Lectures by James L. Pazun © 2012 Pearson Education, Inc. 3 Motion in a Plane.

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Presentation transcript:

Lectures by James L. Pazun © 2012 Pearson Education, Inc. 3 Motion in a Plane

Copyright © 2012 Pearson Education, Inc. publishing as Addison-Wesley Goals for Chapter 3 To study position, velocity, and acceleration vectors. To frame two-dimensional motion as it occurs in the motion of projectiles. To restrain two-dimensional motion to a circular path and understand uniform circular motion. To study the new concept of one motion frame relative to another.

Copyright © 2012 Pearson Education, Inc. publishing as Addison-Wesley Velocity in a plane Vectors in terms of Cartesian x and y coordinates may now also be expressed in terms of displacement and angle.

Copyright © 2012 Pearson Education, Inc. publishing as Addison-Wesley The motion of a model car – Example 3.1 See the worked example on page 70.

Copyright © 2012 Pearson Education, Inc. publishing as Addison-Wesley Accelerations in a plane Acceleration must now be considered during change in magnitude AND/OR change in direction.

Copyright © 2012 Pearson Education, Inc. publishing as Addison-Wesley The model car revisited – Example 3.2 See the worked example on page 74.

Copyright © 2012 Pearson Education, Inc. publishing as Addison-Wesley Special cases for acceleration – Figure 3.8 Acceleration parallel or perpendicular to the object’s velocity.

Copyright © 2012 Pearson Education, Inc. publishing as Addison-Wesley Projectile motion Determined by the initial velocity, gravity, and air resistance. Footballs, baseballs … any projectile will follow this parabolic path.

Copyright © 2012 Pearson Education, Inc. publishing as Addison-Wesley The independence of x and y motion – Figure 3.10 Notice how the vertical motion under free fall spaces out exactly as the vertical motion under projectile motion.

Copyright © 2012 Pearson Education, Inc. publishing as Addison-Wesley Projectile motion revisited – Figure 3.11 Notice the vertical velocity component as the projectile changes horizontal position.

Copyright © 2012 Pearson Education, Inc. publishing as Addison-Wesley Determination of key items x = (v o cos  o )t  = tan -1 (v y /v x ) y = (v o sin  o )t - ½gt 2 v x = v o cos  o v y = v o sin  o - gt

Copyright © 2012 Pearson Education, Inc. publishing as Addison-Wesley The paintball gun – Example 3.3 See the worked example on page 78. Full consideration given to the motion after the dye-filled ball is fired.

Copyright © 2012 Pearson Education, Inc. publishing as Addison-Wesley A home-run hit – Example 3.4 See the fully worked example on pages Details examined for the flight of a baseball hit from home plate toward a fence hundreds of feet away.

Copyright © 2012 Pearson Education, Inc. publishing as Addison-Wesley Horizontal displacement vs angle - Figure 3.17 The motion is symmetrical. The horizontal displacement depends on angle. Observe the maximum at 45 o.

Copyright © 2012 Pearson Education, Inc. publishing as Addison-Wesley Vertical / horizontal displacement – Example 3.4 After a given horizontal displacement, a projectile will have a vertical position. Sports provide a large number of excellent examples. For a field-goal, see worked example on pages

Copyright © 2012 Pearson Education, Inc. publishing as Addison-Wesley Firing at a more complex target – Example 3.7 A moving target presents a real-life scenario. It is possible to solve a falling body as the target. This problem is a “classic” on standardized exams. See the worked example on pages

Copyright © 2012 Pearson Education, Inc. publishing as Addison-Wesley Circular motion as a special application – Figure 3.23 Two dimensional motion in a plane takes on unique features when it is confined to a circle. The acceleration is centripetal (“center seeking”). The velocity vector retains the same magnitude, it changes direction.

Copyright © 2012 Pearson Education, Inc. publishing as Addison-Wesley It is possible to solve for the velocity – Figure 3.24 The problem may be treated by extracting a small portion of the motion such that the Δv arc may be approximated as a straight line.

Copyright © 2012 Pearson Education, Inc. publishing as Addison-Wesley An example you can go try right now – Example 3.8 Refer to the worked example on page 87

Copyright © 2012 Pearson Education, Inc. publishing as Addison-Wesley An problem to try on your next vacation – Example 3.9 Uniform circular motion applied to a daring carnival ride. Referred to the worked example on page 88.

Copyright © 2012 Pearson Education, Inc. publishing as Addison-Wesley A matter of perspective – Figure 3.29 Velocities can carry multiple values depending on the position and motion of the object and the observer.

Copyright © 2012 Pearson Education, Inc. publishing as Addison-Wesley An airplane in a crosswind – Example 3.11 A solved application of relative motion.