The ground state of the Dirac one-electron atom, placed in a weak, static electric field of definite 2 L -polarity, is studied within the framework of the first-order perturbation theory. The Sturmian expansion of the generalized Dirac-Coulomb Green function [R. Szmytkowski, J. Phys. B 30 (1997) 825, erratum: 30 (1997 2747] is used to derive closed-form analytical expressions for various far-field and near-nucleus static electric multipole susceptibilities of the atom. The far-field multipole susceptibilities -the polarizabilities αL, electric-to-magnetic crosssusceptibilities α EL→M(L∓1) and electric-to-toroidal-magnetic cross-susceptibilities αEL→TL -are found to be expressible in terms of one or two non-terminating generalized hypergeometric functions 3F2 with the unit argument. Counterpart formulas for the near-nucleus multipole susceptibilities -the electric nuclear shielding constants σEL→EL, near-nucleus electric-to-magnetic cross-susceptibilities σ EL→M(L∓1) and near-nucleus electric-to-toroidalmagnetic cross-susceptibilities σEL→TL -involve terminating 3F2(1) series and for each L may be rewritten in terms of elementary functions. Exact numerical values of the far-field dipole, quadrupole, octupole and hexadecapole susceptibilities are provided for selected hydrogenic ions. Analytical quasi-relativistic approximations, valid to the second order in αZ, where α is the fine-structure constant and Z is the nuclear charge number, are derived for all types of the far-field and near-nucleus susceptibilities considered in the paper.