  We employ an Einstein-Maxwell-Dilaton (EMD) holographic model, which is known
to be in good agreement with lattice results for the QCD equation of state with
$(2+1)$ flavors and physical quark masses, to investigate the temperature and
baryon chemical potential dependence of the susceptibilities, conductivities,
and diffusion coefficients associated with baryon, electric, and strangeness
conserved charges. We also determine how the bulk and shear viscosities of the
plasma vary in the plane of temperature and baryon chemical potential. The
diffusion of conserved charges and the hydrodynamic viscosities in a baryon
rich quark-gluon plasma are found to be suppressed with respect to the zero net
baryon case. The transition temperatures associated with equilibrium and
non-equilibrium quantities are determined as a function of the baryon chemical
potential for the first time. Because of the crossover nature of the QCD phase
transition even at moderately large values of the chemical potential, we find
that the transition temperatures associated with different quantities are
spread in the interval between $130-200$ MeV and they all decrease with
increasing baryon chemical potential.
