The spin of a gyroscope that undergoes Thomas precession seems to change its direction without any torque, which would mean that conservation of angular momentum is violated. To resolve this paradox, it is shown that the spin dynamics equation describing Thomas precession (the BMT equation) can be written in terms of a torque applied to the spin. A simple method of finding an explicit expression for the torque is presented in the case of a gyroscope performing circular motion. An unexpected oscillatory character of the torque is explained in terms of the difference between the proper spin and the spin observed in the laboratory frame.

1.
L. H.
Thomas
, “
The kinematics of an electron with an axis
,”
Philos. Mag.
3
,
1
22
(
1927
).
2.
R. A.
Muller
, “
Thomas precession: Where is the torque?
,”
Am. J. Phys.
60
,
313
317
(
1992
).
3.
C.
Misner
,
K.
Thorne
, and
J. A.
Wheeler
,
Gravitation
(
Freeman
,
San Francisco
,
1973
), p.
175
.
4.
V.
Bargmann
,
L.
Michel
, and
V. L.
Telegdi
, “
Precession of the polarization of particles moving in a homogeneous electromagnetic field
,”
Phys. Rev. Lett.
2
,
435
436
(
1959
).
5.
K.
Rębilas
, “
Simple approach to relativistic spin dynamics
,”
Am. J. Phys.
79
,
1064
1067
(
2011
).
6.
K.
Rębilas
, “
Thomas precession and the Bargmann-Michel-Telegdi equation
,”
Found. Phys.
41
,
1800
1809
(
2011
).
7.
J. D.
Jackson
,
Classical Electrodynamics
, 3rd ed. (
Wiley
,
New York
,
1999
), Sec. 11.8.
8.
W. K. H.
Panofsky
and
M.
Philips
,
Classical Electricity and Magnetism
(
Addison-Wesley
,
Reading, MA
,
1962
), p.
441
.
9.
R.
Hagedorn
,
Relativistic Kinematics
(
W. A. Benjamin
,
New York
,
1963
), Sec. 9–4.
AAPT members receive access to the American Journal of Physics and The Physics Teacher as a member benefit. To learn more about this member benefit and becoming an AAPT member, visit the Joining AAPT page.