CHAPTER 25 ELECTRIC POTENTIAL

CHAPTER 25 ELECTRIC POTENTIAL CHPTE 5 ELECTIC POTENTIL Potential Diffeence and Electic Potential Conside a chaged paticle of chage in a egion of an electic field E. This filed exets an electic foce on the paticle given by F=E. When

More information

Electrostatics (Electric Charges and Field) #2 2010

Electrostatics (Electric Charges and Field) #2 2010 Electic Field: The concept of electic field explains the action at a distance foce between two chaged paticles. Evey chage poduces a field aound it so that any othe chaged paticle expeiences a foce when

More information

Chapter Sixteen: Electric Charge and Electric Fields

Chapter Sixteen: Electric Charge and Electric Fields Chapte Sixteen: Electic Chage and Electic Fields Key Tems Chage Conducto The fundamental electical popety to which the mutual attactions o epulsions between electons and potons ae attibuted. Any mateial

More information

Physics 11 Chapter 20: Electric Fields and Forces

Physics 11 Chapter 20: Electric Fields and Forces Physics Chapte 0: Electic Fields and Foces Yesteday is not ous to ecove, but tomoow is ous to win o lose. Lyndon B. Johnson When I am anxious it is because I am living in the futue. When I am depessed

More information

Electric Charge and Field

Electric Charge and Field lectic Chage and ield Chapte 6 (Giancoli) All sections ecept 6.0 (Gauss s law) Compaison between the lectic and the Gavitational foces Both have long ange, The electic chage of an object plas the same

More information

Physics Electrostatics: Coulomb s Law

Physics Electrostatics: Coulomb s Law A C U L T Y O E D U C A T I O N Depatment of Cuiculum and Pedagogy Physics Electostatics: Coulomb s Law Science and Mathematics Education Reseach Goup Suppoted by UBC Teaching and Leaning Enhancement und

More information

20-9 ELECTRIC FIELD LINES 20-9 ELECTRIC POTENTIAL. Answers to the Conceptual Questions. Chapter 20 Electricity 241

20-9 ELECTRIC FIELD LINES 20-9 ELECTRIC POTENTIAL. Answers to the Conceptual Questions. Chapter 20 Electricity 241 Chapte 0 Electicity 41 0-9 ELECTRIC IELD LINES Goals Illustate the concept of electic field lines. Content The electic field can be symbolized by lines of foce thoughout space. The electic field is stonge

More information

Extra notes for circular motion: Circular motion : v keeps changing, maybe both speed and

Extra notes for circular motion: Circular motion : v keeps changing, maybe both speed and Exta notes fo cicula motion: Cicula motion : v keeps changing, maybe both speed and diection ae changing. At least v diection is changing. Hence a 0. Acceleation NEEDED to stay on cicula obit: a cp v /,

More information

ELECTRIC CHARGE AND ELECTRIC FIELD

ELECTRIC CHARGE AND ELECTRIC FIELD LCTRIC CHARG AND LCTRIC FILD (a) IDNTIFY and ST UP: Use the chage of one electon ( 6 C) to find the numbe of electons euied to poduce the net chage XCUT: The numbe of ecess electons needed to poduce net

More information

Physics 2B Chapter 22 Notes - Magnetic Field Spring 2018

Physics 2B Chapter 22 Notes - Magnetic Field Spring 2018 Physics B Chapte Notes - Magnetic Field Sping 018 Magnetic Field fom a Long Staight Cuent-Caying Wie In Chapte 11 we looked at Isaac Newton s Law of Gavitation, which established that a gavitational field

More information

OSCILLATIONS AND GRAVITATION

OSCILLATIONS AND GRAVITATION 1. SIMPLE HARMONIC MOTION Simple hamonic motion is any motion that is equivalent to a single component of unifom cicula motion. In this situation the velocity is always geatest in the middle of the motion,

More information

Physics 2212 GH Quiz #2 Solutions Spring 2016

Physics 2212 GH Quiz #2 Solutions Spring 2016 Physics 2212 GH Quiz #2 Solutions Sping 216 I. 17 points) Thee point chages, each caying a chage Q = +6. nc, ae placed on an equilateal tiangle of side length = 3. mm. An additional point chage, caying

More information

Chapter 13 Gravitation

Chapter 13 Gravitation Chapte 13 Gavitation In this chapte we will exploe the following topics: -Newton s law of gavitation, which descibes the attactive foce between two point masses and its application to extended objects

More information

Chapter 4. Newton s Laws of Motion

Chapter 4. Newton s Laws of Motion Chapte 4 Newton s Laws of Motion 4.1 Foces and Inteactions A foce is a push o a pull. It is that which causes an object to acceleate. The unit of foce in the metic system is the Newton. Foce is a vecto

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

Electric Field. y s +q. Point charge: Uniformly charged sphere: Dipole: for r>>s :! ! E = 1. q 1 r 2 ˆr. E sphere. at <0,r,0> at <0,0,r>

Electric Field. y s +q. Point charge: Uniformly charged sphere: Dipole: for r>>s :! ! E = 1. q 1 r 2 ˆr. E sphere. at <0,r,0> at <0,0,r> Electic Field Point chage: E " ˆ Unifomly chaged sphee: E sphee E sphee " Q ˆ fo >R (outside) fo >s : E " s 3,, at z y s + x Dipole moment: p s E E s "#,, 3 s "#,, 3 at

More information

Electricity Revision ELECTRICITY REVISION KEY CONCEPTS TERMINOLOGY & DEFINITION. Physical Sciences X-Sheets

Electricity Revision ELECTRICITY REVISION KEY CONCEPTS TERMINOLOGY & DEFINITION. Physical Sciences X-Sheets Electicity Revision KEY CONCEPTS In this session we will focus on the following: Stating and apply Coulomb s Law. Defining electical field stength and applying the deived equations. Dawing electical field

More information

Objectives: After finishing this unit you should be able to:

Objectives: After finishing this unit you should be able to: lectic Field 7 Objectives: Afte finishing this unit you should be able to: Define the electic field and explain what detemines its magnitude and diection. Wite and apply fomulas fo the electic field intensity

More information

21 MAGNETIC FORCES AND MAGNETIC FIELDS

21 MAGNETIC FORCES AND MAGNETIC FIELDS CHAPTER 1 MAGNETIC ORCES AND MAGNETIC IELDS ANSWERS TO OCUS ON CONCEPTS QUESTIONS 1. (d) Right-Hand Rule No. 1 gives the diection of the magnetic foce as x fo both dawings A and. In dawing C, the velocity

More information

UNIT 3:Electrostatics

UNIT 3:Electrostatics The study of electic chages at est, the foces between them and the electic fields associated with them. UNIT 3:lectostatics S7 3. lectic Chages and Consevation of chages The electic chage has the following

More information

To Feel a Force Chapter 7 Static equilibrium - torque and friction

To Feel a Force Chapter 7 Static equilibrium - torque and friction To eel a oce Chapte 7 Chapte 7: Static fiction, toque and static equilibium A. Review of foce vectos Between the eath and a small mass, gavitational foces of equal magnitude and opposite diection act on

More information

Electric Field, Potential Energy, & Voltage

Electric Field, Potential Energy, & Voltage Slide 1 / 66 lectic Field, Potential negy, & oltage Wok Slide 2 / 66 Q+ Q+ The foce changes as chages move towads each othe since the foce depends on the distance between the chages. s these two chages

More information

Physics 202, Lecture 2

Physics 202, Lecture 2 Physics 202, Lectue 2 Todays Topics Electic Foce and Electic Fields Electic Chages and Electic Foces Coulomb's Law Physical Field The Electic Field Electic Field Lines Motion of Chaged Paticle in Electic

More information

Between any two masses, there exists a mutual attractive force.

Between any two masses, there exists a mutual attractive force. YEAR 12 PHYSICS: GRAVITATION PAST EXAM QUESTIONS Name: QUESTION 1 (1995 EXAM) (a) State Newton s Univesal Law of Gavitation in wods Between any two masses, thee exists a mutual attactive foce. This foce

More information

kg 2 ) 1.9!10 27 kg = Gm 1

kg 2 ) 1.9!10 27 kg = Gm 1 Section 6.1: Newtonian Gavitation Tutoial 1 Pactice, page 93 1. Given: 1.0 10 0 kg; m 3.0 10 0 kg;. 10 9 N; G 6.67 10 11 N m /kg Requied: Analysis: G m ; G m G m Solution: G m N m 6.67!10 11 kg ) 1.0!100

More information

Solutions to Problems : Chapter 19 Problems appeared on the end of chapter 19 of the Textbook

Solutions to Problems : Chapter 19 Problems appeared on the end of chapter 19 of the Textbook Solutions to Poblems Chapte 9 Poblems appeae on the en of chapte 9 of the Textbook 8. Pictue the Poblem Two point chages exet an electostatic foce on each othe. Stategy Solve Coulomb s law (equation 9-5)

More information

! E da = 4πkQ enc, has E under the integral sign, so it is not ordinarily an

! E da = 4πkQ enc, has E under the integral sign, so it is not ordinarily an Physics 142 Electostatics 2 Page 1 Electostatics 2 Electicity is just oganized lightning. Geoge Calin A tick that sometimes woks: calculating E fom Gauss s law Gauss s law,! E da = 4πkQ enc, has E unde

More information

Electrostatics. 3) positive object: lack of electrons negative object: excess of electrons

Electrostatics. 3) positive object: lack of electrons negative object: excess of electrons Electostatics IB 12 1) electic chage: 2 types of electic chage: positive and negative 2) chaging by fiction: tansfe of electons fom one object to anothe 3) positive object: lack of electons negative object:

More information

ELECTRIC CHARGES AND FORCES

ELECTRIC CHARGES AND FORCES ELECTRIC CHARGES AND ORCES 5 Conceptual Questions 5.1. An insulato can be chaged. Plastic is an insulato. A plastic od can be chaged by ubbing it with wool. 5.. A conducto can be chaged. A conducto can

More information

Appendix B The Relativistic Transformation of Forces

Appendix B The Relativistic Transformation of Forces Appendix B The Relativistic Tansfomation of oces B. The ou-foce We intoduced the idea of foces in Chapte 3 whee we saw that the change in the fou-momentum pe unit time is given by the expession d d w x

More information

2. Electrostatics. Dr. Rakhesh Singh Kshetrimayum 8/11/ Electromagnetic Field Theory by R. S. Kshetrimayum

2. Electrostatics. Dr. Rakhesh Singh Kshetrimayum 8/11/ Electromagnetic Field Theory by R. S. Kshetrimayum 2. Electostatics D. Rakhesh Singh Kshetimayum 1 2.1 Intoduction In this chapte, we will study how to find the electostatic fields fo vaious cases? fo symmetic known chage distibution fo un-symmetic known

More information

3.2 Centripetal Acceleration

3.2 Centripetal Acceleration unifom cicula motion the motion of an object with onstant speed along a cicula path of constant adius 3.2 Centipetal Acceleation The hamme thow is a tack-and-field event in which an athlete thows a hamme

More information

Uniform Circular Motion

Uniform Circular Motion Unifom Cicula Motion Intoduction Ealie we defined acceleation as being the change in velocity with time: a = v t Until now we have only talked about changes in the magnitude of the acceleation: the speeding

More information

anubhavclasses.wordpress.com CBSE Solved Test Papers PHYSICS Class XII Chapter : Electrostatics

anubhavclasses.wordpress.com CBSE Solved Test Papers PHYSICS Class XII Chapter : Electrostatics CBS Solved Test Papes PHYSICS Class XII Chapte : lectostatics CBS TST PAPR-01 CLASS - XII PHYSICS (Unit lectostatics) 1. Show does the foce between two point chages change if the dielectic constant of

More information

Chapter 5 Force and Motion

Chapter 5 Force and Motion Chapte 5 Foce and Motion In Chaptes 2 and 4 we have studied kinematics, i.e., we descibed the motion of objects using paametes such as the position vecto, velocity, and acceleation without any insights

More information

Chapter 5 Force and Motion

Chapter 5 Force and Motion Chapte 5 Foce and Motion In chaptes 2 and 4 we have studied kinematics i.e. descibed the motion of objects using paametes such as the position vecto, velocity and acceleation without any insights as to

More information

CHAPTER 10 ELECTRIC POTENTIAL AND CAPACITANCE

CHAPTER 10 ELECTRIC POTENTIAL AND CAPACITANCE CHAPTER 0 ELECTRIC POTENTIAL AND CAPACITANCE ELECTRIC POTENTIAL AND CAPACITANCE 7 0. ELECTRIC POTENTIAL ENERGY Conside a chaged paticle of chage in a egion of an electic field E. This filed exets an electic

More information

m1 m2 M 2 = M -1 L 3 T -2

m1 m2 M 2 = M -1 L 3 T -2 GAVITATION Newton s Univesal law of gavitation. Evey paticle of matte in this univese attacts evey othe paticle with a foce which vaies diectly as the poduct of thei masses and invesely as the squae of

More information

13.10 Worked Examples

13.10 Worked Examples 13.10 Woked Examples Example 13.11 Wok Done in a Constant Gavitation Field The wok done in a unifom gavitation field is a faily staightfowad calculation when the body moves in the diection of the field.

More information

Physics Courseware Physics II Electric Field and Force

Physics Courseware Physics II Electric Field and Force Physics Cousewae Physics II lectic iel an oce Coulomb s law, whee k Nm /C test Definition of electic fiel. This is a vecto. test Q lectic fiel fo a point chage. This is a vecto. Poblem.- chage of µc is

More information

Flux. Area Vector. Flux of Electric Field. Gauss s Law

Flux. Area Vector. Flux of Electric Field. Gauss s Law Gauss s Law Flux Flux in Physics is used to two distinct ways. The fist meaning is the ate of flow, such as the amount of wate flowing in a ive, i.e. volume pe unit aea pe unit time. O, fo light, it is

More information

PHYSICS 272 Electric & Magnetic Interactions

PHYSICS 272 Electric & Magnetic Interactions PHYS 7: Matte and Inteactions II -- Electic And Magnetic Inteactions http://www.physics.pudue.edu/academic_pogams/couses/phys7/ PHYSICS 7 Electic & Magnetic Inteactions Lectue 3 Chaged Objects; Polaization

More information

PHYS 1441 Section 002. Lecture #3

PHYS 1441 Section 002. Lecture #3 PHYS 1441 Section 00 Chapte 1 Lectue #3 Wednesday, Sept. 6, 017 Coulomb s Law The Electic Field & Field Lines Electic Fields and Conductos Motion of a Chaged Paticle in an Electic Field Electic Dipoles

More information

PHYSICS 151 Notes for Online Lecture #36

PHYSICS 151 Notes for Online Lecture #36 Electomagnetism PHYSICS 151 Notes fo Online Lectue #36 Thee ae fou fundamental foces in natue: 1) gavity ) weak nuclea 3) electomagnetic 4) stong nuclea The latte two opeate within the nucleus of an atom

More information

Chapter 25. Electric Potential

Chapter 25. Electric Potential Chapte 25 Electic Potential C H P T E R O U T L I N E 251 Potential Diffeence and Electic Potential 252 Potential Diffeences in a Unifom Electic Field 253 Electic Potential and Potential Enegy Due to Point

More information

Class 2. Lesson 1 Stationary Point Charges and Their Forces. Basic Rules of Electrostatics. Basic Rules of Electrostatics

Class 2. Lesson 1 Stationary Point Charges and Their Forces. Basic Rules of Electrostatics. Basic Rules of Electrostatics Lesson 1 Stationay Point Chages and Thei Foces Class Today we will: lean the basic chaacteistics o the electostatic oce eview the popeties o conductos and insulatos lean what is meant by electostatic induction

More information

Our Universe: GRAVITATION

Our Universe: GRAVITATION Ou Univese: GRAVITATION Fom Ancient times many scientists had shown geat inteest towads the sky. Most of the scientist studied the motion of celestial bodies. One of the most influential geek astonomes

More information

(Sample 3) Exam 1 - Physics Patel SPRING 1998 FORM CODE - A (solution key at end of exam)

(Sample 3) Exam 1 - Physics Patel SPRING 1998 FORM CODE - A (solution key at end of exam) (Sample 3) Exam 1 - Physics 202 - Patel SPRING 1998 FORM CODE - A (solution key at end of exam) Be sue to fill in you student numbe and FORM lette (A, B, C) on you answe sheet. If you foget to include

More information

AST 121S: The origin and evolution of the Universe. Introduction to Mathematical Handout 1

AST 121S: The origin and evolution of the Universe. Introduction to Mathematical Handout 1 Please ead this fist... AST S: The oigin and evolution of the Univese Intoduction to Mathematical Handout This is an unusually long hand-out and one which uses in places mathematics that you may not be

More information

Electrostatics. 1. Show does the force between two point charges change if the dielectric constant of the medium in which they are kept increase?

Electrostatics. 1. Show does the force between two point charges change if the dielectric constant of the medium in which they are kept increase? Electostatics 1. Show does the foce between two point chages change if the dielectic constant of the medium in which they ae kept incease? 2. A chaged od P attacts od R whee as P epels anothe chaged od

More information

Universal Gravitation

Universal Gravitation Chapte 1 Univesal Gavitation Pactice Poblem Solutions Student Textbook page 580 1. Conceptualize the Poblem - The law of univesal gavitation applies to this poblem. The gavitational foce, F g, between

More information

Lecture 3.7 ELECTRICITY. Electric charge Coulomb s law Electric field

Lecture 3.7 ELECTRICITY. Electric charge Coulomb s law Electric field Lectue 3.7 ELECTRICITY Electic chage Coulomb s law Electic field ELECTRICITY Inteaction between electically chages objects Many impotant uses Light Heat Rail tavel Computes Cental nevous system Human body

More information

F g. = G mm. m 1. = 7.0 kg m 2. = 5.5 kg r = 0.60 m G = N m 2 kg 2 = = N

F g. = G mm. m 1. = 7.0 kg m 2. = 5.5 kg r = 0.60 m G = N m 2 kg 2 = = N Chapte answes Heinemann Physics 4e Section. Woked example: Ty youself.. GRAVITATIONAL ATTRACTION BETWEEN SMALL OBJECTS Two bowling balls ae sitting next to each othe on a shelf so that the centes of the

More information

Algebra-based Physics II

Algebra-based Physics II lgebabased Physics II Chapte 19 Electic potential enegy & The Electic potential Why enegy is stoed in an electic field? How to descibe an field fom enegetic point of view? Class Website: Natual way of

More information

4.[1pt] Two small spheres with charges -4 C and -9 C are held 9.5 m apart. Find the magnitude of the force between them.

4.[1pt] Two small spheres with charges -4 C and -9 C are held 9.5 m apart. Find the magnitude of the force between them. . [pt] A peson scuffing he feet on a wool ug on a y ay accumulates a net chage of - 4.uC. How many ecess electons oes this peson get? Coect, compute gets:.63e+4. [pt] By how much oes he mass incease? Coect,

More information

Voltage ( = Electric Potential )

Voltage ( = Electric Potential ) V-1 of 10 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

1 Dark Cloud Hanging over Twentieth Century Physics

1 Dark Cloud Hanging over Twentieth Century Physics We ae Looking fo Moden Newton by Caol He, Bo He, and Jin He http://www.galaxyanatomy.com/ Wuhan FutueSpace Scientific Copoation Limited, Wuhan, Hubei 430074, China E-mail: mathnob@yahoo.com Abstact Newton

More information

DEVIL PHYSICS THE BADDEST CLASS ON CAMPUS IB PHYSICS

DEVIL PHYSICS THE BADDEST CLASS ON CAMPUS IB PHYSICS DEVIL PHYSICS THE BADDEST CLASS ON CAMPUS IB PHYSICS TSOKOS LESSON 10-1 DESCRIBING FIELDS Essential Idea: Electic chages and masses each influence the space aound them and that influence can be epesented

More information

Rigid Body Dynamics 2. CSE169: Computer Animation Instructor: Steve Rotenberg UCSD, Winter 2018

Rigid Body Dynamics 2. CSE169: Computer Animation Instructor: Steve Rotenberg UCSD, Winter 2018 Rigid Body Dynamics 2 CSE169: Compute Animation nstucto: Steve Rotenbeg UCSD, Winte 2018 Coss Poduct & Hat Opeato Deivative of a Rotating Vecto Let s say that vecto is otating aound the oigin, maintaining

More information

PHYS Summer Professor Caillault Homework Solutions. Chapter 9

PHYS Summer Professor Caillault Homework Solutions. Chapter 9 PHYS - Summe 007 - Pofesso Caillault Homewok Solutions Chapte 9 3. Pictue the Poblem The owne walks slowly towad the notheast while the cat uns eastwad and the dog uns nothwad. Stategy Sum the momenta

More information

Physics 2020, Spring 2005 Lab 5 page 1 of 8. Lab 5. Magnetism

Physics 2020, Spring 2005 Lab 5 page 1 of 8. Lab 5. Magnetism Physics 2020, Sping 2005 Lab 5 page 1 of 8 Lab 5. Magnetism PART I: INTRODUCTION TO MAGNETS This week we will begin wok with magnets and the foces that they poduce. By now you ae an expet on setting up

More information

DYNAMICS OF UNIFORM CIRCULAR MOTION

DYNAMICS OF UNIFORM CIRCULAR MOTION Chapte 5 Dynamics of Unifom Cicula Motion Chapte 5 DYNAMICS OF UNIFOM CICULA MOTION PEVIEW An object which is moing in a cicula path with a constant speed is said to be in unifom cicula motion. Fo an object

More information

Look over Chapter 22 sections 1-8 Examples 2, 4, 5, Look over Chapter 16 sections 7-9 examples 6, 7, 8, 9. Things To Know 1/22/2008 PHYS 2212

Look over Chapter 22 sections 1-8 Examples 2, 4, 5, Look over Chapter 16 sections 7-9 examples 6, 7, 8, 9. Things To Know 1/22/2008 PHYS 2212 PHYS 1 Look ove Chapte sections 1-8 xamples, 4, 5, PHYS 111 Look ove Chapte 16 sections 7-9 examples 6, 7, 8, 9 Things To Know 1) What is an lectic field. ) How to calculate the electic field fo a point

More information

Advanced Physics - Coulomb's Law

Advanced Physics - Coulomb's Law Advanced Physics - oulomb's Law We ve leaned that electons have a minus one chage and potons have a positive one chage. This plus and minus one business doesn t wok vey well when we go in and ty to do

More information

PHYSICS 272H Electric & Magnetic Interactions

PHYSICS 272H Electric & Magnetic Interactions PHYSICS 7H Electic & Magnetic Inteactions Physics couse home page: http://www.physics.pudue.edu/academic-pogams/couses/all_couses.php Blackboad Lean: https://mycouses.pudue.edu/webapps/login/ Couse Content

More information

Circular Motion & Torque Test Review. The period is the amount of time it takes for an object to travel around a circular path once.

Circular Motion & Torque Test Review. The period is the amount of time it takes for an object to travel around a circular path once. Honos Physics Fall, 2016 Cicula Motion & Toque Test Review Name: M. Leonad Instuctions: Complete the following woksheet. SHOW ALL OF YOUR WORK ON A SEPARATE SHEET OF PAPER. 1. Detemine whethe each statement

More information

Physics 4A Chapter 8: Dynamics II Motion in a Plane

Physics 4A Chapter 8: Dynamics II Motion in a Plane Physics 4A Chapte 8: Dynamics II Motion in a Plane Conceptual Questions and Example Poblems fom Chapte 8 Conceptual Question 8.5 The figue below shows two balls of equal mass moving in vetical cicles.

More information

AP Physics Electric Potential Energy

AP Physics Electric Potential Energy AP Physics lectic Potential negy Review of some vital peviously coveed mateial. The impotance of the ealie concepts will be made clea as we poceed. Wok takes place when a foce acts ove a distance. W F

More information

Chapter 20 Electrostatics and Coulomb s Law 20.1 Introduction electrostatics Separation of Electric Charge by Rubbing

Chapter 20 Electrostatics and Coulomb s Law 20.1 Introduction electrostatics Separation of Electric Charge by Rubbing I wish to give an account of some investigations which have led to the conclusion that the caies of negative electicity ae bodies, which I have called copuscles, having a mass vey much smalle than that

More information

working pages for Paul Richards class notes; do not copy or circulate without permission from PGR 2004/11/3 10:50

working pages for Paul Richards class notes; do not copy or circulate without permission from PGR 2004/11/3 10:50 woking pages fo Paul Richads class notes; do not copy o ciculate without pemission fom PGR 2004/11/3 10:50 CHAPTER7 Solid angle, 3D integals, Gauss s Theoem, and a Delta Function We define the solid angle,

More information

Chapter 22: Electric Fields. 22-1: What is physics? General physics II (22102) Dr. Iyad SAADEDDIN. 22-2: The Electric Field (E)

Chapter 22: Electric Fields. 22-1: What is physics? General physics II (22102) Dr. Iyad SAADEDDIN. 22-2: The Electric Field (E) Geneal physics II (10) D. Iyad D. Iyad Chapte : lectic Fields In this chapte we will cove The lectic Field lectic Field Lines -: The lectic Field () lectic field exists in a egion of space suounding a

More information

PHYS 110B - HW #7 Spring 2004, Solutions by David Pace Any referenced equations are from Griffiths Problem statements are paraphrased

PHYS 110B - HW #7 Spring 2004, Solutions by David Pace Any referenced equations are from Griffiths Problem statements are paraphrased PHYS 0B - HW #7 Sping 2004, Solutions by David Pace Any efeenced euations ae fom Giffiths Poblem statements ae paaphased. Poblem 0.3 fom Giffiths A point chage,, moves in a loop of adius a. At time t 0

More information

Physics 11 Chapter 4: Forces and Newton s Laws of Motion. Problem Solving

Physics 11 Chapter 4: Forces and Newton s Laws of Motion. Problem Solving Physics 11 Chapte 4: Foces and Newton s Laws of Motion Thee is nothing eithe good o bad, but thinking makes it so. William Shakespeae It s not what happens to you that detemines how fa you will go in life;

More information

17.1 Electric Potential Energy. Equipotential Lines. PE = energy associated with an arrangement of objects that exert forces on each other

17.1 Electric Potential Energy. Equipotential Lines. PE = energy associated with an arrangement of objects that exert forces on each other Electic Potential Enegy, PE Units: Joules Electic Potential, Units: olts 17.1 Electic Potential Enegy Electic foce is a consevative foce and so we can assign an electic potential enegy (PE) to the system

More information

Recap. Centripetal acceleration: v r. a = m/s 2 (towards center of curvature)

Recap. Centripetal acceleration: v r. a = m/s 2 (towards center of curvature) a = c v 2 Recap Centipetal acceleation: m/s 2 (towads cente of cuvatue) A centipetal foce F c is equied to keep a body in cicula motion: This foce poduces centipetal acceleation that continuously changes

More information

Physics 11 Chapter 3: Vectors and Motion in Two Dimensions. Problem Solving

Physics 11 Chapter 3: Vectors and Motion in Two Dimensions. Problem Solving Physics 11 Chapte 3: Vectos and Motion in Two Dimensions The only thing in life that is achieved without effot is failue. Souce unknown "We ae what we epeatedly do. Excellence, theefoe, is not an act,

More information

1) Consider a particle moving with constant speed that experiences no net force. What path must this particle be taking?

1) Consider a particle moving with constant speed that experiences no net force. What path must this particle be taking? Chapte 5 Test Cicula Motion and Gavitation 1) Conside a paticle moving with constant speed that expeiences no net foce. What path must this paticle be taking? A) It is moving in a paabola. B) It is moving

More information

1.1 THE ELECTRIC CHARGE

1.1 THE ELECTRIC CHARGE 1.1 THE ELECTRIC CHARGE - In a dy day, one obseves "light spaks" when a wool pull is taken out o when the finges touch a metallic object. Aound the yea 1600, one classified these effects as electic phenomena.

More information

Chapter 4. Newton s Laws of Motion. Newton s Law of Motion. Sir Isaac Newton ( ) published in 1687

Chapter 4. Newton s Laws of Motion. Newton s Law of Motion. Sir Isaac Newton ( ) published in 1687 Chapte 4 Newton s Laws of Motion 1 Newton s Law of Motion Si Isaac Newton (1642 1727) published in 1687 2 1 Kinematics vs. Dynamics So fa, we discussed kinematics (chaptes 2 and 3) The discussion, was

More information

Phys102 Second Major-182 Zero Version Monday, March 25, 2019 Page: 1

Phys102 Second Major-182 Zero Version Monday, March 25, 2019 Page: 1 Monday, Mach 5, 019 Page: 1 Q1. Figue 1 shows thee pais of identical conducting sphees that ae to be touched togethe and then sepaated. The initial chages on them befoe the touch ae indicated. Rank the

More information

The mass of a water molecule is the mass of two hydrogens and one oxygen: 1u + 1u + 16u = 18u, where. = = 0.05 C/kg m. 65 kg 0.

The mass of a water molecule is the mass of two hydrogens and one oxygen: 1u + 1u + 16u = 18u, where. = = 0.05 C/kg m. 65 kg 0. EECTRIC CHARGE, FORCE, AND FIED 0 EXERCISES Section 0.1 Electic Chage 1. INTERPRET We ll estimate the chage you body would cay if the electon chage slightly diffeed fom the poton chage. DEVEOP Since the

More information

4. Compare the electric force holding the electron in orbit ( r = 0.53

4. Compare the electric force holding the electron in orbit ( r = 0.53 Electostatics WS Electic Foce an Fiel. Calculate the magnitue of the foce between two 3.60-µ C point chages 9.3 cm apat.. How many electons make up a chage of 30.0 µ C? 3. Two chage ust paticles exet a

More information

Force between two parallel current wires and Newton s. third law

Force between two parallel current wires and Newton s. third law Foce between two paallel cuent wies and Newton s thid law Yannan Yang (Shanghai Jinjuan Infomation Science and Technology Co., Ltd.) Abstact: In this pape, the essence of the inteaction between two paallel

More information

Introduction: Vectors and Integrals

Introduction: Vectors and Integrals Intoduction: Vectos and Integals Vectos a Vectos ae chaacteized by two paametes: length (magnitude) diection a These vectos ae the same Sum of the vectos: a b a a b b a b a b a Vectos Sum of the vectos:

More information

Section 8.2 Polar Coordinates

Section 8.2 Polar Coordinates Section 8. Pola Coodinates 467 Section 8. Pola Coodinates The coodinate system we ae most familia with is called the Catesian coodinate system, a ectangula plane divided into fou quadants by the hoizontal

More information

Describing Circular motion

Describing Circular motion Unifom Cicula Motion Descibing Cicula motion In ode to undestand cicula motion, we fist need to discuss how to subtact vectos. The easiest way to explain subtacting vectos is to descibe it as adding a

More information

Gaia s Place in Space

Gaia s Place in Space Gaia s Place in Space The impotance of obital positions fo satellites Obits and Lagange Points Satellites can be launched into a numbe of diffeent obits depending on thei objectives and what they ae obseving.

More information

The Laws of Motion ( ) N SOLUTIONS TO PROBLEMS ! F = ( 6.00) 2 + ( 15.0) 2 N = 16.2 N. Section 4.4. Newton s Second Law The Particle Under a Net Force

The Laws of Motion ( ) N SOLUTIONS TO PROBLEMS ! F = ( 6.00) 2 + ( 15.0) 2 N = 16.2 N. Section 4.4. Newton s Second Law The Particle Under a Net Force SOLUTIONS TO PROBLEMS The Laws of Motion Section 4.3 Mass P4. Since the ca is moving with constant speed and in a staight line, the esultant foce on it must be zeo egadless of whethe it is moving (a) towad

More information

Magnetic Field. Conference 6. Physics 102 General Physics II

Magnetic Field. Conference 6. Physics 102 General Physics II Physics 102 Confeence 6 Magnetic Field Confeence 6 Physics 102 Geneal Physics II Monday, Mach 3d, 2014 6.1 Quiz Poblem 6.1 Think about the magnetic field associated with an infinite, cuent caying wie.

More information

Lecture 3. Basic Physics of Astrophysics - Force and Energy. Forces

Lecture 3. Basic Physics of Astrophysics - Force and Energy. Forces Foces Lectue 3 Basic Physics of Astophysics - Foce and Enegy http://apod.nasa.gov/apod/ Momentum is the poduct of mass and velocity - a vecto p = mv (geneally m is taken to be constant) An unbalanced foce

More information

The Electric Field. Electric Charge HAPTER Historical Origins

The Electric Field. Electric Charge HAPTER Historical Origins C HAPTER17 The Electic Field Y This electical dischage was poduced at the tun of the 0th centuy by invento Nikola Tesla, shown in the photo. ou can obseve static electicity in vaious ways. Walk acoss a

More information

Spring 2001 Physics 2048 Test 3 solutions

Spring 2001 Physics 2048 Test 3 solutions Sping 001 Physics 048 Test 3 solutions Poblem 1. (Shot Answe: 15 points) a. 1 b. 3 c. 4* d. 9 e. 8 f. 9 *emembe that since KE = ½ mv, KE must be positive Poblem (Estimation Poblem: 15 points) Use momentum-impulse

More information

Electric Potential Potential Differences in a Uniform Electric Field Electric Potential and Potential Energy Due to Point Charges

Electric Potential Potential Differences in a Uniform Electric Field Electric Potential and Potential Energy Due to Point Charges P U Z Z L E R Jennife is holding on to an electically chaged sphee that eaches an electic potential of about 100 000 V. The device that geneates this high electic potential is called a Van de Gaaff geneato.

More information

KEPLER S LAWS OF PLANETARY MOTION

KEPLER S LAWS OF PLANETARY MOTION EPER S AWS OF PANETARY MOTION 1. Intoduction We ae now in a position to apply what we have leaned about the coss poduct and vecto valued functions to deive eple s aws of planetay motion. These laws wee

More information