We have analysed the shape of the Fundamental Plane (FP) for a sample
of 226 E and SO galaxies in 10 clusters of galaxies. We find that the
distribution of galaxies is well approximated by a plane of the form l
og r(e) = 1.24 log sigma - 0.82 log [I](e) + gamma for photometry obta
ined in Gunn r. This result is in good agreement with previous determi
nations. The FP has a scatter of 0.084 in log r(e). For galaxies with
velocity dispersion larger than 100 km s(-1) the scatter is 0.073. If
the FP is used for distance determinations this scatter is equivalent
to 17 per cent uncertainties on distances to single galaxies. We find
that the slope of the FP is not significantly different from cluster t
o cluster. Selection effects and measurement errors can introduce bias
es in the derived slope. The residuals of the FP correlate weakly with
the velocity dispersion and the surface brightness, Some of the coeff
icients used in the literature give rather strong correlations between
the residuals and absolute magnitudes, This implies that galaxies nee
d to be selected in a homogeneous way to avoid biases of derived dista
nces on the level of 5-10 per cent or smaller. The FP has significant
intrinsic scatter. No other structural parameters like ellipticity or
isophotal shape can reduce the scatter significantly. This is in contr
adiction to simple models, which predict that the presence of discs in
E and SO galaxies can introduce scatter in the FP. It remains unknown
what the source of scatter is, It is therefore unknown whether this s
ource produces systematic errors in distance determinations. The Mg-2-
sigma relation for the cluster galaxies differs slightly from cluster
to cluster, Galaxies in clusters with lower velocity dispersions have
systematically lower Mg-2. The effect can be caused by both age and me
tallicity variations, With the current stellar population models, the
best agreement with our results regarding the FP is if the offsets are
mainly caused by differences in metallicity, Most of the distances th
at we derive from the FP imply small peculiar motions (< 1000 km s(-1)
). The zero point of the FP must therefore be quite stable. Only for o
ne cluster, located 28 degrees from the direction towards the 'Great A
ttractor', do we find a peculiar motion of 1300 km s(-1). This motion
is reduced to 890 km s(-1) if we use the FP corrected for the offset o
f the Mg-2-sigma relation, This confirms earlier suggestions that the
residuals from the Mg-2-alpha relation can be used to flag galaxies wi
th deviant populations, and possibly to correct the distance determina
tions for the deviations.