The magnetocaloric effect of a given material is typically assessed through indirect estimates of the isothermal magnetic entropy change, $\mathrm{\ensuremath{\Delta}}{S}_{M}$. While estimating the adiabatic temperature difference, $\mathrm{\ensuremath{\Delta}}{T}_{\mathrm{ad}}$, is more relevant from the standpoint of refrigeration device engineering, this requires specialized experimental setups. We here present an approach to directly measure $\mathrm{\ensuremath{\Delta}}{T}_{\mathrm{ad}}$ through time-dependent magnetometry in a commercial superconducting quantum interference device (SQUID) device. We use as reference material gadolinium under a 20-kOe field change, and compare our results with those of the literature. Under nonadiabatic experimental conditions, a remarkably similar $\mathrm{\ensuremath{\Delta}}{T}_{\mathrm{ad}}(T)$ curve profile is obtained; however, its peak amplitude is underestimated. With a simple compensation methodology we are able to further approximate the profile of the $\mathrm{\ensuremath{\Delta}}{T}_{\mathrm{ad}}(T)$ curve obtaining the peak amplitude, the maximizing temperature, and the FWHM within relative errors of $\ensuremath{-}4\mathrm{%}$, $\ensuremath{-}0.7\mathrm{%}$, and 11%, respectively. Our reported approach makes the measurement of both $\mathrm{\ensuremath{\Delta}}{S}_{M}(T)$ and $\mathrm{\ensuremath{\Delta}}{T}_{\mathrm{ad}}(T)$ possible with a single instrument, enabling accelerated progress towards new, competitive, and industry-ready materials.