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Solution
Week 39 (6/9/03)
Viewing the spokes
The contact point on the ground does not look blurred, because it is instantaneously
at rest. But although this is the only point on the wheel that is at rest, there will
be other locations in the picture where the spokes do not appear blurred.
The relevant property of a point in the picture where a spoke does not appear
blurred is that the point lies on the spoke throughout the duration of the camera’s
exposure. (The point in the picture need not, however, actually correspond to the
same atom on the spoke.)
At a given time, consider a spoke in the lower half of the wheel. A short time
later, the spoke will have moved (via both translation and rotation), but it will
intersect its original position. The spoke will not appear blurred at this intersection
point. We must therefore find the locus of these intersections. We can do this in
two ways.
First method: Let R be the radius of the wheel. Consider a spoke that makes an
angle of θ with the vertical at a given time. If the wheel then rolls through a small
angle dθ, the center moves a distance R dθ. The spoke’s motion is a combination
of a translation through this distance R dθ, plus a rotation through the angle dθ
(around the top end).
Let r be the radial position of the intersection of the initial and final positions of
the spoke. In the following figure, we can write down two expressions for the short
segment drawn perpendicular to the initial position of the spoke.
Rdθ
dθ
θ
θ
r
The two expression are (R dθ) cos θ, and r dθ (to first order in dθ). Equating these
gives r = R cos θ. This describes a circle whose diameter is the lower vertical radius
of the wheel, as shown below.
1
R
θ
r=Rcosθ
wheel
Second method: Since the wheel’s contact point with the ground is instanta-
neously at rest, the wheel may be considered to be instantaneously rotating around
this point. This means that every atom in the wheel (both in the spokes and the
rim) instantaneously traces out the arc of a circle centered at the contact point. For
the point P in the figure below, this circle is the dotted one drawn (with Q being
the contact point). A spoke will not appear blurred at the point where this circular
motion is along the direction of the spoke. That is, a spoke will not appear blurred
at the point where the dotted circle is tangent to the spoke, as shown.
R
θ
wheelP
O
Q
We are therefore concerned with the locus of all points P such that the segments
PQ and PO are perpendicular. As seen in the previous diagram above, this locus
is the circle whose diameter is the lower vertical radius of the wheel.
2

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Sol39

  • 1. Solution Week 39 (6/9/03) Viewing the spokes The contact point on the ground does not look blurred, because it is instantaneously at rest. But although this is the only point on the wheel that is at rest, there will be other locations in the picture where the spokes do not appear blurred. The relevant property of a point in the picture where a spoke does not appear blurred is that the point lies on the spoke throughout the duration of the camera’s exposure. (The point in the picture need not, however, actually correspond to the same atom on the spoke.) At a given time, consider a spoke in the lower half of the wheel. A short time later, the spoke will have moved (via both translation and rotation), but it will intersect its original position. The spoke will not appear blurred at this intersection point. We must therefore find the locus of these intersections. We can do this in two ways. First method: Let R be the radius of the wheel. Consider a spoke that makes an angle of θ with the vertical at a given time. If the wheel then rolls through a small angle dθ, the center moves a distance R dθ. The spoke’s motion is a combination of a translation through this distance R dθ, plus a rotation through the angle dθ (around the top end). Let r be the radial position of the intersection of the initial and final positions of the spoke. In the following figure, we can write down two expressions for the short segment drawn perpendicular to the initial position of the spoke. Rdθ dθ θ θ r The two expression are (R dθ) cos θ, and r dθ (to first order in dθ). Equating these gives r = R cos θ. This describes a circle whose diameter is the lower vertical radius of the wheel, as shown below. 1
  • 2. R θ r=Rcosθ wheel Second method: Since the wheel’s contact point with the ground is instanta- neously at rest, the wheel may be considered to be instantaneously rotating around this point. This means that every atom in the wheel (both in the spokes and the rim) instantaneously traces out the arc of a circle centered at the contact point. For the point P in the figure below, this circle is the dotted one drawn (with Q being the contact point). A spoke will not appear blurred at the point where this circular motion is along the direction of the spoke. That is, a spoke will not appear blurred at the point where the dotted circle is tangent to the spoke, as shown. R θ wheelP O Q We are therefore concerned with the locus of all points P such that the segments PQ and PO are perpendicular. As seen in the previous diagram above, this locus is the circle whose diameter is the lower vertical radius of the wheel. 2