  Calculation of the nucleon magnetic moments was performed in the
quasipotential quark model.
  The main contribution into the nucleon magnetic moments is determined by the
SU(6) symmetrical spin-isospin part of the wave function and is equal to 3 and
-2 (in the units of nuclear magnetons) for proton and neutron, respectively.
  Corrections are explained by relative quark motion and are equal to $-4a/3$
and $+a$ for proton and neutron, respectively, where the dimensionless value
$a$ depends on the dimensionless ratio of the oscillator parameter and quark
mass in case of the oscillator interaction.
  It is shown that the independence of the nucleon magnetic moments on nucleon
mass is a consequence of relativistic kinematics.
  The invariant dimensionless parameter is introduced to estimate the violation
of current conservation.
  By means of this parameter it is shown that the current leakage is neglegibly
small in the model.
