( ) ( ) Review of Force. Part 1, Topic 1 Force Fields. Dr. Sven Achenbach - based on a script by Dr. Eric Salt - Outline. Review of Force. F r.

Size: px
Start display at page:

Download "( ) ( ) Review of Force. Part 1, Topic 1 Force Fields. Dr. Sven Achenbach - based on a script by Dr. Eric Salt - Outline. Review of Force. F r."

Transcription

1 S. Achenbach: PHYS 55 (Pat, Topic ) Handouts p. Review of Foce Univesity of Saskatchewan Undegaduate Couse Phys 55 Intoduction to Electicity and Magnetism Basics F o F v denotes foce it is a thee dimensional vecto e.g. in ectangula coodinates F = ( 7,3,) Pat, Topic Foce Fields units of foce (deived in the Système Intenational d Unités, SI) ae Newtons N D. Sven Achenbach - based on a scipt by D. Eic Salt - S. Achenbach S. Achenbach Phys55 -: Foce Fields 3 Outline Review of Foce slide # eview of foce 3 - special vectos - dot poduct - magnitude - angle between foce vectos foce fields 3 wok (tansfe of enegy) 9 - foce not in diection of movement - potential enegy - consevative foce fields - potential enegy evisited - wok done by a changing foce - wok as aea unde a cuve - pependicula component - enegy contou maps - elationship enegy contous & foce lines - estimating foce fom a contou map S. Achenbach Phys55 -: Foce Fields ( ) Special Vectos iˆ =,0,0 unit vecto in the x-diection ˆ j = ( 0,,0 ) unit vecto in the y-diection k ˆ = 0,0, unit vecto in the z-diection ( ) unit vecto means: length of unity () in the espective diection x, y o z with scalas F x, F y, F z : F = ( Fx, Fy, Fz ) = F iˆ x + F ˆ y j + F kˆ z times length (±) of foce diection (x-component) component in x-diection (unit vecto with length =) e.g. F = 7 iˆ + 3 ˆj + kˆ = scala means: a eal numbe without diection ( 7,3,) S. Achenbach Phys55 -: Foce Fields 4

2 S. Achenbach: PHYS 55 (Pat, Topic ) Handouts p. Review of Foce Review of Foce Dot Poduct the dot poduct opeato is a dot the dot poduct function (opeation) poduces a scala fom two aguments (the aguments themselves ae vectos) F G F G + F G + F G x x y y the symbol (sometimes also witten as := ) eads is defined as z z Magnitude the magnitude (i.e. length) of a vecto is a scala always positive denoted F o F defined as F F F = F + F + F x y z S. Achenbach Phys55 -: Foce Fields 5 S. Achenbach Phys55 -: Foce Fields 7 Review of Foce Review of Foce Example ( ) ( ) What is the dot poduct fo F =,,3 and G = 4,5,6? Example (,3, 3) F What is the magnitude of the vecto =? S. Achenbach Phys55 -: Foce Fields 6 S. Achenbach Phys55 -: Foce Fields 8

3 S. Achenbach: PHYS 55 (Pat, Topic ) Handouts p. 3 Review of Foce Review of Foce Example 3 Let F = 30 N, F x = 0 N, F y = 0 N. Find F z. Angle between Foce Vectos geometic intepetation of the angle θ between two vectos F and F : 3-dimensional view of vectos -dimensional view of the plane containing the two 3-dimensional vectos S. Achenbach Phys55 -: Foce Fields 9 S. Achenbach Phys55 -: Foce Fields Review of Foce Review of Foce Angle between Foce Vectos the angle θ between any two vectos is given by F F F F cos θ = = F F F F Example 4 ( ) ( ) Find the angle between the two vectos F = and F =,,3 4,5,6. with dot poduct opeation poducing a scala and the magnitude of a vecto F F = F F + F + F F F = F x F x + F y F y + F z F z x y z cos θ = F F x x F + F x y + F + F y z F y F + F x z + F F y z + F z S. Achenbach Phys55 -: Foce Fields 0 S. Achenbach Phys55 -: Foce Fields

4 S. Achenbach: PHYS 55 (Pat, Topic ) Handouts p. 4 Foce Fields eview of foce - special vectos - dot poduct - magnitude - angle between foce vectos foce fields wok (tansfe of enegy) - foce not in diection of movement - potential enegy - consevative foce fields - potential enegy evisited - wok done by a changing foce - wok as aea unde a cuve - pependicula component - enegy contou maps - elationship enegy contous & foce lines - estimating foce fom a contou map S. Achenbach Phys55 -: Foce Fields 3 Basics example of a gaphical epesentation of a foce field vectos (aows) show the foce on a standad (test) object located at the tail end of the foce aow point indicates (sample) position of object aow indicates diection of the foce.3 numbe indicates magnitude of the foce S. Achenbach Phys55 -: Foce Fields 5 Foce Fields Foce Fields Basics when an object expeiences a foce at evey point in space, it is in a foce field foce fields ae thee-dimensional thee is a 3-dimensional foce vecto associated with each point in 3-dimensional space Example 5 The chat shows the foce vecto acting on a kg mass at a few diffeent positions. The units of foce ae Newtons N. What is the foce on a kg mass located at x = 5 metes, y = 3 metes? fo pupose of illustation and simplicity, often only a plane in the field (-dimensional epesentation) is dawn on pape S. Achenbach Phys55 -: Foce Fields 4 S. Achenbach Phys55 -: Foce Fields 6

5 S. Achenbach: PHYS 55 (Pat, Topic ) Handouts p. 5 Foce Fields Basics altenative gaphical epesentation of a foce field diection of the foce is a tangent cuve magnitude is given at cetain points S. Achenbach Phys55 -: Foce Fields 7 eview of foce - special vectos - dot poduct - magnitude - angle between foce vectos foce fields wok (tansfe of enegy) - foce not in diection of movement - potential enegy - consevative foce fields - potential enegy evisited - wok done by a changing foce - wok as aea unde a cuve - pependicula component - enegy contou maps - elationship enegy contous & foce lines - estimating foce fom a contou map S. Achenbach Phys55 -: Foce Fields 9 Foce Fields Example 6 Estimate the foce vecto at x=4m, y=m. Basics enegy is a scala quantity (eal numbe) associated with an object units of enegy ae Newtons metes, called Joules J enegy can be tansfeed to o fom an object (e.g. while it is moving): wok is the enegy tansfeed to o fom an object by a foce if the foce is pushing o pulling the object - in the diection the object is moving, then the foce is doing positive wok on the object - opposite to the diection negative wok definition: with W = F d - magnitude of foce F applied to the object in the diection of the movement - distance d the object is moved - wok W done by foce F on the object as the object is moved a distance d S. Achenbach Phys55 -: Foce Fields 8 S. Achenbach Phys55 -: Foce Fields 0

6 S. Achenbach: PHYS 55 (Pat, Topic ) Handouts p. 6 Example 7 Foce not in Diection of Movement A foce with a magnitude of 3 N is applied to an object to slide it acoss a table. How much wok is done by the moving foce, if the object is moved 0.7 m? fee body diagam enegy is tansfeed fom the tacto to the box ca via the tow ope analysis of foces (and late enegy) using a fee body diagam foce applied by the ope has a component in the diection of movement does wok on the box ca othe foces (on wheels) act pependicula to the diection of movement do not contibute any wok (do not tansfe enegy to the box ca) S. Achenbach Phys55 -: Foce Fields S. Achenbach Phys55 -: Foce Fields 3 Example 8 A foce, F, with a magnitude of 0 N is applied to a block to slide it acoss a table. A second foce, F, which has the opposite diection of F is applied to the opposite side of the block. The magnitude of F is 6 N. The block is moved. m. ) How much wok is done by foce F? ) How much wok is done by foce F? 3) How much enegy is tansfeed fom F to F? Foce not in Diection of Movement equation fo wok done on an object moved in a staight line is W = F d = F d cos θ = ( F cos θ ) d with diffeence between end position p end and the stat position p stat of the object vecto d = p end p stat angle θ between vectos F and d 4) If the suface of the table is fictionless, how much enegy is used to acceleate the block (i.e. how much enegy is tansfeed fom F to the block)? S. Achenbach Phys55 -: Foce Fields S. Achenbach Phys55 -: Foce Fields 4

7 S. Achenbach: PHYS 55 (Pat, Topic ) Handouts p. 7 Foce not in Diection of Movement an intepetation of W ( F cos θ ) d is that is the component of foce =F F cos θ in the diection the object is moved Foce not in Diection of Movement Suppose the tacto pulls the box ca a distance of 00 m with a steady ope foce of 4000 N. The angle between the ope and the ails is 30 degees. wok done by tacto W = F ope d cos θ with - tensile foce in the ope F ope - distance box ca is moved d - angle θ between F ope and d d is in diection of ails angle between foce and distance vectos is θ = 30 = π / 6 wok done by the tacto on the box ca is W = F ope d cos θ = (4000 N) (00 m) cos ( π / 6 ) = kj S. Achenbach Phys55 -: Foce Fields 5 S. Achenbach Phys55 -: Foce Fields 7 Foce not in Diection of Movement Example 9 A wooden object is dagged m acoss a floo using a ope. fee body diagam component of foce of the tacto pulling the box ca in the diection of movement d has a magnitude F ope cos θ Recall that the diection of the foce exeted by a ope is always in line with the ope. If the magnitude of the foce exeted by Obelix on the ope is 0 N, how much wok is done by him (i.e. how much wok is done on the wooden object by the foce exeted by the ope)? S. Achenbach Phys55 -: Foce Fields 6 S. Achenbach Phys55 -: Foce Fields 8

8 S. Achenbach: PHYS 55 (Pat, Topic ) Handouts p. 8 Example 0 A sail boat is moved fom position (x,y) = (0m, 0m) to (00m, 30m) by a wind that exets a foce of (0 N, -0 N) [i.e. a foce of (0i -0j) N ] on the sail boat. What is the wok done by the wind on the sail boat? Example A 0 kg mass is hoisted by Obelix via a system of fictionless opes and pulleys. ) What is the gavitational foce on the mass? ) How much foce must Obelix apply to the ope to lift the mass? 3) How much wok is done by Obelix if the mass is hoisted m? 4) How much wok is done by the foce due to the gavitational field (gavitational foce)? 5) How much enegy is tansfeed fom Obelix to the mass? 6) Whee is the enegy that was added to the mass? S. Achenbach Phys55 -: Foce Fields 9 S. Achenbach Phys55 -: Foce Fields 3 Potential Enegy enegy can be stoed and etieved at a late time (usually) such enegy is called potential enegy fom latin potentia [foce, ability, powe] Example 3) How much wok is done by Obelix if the mass is hoisted m? e.g. enegy tansfeed by an ache to a bow (late, enegy can be etieved fom the bow and be tansfeed to an aow) fee body diagam enegy in a gavitational field tansfeed by lifting a mass up a vetical distance (late, wok done can be etieved by loweing the mass) Note: when a mass is elevated, we say the mass has potential enegy even though the enegy is stoed in the gavitational field S. Achenbach Phys55 -: Foce Fields 30 Note: Result would be the same if Obelix was pulling the mass vetically up, without pulley. But with pulley with additional tavelling wheel: same enegy distibuted ove double the distance ( half the foce) easie (but twice as long) to pull S. Achenbach Phys55 -: Foce Fields 3

9 S. Achenbach: PHYS 55 (Pat, Topic ) Handouts p. 9 Consevative Foce Fields Consevative Foce Fields Deivation time pemitting a field is called consevative if and only if the enegy equied to move a mass between two points in the field only depends on the stat and end points (and does not depend on the path taken) e.g., the gavitational field is a consevative field moving a mass staight fom A to C takes same enegy as moving the mass fom A to B fist and then fom B to C wok equied to move a mass fom A via B to C is wok to move it fom A to B plus wok to move it fom B to C foce equied to move a mass fom A to B is F with infinitesimal foce ΔF a = Fg + ΔFAB AB 0 in diection fom A to B to get the mass moving, but not doing wok F a F g as obvious fom fee body diagam wok equied to move a mass fom A to B is WAB = Fg d AB, and with = ( ) iˆ + ( y y ) ˆj W AB d AB 0 0 = [ 0 iˆ ( m g) ˆj ] ( 0) iˆ + ( y y0 ) = ()() ( m g) ( y y0 ) = mg ( ) y y 0 [ ˆj ] S. Achenbach Phys55 -: Foce Fields 33 S. Achenbach Phys55 -: Foce Fields 35 Consevative Foce Fields Deivation time pemitting foce equied to move a mass fom A to C is F with infinitesimal foce ΔF a = Fg + ΔFAC AC 0 in diection fom A to C to get the mass moving, but not doing wok F a F g as obvious fom fee body diagam with gavitational constant on eath g=9.8 m / s, and mass m : F g = m g Fa = Fg = ( 0 iˆ ( m g) ˆj ) wok equied to move a mass fom A to C is W = Fa d = ( Fa cos θ ) d = F g d, and with d = x x iˆ + y y ˆ ( 0 ) ( 0 ) j iˆ ( m g) ˆj x x iˆ 0 + y ()( 0 x x0 ) + ( m g)( y y0 ) W = mg ( ) = = [ ] [( ) ( y ) ˆj ] 0 0 W = AC y y 0 S. Achenbach Phys55 -: Foce Fields 34 Consevative Foce Fields wok equied to move a mass fom A via B to C is wok to move it fom A to B plus wok to move it fom B to C foce equied to move a mass fom B to C is F with infinitesimal foce ΔF a = Fg + ΔFBC BC 0 in diection fom B to C to get the mass moving, but not doing wok F a F g as obvious fom fee body diagam wok equied to move a mass fom B to C is WBC = Fg d BC, and with = ( x x ) iˆ ( 0) ˆj W AB d BC 0 + [ 0 iˆ ( m g) ˆj ] ( x x ) iˆ 0 + ( 0) ()( x x ) + ( m ) ( 0) = = g = [ ˆj ] Deivation time pemitting S. Achenbach Phys55 -: Foce Fields 36

10 S. Achenbach: PHYS 55 (Pat, Topic ) Handouts p. 0 Consevative Foce Fields wok equied to move a mass fom A via B to C is wok to move it fom A to B plus wok to move it fom B to C W ABC = WAB + W ABC = mg ( y y0 ) + 0 as expected, W ABC = W AC path does not matte WBC Example A peson with a mass of 70 kg snowboads down a mountain in a zig-zag fashion. How much wok is done by the gavitational field on the peson if the peson stats at a point on the mountain that is 500 m above the day lodge (vetical distance) & ends at the day lodge? with W AC W AB W BC = mg = mg = 0 ( y y 0 ) ( ) y y 0 S. Achenbach Phys55 -: Foce Fields 37 S. Achenbach Phys55 -: Foce Fields 39 Consevative Foce Fields by the way: wok done to move an object in the gavitational field is given by W = mg ( ) y y 0 wok only depends on vaiables mass of the object m vetical distance of movement y -y 0 (it also depends on g, but this is not a vaiable on the suface of the eath) Potential Enegy evisited potential enegy is associated with an object and its location in a field is measued fom a efeence point in space is the enegy that could be etieved if the object was moved fom its pesent location back to the efeence point of an object in a gavitational field is denoted U and is given by U = m g h with - U potential enegy of the object - m mass of the object - g gavitational constant (on the eath suface: g = 9.8 m / s ) - h vetical distance fom the efeence point to the cente of gavity of the object Note: if the object is located below the efeence point, then U and h ae negative S. Achenbach Phys55 -: Foce Fields 38 S. Achenbach Phys55 -: Foce Fields 40

11 S. Achenbach: PHYS 55 (Pat, Topic ) Handouts p. Example 3 A tuck mounted cane is used to lift a 500 kg wecking ball. The cane is mounted to the bed (deck) of the tuck. What is the potential enegy of the wecking ball with espect to the bed of the tuck if the cente of gavity of the ball is 0 m above the bed of the tuck? What is the potential enegy of the ball with espect to the bed of the tuck if the ball is loweed into a hole so that the cente of gavity is m below the bed of the tuck? Wok done by a changing Foce an object is moved a distance D fom S 0 along cuve S the foce acting on the object is a vecto that is a function of its position x on the cuve: decomposition of foces (fo values of x) F(x) is foce acting on the object when it is located a distance x fom S 0 along the cuve S Note: x is not the hoizontal distance fom S 0, but the distance taveled along the cuve F(x) can be boken down in components F(x) = F s (x) + F (x) with F s (x) diection is tangent to the cuve at point x (a distance x fom S 0 along the cuve) F (x) diection is pependicula to the cuve at point x S. Achenbach Phys55 -: Foce Fields 4 S. Achenbach Phys55 -: Foce Fields 43 Wok done by a changing Foce an object is moved a distance D fom S 0 along cuve S the foce acting on the object is a vecto that is a function of its position x on the cuve: F(x) is foce acting on the object when it is located a distance x fom S 0 along the cuve S Note: x is not the hoizontal distance fom S 0, but the distance taveled along the cuve Wok done by a changing Foce theoy to find wok done on an object as it is moved along the cuve (path): ) subdivide the path along the cuve between S and S into N segments of length Δx = (D D ) / N (segments should be small enough to be appoximated by staight lines) S. Achenbach Phys55 -: Foce Fields 4 S. Achenbach Phys55 -: Foce Fields 44

12 S. Achenbach: PHYS 55 (Pat, Topic ) Handouts p. Wok done by a changing Foce theoy to find wok done on an object as it is moved along the cuve (path): ) subdivide the path along the cuve between S and S into N segments of length Δx = (D D ) / N (segments should be small enough to be appoximated by staight lines) ) calculate appoximate wok done on the object as it is moved though each segment, teating the foce as constant ove each individual segment (but changing fom segment to segment) 3) sum wok done in all segments appoximate value fo the wok equied to move the object fom S to S Wok done by a changing Foce 3) total wok done by the foce on an object moved fom S to S is appoximately W ± [ Fs ( D Δx) Δx. segment F s ( D +. Δx) Δx + ( D + ( N + 0. ) Δx) Δx] L 5 F s appoximation becomes equality as N fo N (and Δx dx), limit of the sum is the integal W = x = D. segment F s x = D ( x) N. segment - integal of F s (x) fom x=d to x=d - adding up all values of F s (x) as a function with the sole vaiable x in&times small incements of dx between the stat point x=d and the end point x=d dx S. Achenbach Phys55 -: Foce Fields 45 S. Achenbach Phys55 -: Foce Fields 47 Wok done by a changing Foce ) calculate the wok done on an object as it is moved though one segment (segment i) segment i is the inteval D + i Δx D + i + Δx [ ( ) ), with its mid point X mid point wok done in segment i is Wsegment i ± Fs ( xmid point ) Δx = ± [ F s D + ( i ) Δx Δx F ( x) F ( x) S = S (wok may be pos. o neg. depending on whethe aids o opposes the movement of the object) ( i + 0. ) Δx = D + 5 ( ) ] ( point ) F s x mid S. Achenbach Phys55 -: Foce Fields 46 Wok done by a changing Foce 3) total wok done by the foce on an object moved fom S to S is appoximately W ± [ Fs ( D Δx) Δx. segment F s ( D +. Δx) Δx + ( D + ( N + 0. ) Δx) Δx] L 5 F s appoximation becomes equality as N fo N (and Δx dx), limit of the sum is the integal W = x = D. segment N. segment Note: integals fo many functions ae well known f0 e.g., one impotant function is F s ( x) = (f 0 is a constant) x F s x = D S. Achenbach Phys55 -: Foce Fields 48 ( x) dx f D dx = D x D D f f

13 S. Achenbach: PHYS 55 (Pat, Topic ) Handouts p. 3 Wok as Aea unde a Cuve fo a function F s (x) that epesents foce as a function of distance integal F s (x) dx has units foce times distance [Nm] aea unde the cuve F s (x) in a foce-vesus-distance gaph has units foce times distance [Nm] wok done [Nm = J] is gaphically epesented by aea unde the cuve F s (x) vesus x between x=d and x=d Gavitational Foce Field a familia consevative foce field is that of gavity magnitude of the foce due to gavitational attaction on the eath (fo an object located above the suface of the eath, i.e. x eath = m) mass 4 m m N F = x kg with - F magnitude of the foce on the object - m mass of the object - x distance fom the cente of the eath to the object units: if m [kg] and x [m] F [N] diection of the foce: towads the cente of the eath Note: stength of the foce due to gavitational attaction deceases quadatically with inceased distance S. Achenbach Phys55 -: Foce Fields 49 S. Achenbach Phys55 -: Foce Fields 5 Example 4 An object is moved a distance of m by a foce. The object is moved along a cuve stating at a point 0 m fom a efeence point S 0 to a point m fom S 0. The tangential component of the foce is F s ( x) = N (x is the distance fom S 0 in metes) x How much enegy is tansfeed fom the foce to the object, i.e. how much wok is done by the foce moving the object? Example 5 How much enegy is equied to move an object with the mass m fom the eath s suface to oute space? S. Achenbach Phys55 -: Foce Fields 50 S. Achenbach Phys55 -: Foce Fields 5

14 S. Achenbach: PHYS 55 (Pat, Topic ) Handouts p. 4 Fequently asked Question Why ae we always consideing the tangential component, e.g. F s (x), only? Answe: Because all the wok is done by the tangential component of the foce, and none by the pependicula component. And why is no wok done by the pependicula component? Answe: - with W = F d = F d cos θ and pependicula θ = 90 cos 90 = 0 wok pependicula to the motion = 0 - and how about motion pependicula to field lines? Well, look. Once upon a time, thee was a table... S. Achenbach Phys55 -: Foce Fields 53 Fequently asked Question Find the wok done if the puck is moved adially away fom the hole, fom 0 cm to 0 cm. F move is in the diection of motion wok done by extenal foce F move will be positive F move is exactly in the diection of motion θ = 0, cos θ = wok done is W = F move d cos θ = F move d = (9.8 N) (0 cm) = 0.98 Nm = 0.98 J In tems of the synthetic plana field, it would be said that the potential enegy of the puck inceased by 0.98 J. But eally, the potential enegy of the kg mass unde the table inceased as it was lifted 0 cm and gained mgh = 0.98 J. we could say the enegy is stoed in the synthetic plana foce field, but eally it is stoed in the gavitational field S. Achenbach Phys55 -: Foce Fields 55 Fequently asked Question conside the synthetic plana foce field set up on the suface of a table the,object is a weightless puck with a nail in it the field foce is ceated synthetically by a sting foce on the sting is povided by a kg mass dangling below the table the suface of the table is fictionless the foce on the puck - is always in the diection to the hole in the table - has a magnitude of mg = 9.8 N fo any position on the table Pependicula Comp. does no Wok component of the wok tangential to the motion (following the diection of field lines) what about the pependicula component? conside the wok done if the puck was moved in a semicicle (pependicula to field lines) ) use common sense to find the wok done potential enegy changes if wok is done potential enegy of the mass unde the table would have to change height of the mass unde the table would have to change height of the mass does not change no wok done while moving puck pependicula to natual movement along field lines S. Achenbach Phys55 -: Foce Fields 54 S. Achenbach Phys55 -: Foce Fields 56

15 S. Achenbach: PHYS 55 (Pat, Topic ) Handouts p. 5 Pependicula Comp. does no Wok component of the wok tangential to the motion (following the diection of field lines) what about the pependicula component? conside the wok done if the puck was moved in a semicicle (pependicula to field lines) ) find the wok done mathematically let x be the distance along the cicula path (x = 0 at stat position of the puck); (x = π = π 0 cm = 0.34 m at end position) fictionless movement on the cicle (mass not lifted): foce along that path F s (x) = 0 (constant fo all x) W = F d = (0 N) (0.34 m) = 0 J Enegy Contou Maps enegy contou maps show the potential enegy of an object as a function of position with espect to a efeence point e.g., - potential enegy of the puck at point B is J moe than when it is at point A (this is equivalent to saying potential enegy of the puck at point B with espect to point A is J ) - potential enegy of the puck at point C with espect to point A is - J - potential enegy of the puck at point B with espect to point C is 4 J no wok done while moving puck pependicula to natual movement along field lines S. Achenbach Phys55 -: Foce Fields 57 S. Achenbach Phys55 -: Foce Fields 59 Enegy Contou Maps enegy contous (o equipotential sufaces) ae sufaces ove which an object can be moved without changing its potential enegy all consevative foce fields have enegy contous e.g., an enegy contou fo the gavitational field of the eath is the suface of a sphee whose cente coesponds with the cente of the eath an object can be moved along an enegy contou with zeo foce (actually, with infinitesimal foce) because component of the field tangent to the enegy contou (pependicula to field line o line of foce ) is zeo Relationship En. Cont. Foce Lines enegy contous must be pependicula to lines of foce set up by the foce field (enegy contous and foce lines intesect at ight angles) in a plane of a foce field, enegy contous ae lines (equipotential lines) e.g., in the plana puck-on-a-sting field : enegy contous ae the cicumfeences of cicles (emembe: it takes no wok to move the puck in a cicumfeence of a cicle centeed on the hole in the table pot. enegy unchanged) S. Achenbach Phys55 -: Foce Fields 58 S. Achenbach Phys55 -: Foce Fields 60

16 S. Achenbach: PHYS 55 (Pat, Topic ) Handouts p. 6 Relationship En. Cont. Foce Lines an enegy contou can be found & dawn on a map that only has the lines of foce shown: daw a line pependicula to the foce line at the choosen point A extend this line so that it is pependicula to all foce lines Relationship En. Cont. Foce Lines e.g., conside a plane of the gavitational field of the eath (containing the cente of the eath, fo example though the equato) a satellite with an elliptical obit does not stay on a cicula enegy contou satellite expeiences a foce in (o opposite to) the diection of motion satellite peiodically changes speed thoughout the obit S. Achenbach Phys55 -: Foce Fields 6 S. Achenbach Phys55 -: Foce Fields 63 Relationship En. Cont. Foce Lines e.g., conside a plane of the gavitational field of the eath (containing the cente of the eath, fo example though the equato) a satellite with a cicula obit stays on a cicula enegy contou satellite expeiences no foce in the diection of motion satellite neve changes speed Relationship En. Cont. Foce Lines an enegy contou can be found & dawn on a map that only has the lines of foce shown: stat with a map showing the foce lines choose a efeence point stating at that point, daw an enegy contou pependicula (intesecting at 90 ) to all foce lines fist enegy countou fo moe contou lines: stat at intesection of the contou line and a foce line and find the distance (on the foce line) that the standad object must be moved fo (e.g.) J of wok (o 0 J o 0 J,...) stating at this new point, daw anothe contou line epeat until complete map is geneated S. Achenbach Phys55 -: Foce Fields 6 S. Achenbach Phys55 -: Foce Fields 64

17 S. Achenbach: PHYS 55 (Pat, Topic ) Handouts p. 7 Example 6 Geneate the enegy contous fo this foce field. The magnitude of the foce on the foce line labled S is constant at F/m = 4.0 N / kg. The efeence enegy contou should go though A. Othe enegy contous should be 0 J / kg apat. Estimating Foce fom a Contou Map enegy contou maps can be used to estimate the aveage foce exeted on an object that is moved between contou lines this foce is appoximately equal to the foce at a point half way between the contous suppose an object is moved along a cuve between points x = D and x = D with a tangential foce opposing the motion F s (x) x D wok done is W = = Fs ( x)dx x = D epesented by aea undeneath the cuve F s (x) between D and D ( ) wok also given by W = Fave D D with F ave = aveage of F s (x) on the inteval (D, D ) S. Achenbach Phys55 -: Foce Fields 65 if W and (D, D ) ae known, F ave can be obtained fom F ave W = D D S. Achenbach Phys55 -: Foce Fields 67 Example 7 Conside the gavitational foce field of the eath. Using the suface of a sphee with the adius i = m as a efeence, find the adius of the sphee whose suface is at an enegy of 0 6 J/kg above the efeence. I.e., at what adius would be a mass of kg if it is lifted fom the suface of the eath (efeence) outwad until a wok of 0 6 J is done? Estimating Foce fom a Contou Map e.g., finding the aveage foce fo a staight line path fom an enegy contou map aveage foce in the diection of movement fom points A to B (with a distance D AB ) F = ave W D AB (D AB can be measued with a ule) 0 J 0 J = = 33.3 N 0.3 m if points A and B ae on the same field line F ave is the aveage of ± F ( x) ove the inteval between points A and B as stated befoe, with x mid point half way between points A and B F ± F ave x mid ( ) point S. Achenbach Phys55 -: Foce Fields 66 S. Achenbach Phys55 -: Foce Fields 68

18 S. Achenbach: PHYS 55 (Pat, Topic ) Handouts p. 8 Example 8 Appoximating the foce at a point with an aveage foce: ) A kg object is moved in a staight line fom A to B, which ae at a distance of m. What is the aveage value of the component of foce that does the wok in moving the object? ) Estimate the foce (i.e. F = F iˆ x + F ˆ y j ) the field exets on a kg mass located at point D. Example 8 ) Estimate the foce (i.e. F = F iˆ x + F ˆ y j ) the field exets on a kg mass located at point D. Solution: Note: this esult is an appoximation because field foce at point D was appoximated with an aveage foce potential eos dawing the field line though point D potential angula eos dawing the un and ise potential measuement eos of the un and ise magnitude? diection / components? S. Achenbach Phys55 -: Foce Fields 69 S. Achenbach Phys55 -: Foce Fields 7 Example 8 ) Estimate the foce (i.e. F = F iˆ x + F ˆ y j ) the field exets on a kg mass located at point D. Solution: the diection of the foce exeted by the field is the same as the diection of the field foce line diection of the field foce line is always fom a point of highe enegy to a point of lowe enegy to sepaate the magnitude of foce F D = 0 N into x and y components, slope of the field line (ise ove un) must be measued (e.g. with a ule) hee: ise = un = ( / ) m F slope = - y = F y = - F F x x fom diection of foce line, F x is negative, F y is positive S. Achenbach Phys55 -: Foce Fields 70

( ) ( ) Review of Force. Review of Force. r = =... Example 1. What is the dot product for F r. Solution: Example 2 ( )

( ) ( ) Review of Force. Review of Force. r = =... Example 1. What is the dot product for F r. Solution: Example 2 ( ) : PHYS 55 (Pat, Topic ) Eample Solutions p. Review of Foce Eample ( ) ( ) What is the dot poduct fo F =,,3 and G = 4,5,6? F G = F G + F G + F G = 4 +... = 3 z z Phs55 -: Foce Fields Review of Foce Eample

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

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 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

ω = θ θ o = θ θ = s r v = rω

ω = θ θ o = θ θ = s r v = rω Unifom Cicula Motion Unifom cicula motion is the motion of an object taveling at a constant(unifom) speed in a cicula path. Fist we must define the angula displacement and angula velocity The angula displacement

More information

= 4 3 π( m) 3 (5480 kg m 3 ) = kg.

= 4 3 π( m) 3 (5480 kg m 3 ) = kg. CHAPTER 11 THE GRAVITATIONAL FIELD Newton s Law of Gavitation m 1 m A foce of attaction occus between two masses given by Newton s Law of Gavitation Inetial mass and gavitational mass Gavitational potential

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

AH Mechanics Checklist (Unit 2) AH Mechanics Checklist (Unit 2) Circular Motion

AH Mechanics Checklist (Unit 2) AH Mechanics Checklist (Unit 2) Circular Motion AH Mechanics Checklist (Unit ) AH Mechanics Checklist (Unit ) Cicula Motion No. kill Done 1 Know that cicula motion efes to motion in a cicle of constant adius Know that cicula motion is conveniently descibed

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

PHYS 1114, Lecture 21, March 6 Contents:

PHYS 1114, Lecture 21, March 6 Contents: PHYS 1114, Lectue 21, Mach 6 Contents: 1 This class is o cially cancelled, being eplaced by the common exam Tuesday, Mach 7, 5:30 PM. A eview and Q&A session is scheduled instead duing class time. 2 Exam

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

Ch 13 Universal Gravitation

Ch 13 Universal Gravitation Ch 13 Univesal Gavitation Ch 13 Univesal Gavitation Why do celestial objects move the way they do? Keple (1561-1630) Tycho Bahe s assistant, analyzed celestial motion mathematically Galileo (1564-1642)

More information

B. Spherical Wave Propagation

B. Spherical Wave Propagation 11/8/007 Spheical Wave Popagation notes 1/1 B. Spheical Wave Popagation Evey antenna launches a spheical wave, thus its powe density educes as a function of 1, whee is the distance fom the antenna. We

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. s r. check whether your calculator is in all other parts of the body. When a rigid body rotates through a given angle, all

Chapter. s r. check whether your calculator is in all other parts of the body. When a rigid body rotates through a given angle, all conveted to adians. Also, be sue to vanced to a new position (Fig. 7.2b). In this inteval, the line OP has moved check whethe you calculato is in all othe pats of the body. When a igid body otates though

More information

AP-C WEP. h. Students should be able to recognize and solve problems that call for application both of conservation of energy and Newton s Laws.

AP-C WEP. h. Students should be able to recognize and solve problems that call for application both of conservation of energy and Newton s Laws. AP-C WEP 1. Wok a. Calculate the wok done by a specified constant foce on an object that undegoes a specified displacement. b. Relate the wok done by a foce to the aea unde a gaph of foce as a function

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

Chap 5. Circular Motion: Gravitation

Chap 5. Circular Motion: Gravitation Chap 5. Cicula Motion: Gavitation Sec. 5.1 - Unifom Cicula Motion A body moves in unifom cicula motion, if the magnitude of the velocity vecto is constant and the diection changes at evey point and is

More information

Physics 111 Lecture 5 Circular Motion

Physics 111 Lecture 5 Circular Motion Physics 111 Lectue 5 Cicula Motion D. Ali ÖVGÜN EMU Physics Depatment www.aovgun.com Multiple Objects q A block of mass m1 on a ough, hoizontal suface is connected to a ball of mass m by a lightweight

More information

AP * PHYSICS B. Circular Motion, Gravity, & Orbits. Teacher Packet

AP * PHYSICS B. Circular Motion, Gravity, & Orbits. Teacher Packet AP * PHYSICS B Cicula Motion, Gavity, & Obits Teache Packet AP* is a tademak of the College Entance Examination Boad. The College Entance Examination Boad was not involved in the poduction of this mateial.

More information

Math Notes on Kepler s first law 1. r(t) kp(t)

Math Notes on Kepler s first law 1. r(t) kp(t) Math 7 - Notes on Keple s fist law Planetay motion and Keple s Laws We conside the motion of a single planet about the sun; fo simplicity, we assign coodinates in R 3 so that the position of the sun is

More information

PS113 Chapter 5 Dynamics of Uniform Circular Motion

PS113 Chapter 5 Dynamics of Uniform Circular Motion PS113 Chapte 5 Dynamics of Unifom Cicula Motion 1 Unifom cicula motion Unifom cicula motion is the motion of an object taveling at a constant (unifom) speed on a cicula path. The peiod T is the time equied

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

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

Momentum is conserved if no external force

Momentum is conserved if no external force Goals: Lectue 13 Chapte 9 v Employ consevation of momentum in 1 D & 2D v Examine foces ove time (aka Impulse) Chapte 10 v Undestand the elationship between motion and enegy Assignments: l HW5, due tomoow

More information

b) (5) What is the magnitude of the force on the 6.0-kg block due to the contact with the 12.0-kg block?

b) (5) What is the magnitude of the force on the 6.0-kg block due to the contact with the 12.0-kg block? Geneal Physics I Exam 2 - Chs. 4,5,6 - Foces, Cicula Motion, Enegy Oct. 13, 2010 Name Rec. Inst. Rec. Time Fo full cedit, make you wok clea to the gade. Show fomulas used, essential steps, and esults with

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

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

Physics 111. Ch 12: Gravity. Newton s Universal Gravity. R - hat. the equation. = Gm 1 m 2. F g 2 1. ˆr 2 1. Gravity G =

Physics 111. Ch 12: Gravity. Newton s Universal Gravity. R - hat. the equation. = Gm 1 m 2. F g 2 1. ˆr 2 1. Gravity G = ics Announcements day, embe 9, 004 Ch 1: Gavity Univesal Law Potential Enegy Keple s Laws Ch 15: Fluids density hydostatic equilibium Pascal s Pinciple This week s lab will be anothe physics wokshop -

More information

Lab #9: The Kinematics & Dynamics of. Circular Motion & Rotational Motion

Lab #9: The Kinematics & Dynamics of. Circular Motion & Rotational Motion Reading Assignment: Lab #9: The Kinematics & Dynamics of Cicula Motion & Rotational Motion Chapte 6 Section 4 Chapte 11 Section 1 though Section 5 Intoduction: When discussing motion, it is impotant to

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 8. Accelerated Circular Motion

Chapter 8. Accelerated Circular Motion Chapte 8 Acceleated Cicula Motion 8.1 Rotational Motion and Angula Displacement A new unit, adians, is eally useful fo angles. Radian measue θ(adians) = s = θ s (ac length) (adius) (s in same units as

More information

Uniform Circular Motion

Uniform Circular Motion Unifom Cicula Motion constant speed Pick a point in the objects motion... What diection is the velocity? HINT Think about what diection the object would tavel if the sting wee cut Unifom Cicula Motion

More information

- 5 - TEST 1R. This is the repeat version of TEST 1, which was held during Session.

- 5 - TEST 1R. This is the repeat version of TEST 1, which was held during Session. - 5 - TEST 1R This is the epeat vesion of TEST 1, which was held duing Session. This epeat test should be attempted by those students who missed Test 1, o who wish to impove thei mak in Test 1. IF YOU

More information

TAMPINES JUNIOR COLLEGE 2009 JC1 H2 PHYSICS GRAVITATIONAL FIELD

TAMPINES JUNIOR COLLEGE 2009 JC1 H2 PHYSICS GRAVITATIONAL FIELD TAMPINES JUNIOR COLLEGE 009 JC1 H PHYSICS GRAVITATIONAL FIELD OBJECTIVES Candidates should be able to: (a) show an undestanding of the concept of a gavitational field as an example of field of foce and

More information

PHYSICS NOTES GRAVITATION

PHYSICS NOTES GRAVITATION GRAVITATION Newton s law of gavitation The law states that evey paticle of matte in the univese attacts evey othe paticle with a foce which is diectly popotional to the poduct of thei masses and invesely

More information

Conflict Exam Issue. Sorry, Can t do it. Please see Kevin Pitts if you have any additional questions or concerns about this. Office is 231 Loomis

Conflict Exam Issue. Sorry, Can t do it. Please see Kevin Pitts if you have any additional questions or concerns about this. Office is 231 Loomis Conflict Exam Issue. Soy, Can t do it I was told that: Students can only be excused fom the scheduled final fo illness, death in the family o eligious holiday. No exceptions. Please see Kevin Pitts if

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

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

! 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

Physics 181. Assignment 4

Physics 181. Assignment 4 Physics 181 Assignment 4 Solutions 1. A sphee has within it a gavitational field given by g = g, whee g is constant and is the position vecto of the field point elative to the cente of the sphee. This

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

Chapter 5. Uniform Circular Motion. a c =v 2 /r

Chapter 5. Uniform Circular Motion. a c =v 2 /r Chapte 5 Unifom Cicula Motion a c =v 2 / Unifom cicula motion: Motion in a cicula path with constant speed s v 1) Speed and peiod Peiod, T: time fo one evolution Speed is elated to peiod: Path fo one evolution:

More information

Gravitation. AP/Honors Physics 1 Mr. Velazquez

Gravitation. AP/Honors Physics 1 Mr. Velazquez Gavitation AP/Honos Physics 1 M. Velazquez Newton s Law of Gavitation Newton was the fist to make the connection between objects falling on Eath and the motion of the planets To illustate this connection

More information

Motion in One Dimension

Motion in One Dimension Motion in One Dimension Intoduction: In this lab, you will investigate the motion of a olling cat as it tavels in a staight line. Although this setup may seem ovesimplified, you will soon see that a detailed

More information

Circular Orbits. and g =

Circular Orbits. and g = using analyse planetay and satellite motion modelled as unifom cicula motion in a univesal gavitation field, a = v = 4π and g = T GM1 GM and F = 1M SATELLITES IN OBIT A satellite is any object that is

More information

MAGNETIC FIELD INTRODUCTION

MAGNETIC FIELD INTRODUCTION MAGNETIC FIELD INTRODUCTION It was found when a magnet suspended fom its cente, it tends to line itself up in a noth-south diection (the compass needle). The noth end is called the Noth Pole (N-pole),

More information

When a mass moves because of a force, we can define several types of problem.

When a mass moves because of a force, we can define several types of problem. Mechanics Lectue 4 3D Foces, gadient opeato, momentum 3D Foces When a mass moves because of a foce, we can define seveal types of poblem. ) When we know the foce F as a function of time t, F=F(t). ) When

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 101 Lecture 6 Circular Motion

Physics 101 Lecture 6 Circular Motion Physics 101 Lectue 6 Cicula Motion Assist. Pof. D. Ali ÖVGÜN EMU Physics Depatment www.aovgun.com Equilibium, Example 1 q What is the smallest value of the foce F such that the.0-kg block will not slide

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

(read nabla or del) is defined by, k. (9.7.1*)

(read nabla or del) is defined by, k. (9.7.1*) 9.7 Gadient of a scala field. Diectional deivative Some of the vecto fields in applications can be obtained fom scala fields. This is vey advantageous because scala fields can be handled moe easily. The

More information

Midterm Exam #2, Part A

Midterm Exam #2, Part A Physics 151 Mach 17, 2006 Midtem Exam #2, Pat A Roste No.: Scoe: Exam time limit: 50 minutes. You may use calculatos and both sides of ONE sheet of notes, handwitten only. Closed book; no collaboation.

More information

Physics C Rotational Motion Name: ANSWER KEY_ AP Review Packet

Physics C Rotational Motion Name: ANSWER KEY_ AP Review Packet Linea and angula analogs Linea Rotation x position x displacement v velocity a T tangential acceleation Vectos in otational motion Use the ight hand ule to detemine diection of the vecto! Don t foget centipetal

More information

Chapter 5. really hard to start the object moving and then, once it starts moving, you don t have to push as hard to keep it moving.

Chapter 5. really hard to start the object moving and then, once it starts moving, you don t have to push as hard to keep it moving. Chapte 5 Fiction When an object is in motion it is usually in contact with a viscous mateial (wate o ai) o some othe suface. So fa, we have assumed that moving objects don t inteact with thei suoundings

More information

Objective Notes Summary

Objective Notes Summary Objective Notes Summay An object moving in unifom cicula motion has constant speed but not constant velocity because the diection is changing. The velocity vecto in tangent to the cicle, the acceleation

More information

Chapter 12. Kinetics of Particles: Newton s Second Law

Chapter 12. Kinetics of Particles: Newton s Second Law Chapte 1. Kinetics of Paticles: Newton s Second Law Intoduction Newton s Second Law of Motion Linea Momentum of a Paticle Systems of Units Equations of Motion Dynamic Equilibium Angula Momentum of a Paticle

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

Physics 1114: Unit 5 Hand-out Homework (Answers)

Physics 1114: Unit 5 Hand-out Homework (Answers) Physics 1114: Unit 5 Hand-out Homewok (Answes) Poblem set 1 1. The flywheel on an expeimental bus is otating at 420 RPM (evolutions pe minute). To find (a) the angula velocity in ad/s (adians/second),

More information

Phys 201A. Homework 6 Solutions. F A and F r. B. According to Newton s second law, ( ) ( )2. j = ( 6.0 m / s 2 )ˆ i ( 10.4m / s 2 )ˆ j.

Phys 201A. Homework 6 Solutions. F A and F r. B. According to Newton s second law, ( ) ( )2. j = ( 6.0 m / s 2 )ˆ i ( 10.4m / s 2 )ˆ j. 7. We denote the two foces F A + F B = ma,sof B = ma F A. (a) In unit vecto notation F A = ( 20.0 N)ˆ i and Theefoe, Phys 201A Homewok 6 Solutions F A and F B. Accoding to Newton s second law, a = [ (

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

15 B1 1. Figure 1. At what speed would the car have to travel for resonant oscillations to occur? Comment on your answer.

15 B1 1. Figure 1. At what speed would the car have to travel for resonant oscillations to occur? Comment on your answer. Kiangsu-Chekiang College (Shatin) F:EasteHolidaysAssignmentAns.doc Easte Holidays Assignment Answe Fom 6B Subject: Physics. (a) State the conditions fo a body to undego simple hamonic motion. ( mak) (a)

More information

to point uphill and to be equal to its maximum value, in which case f s, max = μsfn

to point uphill and to be equal to its maximum value, in which case f s, max = μsfn Chapte 6 16. (a) In this situation, we take f s to point uphill and to be equal to its maximum value, in which case f s, max = μsf applies, whee μ s = 0.5. pplying ewton s second law to the block of mass

More information

Physics: Work & Energy Beyond Earth Guided Inquiry

Physics: Work & Energy Beyond Earth Guided Inquiry Physics: Wok & Enegy Beyond Eath Guided Inquiy Elliptical Obits Keple s Fist Law states that all planets move in an elliptical path aound the Sun. This concept can be extended to celestial bodies beyond

More information

Revision Guide for Chapter 11

Revision Guide for Chapter 11 Revision Guide fo Chapte 11 Contents Revision Checklist Revision Notes Momentum... 4 Newton's laws of motion... 4 Wok... 5 Gavitational field... 5 Potential enegy... 7 Kinetic enegy... 8 Pojectile... 9

More information

CIRCULAR MOTION. Particle moving in an arbitrary path. Particle moving in straight line

CIRCULAR MOTION. Particle moving in an arbitrary path. Particle moving in straight line 1 CIRCULAR MOTION 1. ANGULAR DISPLACEMENT Intoduction: Angle subtended by position vecto of a paticle moving along any abitay path w..t. some fixed point is called angula displacement. (a) Paticle moving

More information

10. Force is inversely proportional to distance between the centers squared. R 4 = F 16 E 11.

10. Force is inversely proportional to distance between the centers squared. R 4 = F 16 E 11. NSWRS - P Physics Multiple hoice Pactice Gavitation Solution nswe 1. m mv Obital speed is found fom setting which gives v whee M is the object being obited. Notice that satellite mass does not affect obital

More information

Potential Energy and Conservation of Energy

Potential Energy and Conservation of Energy Potential Enegy and Consevation of Enegy Consevative Foces Definition: Consevative Foce If the wok done by a foce in moving an object fom an initial point to a final point is independent of the path (A

More information

Chapter 7-8 Rotational Motion

Chapter 7-8 Rotational Motion Chapte 7-8 Rotational Motion What is a Rigid Body? Rotational Kinematics Angula Velocity ω and Acceleation α Unifom Rotational Motion: Kinematics Unifom Cicula Motion: Kinematics and Dynamics The Toque,

More information

Lab 10: Newton s Second Law in Rotation

Lab 10: Newton s Second Law in Rotation Lab 10: Newton s Second Law in Rotation We can descibe the motion of objects that otate (i.e. spin on an axis, like a popelle o a doo) using the same definitions, adapted fo otational motion, that we have

More information

EN40: Dynamics and Vibrations. Midterm Examination Thursday March

EN40: Dynamics and Vibrations. Midterm Examination Thursday March EN40: Dynamics and Vibations Midtem Examination Thusday Mach 9 2017 School of Engineeing Bown Univesity NAME: Geneal Instuctions No collaboation of any kind is pemitted on this examination. You may bing

More information

PHYS 1410, 11 Nov 2015, 12:30pm.

PHYS 1410, 11 Nov 2015, 12:30pm. PHYS 40, Nov 205, 2:30pm. A B = AB cos φ x = x 0 + v x0 t + a 2 xt 2 a ad = v2 2 m(v2 2 v) 2 θ = θ 0 + ω 0 t + 2 αt2 L = p fs µ s n 0 + αt K = 2 Iω2 cm = m +m 2 2 +... m +m 2 +... p = m v and L = I ω ω

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

SHORT ANSWER. Write the word or phrase that best completes each statement or answers the question.

SHORT ANSWER. Write the word or phrase that best completes each statement or answers the question. Math Pecalculus Ch. 6 Review Name SHORT ANSWER. Wite the wod o phase that best completes each statement o answes the question. Solve the tiangle. ) ) 6 7 0 Two sides and an angle (SSA) of a tiangle ae

More information

Phys 201A. Homework 5 Solutions

Phys 201A. Homework 5 Solutions Phys 201A Homewok 5 Solutions 3. In each of the thee cases, you can find the changes in the velocity vectos by adding the second vecto to the additive invese of the fist and dawing the esultant, and by

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

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

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

PHYS Summer Professor Caillault Homework Solutions. Chapter 5

PHYS Summer Professor Caillault Homework Solutions. Chapter 5 PHYS 1111 - Summe 2007 - Pofesso Caillault Homewok Solutions Chapte 5 7. Pictue the Poblem: The ball is acceleated hoizontally fom est to 98 mi/h ove a distance of 1.7 m. Stategy: Use equation 2-12 to

More information

Force can be exerted by direct contact between bodies: Contact Force.

Force can be exerted by direct contact between bodies: Contact Force. Chapte 4, Newton s Laws of Motion Chapte IV NEWTON S LAWS OF MOTION Study of Dynamics: cause of motion (foces) and the esistance of objects to motion (mass), also called inetia. The fundamental Pinciples

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

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

c) (6) Assuming the tires do not skid, what coefficient of static friction between tires and pavement is needed?

c) (6) Assuming the tires do not skid, what coefficient of static friction between tires and pavement is needed? Geneal Physics I Exam 2 - Chs. 4,5,6 - Foces, Cicula Motion, Enegy Oct. 10, 2012 Name Rec. Inst. Rec. Time Fo full cedit, make you wok clea to the gade. Show fomulas used, essential steps, and esults with

More information

2 E. on each of these two surfaces. r r r r. Q E E ε. 2 2 Qencl encl right left 0

2 E. on each of these two surfaces. r r r r. Q E E ε. 2 2 Qencl encl right left 0 Ch : 4, 9,, 9,,, 4, 9,, 4, 8 4 (a) Fom the diagam in the textbook, we see that the flux outwad though the hemispheical suface is the same as the flux inwad though the cicula suface base of the hemisphee

More information

ROTATORY MOTION HORIZONTAL AND VERTICAL CIRCULAR MOTION

ROTATORY MOTION HORIZONTAL AND VERTICAL CIRCULAR MOTION ROTATORY MOTION HORIZONTAL AND VERTICAL CIRCULAR MOTION POINTS TO REMEMBER 1. Tanslatoy motion: Evey point in the body follows the path of its peceding one with same velocity including the cente of mass..

More information

Chapter 4: The laws of motion. Newton s first law

Chapter 4: The laws of motion. Newton s first law Chapte 4: The laws of motion gavitational Electic magnetic Newton s fist law If the net foce exeted on an object is zeo, the object continues in its oiginal state of motion: - an object at est, emains

More information

Δt The textbook chooses to say that the average velocity is

Δt The textbook chooses to say that the average velocity is 1-D Motion Basic I Definitions: One dimensional motion (staight line) is a special case of motion whee all but one vecto component is zeo We will aange ou coodinate axis so that the x-axis lies along the

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

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

PHYSICS 1210 Exam 2 University of Wyoming 14 March ( Day!) points

PHYSICS 1210 Exam 2 University of Wyoming 14 March ( Day!) points PHYSICS 1210 Exam 2 Univesity of Wyoming 14 Mach ( Day!) 2013 150 points This test is open-note and closed-book. Calculatos ae pemitted but computes ae not. No collaboation, consultation, o communication

More information

Unit 6 Practice Test. Which vector diagram correctly shows the change in velocity Δv of the mass during this time? (1) (1) A. Energy KE.

Unit 6 Practice Test. Which vector diagram correctly shows the change in velocity Δv of the mass during this time? (1) (1) A. Energy KE. Unit 6 actice Test 1. Which one of the following gaphs best epesents the aiation of the kinetic enegy, KE, and of the gaitational potential enegy, GE, of an obiting satellite with its distance fom the

More information

PY208 Matter & Interactions Final Exam S2005

PY208 Matter & Interactions Final Exam S2005 PY Matte & Inteactions Final Exam S2005 Name (pint) Please cicle you lectue section below: 003 (Ramakishnan 11:20 AM) 004 (Clake 1:30 PM) 005 (Chabay 2:35 PM) When you tun in the test, including the fomula

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

MODULE 5 ADVANCED MECHANICS GRAVITATIONAL FIELD: MOTION OF PLANETS AND SATELLITES VISUAL PHYSICS ONLINE

MODULE 5 ADVANCED MECHANICS GRAVITATIONAL FIELD: MOTION OF PLANETS AND SATELLITES VISUAL PHYSICS ONLINE VISUAL PHYSICS ONLINE MODULE 5 ADVANCED MECHANICS GRAVITATIONAL FIELD: MOTION OF PLANETS AND SATELLITES SATELLITES: Obital motion of object of mass m about a massive object of mass M (m

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

MODULE 5 ADVANCED MECHANICS GRAVITATIONAL FIELD: MOTION OF PLANETS AND SATELLITES VISUAL PHYSICS ONLINE

MODULE 5 ADVANCED MECHANICS GRAVITATIONAL FIELD: MOTION OF PLANETS AND SATELLITES VISUAL PHYSICS ONLINE VISUAL PHYSICS ONLIN MODUL 5 ADVANCD MCHANICS GRAVITATIONAL FILD: MOTION OF PLANTS AND SATLLITS SATLLITS: Obital motion of object of mass m about a massive object of mass M (m

More information

Physics 211: Newton s Second Law

Physics 211: Newton s Second Law Physics 211: Newton s Second Law Reading Assignment: Chapte 5, Sections 5-9 Chapte 6, Section 2-3 Si Isaac Newton Bon: Januay 4, 1643 Died: Mach 31, 1727 Intoduction: Kinematics is the study of how objects

More information

Rotational Motion: Statics and Dynamics

Rotational Motion: Statics and Dynamics Physics 07 Lectue 17 Goals: Lectue 17 Chapte 1 Define cente of mass Analyze olling motion Intoduce and analyze toque Undestand the equilibium dynamics of an extended object in esponse to foces Employ consevation

More information

ESCI 342 Atmospheric Dynamics I Lesson 3 Fundamental Forces II

ESCI 342 Atmospheric Dynamics I Lesson 3 Fundamental Forces II Reading: Matin, Section. ROTATING REFERENCE FRAMES ESCI 34 Atmospheic Dnamics I Lesson 3 Fundamental Foces II A efeence fame in which an object with zeo net foce on it does not acceleate is known as an

More information

UNIVERSITY OF SASKATCHEWAN Department of Physics and Engineering Physics

UNIVERSITY OF SASKATCHEWAN Department of Physics and Engineering Physics UNIVERSITY OF SASKATCHEWAN Depatment of Physics and Engineeing Physics Physics 115.3 Physics and the Univese FINAL EXAMINATION Decembe 21, 2016 NAME: (Last) Please Pint (Given) Time: 3 hous STUDENT NO.:

More information