Abstract
Colormagnetic confinement as a natural component of the QCD confinement is explained and treated in the framework of the Field Correlator Method (FCM). 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 ownbound 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.In particular the CM string tension and the Debye screening mass calculated in FCM are compared with lattice data.
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