We have studied the microwave electrodynamics of single crystal iron-based superconductors Ba0.72K0.28Fe2As2 (hole-doped, Tc ≈ 30 K) and Ba(Fe0.95Co0.05)2As2 (electron-doped, Tc ≈20 K), by cavity perturbation and broadband spectroscopy. SQUID magnetometry was used to confirm the quality and homogeneity of the samples under study. Through cavity perturbation techniques, the temperature dependence of the in-plane London penetration depth ∆λ(T ), and therefore the superfluid phase stiffness λ 2 (0)/λ 2 (T ) was measured. Down to 0.4 K, the data do not show the exponential saturation at low temperatures expected from a singly-, fully-gapped superconductor. Rather, both the electron-and the hole-doped systems seem to be best described by a power law behavior, with λ 2 (0)/λ 2 (T ) ∼ T n and n ≈ 2.5. In the three samples we studied, a weak feature near the sensitivity limit of our measurements appears near T /Tc = 0.04, hinting at a corresponding low energy feature in the superconducting density of states. The data can also be relatively well-described by a simple two-gap s-wave model of the order parameter, but this yields parameters which seem unrealistic and dependent on the fit range. Broadband surface resistance measurements reveal a sample dependent residual loss whose origin is unclear. The data from the Ba0.72K0.28Fe2As2 samples can be made to scale as ω 2 if the extrinsic loss is treated as an additive component, indicating large scattering rates. Finally, the temperature dependence of the surface resistance at 13 GHz obeys a power law very similar to those observed for ∆λ(T ).