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Physics C Vectors Review

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1 Physics C Vectors Review
Wednesday, August 27, 2008 Vectors Review Bertrand

2 Announcements Lab fee? Chris, Liam, Greg?
Physics C Announcements Lab fee? Chris, Liam, Greg? Lab books due today with Kinematics Graphing lab. Bertrand

3 Scalars vs Vectors R head tail  Scalars have magnitude only
Physics C Scalars vs Vectors Scalars have magnitude only Distance, speed, time, mass Vectors have both magnitude and direction displacement, velocity, acceleration R head tail Bertrand

4 Physics C Direction of Vectors The direction of a vector is represented by the direction in which the ray points. This is typically given by an angle. A x Bertrand

5 Magnitude of Vectors B A
Physics C Magnitude of Vectors The magnitude of a vector is the size of whatever the vector represents. The magnitude is represented by the length of the vector. Symbolically, the magnitude is often represented as │A │ B Then vector B, which is twice as long, would represent a displacement of six miles to the north! A If vector A represents a displacement of three miles to the north… Bertrand

6 Physics C Equal Vectors Equal vectors have the same length and direction, and represent the same quantity (such as force or velocity). Bertrand

7 Physics C Inverse Vectors Inverse vectors have the same length, but opposite direction. A -A Bertrand

8 Graphical Addition of Vectors
Physics C Graphical Addition of Vectors Vectors are added graphically together head-to-tail. The sum is called the resultant. The inverse of the sum is called the equilibrant B A R A + B = R Bertrand

9 Component Addition of Vectors
Physics C Component Addition of Vectors Resolve each vector into its x- and y-components. Ax = Acos Ay = Asin Bx = Bcos By = Bsin etc. Add the x-components together to get Rx and the y-components to get Ry. Use the Pythagorean Theorem to get the magnitude of the resultant. Use the inverse tangent function to get the angle. Bertrand

10 Physics C Sample problem: Add together the following graphically and by component, giving the magnitude and direction of the resultant and the equilibrant. Vector A: o Vector B: o Vector C: o Bertrand

11 Physics C Bertrand

12 Physics C Thursday, August 28, 2008 Unit Vectors Bertrand

13 Announcements Lab fee? Chris, Liam, Greg? HW Quiz: Chapter 2
Physics C Announcements Lab fee? Chris, Liam, Greg? HW Quiz: Chapter 2 Problems 30, 36, 39, 42, 49, 52 Roll the die! Bertrand

14 Consider Three Dimensions
Physics C Consider Three Dimensions Polar Angle z Azimuthal Angle az a q ay y f ax xy Projection x Bertrand

15 Physics C Unit Vectors Unit vectors are quantities that specify direction only. They have a magnitude of exactly one, and typically point in the x, y, or z directions. Bertrand

16 Physics C Unit Vectors z k j i y x Bertrand

17 Physics C Unit Vectors Instead of using magnitudes and directions, vectors can be represented by their components combined with their unit vectors. Example: displacement of 30 meters in the +x direction added to a displacement of 60 meters in the –y direction added to a displacement of 40 meters in the +z direction yields a displacement of: Bertrand

18 Adding Vectors Using Unit Vectors
Physics C Adding Vectors Using Unit Vectors Simply add all the i components together, all the j components together, and all the k components together. Bertrand

19 Sample problem: Consider two vectors, A = 3. 00 i + 7. 50 j and B = -5
Sample problem: Consider two vectors, A = 3.00 i j and B = i j. Calculate C where C = A + B. Physics C Bertrand

20 Sample problem: You move 10 meters north and 6 meters east
Sample problem: You move 10 meters north and 6 meters east. You then climb a 3 meter platform, and move 1 meter west on the platform. What is your displacement vector? (Assume East is in the +x direction). Physics C Bertrand

21 Suppose I need to convert unit vectors to a magnitude and direction?
Physics C Suppose I need to convert unit vectors to a magnitude and direction? Given the vector Bertrand

22 Sample problem: You move 10 meters north and 6 meters east
Sample problem: You move 10 meters north and 6 meters east. You then climb a 3 meter platform, and move 1 meter west on the platform. How far are you from your starting point? Physics C Bertrand

23 Position, Velocity, and Acceleration Vectors in Multiple Dimensions
Physics C Friday, August 29, 2008 Position, Velocity, and Acceleration Vectors in Multiple Dimensions Bertrand

24 1 Dimension 2 or 3 Dimensions
Physics C 1 Dimension 2 or 3 Dimensions x: position x: displacement v: velocity a: acceleration r: position r: displacement v: velocity a: acceleration r = x i + y j + z k r = x i + y j + z k v = vx i + vy j + vz k a = ax i + ay j + az k In Unit Vector Notation Bertrand

25 Sample problem: The position of a particle is given by r = (80 + 2t)i – 40j - 5t2k. Derive the velocity and acceleration vectors for this particle. What does motion “look like”? Physics C Bertrand

26 a) Determine the velocity and acceleration functions.
Sample problem: A position function has the form r = x i + y j with x = t3 – 6 and y = 5t - 3. a) Determine the velocity and acceleration functions. b) Determine the velocity and speed at 2 seconds. Physics C Bertrand

27 Miscellaneous Let’s look at some video analysis.
Physics C Miscellaneous Let’s look at some video analysis. Let’s look at a documentary. Homework questions? Bertrand

28 Multi-Dimensional Motion with Constant (or Uniform) Acceleration
Physics C Tuesday, September 2, 2008 Multi-Dimensional Motion with Constant (or Uniform) Acceleration Bertrand

29 Sample Problem: A baseball outfielder throws a long ball
Sample Problem: A baseball outfielder throws a long ball. The components of the position are x = (30 t) m and y = (10 t – 4.9t2) m a) Write vector expressions for the ball’s position, velocity, and acceleration as functions of time. Use unit vector notation! b) Write vector expressions for the ball’s position, velocity, and acceleration at 2.0 seconds. Physics C Bertrand

30 Sample problem: A particle undergoing constant acceleration changes from a velocity of 4i – 3j to a velocity of 5i + j in 4.0 seconds. What is the acceleration of the particle during this time period? What is its displacement during this time period? Physics C Bertrand

31 Trajectory of Projectile
Physics C Trajectory of Projectile g g g g g This shows the parabolic trajectory of a projectile fired over level ground. Acceleration points down at 9.8 m/s2 for the entire trajectory. Bertrand

32 Trajectory of Projectile
Physics C Trajectory of Projectile vx vy vx vy vx vy vx vx vy The velocity can be resolved into components all along its path. Horizontal velocity remains constant; vertical velocity is accelerated. Bertrand

33 Physics C Position graphs for 2-D projectiles. Assume projectile fired over level ground. x y t y t x Bertrand

34 Physics C Velocity graphs for 2-D projectiles. Assume projectile fired over level ground. Vy Vx t t Bertrand

35 Physics C Acceleration graphs for 2-D projectiles. Assume projectile fired over level ground. ay ax t t Bertrand

36 Remember… To work projectile problems…
Physics C Remember… To work projectile problems… …resolve the initial velocity into components. Vo,y = Vo sin  Vo Vo,x = Vo cos  Bertrand

37 Sample problem: A soccer player kicks a ball at 15 m/s at an angle of 35o above the horizontal over level ground. How far horizontally will the ball travel until it strikes the ground? Physics C Bertrand

38 Sample problem: A cannon is fired at a 15o angle above the horizontal from the top of a 120 m high cliff. How long will it take the cannonball to strike the plane below the cliff? How far from the base of the cliff will it strike? Physics C Bertrand

39 Sample problem: derive the trajectory equation.
Physics C Bertrand

40 Sample problem: Derive the range equation for a projectile fired over level ground.
Physics C Bertrand

41 Sample problem: Show that maximum range is obtained for a firing angle of 45o.
Physics C Bertrand

42 Physics C Wednesday, September 3, 2008 Monkey Gun Bertrand

43 Physics C Announcements Homework policy change. Bertrand

44 Physics C Will the projectile always hit the target presuming it has enough range? The target will begin to fall as soon as the projectile leaves the gun. Bertrand

45 Physics C Review of Uniform Circular Motion
Friday, September 5, 2008 Review of Uniform Circular Motion Bertrand

46 Uniform Circular Motion
Physics C Uniform Circular Motion Occurs when an object moves in a circle without changing speed. Despite the constant speed, the object’s velocity vector is continually changing; therefore, the object must be accelerating. The acceleration vector is pointed toward the center of the circle in which the object is moving, and is referred to as centripetal acceleration. Bertrand

47 Vectors in Uniform Circular Motion
Physics C Vectors in Uniform Circular Motion v v a a a = v2 / r v a v a Bertrand

48 Physics C Sample Problem The Moon revolves around the Earth every 27.3 days. The radius of the orbit is 382,000,000 m. What is the magnitude and direction of the acceleration of the Moon relative to Earth? Bertrand

49 Sample problem: Space Shuttle astronauts typically experience accelerations of 1.4 g during takeoff. What is the rotation rate, in rps, required to give an astronaut a centripetal acceleration equal to this in a simulator moving in a 10.0 m circle. Physics C Bertrand

50 Physics C Radial and Tangential Acceleration
Wednesday, September 10, 2008 Radial and Tangential Acceleration Bertrand

51 Tangential acceleration
Physics C Tangential acceleration Sometimes the speed of an object in circular motion is not constant (in other words, it’s not uniform circular motion). An acceleration component is tangent to the path, aligned with the velocity. This is called tangential acceleration. The centripetal acceleration component causes the object to continue to turn as the tangential component causes the radius or speed to change. Bertrand

52 Tangential Acceleration
Physics C Tangential Acceleration radial or centripetal component (ar or ac ) tangential component (aT ) v a If tangential acceleration exists, the orbit is not stable. Bertrand

53 Sample Problem: Given the figure at right rotating at constant radius, find the radial and tangential acceleration components if q = 30o and a has a magnitude of 15.0 m/s2. What is the speed of the particle? How is it behaving? Physics C 5.00 m a q Bertrand

54 Physics C Sample problem: Suppose you attach a ball to a 60 cm long string and swing it in a vertical circle. The speed of the ball is 4.30 m/s at the highest point and 6.50 m/s at the lowest point. Find the acceleration of the ball at the highest and lowest points. Bertrand

55 Sample problem: A car is rounding a curve on the interstate, slowing from 30 m/s to 22 m/s in 7.0 seconds. The radius of the curve is 30 meters. What is the acceleration of the car? Physics C Bertrand

56 Physics C Relative Motion
Thursday, September 11, 2008 Relative Motion Bertrand

57 Physics C Relative Motion When observers are moving at constant velocity relative to each other, we have a case of relative motion. The moving observers can agree about some things, but not about everything, regarding an object they are both observing. Bertrand

58 Physics C Consider two observers and a particle. Suppose observer B is moving relative to observer A. P particle vrel A observer B observer Bertrand

59 Also suppose particle P is also moving relative to observer A.
Physics C Also suppose particle P is also moving relative to observer A. vA P particle In this case, it looks to A like P is moving to the right at twice the speed that B is moving in the same direction. vrel A observer B observer Bertrand

60 However, from the perspective of observer B…
Physics C However, from the perspective of observer B… vA vB P particle it looks like P is moving to the right at the same speed that A is moving in the opposite direction, and this speed is half of what A reports for P. vrel -vrel A observer B observer Bertrand

61 vB = vA – vrel vA = vB + vrel P A B vrel -vrel
Physics C The velocity measured by two observers depends upon the observers’ velocity relative to each other. vA vB P particle vB = vA – vrel vA = vB + vrel vrel -vrel A observer B observer Bertrand

62 Sample problem: Now show that although velocity of the observers is different, the acceleration they measure for a third particle is the same provided vrel is constant. Begin with vB = vA - vrel Physics C Bertrand

63 Galileo’s Law of Transformation of Velocities
Physics C Galileo’s Law of Transformation of Velocities If observers are moving but not accelerating relative to each other, they agree on a third object’s acceleration, but not its velocity! Bertrand

64 Inertial Reference Frames
Physics C Inertial Reference Frames Frames of reference which may move relative to each other but in which observers find the same value for the acceleration of a third moving particle. Inertial reference frames are moving at constant velocity relative to each other. It is impossible to identify which one may be at rest. Newton’s Laws hold only in inertial reference frames, and do not hold in reference frames which are accelerating. Bertrand

65 Sample problem: How long does it take an automobile traveling in the left lane at 60.0km/h to pull alongside a car traveling in the right lane at 40.0 km/h if the cars’ front bumpers are initially 100 m apart? Physics C Bertrand

66 Sample problem: A pilot of an airplane notes that the compass indicates a heading due west. The airplane’s speed relative to the air is 150 km/h. If there is a wind of 30.0 km/h toward the north, find the velocity of the airplane relative to the ground. Physics C Bertrand


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