JASA
https:/doi.org/10.1121/10.0043324
Measured-Scaled Median and Mean RNL
N
— A Median RNL
— A Mean RNL
generic speed effect is inherently limited. The negative corre-
lation between RNL and distance, increasing with frequency,
indicates that a residual distance dependence remains in the
data. Since a negative correlation means that RNLs decrease
with increasing distance, this pattern implies that, particularly
at higher frequencies, more distant vessels are associated with
systematically lower RNLs.
While the bivariate analyses provide useful first-order
insights, they do not capture potential interactions between
vessel properties and operational parameters. To address
this, we applied GAM and RF regressions per frequency
band to assess the relative importance of each parameter.
GAMs and RFs were computed across eight different com-
binations of the following predictors: speed, length, dis-
tance, propulsion type, and individual vessel [Maritime
Mobile Service Identity (MMSI)]. Three different propul-
sion types were found for the investigated CTVs: controlla-
ble pitch propellers (CPPs), fixed pitch propellers (FPPs),
and APs. Model performance was evaluated using the
adjusted coefficient of determination (adjusted R?), which
accounts for differences in model complexity and allows a
fair comparison between models with different numbers of
predictors. All GAMSs were statistically significant (F tests,
p < 0.05 across frequency bands), confirming that the evalu-
ated predictor sets explain a non-random fraction of the
observed RNL variability. For the RF models, statistical sig-
nificance in the classical sense cannot be assessed via p val-
ues. Model performance is therefore evaluated
comparatively, based on explained variance (adjusted R?).
The frequency-dependent effects and relative impor-
tance of the individual predictors inferred from the GAMs
and RF models are illustrated in Fig. S5 in the supplemen-
tary material, providing insight into how the explanatory
power of the multivariate models is distributed across pre-
dictors and frequency bands.
Overall model performance is summarized in Table III.
which reports mean adjusted R* values averaged over all 37
Me
=
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410-
103 10%
Frequency (Hz)
10%
FIG. 6. Differences between J-E scaled and unscaled RNL spectra (mean
and median), illustrating the limited effect of J-E speed and length scaling
on the observed RNL variability.
vessel speed, length, and DCPA (see Fig. 7). The resulting
relationships between RNL, speed, and length are frequency
dependent. While speed primarily influences sound levels at
40 and 8SOHz, there is a noticeable trend suggesting that lev-
e]s above 1kHz tend to increase with vessel length.
However, the maximum correlation of approximately 0.5 is
relatively weak, indicating that these bivariate relationships
between RNL and individual predictors explain only a lim-
ited fraction of the observed variability when considered in
isolation.
It is also important to note that ship-specific correlations
‘gray lines in Fig. 7) differ significantly from the overall cor-
relation for speed. Additionally, the observed trend with ves-
sel length is based on only 13 vessels with a limited range of
lengths and is therefore not conclusive. Given the relatively
narrow speed distributions in our dataset (10-25 kn) (Table
[I; see Fig. 9, right panel, below), statistical power to isolate a
RNL vs. Speed
RNL vs. Length
RNL vs. Distance
).5
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BP
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ge Va
fm
ab
vet
daft
103 104 107 10? 10? 10% 2201 a
Frequency (Hz) Frequency (Hz)
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A
a PAS
ha He
Vi 1,8 Ba
Fre an
quency (H.
zZ)
10%
FIG. 7. Spearman correlation coefficients of the RNLs with speed, length, and distance. Gray lines represent correlations with individual vessels.
J. Acoust. Soc. Am. 159 (4), April 2026
Basan et al. 341‘