Math 259 Winter Handout 6: In-class Review for the Cumulative Final Exam

Size: px
Start display at page:

Download "Math 259 Winter Handout 6: In-class Review for the Cumulative Final Exam"

Transcription

1 Math 259 Winte 2009 Handout 6: In-class Review fo the Cumulative Final Exam The topics coveed by the cumulative final exam include the following: Paametic cuves. Finding fomulas fo paametic cuves. Dawing gaphs of cuves defined by paametic equations. Finding tangent lines to cuves defined by paametic equations. Finding the aea beneath (between the cuve and the x-axis) a paametic cuve. Finding the ac length of a paametic cuve. Pola coodinates fo the xy-plane. Identifying egions of the xy-plane descibed by pola coodinates. Conveting Catesian equations to pola equations. Conveting pola equations to Catesian equations. Sketching cuves in the xy-plane defined by pola equations. Finding fomulas fo tangent lines to cuves defined by pola equations. Finding aeas enclosed by pola cuves. Finding ac lengths of cuves defined by pola equations. Conic sections in Catesian and pola coodinates. Sketching conic sections defined by pola equations. Identifying eccenticity, diectix, etc. fom a pola equation. Classifying conic sections using eccenticity. Equations of lines, planes and sphees in 3D. Combining vectos. Magnitude of a vecto. Unit vectos. Applications of vectos in physics. Dot poduct of vectos. Angle between vectos. Othogonality. Vecto pojections. Coss poduct of vectos. Geomety of the coss poduct. Coss poduct and aeas. Calculating volumes with the scala tiple poduct. Finding equations fo lines and planes in 3D using the coss poduct. Distances fom points to lines and planes, and fom lines to planes. Symmetic equations. Sketching sufaces in 3D using contou plots. Intepeting contou plots. Classifying quadic sufaces. Recognizing planes, quadic sufaces and cylindes fom thei equations. Ceating and using vecto functions in 3D. Velocities and tangent vectos fo vecto functions (including unit tangent vectos). Showing that limits in 2D do not exist using a vaiety of stategies (e.g. y = mx, contou plots o tables). Evaluating and using functions with seveal input vaiables. Poving that limits do exist using the ε-δ definition. Calculating values fo limits/showing limits exist using the Squeezing Theoem. Calculating and intepeting patial deivatives. Finding equations fo tangent planes. Using the tangent plane to calculate a linea appoximation. Calculating total diffeentials fo functions. Using total diffeentials to estimate changes and eos. Using the Chain Rule fo functions of seveal vaiables. Calculating diectional deivatives fo functions. Calculating gadient vectos. Finding the diection of maximum ate of change (and magnitude of the maximum ate of change). Intepeting the pactical meaning of a diectional deivative. Finding and classifying (local maximum, local minimum, saddle point) the citical points of a function of seveal vaiables using patial deivatives and the Jacobian deteminant. Finding the global maximum and global minimum of a continuous function ove a egion in the xy-plane. Lagange Multiplies. Lagange Multiplies with two constaints. Wod poblems that can be solved using Lagange Multiplies.

2 Double Riemann sums. The Midpoint Rule fo double Riemann sums (no eo estimates). Setting up double integals. Changing the ode of integation in a double integal. Evaluating double integals. Applications of double integals to chemisty and physics (e.g. volume, mass, cente of mass). Pola coodinates. Conveting double integals fom Catesian to pola coodinates. Setting up double integals in pola coodinates. Evaluating double integals in pola coodinates. Setting up tiple integals. Changing the ode of integation fo a tiple integal. Evaluating tiple integals. Applications of tiple integals (e.g. calculating volume and mass). Setting up and evaluating tiple integals in cylindical/pola coodinates. Setting up and evaluating tiple integals in spheical coodinates. Dawing two-dimensional vecto fields. Associating fomulas fo two-dimensional vecto fields with visual epesentations. Detemining whethe a vecto field is consevative o not. Finding potential functions fo consevative vecto fields. Setting up paametic equations fo cuves in two dimensions. Setting up and evaluating (diectly) line integals of functions in two dimensions. Setting up and evaluating (diectly) line integals of vecto fields in two and thee dimensions. Calculating line integals of consevative vecto fields using the Fundamental Theoem. Calculating line integals in two dimensions using Geen s Theoem. Divegence and cul opeatos. Setting up and evaluating suface integals. Evaluating suface integals using Stoke s Theoem and the Divegence Theoem. 1. Find symmetic equations fo the line of intesection of the planes: x - y + z = 5 2x + y - 3z = 4.

3 2. Find the aeas of the plana (flat) shapes that have vetices located at: (a) (0, 0), (4, 1), (2, 3), and (6, 4). (b) (2, -3), (1, 1), (5, -6), and (4, -2). (c) (0, 0, 0), (0, 1, 0), and (1, 1, 0). (d) (1, 3, 0), (0, 2, 5), and (-1, 0, 2).

4 3. (a) Detemine values of λ and µ so that the points (-1, 3, 2), (-4, 2, -2) and (5, λ, µ) lie on a staight line. (b) Find a value of λ that will make the thee vectos: a = I + j + k b = 2I - 4k c = I + λj +3k coplana. (c) Suppose that the pais of vectos A and B, and C and D each detemine a plane. Show that if these planes ae paallel, then: (A B) (C D) = 0.

5 4. Conside the cuve in the plane defined by the paametic equations: x(t) = sin(t) y(t) = sin(2t) 0 t π. (a) Sketch the gaph of this cuve in the xy plane. (b) Find the total length of the cuve. (c) Find the aea enclosed by this cuve.

6 5. In this poblem we will conside the two lines given by: x = 1 - t, y = -2 + t, z = 2t and x = 4+ s, y = 1 + 3s, z = -3 + s. (a) Detemine whethe o not these lines ae paallel. (b) If the lines ae not paallel, do they intesect? If so, find the coodinates of the point of intesection. (c) Find the minimum distance between the two lines?

7 6. In each of the following cases, find the volume of the paallelpiped that has vetices at the points listed. (a) (1, 1, 1), (-4, 2, 7), (3, 5, 7) and (0, 1, 6). (b) (1, 6, 1), (-2, 4, 2), (3, 0, 0), and (2, 2, -4). (c) (1, 1, 1), (2, 2, 2), (6, 1, 3), and (-2, 4, 6).

8 7. An astoid (not to be confused with an asteoid) is a mathematical cuve with the equation, x 2 / 3 + y 2 / 3 =1. This cuve can be descibed by the paametic equations: x = cos 3 (t) and y = sin 3 (t) with 0 t 2π. (a) Sketch a gaph of the astoid. (b) Find a fomula fo dy dx the astoid. (c) What is the total length of the astoid? (d) Set up an integal that gives the aea enclosed by the astoid.

9 8. The position vecto of a paticle moving in the xy plane is given below. (t) = e t sin(t)i + e t cos(t)j (a) Sketch the path of the paticle beginning with t = 0. (b) Find the tangential component of the paticle s acceleation. (That is, the vecto pojection of the acceleation vecto onto the velocity vecto.) (c) Find the nomal component of the paticle s acceleation. (That is, the component of the acceleation vecto that is nomal to the velocity vecto.) (d) How could you deduce fom the sketch in pat (a) that the nomal component of the acceleation was going to be non-zeo? (e) Descibe the motion of a paticle that would have a zeo nomal component of acceleation.

10 9. (a) Find an equation fo the plane that includes both the point (1, 3, 0) and the line x, y,z = 2,7,1 + t " #1,1,1. Expess you final answe in the fom: ax + by + cz = d. (b) The diagam given below shows a weight of 10 pounds suspended fom a cod. Calculate the tension vecto, T 2, in the cod to the ight of the suspended weight. Calculate the vecto, not just the magnitude of the vecto. 45 o 30 o T 1 T 2 10 pounds

11 10. In this poblem u, v and w will always efe to the following vectos: (a) u = <1, 2, 3> Calculate v " w. v = < 7, 14, 21> w = <0, 1, 1>. (b) Calculate the volume of the paallelpiped whose sides ae fomed by the vectos u, v and w. (c) Calculate u " v. (d) What can you conclude about the vectos u and v? Cicle any of the statements that you believe to be tue. i. ii. iii. iv. v. u and v ae paallel (o anti-paallel). u and v ae both pependicula to the vecto v " w. u and v ae othogonal. u and v ae unit vectos. u is a unit vecto. v

12 11. Two lines ae defined below using thei symmetic equations. and x - 1 = 2(y + 1) = 3(z - 2) x - 3 = 2(y - 1) = 3(z + 1). (a) Show that these lines ae paallel. (b) Find an equation fo the plane that contains these lines.

13 12. Conside the suface defined by the equation, z = cos(xy). (a) Calculate the equations of the level cuves of this suface. (b) Sketch some of the level cuves in the xy plane. (c) Use the level cuves to sketch a pictue of the suface in thee dimensions.

14 13. Find and classify all of the citical points (local minimums, local maximums, saddle points, etc.) of the suface defined by the equation: f(x, y) = x 2 + xy + y 2 6x + 2.

15 14. In this poblem, g(x, y) will efe to the function defined by the fomula: g( x, y) = xy x 2 + y 2. (a) The gaph z = g(x, y) is shown below. Based on the appeaance of this gaph, do you think that g(x, y) has a limit as (x, y) (0, 0)? (b) Eithe pove that g(x, y) has a limit as (x, y) (0, 0) o show that the limit does not exist. ( Pove hee means use the ε δ definition.)

16 15. Descibe the level sufaces of the following functions. In each case, pove that the function has a limit as (x, y) (0, 0) o show that the limit does not exist. ( Pove hee means use the ε δ definition.) (a) f(x, y) = xy (b) f ( x, y) = x + y x " y (c) f ( x, y) = e 1/ ( x 2 +y 2 )

17 16. Find the equation of the tangent plane to the given suface at the given point. (a) z = y 2 - x 2. (-4, 5, 9) (b) z = ln(2x + y). (-1, 3, 0) (c) f ( x, y) = x 2 + 3y 2 " 2xy, (2, 2, 8).

18 17. The tempeatue, T, in a metal ball is invesely popotional to the distance fom the cente of the ball (which we will assume is located at the oigin). The tempeatue at the point (1, 2, 2) is 120 degees centigade. (a) Find the ate of change in T at (1, 2, 2) in the diection towads the point (2, 1, 3). (b) Show that at any point in the ball, the diection of geatest incease in tempeatue is a vecto pointing diectly towads the oigin. (c) Find a fomula fo the geatest possible ate of change of tempeatue at the point (x, y, z) (whee (x, y, z) (0, 0, 0)).

19 18. In this poblem the function f(x, y, z) will always efe to the function defined by the fomula: f ( x, y,z) =10e "0.01 ( 3x 2 "y 2 "2z 2 ). This function gives the tempeatue of a snake (on a plane) in degees Celsius ( o C). The coodinates of the snake s physical location (x, y, z) ae all measued in metes. (a) The snake is located at the point (1, 1, 1) and plans to slithe in the diection given by the vecto v = 1,2,3. What is the ate of change of tempeatue that the snake will expeience? Give appopiate units with you answe. (b) Snakes ae cold blooded and enjoy wamth. Conside the snake sitting at the point (1, 1, 1). In what diection should the snake slithe to maximize the ate of change of tempeatue? (c) What ate of change of tempeatue will the snake expeience if it stats at the point (1, 1, 1) and slithes in the diection you calculated in (b)? Give appopiate units with you answe.

20 19. In this poblem, z = f(x, y) is the function of x and y defined by the following fomula: z = f (x, y) = e "x +y 2. (a) Suppose that x and y ae both functions of t. All that you can assume about the functions x and y is listed below. Calculate z "(2). x(2) =1 y(2) = "1 x "(2) = #3 y "(2) = 1 2 (b) Suppose instead that x and y ae both functions of t and s, i.e. x = x(t, s) and y = y(t, s). All that you can assume about the functions x and y is listed below. x(2,0) =1 y(2,0) = "1 x t (2,0) = "3 y t (2,0) = 2 x s (2,0) = " 1 y 2 s (2,0) =1 Calculate z s ( 2,0). Show you wok!

21 20. The mantis shimp (Squilla empusa) is a small shimp-like custacean with vey poweful font claws. These shimp ae sometimes called thumb splittes because they can hit so had with thei claws that they sometimes split peoples thumbs open. A public aquaium is planning to exhibit mantis shimp. They will need to build a special tank with a slate bottom and glass sides. The eason fo this is that sometimes the shimp pound on the bottom of the tank with thei claws and can beak a glass bottom. The shimp don t jump, so the tank doesn t need a lid. The tank must have a volume of 1,000,000 cm 3 of wate. Glass costs 10 cents pe squae centimete, and slate costs 50 cents pe squae centimete. Find the dimensions of the least expensive tank that will hold 1,000,000 cm 3 of wate.

22 21. Find the coodinates of the point (o points) on the suface, that ae closest to the oigin (0, 0, 0). xy 2 z 3 = 2

23 22. When an electical cuent I entes two esistos with esistances R 1 and R 2, that ae connected in paallel (see below), it splits into two cuents I 1 and I 2 (with I = I 1 + I 2 ) so that the total electical powe, P = R 1 I R 2 I 2 2 is minimized. (a) Find fomulas fo I 1 and I 2 in tems of I and the two esistances, R 1 and R 2. (b) Show that the two esistances ae equivalent to a single esistance, R, whee: 1 R = 1 R R 2.

24 23. A snake (on a plane) has found a wam metal plate to slithe aound on. The tempeatue of the plate (given in o C) at a point (x and y ae both measued in metes) is given by the function: T( x, y) = 4x 2 " 4xy + y 2. The snake slithes aound in a path that looks exactly like a cicle of adius 5 metes centeed on the oigin. What ae the highest and lowest tempeatues encounteed by the snake as it slithes aound this cicula path?

25 24. In this poblem the function f(x, y) will always efe to the function defined by the fomula: f ( x, y) = xy " x " y + 3. (a) Find the x and y coodinates of any citical points of f(x, y). (b) Classify the citical points that you found in Pat (a) as local maximums, local minimums o saddle points. (c) Find the global maximum and global minimum of f(x, y) on the tiangula egion of the fist quadant with vetices located at the points (0, 0), (2, 0) and (0, 4).

26 25. Each of the following integals is vey difficult to wok out. Revese the ode of integation to make the integal easie, and then evaluate. 1 3 (a) " " e x 2 dxdy 0 3y ( ) 3 9 (b) " " y cos x 2 dxdy 0 y 2 (c) # 1 0 " / 2 # cos( x) 1+ cos 2 ( x) dxdy acsin( y)

27 26. Find the volumes of the egions descibed below. (a) Unde the paaboloid z = x 2 + y 2 and above the egion bounded by y = x 2 and x = y 2. (b) Unde the suface z = xy and above the tiangle with vetices (1, 1), (4, 1) and (1, 2). (c) Bounded by the cylinde x 2 + y 2 = 9 and the planes x = 0, y = 0, x + 2y = 2 in the fist octant.

28 27. Use pola coodinates to evaluate the integals given below. (a) "" xyda whee R is the egion in the fist quadant between the cicles x 2 + y 2 = 4 and x 2 + y 2 = R 25. (b) e "x 2 "y ## 2 da whee D is the egion bounded by the semi-cicle x = 4 " y 2 and the y-axis. D (c) 1 x 2 x 2 4"x # # xydydx + # # xydydx + # # 2 xydydx. 1/ 2 1"x

29 28. Find the coodinates of the cente of mass of a unifom sheet of mateial in the shape of an isosceles ight tiangle. The two equal sides both have length a, and the density of the mateial is popotional to the squae of the distance fom the vetex opposite the hypoteneuse.

30 29. The aveage value of a function f(x, y, z) ove a solid egion E is defined to be: aveage = 1 V E ( ) """ f ( x, y,z)dv, E whee V(E) is the volume of the egion E. Find the aveage value of f(x, y, z) = xyz ove the cube with side length L with one vetex at the oigin and sides paallel to the coodinate axes.

31 30. (a) Calculate the value of the tiple integal: e " ( x 2 +y 2 +z 2 ) 3 2 ### dv, whee B is the solid sphee of adius a > 0 centeed at the oigin. You final answe should contain the lette a. B (b) Conside the vecto field F x, y,z ( ) defined by the fomula: F ( x, y,z) = "3x x 2 + y 2 + z 2 # e " ( x 2 +y 2 +z 2 ) 3 2,"3y x 2 + y 2 + z 2 # e " ( x 2 +y 2 +z 2 ) 3 2,"3z x 2 + y 2 + z 2 # e " ( x 2 +y 2 +z 2 ) 3 2 Calculate value of the line integal: 0, 0) and (0, 1, 1). " F d, whee C is the line segment joining the points (2, C

32 31. (a) The suface S is the pat of the paaboloid z = x 2 + y 2 that lies inside the cylinde x 2 + y 2 = 4. Use the axes povided below to make an accuate sketch of the suface S. z x y (b) Set up a tiple integal in x, y, z coodinates that will give the volume enclosed by the suface S, the cylinde x 2 + y 2 = 4 and the plane z = 0. (c) Convet you integal fom Pat (b) to cylindical coodinates and use this to calculate the volume enclosed by the suface S, the cylinde x 2 + y 2 = 4 and the plane z = 0.

33 32. The diagams given below show fou vecto fields. Match each pictue of a vecto field with one of the fomulas given below. You should have one unmatched fomula at the end of the poblem. DIAGRAM A DIAGRAM B DIAGRAM C DIAGRAM D (a) F x, y ( ) = x, 1 y MATCHING PICTURE: (b) F ( x, y) = 1 y,y MATCHING PICTURE: (c) (d) F x, y ( ) = sin x ( ), y MATCHING PICTURE: F ( x, y) = 1 y,x MATCHING PICTURE: (e) F x, y ( ) = y, x MATCHING PICTURE:

34 # diectly (i.e. not using Geen s C Theoem) whee C is the cuve shown in the diagam given below. 33. (a) Evaluate the line integal: y 2 dx + 3xy " dy 2 y (!1, 1.5) (1, 1.5) 1 x -1 1 (b) Evaluate the line integal: y 2 dx + 3xy " dy # using Geen s Theoem. C

35 "", whee S is the suface of the ectangula S pism shown in the diagam given below with positive oientation. (The vetex of the pism obscued in the diagam is ( 4, 2, 1).) 34. Evaluate the suface integal 3x,4 y,5z ds z (-4, -2, 1) (-4, 2, 1) (4, -2, 1) (4, 2, 1) (-4, 2, -1) y (4, -2, -1) (4, 2, -1) x

36 "", whee f x, y 35. (a) Evaluate the suface integal f ( x, y,z)ds of the paaboloid z = x 2 + y 2 that lies inside the cylinde x 2 + y 2 = 4. S ( ) =1+ xy and S is the pat NOTE: The following integal fomula may be helpful: " d = ( 1+ 42) C. (b) Evaluate the suface integal: ## xz,"yz,"5 ds, whee S is the hemispheical suface z = 4 " x 2 " y 2. S NOTE: The following integal fomula may be helpful: " sin 2 ( x)dx = 1 x # 1 sin 2x 2 4 ( ) + C and cos2 x " ( )dx = 1 x sin ( 2x ) + C.

Math 2263 Solutions for Spring 2003 Final Exam

Math 2263 Solutions for Spring 2003 Final Exam Math 6 Solutions fo Sping Final Exam ) A staightfowad appoach to finding the tangent plane to a suface at a point ( x, y, z ) would be to expess the cuve as an explicit function z = f ( x, y ), calculate

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

Question Bank. Section A. is skew-hermitian matrix. is diagonalizable. (, ) , Evaluate (, ) 12 about = 1 and = Find, if

Question Bank. Section A. is skew-hermitian matrix. is diagonalizable. (, ) , Evaluate (, ) 12 about = 1 and = Find, if Subject: Mathematics-I Question Bank Section A T T. Find the value of fo which the matix A = T T has ank one. T T i. Is the matix A = i is skew-hemitian matix. i. alculate the invese of the matix = 5 7

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

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

The Divergence Theorem

The Divergence Theorem 13.8 The ivegence Theoem Back in 13.5 we ewote Geen s Theoem in vecto fom as C F n ds= div F x, y da ( ) whee C is the positively-oiented bounday cuve of the plane egion (in the xy-plane). Notice this

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

Problem 1: Multiple Choice Questions

Problem 1: Multiple Choice Questions Mathematics 102 Review Questions Poblem 1: Multiple Choice Questions 1: Conside the function y = f(x) = 3e 2x 5e 4x (a) The function has a local maximum at x = (1/2)ln(10/3) (b) The function has a local

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

Recall from last week:

Recall from last week: Recall fom last week: Length of a cuve '( t) dt b Ac length s( t) a a Ac length paametization ( s) with '( s) 1 '( t) Unit tangent vecto T '(s) '( t) dt Cuvatue: s ds T t t t t t 3 t ds u du '( t) dt Pincipal

More information

Math 209 Assignment 9 Solutions

Math 209 Assignment 9 Solutions Math 9 Assignment 9 olutions 1. Evaluate 4y + 1 d whee is the fist octant pat of y x cut out by x + y + z 1. olution We need a paametic epesentation of the suface. (x, z). Now detemine the nomal vecto:

More information

Related Rates - the Basics

Related Rates - the Basics Related Rates - the Basics In this section we exploe the way we can use deivatives to find the velocity at which things ae changing ove time. Up to now we have been finding the deivative to compae the

More information

MCV4U Final Exam Review. 1. Consider the function f (x) Find: f) lim. a) lim. c) lim. d) lim. 3. Consider the function: 4. Evaluate. lim. 5. Evaluate.

MCV4U Final Exam Review. 1. Consider the function f (x) Find: f) lim. a) lim. c) lim. d) lim. 3. Consider the function: 4. Evaluate. lim. 5. Evaluate. MCVU Final Eam Review Answe (o Solution) Pactice Questions Conside the function f () defined b the following gaph Find a) f ( ) c) f ( ) f ( ) d) f ( ) Evaluate the following its a) ( ) c) sin d) π / π

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

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

Chapter 10 Sample Exam

Chapter 10 Sample Exam Chapte Sample Exam Poblems maked with an asteisk (*) ae paticulaly challenging and should be given caeful consideation.. Conside the paametic cuve x (t) =e t, y (t) =e t, t (a) Compute the length of the

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

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

( ) Make-up Tests. From Last Time. Electric Field Flux. o The Electric Field Flux through a bit of area is

( ) Make-up Tests. From Last Time. Electric Field Flux. o The Electric Field Flux through a bit of area is Mon., 3/23 Wed., 3/25 Thus., 3/26 Fi., 3/27 Mon., 3/30 Tues., 3/31 21.4-6 Using Gauss s & nto to Ampee s 21.7-9 Maxwell s, Gauss s, and Ampee s Quiz Ch 21, Lab 9 Ampee s Law (wite up) 22.1-2,10 nto to

More information

$ i. !((( dv vol. Physics 8.02 Quiz One Equations Fall q 1 q 2 r 2 C = 2 C! V 2 = Q 2 2C F = 4!" or. r ˆ = points from source q to observer

$ i. !((( dv vol. Physics 8.02 Quiz One Equations Fall q 1 q 2 r 2 C = 2 C! V 2 = Q 2 2C F = 4! or. r ˆ = points from source q to observer Physics 8.0 Quiz One Equations Fall 006 F = 1 4" o q 1 q = q q ˆ 3 4" o = E 4" o ˆ = points fom souce q to obseve 1 dq E = # ˆ 4" 0 V "## E "d A = Q inside closed suface o d A points fom inside to V =

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

ME 210 Applied Mathematics for Mechanical Engineers

ME 210 Applied Mathematics for Mechanical Engineers Tangent and Ac Length of a Cuve The tangent to a cuve C at a point A on it is defined as the limiting position of the staight line L though A and B, as B appoaches A along the cuve as illustated in the

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

So, if we are finding the amount of work done over a non-conservative vector field F r, we do that long ur r b ur =

So, if we are finding the amount of work done over a non-conservative vector field F r, we do that long ur r b ur = 3.4 Geen s Theoem Geoge Geen: self-taught English scientist, 793-84 So, if we ae finding the amount of wok done ove a non-consevative vecto field F, we do that long u b u 3. method Wok = F d F( () t )

More information

Math 1105: Calculus I (Math/Sci majors) MWF 11am / 12pm, Campion 235 Written homework 3

Math 1105: Calculus I (Math/Sci majors) MWF 11am / 12pm, Campion 235 Written homework 3 Math : alculus I Math/Sci majos MWF am / pm, ampion Witten homewok Review: p 94, p 977,8,9,6, 6: p 46, 6: p 4964b,c,69, 6: p 47,6 p 94, Evaluate the following it by identifying the integal that it epesents:

More information

3.6 Applied Optimization

3.6 Applied Optimization .6 Applied Optimization Section.6 Notes Page In this section we will be looking at wod poblems whee it asks us to maimize o minimize something. Fo all the poblems in this section you will be taking the

More information

EM-2. 1 Coulomb s law, electric field, potential field, superposition q. Electric field of a point charge (1)

EM-2. 1 Coulomb s law, electric field, potential field, superposition q. Electric field of a point charge (1) EM- Coulomb s law, electic field, potential field, supeposition q ' Electic field of a point chage ( ') E( ) kq, whee k / 4 () ' Foce of q on a test chage e at position is ee( ) Electic potential O kq

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

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

Page 1 of 6 Physics II Exam 1 155 points Name Discussion day/time Pat I. Questions 110. 8 points each. Multiple choice: Fo full cedit, cicle only the coect answe. Fo half cedit, cicle the coect answe and

More information

Gauss Law. Physics 231 Lecture 2-1

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

More information

Motions and Coordinates

Motions and Coordinates Chapte Kinematics of Paticles Motions and Coodinates Motion Constained motion Unconstained motion Coodinates Used to descibe the motion of paticles 1 ectilinea motion (1-D) Motion Plane cuvilinea motion

More information

Phys-272 Lecture 17. Motional Electromotive Force (emf) Induced Electric Fields Displacement Currents Maxwell s Equations

Phys-272 Lecture 17. Motional Electromotive Force (emf) Induced Electric Fields Displacement Currents Maxwell s Equations Phys-7 Lectue 17 Motional Electomotive Foce (emf) Induced Electic Fields Displacement Cuents Maxwell s Equations Fom Faaday's Law to Displacement Cuent AC geneato Magnetic Levitation Tain Review of Souces

More information

University Physics (PHY 2326)

University Physics (PHY 2326) Chapte Univesity Physics (PHY 6) Lectue lectostatics lectic field (cont.) Conductos in electostatic euilibium The oscilloscope lectic flux and Gauss s law /6/5 Discuss a techniue intoduced by Kal F. Gauss

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

Welcome to Physics 272

Welcome to Physics 272 Welcome to Physics 7 Bob Mose mose@phys.hawaii.edu http://www.phys.hawaii.edu/~mose/physics7.html To do: Sign into Masteing Physics phys-7 webpage Registe i-clickes (you i-clicke ID to you name on class-list)

More information

Ch 30 - Sources of Magnetic Field! The Biot-Savart Law! = k m. r 2. Example 1! Example 2!

Ch 30 - Sources of Magnetic Field! The Biot-Savart Law! = k m. r 2. Example 1! Example 2! Ch 30 - Souces of Magnetic Field 1.) Example 1 Detemine the magnitude and diection of the magnetic field at the point O in the diagam. (Cuent flows fom top to bottom, adius of cuvatue.) Fo staight segments,

More information

transformation Earth V-curve (meridian) λ Conical projection. u,v curves on the datum surface projected as U,V curves on the projection surface

transformation Earth V-curve (meridian) λ Conical projection. u,v curves on the datum surface projected as U,V curves on the projection surface . CONICAL PROJECTIONS In elementay texts on map pojections, the pojection sufaces ae often descibed as developable sufaces, such as the cylinde (cylindical pojections) and the cone (conical pojections),

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. Chapte 7-8 Review Math 1316 Name SHORT ANSWER. Wite the wod o phase that best completes each statement o answes the question. Solve the tiangle. 1) B = 34.4 C = 114.2 b = 29.0 1) Solve the poblem. 2) Two

More information

Newton s Laws, Kepler s Laws, and Planetary Orbits

Newton s Laws, Kepler s Laws, and Planetary Orbits Newton s Laws, Keple s Laws, and Planetay Obits PROBLEM SET 4 DUE TUESDAY AT START OF LECTURE 28 Septembe 2017 ASTRONOMY 111 FALL 2017 1 Newton s & Keple s laws and planetay obits Unifom cicula motion

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

THE LAPLACE EQUATION. The Laplace (or potential) equation is the equation. u = 0. = 2 x 2. x y 2 in R 2

THE LAPLACE EQUATION. The Laplace (or potential) equation is the equation. u = 0. = 2 x 2. x y 2 in R 2 THE LAPLACE EQUATION The Laplace (o potential) equation is the equation whee is the Laplace opeato = 2 x 2 u = 0. in R = 2 x 2 + 2 y 2 in R 2 = 2 x 2 + 2 y 2 + 2 z 2 in R 3 The solutions u of the Laplace

More information

Chapter 22 The Electric Field II: Continuous Charge Distributions

Chapter 22 The Electric Field II: Continuous Charge Distributions Chapte The lectic Field II: Continuous Chage Distibutions A ing of adius a has a chage distibution on it that vaies as l(q) l sin q, as shown in Figue -9. (a) What is the diection of the electic field

More information

Hopefully Helpful Hints for Gauss s Law

Hopefully Helpful Hints for Gauss s Law Hopefully Helpful Hints fo Gauss s Law As befoe, thee ae things you need to know about Gauss s Law. In no paticula ode, they ae: a.) In the context of Gauss s Law, at a diffeential level, the electic flux

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

ECE 3318 Applied Electricity and Magnetism. Spring Prof. David R. Jackson ECE Dept. Notes 13

ECE 3318 Applied Electricity and Magnetism. Spring Prof. David R. Jackson ECE Dept. Notes 13 ECE 338 Applied Electicity and Magnetism ping 07 Pof. David R. Jackson ECE Dept. Notes 3 Divegence The Physical Concept Find the flux going outwad though a sphee of adius. x ρ v0 z a y ψ = D nˆ d = D ˆ

More information

e.g: If A = i 2 j + k then find A. A = Ax 2 + Ay 2 + Az 2 = ( 2) = 6

e.g: If A = i 2 j + k then find A. A = Ax 2 + Ay 2 + Az 2 = ( 2) = 6 MOTION IN A PLANE 1. Scala Quantities Physical quantities that have only magnitude and no diection ae called scala quantities o scalas. e.g. Mass, time, speed etc. 2. Vecto Quantities Physical quantities

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

B da = 0. Q E da = ε. E da = E dv

B da = 0. Q E da = ε. E da = E dv lectomagnetic Theo Pof Ruiz, UNC Asheville, doctophs on YouTube Chapte Notes The Maxwell quations in Diffeential Fom 1 The Maxwell quations in Diffeential Fom We will now tansfom the integal fom of the

More information

ANTENNAS. Vector and Scalar Potentials. Maxwell's Equations. D = εe. For a linear, homogeneous, isotropic medium µ and ε are contant.

ANTENNAS. Vector and Scalar Potentials. Maxwell's Equations. D = εe. For a linear, homogeneous, isotropic medium µ and ε are contant. ANTNNAS Vecto and Scala Potentials Maxwell's quations jωb J + jωd D ρ B (M) (M) (M3) (M4) D ε B Fo a linea, homogeneous, isotopic medium and ε ae contant. Since B, thee exists a vecto A such that B A and

More information

Lecture 8 - Gauss s Law

Lecture 8 - Gauss s Law Lectue 8 - Gauss s Law A Puzzle... Example Calculate the potential enegy, pe ion, fo an infinite 1D ionic cystal with sepaation a; that is, a ow of equally spaced chages of magnitude e and altenating sign.

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

Module 05: Gauss s s Law a

Module 05: Gauss s s Law a Module 05: Gauss s s Law a 1 Gauss s Law The fist Maxwell Equation! And a vey useful computational technique to find the electic field E when the souce has enough symmety. 2 Gauss s Law The Idea The total

More information

Lecture 1a: Satellite Orbits

Lecture 1a: Satellite Orbits Lectue 1a: Satellite Obits Outline 1. Newton s Laws of Motion 2. Newton s Law of Univesal Gavitation 3. Calculating satellite obital paametes (assuming cicula motion) Scala & Vectos Scala: a physical quantity

More information

Review Exercise Set 16

Review Exercise Set 16 Review Execise Set 16 Execise 1: A ectangula plot of famland will be bounded on one side by a ive and on the othe thee sides by a fence. If the fame only has 600 feet of fence, what is the lagest aea that

More information

Math 451: Euclidean and Non-Euclidean Geometry MWF 3pm, Gasson 204 Homework 9 Solutions

Math 451: Euclidean and Non-Euclidean Geometry MWF 3pm, Gasson 204 Homework 9 Solutions Math 451: Euclidean and Non-Euclidean Geomety MWF 3pm, Gasson 04 Homewok 9 Solutions Execises fom Chapte 3: 3.3, 3.8, 3.15, 3.19, 3.0, 5.11, 5.1, 5.13 Execise 3.3. Suppose that C and C ae two cicles with

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

PHYS 2135 Exam I February 13, 2018

PHYS 2135 Exam I February 13, 2018 Exam Total /200 PHYS 2135 Exam I Febuay 13, 2018 Name: Recitation Section: Five multiple choice questions, 8 points each Choose the best o most nealy coect answe Fo questions 6-9, solutions must begin

More information

Physics 235 Chapter 5. Chapter 5 Gravitation

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

More information

Physics 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

Chapter 2: Basic Physics and Math Supplements

Chapter 2: Basic Physics and Math Supplements Chapte 2: Basic Physics and Math Supplements Decembe 1, 215 1 Supplement 2.1: Centipetal Acceleation This supplement expands on a topic addessed on page 19 of the textbook. Ou task hee is to calculate

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

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

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

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

Kinematics in 2-D (II)

Kinematics in 2-D (II) Kinematics in 2-D (II) Unifom cicula motion Tangential and adial components of Relative velocity and acceleation a Seway and Jewett 4.4 to 4.6 Pactice Poblems: Chapte 4, Objective Questions 5, 11 Chapte

More information

A moving charged particle creates a magnetic field vector at every point in space except at its position.

A moving charged particle creates a magnetic field vector at every point in space except at its position. 1 Pat 3: Magnetic Foce 3.1: Magnetic Foce & Field A. Chaged Paticles A moving chaged paticle ceates a magnetic field vecto at evey point in space ecept at its position. Symbol fo Magnetic Field mks units

More information

F Q E v B MAGNETOSTATICS. Creation of magnetic field B. Effect of B on a moving charge. On moving charges only. Stationary and moving charges

F Q E v B MAGNETOSTATICS. Creation of magnetic field B. Effect of B on a moving charge. On moving charges only. Stationary and moving charges MAGNETOSTATICS Ceation of magnetic field. Effect of on a moving chage. Take the second case: F Q v mag On moving chages only F QE v Stationay and moving chages dw F dl Analysis on F mag : mag mag Qv. vdt

More information

16.4 Volume of Spheres

16.4 Volume of Spheres Name Class Date 16.4 Volume of Sphees Essential Question: How can you use the fomula fo the volume of a sphee to calculate the volumes of composite figues? Exploe G.11.D Apply the fomulas fo the volume

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

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

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 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

2 Cut the circle along the fold lines to divide the circle into 16 equal wedges. radius. Think About It

2 Cut the circle along the fold lines to divide the circle into 16 equal wedges. radius. Think About It Activity 8.7 Finding Aea of Cicles Question How do you find the aea of a cicle using the adius? Mateials compass staightedge scissos Exploe 1 Use a compass to daw a cicle on a piece of pape. Cut the cicle

More information

13. The electric field can be calculated by Eq. 21-4a, and that can be solved for the magnitude of the charge N C m 8.

13. The electric field can be calculated by Eq. 21-4a, and that can be solved for the magnitude of the charge N C m 8. CHAPTR : Gauss s Law Solutions to Assigned Poblems Use -b fo the electic flux of a unifom field Note that the suface aea vecto points adially outwad, and the electic field vecto points adially inwad Thus

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

Physics 111 Lecture 5 (Walker: 3.3-6) Vectors & Vector Math Motion Vectors Sept. 11, 2009

Physics 111 Lecture 5 (Walker: 3.3-6) Vectors & Vector Math Motion Vectors Sept. 11, 2009 Physics 111 Lectue 5 (Walke: 3.3-6) Vectos & Vecto Math Motion Vectos Sept. 11, 2009 Quiz Monday - Chap. 2 1 Resolving a vecto into x-component & y- component: Pola Coodinates Catesian Coodinates x y =

More information

Chapter 23: GAUSS LAW 343

Chapter 23: GAUSS LAW 343 Chapte 23: GAUSS LAW 1 A total chage of 63 10 8 C is distibuted unifomly thoughout a 27-cm adius sphee The volume chage density is: A 37 10 7 C/m 3 B 69 10 6 C/m 3 C 69 10 6 C/m 2 D 25 10 4 C/m 3 76 10

More information

Faraday s Law (continued)

Faraday s Law (continued) Faaday s Law (continued) What causes cuent to flow in wie? Answe: an field in the wie. A changing magnetic flux not only causes an MF aound a loop but an induced electic field. Can wite Faaday s Law: ε

More information

Review: Electrostatics and Magnetostatics

Review: Electrostatics and Magnetostatics Review: Electostatics and Magnetostatics In the static egime, electomagnetic quantities do not vay as a function of time. We have two main cases: ELECTROSTATICS The electic chages do not change postion

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

AE301 Aerodynamics I UNIT B: Theory of Aerodynamics

AE301 Aerodynamics I UNIT B: Theory of Aerodynamics AE301 Aeodynamics I UNIT B: Theoy of Aeodynamics ROAD MAP... B-1: Mathematics fo Aeodynamics B-2: Flow Field Repesentations B-3: Potential Flow Analysis B-4: Applications of Potential Flow Analysis AE301

More information

Physics Tutorial V1 2D Vectors

Physics Tutorial V1 2D Vectors Physics Tutoial V1 2D Vectos 1 Resolving Vectos & Addition of Vectos A vecto quantity has both magnitude and diection. Thee ae two ways commonly used to mathematically descibe a vecto. y (a) The pola fom:,

More information

In many engineering and other applications, the. variable) will often depend on several other quantities (independent variables).

In many engineering and other applications, the. variable) will often depend on several other quantities (independent variables). II PARTIAL DIFFERENTIATION FUNCTIONS OF SEVERAL VARIABLES In man engineeing and othe applications, the behaviou o a cetain quantit dependent vaiable will oten depend on seveal othe quantities independent

More information

CBN 98-1 Developable constant perimeter surfaces: Application to the end design of a tape-wound quadrupole saddle coil

CBN 98-1 Developable constant perimeter surfaces: Application to the end design of a tape-wound quadrupole saddle coil CBN 98-1 Developale constant peimete sufaces: Application to the end design of a tape-wound quadupole saddle coil G. Dugan Laoatoy of Nuclea Studies Conell Univesity Ithaca, NY 14853 1. Intoduction Constant

More information

Question 1: The dipole

Question 1: The dipole Septembe, 08 Conell Univesity, Depatment of Physics PHYS 337, Advance E&M, HW #, due: 9/5/08, :5 AM Question : The dipole Conside a system as discussed in class and shown in Fig.. in Heald & Maion.. Wite

More information

Motithang Higher Secondary School Thimphu Thromde Mid Term Examination 2016 Subject: Mathematics Full Marks: 100

Motithang Higher Secondary School Thimphu Thromde Mid Term Examination 2016 Subject: Mathematics Full Marks: 100 Motithang Highe Seconday School Thimphu Thomde Mid Tem Examination 016 Subject: Mathematics Full Maks: 100 Class: IX Witing Time: 3 Hous Read the following instuctions caefully In this pape, thee ae thee

More information

r cos, and y r sin with the origin of coordinate system located at

r cos, and y r sin with the origin of coordinate system located at Lectue 3-3 Kinematics of Rotation Duing ou peious lectues we hae consideed diffeent examples of motion in one and seeal dimensions. But in each case the moing object was consideed as a paticle-like object,

More information

Gauss s Law Simulation Activities

Gauss s Law Simulation Activities Gauss s Law Simulation Activities Name: Backgound: The electic field aound a point chage is found by: = kq/ 2 If thee ae multiple chages, the net field at any point is the vecto sum of the fields. Fo a

More information

Stress, Cauchy s equation and the Navier-Stokes equations

Stress, Cauchy s equation and the Navier-Stokes equations Chapte 3 Stess, Cauchy s equation and the Navie-Stokes equations 3. The concept of taction/stess Conside the volume of fluid shown in the left half of Fig. 3.. The volume of fluid is subjected to distibuted

More information

School of Electrical and Computer Engineering, Cornell University. ECE 303: Electromagnetic Fields and Waves. Fall 2007

School of Electrical and Computer Engineering, Cornell University. ECE 303: Electromagnetic Fields and Waves. Fall 2007 School of Electical and Compute Engineeing, Conell Univesity ECE 303: Electomagnetic Fields and Waves Fall 007 Homewok 8 Due on Oct. 19, 007 by 5:00 PM Reading Assignments: i) Review the lectue notes.

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

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

06 - ROTATIONAL MOTION Page 1 ( Answers at the end of all questions )

06 - ROTATIONAL MOTION Page 1 ( Answers at the end of all questions ) 06 - ROTATIONAL MOTION Page ) A body A of mass M while falling vetically downwads unde gavity beaks into two pats, a body B of mass ( / ) M and a body C of mass ( / ) M. The cente of mass of bodies B and

More information

. Using our polar coordinate conversions, we could write a

. Using our polar coordinate conversions, we could write a 504 Chapte 8 Section 8.4.5 Dot Poduct Now that we can add, sutact, and scale vectos, you might e wondeing whethe we can multiply vectos. It tuns out thee ae two diffeent ways to multiply vectos, one which

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

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

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