Abstract

Given the ecological and economic importance of eastern boundary upwelling systems like the California Current System (CCS), their evolution under climate change is of considerable interest for resource management. However, the spatial resolution of global earth system models (ESMs) is typically too coarse to properly resolve coastal winds and upwelling dynamics that are key to structuring these ecosystems. Here we use a high-resolution (0.1°) regional ocean circulation model coupled with a biogeochemical model to dynamically downscale ESMs and produce climate projections for the CCS under the high emission scenario, Representative Concentration Pathway 8.5. To capture model uncertainty in the projections, we downscale three ESMs: GFDL-ESM2M, HadGEM2-ES, and IPSL-CM5A-MR, which span the CMIP5 range for future changes in both the mean and variance of physical and biogeochemical CCS properties. The forcing of the regional ocean model is constructed with a “time-varying delta” method, which removes the mean bias of the ESM forcing and resolves the full transient ocean response from 1980 to 2100. We found that all models agree in the direction of the future change in offshore waters: an intensification of upwelling favorable winds in the northern CCS, an overall surface warming, and an enrichment of nitrate and corresponding decrease in dissolved oxygen below the surface mixed layer. However, differences in projections of these properties arise in the coastal region, producing different responses of the future biogeochemical variables. Two of the models display an increase of surface chlorophyll in the northern CCS, consistent with a combination of higher nitrate content in source waters and an intensification of upwelling favorable winds. All three models display a decrease of chlorophyll in the southern CCS, which appears to be driven by decreased upwelling favorable winds and enhanced stratification, and, for the HadGEM2-ES forced run, decreased nitrate content in upwelling source waters in nearshore regions. While trends in the downscaled models reflect those in the ESMs that force them, the ESM and downscaled solutions differ more for biogeochemical than for physical variables.

Highlights

  • The California Current System (CCS) is one of the four global eastern boundary upwelling systems (EBUSs) characterized by extraordinary biological productivity that supports a variety of human uses including tourism, fisheries, and recreation (e.g., Checkley and Barth, 2009)

  • The Southern California Bight (SCB) shows the largest sea surface temperature (SST) bias (∼1.4◦C), which is comparable with other numerical simulations of the CCS (e.g., Veneziani et al, 2009; Renault et al, 2016) and is likely due to the poor representation of cloud cover and the cross-shore gradient in alongshore winds resulting from coarse spatial resolution in the forcing reanalysis data (Renault et al, 2020)

  • The annual mean subsurface patterns of nitrate and dissolved oxygen in the control simulation (CTRL) simulation are well represented compared to climatological values from the World Ocean Atlas (WOA)

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Summary

Introduction

The California Current System (CCS) is one of the four global eastern boundary upwelling systems (EBUSs) characterized by extraordinary biological productivity that supports a variety of human uses including tourism, fisheries, and recreation (e.g., Checkley and Barth, 2009). Global climate models suggest that the Bakun hypothesis is overly simplified; projected changes in upwelling are likely to be season- and latitude-dependent, with intensification of CCS upwelling during spring, especially in the southern CCS, followed by a significant weakening of upwelling during the summer months, especially in the northern region of the CCS (e.g., García-Reyes et al, 2015; Rykaczewski et al, 2015; Wang et al, 2015) These anthropogenic trends in upwelling are not likely to be emergent until mid-century (∼2050) in the southern CCS and even later (∼2080) in the northern CCS (Brady et al, 2017), as strong decadal variability remains the dominant signal on shorter time horizons

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