Heterogeneous, non-stationary noise sources can cause traveltime errors in noise-based seismic monitoring. The effect worsens with increasing temporal resolution. This may lead to costly false alarms in response to safety concerns and limit our confidence in the results when these systems are used for quasi real-time monitoring of subsurface changes. We therefore develop a new method to quantify and correct these traveltime errors to more accurately monitor subsurface conditions at daily or even hourly timescales. This is based on the inversion of noise correlation asymmetries for the time-dependent distribution of noise sources. The source model is then used to simulate time-dependent ambient noise correlations. The comparison to correlations computed for homogeneous noise sources yields 1 Downloaded 04/23/17 to 132.239.1.231. Redistribution subject to SEG license or copyright; see Terms of Use at http://library.seg.org/ traveltime errors that translate into spurious changes of the subsurface. The application of our method to data acquired at Statoil's SWIM array, a permanent seismic installation at the Oseberg field, demonstrates that fluctuations in the noise source distribution may induce apparent velocity changes of 0.25 % within one day. Such biases thereby likely mask realistic subsurface variations expected on these timescales. These errors are systematic, dependent primarily on the noise source location and strength, and not on inter-station distance. Our method can then be used to correct for source-induced traveltime errors by subtracting these quantified biases in either data or model space. It can furthermore establish a minimum threshold for which we may reliably attribute traveltime changes to actual subsurface changes, should we not correct for these errors. In addition to the aforementioned real data scenario, we apply our method to a synthetic case for a daily passive monitoring overburden feasibility study. Both synthetics and field experiments validate the method's theory and application.2 Downloaded 04/23/17 to 132.239.1.231. Redistribution subject to SEG license or copyright; see Terms of Use at http://library.seg.org/ source distribution. Finally, instead of blindly performing waveform inversion with these biased traveltimes, we formulate how to remove these errors so that our velocities are unaffected by noise source non-stationarity. Preferably, this is done in the data space before proceeding to the tomography. We now discuss these steps in further detail.The SWIM array, shown in Figure 1, consists of 172 four-component receivers (MEMS accelerometer and hydrophone) linked through a single ocean-bottom cable. The configuration lies along the ocean floor, roughly 108 m below mean sea level, about 150 m south of the Oseberg C platform. Its purpose is to monitor cuttings injected into the overburden.Receiver spacing is ∼ 50 m for receivers on the outside boundaries of the array and reduces to ∼ 25 m for receivers in its inner portion. The spread of the array's outer right-side is around 1.74...