Beach morphology dynamics are driven by the interaction of water motion and sediment over a geological substratum. Coastal sediment transport is still poorly understood so that model representations largely rely on simplifications and parameterisations (Amoudry & Souza, 2011). At length scales comparable to the surf zone width or larger (>10-100 m), sediment transport can be conceptually decomposed into two main components. Longshore transport is driven by the surf-zone longshore current generated by breaking waves if they approach obliquely to the coast. Cross-shore transport is the main cause of the cross-shore beach profile sloping up onshore, sometimes with shore parallel sand bars. The main sources of cross-shore transport are onshore transport driven by wave asymmetry and skewness, offshore transport due to undertow (bed-return current) and downslope transport due to gravity (Fernández-Mora et al., 2015). An equilibrium bed profile is achieved if the three components are in balance. Finally, there are more contributions to sediment transport that do not fall into the longshore or cross-shore categories (e.g., those associated to rip current circulation or to low frequency motions).On sandy coasts, beach morphology is rarely alongshore uniform. Typically, the shoreline has undulations and the nearshore sea bed features shallows and deeps alongshore. Transverse bar systems (Ribas et al., 2015) are a well-known example, encompassing a series of shallows or bars separated by deeps called rip channels (Figure 1). These systems are not only fascinating but also relevant from a scientific point of