Physics of Rolling Ball Coasters - PowerPoint PPT Presentation

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Physics of Rolling Ball Coasters

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The cross product is always perpendicular to the vectors a and b. ... Second is in terms of the moment of inertia and the angular acceleration. ... – PowerPoint PPT presentation

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Title: Physics of Rolling Ball Coasters


1
Physics of Rolling Ball Coasters
  • Cross Product
  • Torque
  • Inclined Plane
  • Inclined Ramp
  • Curved Path
  • Examples

2
Cross Product (1)
  • The Cross Product of two three-dimensional
    vectors a lta1,a2,a3gt and b ltb1,b2,b3gt is
    defined as follows
  • If q is the angle between the vectors, then

3
Cross Product (2)
  • Important facts about the cross product
  • The cross product is always perpendicular to the
    vectors a and b.
  • The direction of the cross product is given by
    the right hand rule (see diagram, where
    ).
  • The cross product is greatest when
  • While the dot product produces a scalar, the
    cross product produces a vector. Therefore it is
    sometimes called a vector product.

4
Digression
  • Earlier, the definition of angular velocity was
    given, but details on the use of the cross
    product were not explained. Now that we have the
    cross product, we define the relation between
    tangential and angular velocity in general
  • For circular motion, the velocity is always
    perpendicular to the position vector and this
    reduces to v r w.
  • Similarly we define the relationship between
    tangential and angular acceleration

5
Torque (1)
  • Before dealing with a rolling ball, we must
    discuss how forces act on a rotating object.
  • Consider opening a door. Usually you grab the
    handle, which is on the side opposite the hinge,
    and you pull it directly toward yourself (at a
    right angle to the plane of the door). This is
    easier than pulling a handle in the center of the
    door, and than pulling at any other angle. Why?
  • When causing an object to rotate, it is important
    where and how the force is applied, in addition
    to the magnitude.
  • Torque is a turning or twisting force, and it is
    a measure of a force's tendency to produce
    rotation about an axis.

6
Torque (2)
  • There are two definitions of torque. First is in
    terms of the vectors F and r, referring to the
    force and position, respectively
  • Second is in terms of the moment of inertia and
    the angular acceleration. (Angular acceleration
    is the time derivative of angular velocity).
  • (Note the similarity to Newtons Second Law, F
    m a. Here all the terms have an angular
    counterpart.)

7
Inclined Plane
  • Consider a ball rolling down an inclined plane as
    pictured. Assume that it starts at rest, and
    after rolling a distance d along the ramp, it has
    fallen a distance h in the y-direction.

8
Inclined Plane (2)
  • We will now consider the energy of the system.
    The system is closed, so energy must be
    conserved. Set the reference point for potential
    energy such that the ball starts at a height of
    h.
  • Initially the ball is at rest, so at this instant
    it contains only potential energy. When it has
    traveled the distance d along the ramp, it has
    only kinetic energy (translational and
    rotational).
  • We can also express h in terms of d.
  • This gives us the square velocity after the
    particle moves the distance d.

9
Inclined Plane (3)
From the previous slide
  • If you know the square velocity of a particle
    after it travels a distance d, and you know that
    the acceleration is constant, then that
    acceleration is unique. This derivation shows
    why, using definitions of average velocity and
    average acceleration.

Eliminating t and vi0, these expressions give
Comparing this result to the previous slide, we
can see that
10
Inclined Track (1)
  • When using physics to determine values like
    acceleration, there are often two perfectly
    correct approaches one is using energy (like we
    just did), and a second is by using forces. While
    energy is often simpler computationally, it is
    not always as satisfying. For this next
    situation, the previous approach would also work,
    with the only difference being that
    However, to demonstrate the physics more
    explicitly, we will take an approach using
    forces.
  • When we build a track for a rolling ball
  • coaster, there will actually be two
  • contact points, one on each rail. Because
  • the ball will now rest inside the track, we
  • need to re-set the stage. The picture shows
  • a sphere on top of a 2-rail track, with the
  • radius R and the height off the track b marked in.

11
Inclined Track (2)
  • These are all the forces acting on the ball
    friction, gravity, and a normal force.
  • The black square in the center represents the
    axis of rotation, which in this case is the axis
    connecting the two points where the ball contacts
    the track.
  • The yellow arrow represents friction and the blue
    arrow represents the normal force. Neither of
    these forces torque the ball because they act at
    the axis of rotation. Thus the vector r is 0.
  • The green arrow represents gravity.
  • Convince yourself that the total torque is given
    by

12
Inclined Track (3)
  • We also have a second definition of torque
  • Setting these equal and solving for acceleration
    down the track
  • Notice that if b R, then this reduces to the
    previous expression for acceleration
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