Gluon jets are identified in hadronic Z(0) decays as all the particles in a
hemisphere opposite to a hemisphere containing two tagged quark jets. Gluo
n jets defined in this manner are equivalent to gluon jets produced from a
color singlet point source and thus correspond to the definition employed f
or most theoretical calculations. In a separate stage of the analysis, we s
elect quark jets in a manner to correspond to calculations, as the particle
s in hemispheres of flavor tagged light quark (uds) events. We present the
distributions of rapidity, scaled energy, the logarithm of the momentum, an
d transverse momentum with respect to the jet axes, for charged particles i
n these gluon and quark jets. We also examine the charged particle multipli
city distributions of the jets in restricted intervals of rapidity. For sof
t particles at large pr, we observe the charged particle multiplicity ratio
of gluon to quark jets to be 2.291+/-0.09 (stat.)+/-0.15 (syst.), in agree
ment with the prediction that this ratio should approximately equal the rat
io of QCD color factors, C-A/C-F = 2.25. The intervals used to define soft
particles and large p(T) for this result, p < 4 GeV/c and 0.8 < p(T) < 3.0
GeV/c, are motivated by the predictions of the Herwig Monte Carlo multihadr
onic event generator. Additionally, our gluon jet data allow a sensitive te
st of the phenomenon of non-leading QCD terms known as color reconnection.
We test the model of color reconnection implemented in the Ariadne Monte Ca
rlo multihadronic event generator and find it to be disfavored by our data.