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Motion in Two Dimensions

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36 diapositives · 599 Views · Jul 29, 2014

Motion in Two Dimensions. Using + or – signs is not always sufficient to fully describe motion in more than one dimension Vectors can be used to more fully describe motion. Displacement. The position of an object is described by its position vector, r

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Motion in Two Dimensions
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Transcription de la présentation
  1. Motion in Two Dimensions • Using + or – signs is not always sufficient to fully describe motion in more than one dimension • Vectors can be used to more fully describe motion

  2. Displacement • The position of an object is described by its position vector, r • The displacement of the object is defined as the change in its position • Δr = rf - ri

  3. Velocity • The average velocity is the ratio of the displacement to the time interval for the displacement • The instantaneous velocity is the limit of the average velocity as Δt approaches zero • The direction of the instantaneous velocity is along a line that is tangent to the path of the particle and in the direction of motion

  4. Acceleration • The average acceleration is defined as the rate at which the velocity changes • The instantaneous acceleration is the limit of the average acceleration as Δt approaches zero

  5. Ways an Object Might Accelerate • The magnitude of the velocity (the speed) can change • The direction of the velocity can change • Even though the magnitude is constant • Both the magnitude and the direction can change

  6. Projectile Motion • An object may move in both the x and y directions simultaneously • It moves in two dimensions • The form of two dimensional motion we will deal with is called projectile motion

  7. Assumptions of Projectile Motion • We may ignore air friction • We may ignore the rotation of the earth • With these assumptions, an object in projectile motion will follow a parabolic path

  8. Rules of Projectile Motion • The x- and y-directions of motion can be treated independently • The x-direction is uniform motion • ax = 0 • The y-direction is free fall • ay = -g • The initial velocity can be broken down into its x- and y-components

  9. Projectile Motion

  10. Some Details About the Rules • x-direction • ax = 0 • x = vxot • This is the only operative equation in the x-direction since there is uniform velocity in that direction

  11. More Details About the Rules • y-direction • free fall problem • a = -g • take the positive direction as upward • uniformly accelerated motion, so the motion equations all hold

  12. Velocity of the Projectile • The velocity of the projectile at any point of its motion is the vector sum of its x and y components at that point

  13. Some Variations of Projectile Motion • An object may be fired horizontally • The initial velocity is all in the x-direction • vo = vx and vy = 0 • All the general rules of projectile motion apply

  14. Non-Symmetrical Projectile Motion • Follow the general rules for projectile motion • Break the y-direction into parts • up and down • symmetrical back to initial height and then the rest of the height