The nongravitational motion of the periodic comet Comas Sola is studie
d on the basis of positional observations made during nine consecutive
revolutions around the Sun. Nongravitational effects in the comet mot
ion have been examined for Sekanina's forced precession model of the r
otating nucleus. We present three models which successfully link all t
he observed apparitions of the comet during 1926-1996. Two solutions (
Models II and III) represent oblate spheroids and the third one (Model
I)- a prolate spheroid (nucleus rotation around its longer axis). We
have determined values of eight parameters: A, eta , I, phi connected
with the rotating comet nucleus, f(p) and s describing the precession
of spin-axis of the nucleus, and two constant time shifts tau(1) and t
au(2) The last two parameters describe displacements of the maximum va
lue of the known function g(r) with respect to the perihelion time. Th
e best solution was obtained assuming that between the apparitions of
1935 and of 1944 the time shift changed its value, thus tau(1) and tau
(2) refer to apparitions before and after 1940 Jan. 1, respectively. V
ariations of angles I and phi with time, describing the nucleus spin-a
xis orientation, are presented. It appears that forced precession caus
es the moderate changes of the position of the rotation axis in space.
The ratio of rotational period to radius of the nucleus was found for
each model. The present precession models are in agreement with sizes
and periods of rotation of other cometary nuclei deduced from observa
tions. The obtained models give some strong constraints on the physica
l parameters of the nucleus of comet P/Comas Sola. Assuming a prolate
spheroid for the nucleus of the comet, the expected rotational period
is 14 +/- 4 hours for an equatorial radius of 2 km. For the same radiu
s, the oblate Model II gives the much smaller rotational period of 2.4
+/- 0.4 hours. The polar radii are 2.2 km and 1.3 km for the prolate
and oblate model, respectively.