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    Motion in Two Dimensions
+
    Projectile Motion

    ļ®   Two-dimensional motion is called projectile motion.

    ļ®   Objects that are thrown or launched into the air and are subject
        to gravity are called projectiles.

    ļ®   Some examples of projectiles are

    ļ®   Softballs,

    ļ®   Footballs

    ļ®   Arrows
+


    ļ®   The parabolic path which is common for all projectile motion is
        called trajectory.

    ļ®   The horizontal distance covered by a projectile which returns its
        original height is called the range of the projectile.
+


    An object is
    projected with an
    initial velocity, vi, at
    an angle of Īø.
    Resolve the initial
    velocity into its x and
    ycomponents. Then,
    the kinematic
    equations can be
    applied to describe
    the motion of the
    projectile throughout
    its flight.
+

                      Suppose the initial velocity vector
                      makes an angle Īø with the
                      horizontal. Again, to analyze the
                      motion of such a projectile, you
                      must resolve the initial velocity
                      vector into its components.



    vx,i= vicosĪø and vy,i= visinĪø
+
    Example:




          (a) Without air resistance, the soccer ball would
          travel along a parabola.
          (b) With air resistance, the soccer ball would
          travel along a shorter path.
+
    Example:




      (a) A long jumperā€™s velocity while sprinting along the runway can be
      represented by a horizontal vector.
      (b) Once the jumper is airborne, the jumperā€™s velocity at any instant
      can be described by the components of the velocity.
+   We can substitute these values for v0x and v0y into the
    kinematic equations to obtain a set of equations that
    can be used to analyze the motion of a projectile
    launched at an angle.


    v0x=v0cosĪø                       For the motion on x
    x = v0xt = v0cosĪøt               axis

    v0y=v0sinĪø
    vy = v0y ā€“ gt
    Ī”y =v0yt ā€“ (1/2)gt2              For the motion on y
    Ī”y = (1/2)(v0y+vy)t              axis
    vy2 = v0y2 ā€“ 2gĪ”y
                                     The relation between
    v2 =   vx2   +   vy2             speeds
+
    Example

    ļ®    A ball is launched at a velocity of 8 m/s and an angle of 53o
         with the horizontal line axis.

    a)     Calculate the time for the ball to reach its max. height.

    b)     How high will the ball rise?

    c)     What is the range of the ball?

    d)     What is the ballā€™s velocity just before it strikes the ground?
+
    Example

    ļ®    A rocket is launched at a velocity of 25 m/s and an angle of 37o
         with the horizontal line axis.

    a)     Calculate the time for the ball to reach its max. height.

    b)     How high will the ball rise?

    c)     What is the range of the ball?

    d)     What is the ballā€™s velocity just before it strikes the ground?

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Motion in two dimensions

  • 1. +
  • 2. + Motion in Two Dimensions
  • 3. + Projectile Motion ļ® Two-dimensional motion is called projectile motion. ļ® Objects that are thrown or launched into the air and are subject to gravity are called projectiles. ļ® Some examples of projectiles are ļ® Softballs, ļ® Footballs ļ® Arrows
  • 4. + ļ® The parabolic path which is common for all projectile motion is called trajectory. ļ® The horizontal distance covered by a projectile which returns its original height is called the range of the projectile.
  • 5. + An object is projected with an initial velocity, vi, at an angle of Īø. Resolve the initial velocity into its x and ycomponents. Then, the kinematic equations can be applied to describe the motion of the projectile throughout its flight.
  • 6. + Suppose the initial velocity vector makes an angle Īø with the horizontal. Again, to analyze the motion of such a projectile, you must resolve the initial velocity vector into its components. vx,i= vicosĪø and vy,i= visinĪø
  • 7. + Example: (a) Without air resistance, the soccer ball would travel along a parabola. (b) With air resistance, the soccer ball would travel along a shorter path.
  • 8. + Example: (a) A long jumperā€™s velocity while sprinting along the runway can be represented by a horizontal vector. (b) Once the jumper is airborne, the jumperā€™s velocity at any instant can be described by the components of the velocity.
  • 9. + We can substitute these values for v0x and v0y into the kinematic equations to obtain a set of equations that can be used to analyze the motion of a projectile launched at an angle. v0x=v0cosĪø For the motion on x x = v0xt = v0cosĪøt axis v0y=v0sinĪø vy = v0y ā€“ gt Ī”y =v0yt ā€“ (1/2)gt2 For the motion on y Ī”y = (1/2)(v0y+vy)t axis vy2 = v0y2 ā€“ 2gĪ”y The relation between v2 = vx2 + vy2 speeds
  • 10. + Example ļ® A ball is launched at a velocity of 8 m/s and an angle of 53o with the horizontal line axis. a) Calculate the time for the ball to reach its max. height. b) How high will the ball rise? c) What is the range of the ball? d) What is the ballā€™s velocity just before it strikes the ground?
  • 11. + Example ļ® A rocket is launched at a velocity of 25 m/s and an angle of 37o with the horizontal line axis. a) Calculate the time for the ball to reach its max. height. b) How high will the ball rise? c) What is the range of the ball? d) What is the ballā€™s velocity just before it strikes the ground?