“…The possible reason for this was the noticeable uncertainty in the half-lives of both approaches, caused by the low dissipation signal in the SMPC data and the attached high uncertainty of the measurement points themselves. In contrast to this, a clear, almost 1:1 relationship emerged in SMPC P3 (Figure , f (DT 50,model ) = 1.01 × f (DT 50,bench ), adjusted R 2 = 0.84, p = 1 × 10 –9 , for compounds with strictly positive half-lives, where DT 50,bench is the half-life estimated from benchmarking, DT 50,model is the half-life calculated from the Rhine model of Seller et al, and f () in the regression equation denotes a log-shift transformation that maps all DT 50 values to the positive domain: f ( x ) = ln( x ) + 2). The better performance of SMPC P3 compared to SMPC P1 can be attributed to the shorter half-lives and the much lower uncertainty of that data set, which improved the fit of both the benchmark method and the stream network transport model.…”