The Gd2Sn2O7 pyrochlore Heisenberg antiferromagnet displays a phase transition to a four sublattice Néel ordered state at a critical temperature Tc ∼ 1 K. The low-temperature state found via neutron scattering corresponds to that predicted by a classical model that considers nearest-neighbor antiferromagnetic exchange and long-range dipolar interactions. Despite the seemingly conventional nature of the ordered state, the specific heat Cv has been found to be described in the temperature range 350 mK ≤ T ≤ 800 mK by an anomalous power law, Cv ∼ T 2 . A similar temperature dependence of Cv has also been reported for Gd2Ti2O7, another pyrochlore Heisenberg material. Such behavior is to be contrasted with the typical T 3 behavior expected for a three-dimensional antiferromagnet with conventional long-range order which is then generally accompanied by an exp(−∆/T ) behavior at lower temperature where anisotropy effects induce a gap ∆ to collective spin excitations. Such anomalous T 2 behavior in Cv has been argued to be correlated to an unusual energy-dependence of the density of states which also seemingly manifests itself in low-temperature spin fluctuations found in muon spin relaxation experiments. In this paper, we report calculations of Cv that consider spin wave like excitations out of the Néel order observed in Gd2Sn2O7 via neutron scattering. We argue that the parametric Cv ∝ T 2 does not reflect the true low-energy excitations of Gd2Sn2O7. Rather, we find that the low-energy excitations of this material are antiferromagnetic magnons gapped by single-ion and dipolar anisotropy effects, and that the lowest temperature of 350 mK considered in previous specific heat measurements accidentally happens to coincide with a crossover temperature below which magnons become thermally activated and Cv takes an exponential form. We argue that further specific heat measurements that extend down to at least 100 mK are required in order to ascribe an unconventional description of magnetic excitations out of the ground state of Gd2Sn2O7 or to invalidate the standard picture of gapped excitations proposed herein.