  Colormagnetic confinement as a natural component of the QCD confinement is
explained and treated in the framework of the Field Correlator Method. For
quarks and gluons in hadrons the effects of the colormagnetic confinement are
discussed at zero temperature, where it contributes to the spectrum properties
and can create its own bound states, while at nonzero temperature in the EoS of
the quark gluon plasma the colormagnetic confinement plays a dominating role.
Its properties in the QCD thermodynamics are discussed in detail.
