We discuss a project on rigid-body motion that is appropriate for students in an upper-division course in classical mechanics. We analyze the motion of Hurricane Balls, two spheres that are welded (or glued) together so they act as a single object that can be spun like a top. The steady-state motion consists of purely rotational motion about the center of mass, such that only one ball is in contact with the table as it rolls without slipping. We give a qualitative explanation for why one ball rises into the air, and we theoretically analyze the system using multiple approaches. We also perform a high-speed video analysis to obtain experimental data on how the orientation depends on the spin rate, and find agreement within a few percent of the theory.

1.
Virtually all modern classical mechanics textbooks discuss the motion of a heavy symmetric top. See, for example,
John R.
Taylor
,
Classical Mechanics
(
University Science Books
,
Sausalito
,
2005
), Sec. 10.10.
2.
Official
” Hurricane Balls were available from a company specializing in science toys called Grand Illusions (<http://www.grand-illusions.com>) but were no longer available at the time this article was written. However, a replacement item called tornado balls, which appears to be identical to the original Hurricane Balls (though manufactured by a different company), is available.
3.
A. D.
Fokker
, “
The rising top, experimental evidence and theory
,”
Physica
8
,
591
596
(
1941
).
4.
A recent article that discusses several aspects of spinning tops, including the behavior of a tippe top, is
R.
Cross
, “
The rise and fall of spinning tops
,”
Am. J. Phys.
81
,
280
289
(
2013
).
5.
A very readable presentation of the basic mechanism responsible for the behavior of a rattleback can be found in
W.
Case
and
S.
Jalal
, “
The rattleback revisited
,”
Am. J. Phys.
82
,
654
658
(
2014
).
6.
According to Ref. 5, the rattleback was investigated as far back as 1896 (
G. T.
Walker
, “
On a dynamical top
,”
Q. J. Pure Appl. Math.
28
,
175
184
(
1896
)),
but the toy was popularized in the 1970s by
J.
Walker
, “
The mysterious ‘rattleback’: A stone that spins in one direction and then reverses
,”
Sci. Am.
241
,
172
184
(
1979
).
7.
As described in
Richard P.
Feynman's
book,
Surely, You're Joking, Mr. Feynman!
(
Norton
,
New York
,
1997
),
a cafeteria plate tossed in the air provides another simple example of torque-free motion, one in which Feynman noticed that there was a relationship between the spinning and the wobbling. An analysis of this situation is given by
Slavomir
Tuleja
,
Boris
Gazovic
, and
Alexander
Tomori
, “
Feynman's wobbling plate
,”
Am. J. Phys.
75
,
240
244
(
2007
).
8.
An early article that discusses the “wobbling” motion of symmetric objects, including a description of a stroboscopic apparatus to view “slow motion,” is
L. A.
Whitehead
and
F. L.
Curzon
, “
Spinning objects on horizontal planes
,”
Am. J. Phys.
51
449
452
(
1983
).
9.
W. L.
Andersen
and
Steven
Werner
, “
The dynamics of Hurricane Balls
,”
Eur. J. Phys.
36
,
055013-1
7
(
2015
).
10.

We note here that the analysis is not symmetric; that is, if the left ball in Fig. 2 were to momentarily lose contact with the table, this would not result in the left ball rising into the air.

11.

The fact that the steady-state motion of the double-sphere is one of steady precession without nutation is not completely obvious. Evidently, in dissipating energy, the frictional force (and to a lesser extent air drag) quickly damps out any nutation until the condition θ̇=0 is reached (see Fig. 4). This observed fact allows one to approach this problem using an energy-minimization procedure, as discussed in  Appendix B 2.

12.
See Taylor, Ref. 1, p. 342.
13.
A modern and very engaging toy with a motion similar to a double-sphere is Euler's Disk (official website <http://www.eulersdisk.com>). One intriguing aspect of this toy is that while the double-sphere's rotational frequency decreases as energy is lost from the system (θπ/2), Euler's disk has the property that the rotational frequency increases as energy is lost from the system (θ0). Thus, you can hear the rotation rate increase dramatically as both θ and L approach the vertical. See, for example,
H. K.
Moffat
, “
Euler's disk and its finite-time singularity
,”
Nature
404
,
833
834
(
2000
).
14.

Interestingly, using the condition α = 0 to calculate θmin leads to the expression θmin=2tan13/7, whereas we previously determine that θmin=cos1(2/5). Students might be amused to learn that cos1(2/5)=2tan13/7 and can be challenged to prove this fact.

15.

While higher frame rates will result in more accurate data, a 2,000 fps camera is not necessary to obtain reasonable experimental data. In order to prevent aliasing, the frame rate needs to be at least double the rotation frequency of the motion (but of course higher frame rates are always better). Thus, spin rates up to 6,000rpm100 Hz can be analyzed using a camera with a frame rate of only 200 fps, which is within the capabilities of many cell-phone cameras. It is worth noting, however, that to make high-quality slow-motion videos of this motion, such as the movie linked to Fig. 3, requires frame rates that are about an order of magnitude higher than what is minimally necessary to obtain useable data.

16.
Tracker is a free video analysis and modeling tool built on the Open Source Physics (OSP) Java framework, designed to be used in physics education. More information on Tracker can be found at <https://www.cabrillo.edu/~dbrown/tracker>.
17.
Though not quite as engaging as Hurricane Balls, another real-life situation that most people are familiar with is discussed by
M. G.
Olsson
, “
Coin spinning on a table
,”
Am. J. Phys.
40
,
1543
1545
(
1977
).
18.
A detailed analysis of the rolling disk problem is given by
A. J.
McDonald
and
K. T.
McDonald
, “
The rolling motion of a disk on a horizontal plane
,”
2001
. <http://www.hep.princeton.edu/~mcdonald/examples/rollingdisk.pdf>.
19.
W. L.
Andersen
, “
Noncalculus treatment of steady-state rolling of a thin disk on a horizontal surface
,”
Phys. Teach.
45
,
430
433
(
2007
).
20.
Attaching objects to spheres has been discussed as a possible way to produce a tippe top; see
R.
Cross
, “
Spherical tippe tops
,”
Phys. Teach.
51
,
144
145
(
2013
).
21.
A passive rotation matrix is used when the coordinate axes are rotated while the vector remains fixed. An active rotation matrix is used when the vector itself is rotated and the coordinate axes remain fixed. These rotation matrices are related to each other by θθ. See, for example,
Mary L.
Boas
,
Mathematical Methods in the Physical Sciences
, 3rd ed. (
Wiley
,
Hoboken, NJ
,
2006
), pp.
124
130
.
22.

This approach is a standard feature of most textbooks in classical mechanics when dealing with a spinning top, and typically includes a discussion of the energy. See, for example, Taylor, Ref. 1, pp. 401–407.

23.

When analyzing the motion of a spinning top with a fixed point of contact, most textbooks do not specifically mention that the motion of the center of mass is being neglected. But save for the trivial case of a “sleeping” top, the center of mass will be in obvious motion, even for the case of steady precession. Thus, even if explicitly stated (and valid), such an assumption can be mystifying to a student who can plainly observe such center-of-mass motion. The motion of a double-sphere, on the other hand, is such that the center of mass appears to be (very nearly) at rest.

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