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Connection of Isolated Stereoclusters by Combining 13C-RCSA, RDC, and J-Based Configurational Analyses and Structural Revision of a Tetraprenyltoluquinol Chromane Meroterpenoid from Sargassum muticum

The seaweed Sargassum muticum, collected on the southern coast of Galicia, yielded a tetraprenyltoluquinol chromane meroditerpene compound known as 1b, whose structure is revised. The relative configuration of 1b was determined by J-based configurational methodology combined with an iJ/DP4 statistical analysis and further confirmed by measuring two anisotropic properties: carbon residual chemical shift anisotropies (13C-RCSAs) and one-bond 1H-13C residual dipolar couplings (1DCH-RDCs). The absolute configuration of 1b was deduced by ECD/OR/TD-DFT methods and established as 3R,7S,11R.


Introduction
Sargassum muticum (SM), also known as Japanese wireweed, is a brown alga, first described and classified by Yendo in 1907 as Sargassum kjellmanianum form muticum, based on morphological and ecological differences [1]. In 1955, Fensholt reconsidered this form as sufficiently differentiated from S. kjellmanianum and separated it into two species of their own, until it was finally named Sargassum muticum (Yendo) Fensholt [2,3]. This species has been the object of a multitude of studies. In 2017, Balboa et al. reported the use of SM as a potential antioxidant agent and as a preservative in the preparation of cosmetics [4]. Another work, conducted by Park, investigated the feasibility of using SM as a source of bioactive compounds [5]. This study concluded that adding SM pills to the normal diet showed liver benefits in addition to decreasing fatigue and stress. These effects were related to bioactive compounds compatible with meroterpenes or fucoxanthines [6].
Meroditerpenoids of the chromene, where the polyprenyl moiety is bonded to a hydroquinone or similar aromatic ring [7], constitute a very important family of compounds isolated from Sargassum. Almost a hundred meroditerpenes have been reported from marine organisms such as fish, macroalgae, sponges, coelenterates, and tunicates [7][8][9][10]. These compounds have been used in various cancer therapies based on their ability to protect against oxidative damage [11,12].
Meroditerpenoids of the chromene, where the polyprenyl moiety is bonded to a hydroquinone or similar aromatic ring [7], constitute a very important family of compounds isolated from Sargassum. Almost a hundred meroditerpenes have been reported from marine organisms such as fish, macroalgae, sponges, coelenterates, and tunicates [7][8][9][10]. These compounds have been used in various cancer therapies based on their ability to protect against oxidative damage [11,12].
In 1993, Praud et al. isolated C3-epimeric meroditerpenoids 1a and 1b from Cystoseira baccata [13]. They proposed a cis-fused chromene ring structure, although the configuration at C3 could not be established at that point. Rapid epimer interconversion was observed in CDCl3. Later, Varela et al. also reported antileishmanial activity in those compounds [14]. In 2015, we isolated tetraprenyltoluquinol chromane meroterpenoids 1a and 1b as an epimeric mixture at position C3 from the methanolic extract of the alga (See Figure 1). Moreover, we described their use as photoprotective agents used to mitigate skin damage caused by UV exposure [10]. Considering that obtaining the 1a/1b mixture was probably due to the use of CDCl3 [10,13,15], we repeated the isolation procedure recording the NMR analysis in CD2Cl2. Additionally, the relative configuration of two well-separated stereoclusters (C3 and C7/C11) in 1a-1b was determined by J-based configurational analysis along with 13 C-residual chemical shift anisotropies ( 13 C-RCSA) [16] and residual dipolar couplings (RDCs) [17].

Results and Discussion
From the methanolic extract of SM, the n-hexane soluble fraction was separated by flash column chromatography and then purified by HPLC to obtain one of the epimers at position 3. The 950 MHz NMR spectra collected in CD2Cl2 did not show any evidence of epimerization for compound 1b. We observed the epimerization of the pure compound in CDCl3 after 25 min. The high resolution mass spectrum showed peaks at m/z 441.2969 ((M + H) + ), 463.2811 ((M + Na) + ), and 903.5741 ((2M + Na) + ), thus confirming the molecular formula C28H40O4. The 1 H NMR spectrum of 1b (Table 1) was then assigned in CD2Cl2, showing a singlet signal at δH 3.701, corresponding to the methoxy group attached to the aromatic nucleus. Two doublets, at δH 6.563 and 6.450, were assigned to aromatic protons, a harmonious relationship then being revealed between the small coupling constant (J = 3.0 Hz) and the 1′,2′,4′,6′-substituents meta-arranged around the benzene ring. A spin system formed by two contiguous methylene groups was also assigned by observing a 1 H-1 H COSY correlation between the protons at δH 1.805 (J = 13.5 Hz and 6.9 Hz) and at δH 2.774 (J = 6.9 Hz) disclosing the remaining chromane moiety. The five singlet signals belonging to methyl groups on sp 3   Considering that obtaining the 1a/1b mixture was probably due to the use of CDCl 3 [10,13,15], we repeated the isolation procedure recording the NMR analysis in CD 2 Cl 2 . Additionally, the relative configuration of two well-separated stereoclusters (C3 and C7/C11) in 1a-1b was determined by J-based configurational analysis along with 13 C-residual chemical shift anisotropies ( 13 C-RCSA) [16] and residual dipolar couplings (RDCs) [17].

Results and Discussion
From the methanolic extract of SM, the n-hexane soluble fraction was separated by flash column chromatography and then purified by HPLC to obtain one of the epimers at position 3. The 950 MHz NMR spectra collected in CD 2 Cl 2 did not show any evidence of epimerization for compound 1b. We observed the epimerization of the pure compound in CDCl 3 after 25 min. The high resolution mass spectrum showed peaks at m/z 441.2969 ((M + H) + ), 463.2811 ((M + Na) + ), and 903.5741 ((2M + Na) + ), thus confirming the molecular formula C 28 H 40 O 4 . The 1 H NMR spectrum of 1b (Table 1) was then assigned in CD 2 Cl 2 , showing a singlet signal at δ H 3.701, corresponding to the methoxy group attached to the aromatic nucleus. Two doublets, at δ H 6.563 and 6.450, were assigned to aromatic protons, a harmonious relationship then being revealed between the small coupling constant (J = 3.0 Hz) and the 1 ,2 ,4 ,6 -substituents meta-arranged around the benzene ring. A spin system formed by two contiguous methylene groups was also assigned by observing a 1 H-1 H COSY correlation between the protons at δ H 1.805 (J = 13.5 Hz and 6.9 Hz) and at δ H 2.774 (J = 6.9 Hz) disclosing the remaining chromane moiety. The five singlet signals belonging to methyl groups on sp 3 quaternary carbons were observed at δ H 0.804, 1.041, 1.105, 1.225, and 1.235, along with the three isolated methylene systems at δ H 2.705/2.514 (J = 13.7 Hz), 3.028/2.237 (J = 18.7 Hz), and 2.570/2.506 (J = 14.3 Hz). These three pairs were easily assigned to non-equivalent protons located at C4, C6, and C14. The remaining structure of 1b was completed by 1 H and 13 C data, 2D NMR ( 1 H-1 H COSY, HSQC, HMBC), and mass spectral data (see Figures S3-S13 and Table 1) confirmed the structure of the epimers previously isolated from Sargassum muticum and from a macroalgae belonging to the Cystoseira genus [13,14]. Configurational analysis of 1b. Surprisingly, when we tried to confirm the reported cis relationship of the two methyl groups at C7 and C11 in the hydrindane skeleton [10,13,14], we found an unexpected lack of NOE contact between Me18 and Me19 when both were selectively irradiated in a 1D-NOE experiment. A deeper NOE study (see Figure 2), along with a J-based configurational analysis [18][19][20][21] was performed through both 3 J CH and 2 J CH coupling constants obtained from IPAP-HSQMBC spectra and 1 J CC from a 2D J-modulated ADEQUATE spectrum (see Figure 3) to deduce the bicyclo[4.3.0]nonane fusion present in 1b (see Figures S14-S22 and Table S4).
Mar. Drugs 2022, 20, x FOR PEER REVIEW 4 of 17 J-modulated ADEQUATE spectrum (see Figure 3) to deduce the bicyclo[4.3.0]nonane fusion present in 1b (see Figures S14-S22 and Table S4).  The relative configuration of the C6 prochiral protons could be established just by the observation of NOE contacts between H19 and H6a and between H10a and H6a. The NOE correlations observed between H6b/H18 and H10b/H18, and between H6a/H19 and   Table S4).  The relative configuration of the C6 prochiral protons could be established just by the observation of NOE contacts between H19 and H6a and between H10a and H6a. The NOE correlations observed between H6b/H18 and H10b/H18, and between H6a/H19 and  Figure 3. Experimental 1 J CC and 3 J CH values in 1b extracted from an IPAP-HSQMBC used in the Jbased configurational analysis vs. DFT-calculated 1 J CC and 3 J CH (GIAO/OLYP/Def2TZV//B3LYP/6-31G(d) gas phase) values in silico models 2 and 3. Several 1 J CC were measured from a 2D J-modulated ADEQUATE experiment. Santonin and strychnine were used as tests. Strongly deviating couplings allowing the assignment of relative configuration are boxed. All vales are expressed in Hz.
The relative configuration of the C6 prochiral protons could be established just by the observation of NOE contacts between H19 and H6a and between H10a and H6a. The NOE correlations observed between H6b/H18 and H10b/H18, and between H6a/H19 and H8a/H10a, suggested that the relative configuration at C7 and C11 must be trans-7S*,11R* rather than cis. The high 3 J CH values measured between H10a and C18 of 8.2 Hz, and between H6b and C19 of 6.4 Hz in an IPAP-HSQMBC experiment (Figures S14-S18) were in harmony with a trans disposition between both methyl groups (see Figure 2).
To discriminate between cis and trans dimethyl configurations, 2 J CH and 3 J CH couplings were computed on in silico models 2 (trans) and 3 (cis) (see Figure 3) by using DFT calculations and compared with the experimental values of 1b. We tested different combinations of functional/basis set/gas phase, and solvent models to obtain heteronuclear couplings as accurate as possible, by using (-)-α-santonin and strychnine as test systems [22][23][24], (see Figure 3). To further improve accuracy, a scaling factor was used in the computations as described in the Supplementary Information (SI).
Overall, 46 DFT methods were examined using an empirical scaling factor to improve the accuracy of the computations (see SI) [25][26][27][28][29][30][31][32][33][34][35]. Heteronuclear 2 J CH and 3 J CH for (-)-α-santonin and strychnine were measured in DMSO-d 6 from IPAP-HSQMBC and HECADE-HSQC experiments. Among all the methodologies tested, the combination GIAO/OLYP/Def2TZV gave the best performance/computation time ratio. Afterwards, the standard deviation (σ) and the coefficient of determination (R 2 ) were computed ( 2 J CH : σ = 1.5 Hz, R 2 = 0.967, 3 J CH : σ = 2.3 Hz, R 2 = 0.978; see all details in SI). The good performance of OLYP is notable considering it is a pure GGA functional that does not include exact exchange. The DFT-calculated heteronuclear coupling constant values involving C7 and C11 in the trans-model 2 were in much better agreement with those of 1b in relation to the theoretical data computed for the cis-model 3 (see Figure 3). The trans fusion was also confirmed for this hydrindane by measuring the one-bond carbon-carbon scalar coupling constants ( 1 J CC ) between C7-C19 and C11-C18 in 1b from the 2D J-modulated ADEQUATE spectrum and comparing them to those theoretically obtained by DFT computation for models 2 and 3 at the same OLYP/Def2TZV level of theory. Both 1 J C7C19 and 1 J C11C18 of 28.7 Hz betokened the dimethyl trans configuration (DFT-calculated 1 J C7C19 and 1 J C11C18 are 33.1 and 30.8 Hz, respectively).
Once the relative configuration of 7S*,11R* for 1b was unequivocally assigned, we allocated its relation to C3. Unfortunately, J-based configurational analyses and NOE measurements were not able to discriminate the possible configurations for the two stereoclusters, whether (3R*,7S*,11R*) or (3S*,7S*,11R*) of 1b (Figure 4 only shows the analysis of 3R*,7S*,11R*; for 3S*,7S*,11R*, see Figure S31). H8a/H10a, suggested that the relative configuration at C7 and C11 must be trans-7S*,11R* rather than cis. The high 3 JCH values measured between H10a and C18 of 8.2 Hz, and between H6b and C19 of 6.4 Hz in an IPAP-HSQMBC experiment (Figures S14-S18) were in harmony with a trans disposition between both methyl groups (see Figure 2). To discriminate between cis and trans dimethyl configurations, 2 JCH and 3 JCH couplings were computed on in silico models 2 (trans) and 3 (cis) (see Figure 3) by using DFT calculations and compared with the experimental values of 1b. We tested different combinations of functional/basis set/gas phase, and solvent models to obtain heteronuclear couplings as accurate as possible, by using (-)--santonin and strychnine as test systems [22][23][24], (see Figure 3). To further improve accuracy, a scaling factor was used in the computations as described in the Supplementary Information (SI).
Overall, 46 DFT methods were examined using an empirical scaling factor to improve the accuracy of the computations (see SI) [25][26][27][28][29][30][31][32][33][34][35]. Heteronuclear 2 JCH and 3 JCH for (-)-αsantonin and strychnine were measured in DMSO-d6 from IPAP-HSQMBC and HECADE-HSQC experiments. Among all the methodologies tested, the combination GIAO/OLYP/Def2TZV gave the best performance/computation time ratio. Afterwards, the standard deviation (σ) and the coefficient of determination (R 2 ) were computed ( 2 JCH: σ = 1.5 Hz, R 2 = 0.967, 3 JCH: σ = 2.3 Hz, R 2 = 0.978; see all details in SI). The good performance of OLYP is notable considering it is a pure GGA functional that does not include exact exchange. The DFT-calculated heteronuclear coupling constant values involving C7 and C11 in the trans-model 2 were in much better agreement with those of 1b in relation to the theoretical data computed for the cis-model 3 (see Figure 3). The trans fusion was also confirmed for this hydrindane by measuring the one-bond carbon-carbon scalar coupling constants ( 1 JCC) between C7-C19 and C11-C18 in 1b from the 2D J-modulated ADE-QUATE spectrum and comparing them to those theoretically obtained by DFT computation for models 2 and 3 at the same OLYP/Def2TZV level of theory. Both 1 JC7C19 and 1 JC11C18 of 28.7 Hz betokened the dimethyl trans configuration (DFT-calculated 1 JC7C19 and 1 JC11C18 are 33.1 and 30.8 Hz, respectively).
This conformational flip/flop is characteristic of this type of chromane conformer on the dihydropyran ring (see Figures 4,S24 and S25), as it was deduced from the isochronic chemical shifts observed in both H1 and the averaged coupling constant measured for 3 J H1H2a = 6.7 Hz, 2 J C3H2a = 3.4 Hz, and 2 J C3H2b = 2.8 Hz (see Figure S21). From the observed coupling constants, we were able to deduce an equilibrium between P-helicity and Mhelicity conformers in a 3:2 ratio.
Trying to establish the relative configuration at C3, we followed the iJ/DP4 protocol of Daranas, Sarotti et al., involving a conformational search within a 5-kcal/mol interval, and then calculated the theoretical chemical shifts at the B3LYP/6-31G(d,p) level [36][37][38]. Contrasting calculated vs. experimental chemical shifts gave rise to a better DP4 score for the (3R*,7S*,11R*)-1b diastereoisomer (C/DP4: 94.25%, H/DP4: 100%). Next, 3 J C2H4a = 2.0 Hz, 3 J C2H4b = 2.1 Hz, 3 J C20H4a = 5.6 Hz, 3 J C20H4b = 0.2 Hz, | 2 J C3H4a |= 6.7 Hz, and | 2 J C3H4b |= 1.9 Hz from IPAP-HSQMBC experiments (see Newman projection on Figure 4) were read into the application of the iJ/DP4, implying four dihedral angle restrictions around the C3-C4 bond, to wit: Using iJ/DP4, we fully predicted the (3R*,7S*,11R*)-1b isomer, a slight 95.43% improvement being gained at 13 C and a complete one at 1 H (see Figure 5). Most populated conformers in both plausible configurations in the DP4 ensembles, generated by an unrestricted conformational search, satisfy the main constraints of chromane helicities, prochiral protons at C4 and C14, and weak hydrogen bonding between OH at C15 and C12 (C=O). Similarly, the forementioned set of conformers of plausible configurations of 1b was studied by applying the Computer-Assisted 3D Structure Elucidation (CASE-3D) strategy, as implemented in MNova StereoFitter [39,40], which makes no a priori assumptions about the conformational space. Only isotropic NMR data were utilized to elucidate the relative configuration of 1b. Both constitutions were ranked according to chemical shift predictions at the DFT level (GIAO/B3LYP/6-31G(d,p)) and 3 J CH coupling computed by Karplus-like equations. The CASE-3D analysis scored the (3R*,7S*,11R*)-1b configuration slightly better (See Figure S42). Anisotropic measurements of 1b: 13 C-RCSA and 1 D CH -RDC. To revalidate the structure of 1b deduced from chemical shift-based configurational analyses, anisotropic parameters such as carbon residual chemical shift anisotropy ( 13 C-RCSA) were utilized to relate both stereoclusters, separated from each other by four bonds. The RCSAs are manifested by the change in the chemical shift when the analyte is placed in a weak alignment medium such as a gel or a liquid crystal. The carbon RCSAs provide the relative orientations of the structural moieties, including those of non-protonated carbons C3, C7, and C11 as in our case study [16,41,42].
The conformational ensemble used for this analysis is shown for the correct configuration in Figure 6. Twenty-eight 13 C-RCSA values were measured using an in-house made 3 mm compression device and compressible PMMA-d 8 gel. Before applying the former to the RCSA data collection of 1b, its performance was tested using estrone as a standard sample (see Section S6 in SI). RCSAs were induced although small isotropic chemical shift changes also ensued because of the change in the solvent to gel ratio under compressed conditions (See Figure S32) [16]. These ∆RCSA values, not corrected for isotropic contributions, ranged between −7.4 and 5.5 Hz (see Table S7). Aromatic and carbonyl carbons exhibited larger ∆RCSAs than aliphatic carbons, reflecting the respective sizes of the CSA tensors [16,40]. A higher error in the fitting curve was noticed in the (3S*,7S*,11R*)-1b diastereoisomer relative to the other plausible configuration, even though automatic isotropic shift correction was not applied (Figures 6c and S38).
Consequently, we were able to differentiate between both plausible diastereomers by 13 C RCSA and to establish the relative configuration between the stereocenter at C3 and the stereocluster C7-C11 located four bonds away.
One-bond 13 C-1 H residual dipolar couplings ( 1 D CH -RDC) measurements were also conducted to confirm the relative configuration of 1b. Thus, a CLIP/CLAP-HSQC, spurred by non-uniform sampling [45,46] with a 1.6 mg sample, and using a deuterated PMMAd 8 (70/0.25) in a low viscosity solvent (CD 2 Cl 2 ), was measured to obtain RDC values. The accuracy of the 1 D CH values was enhanced as there was almost no interference from deuterated polymer background signals.
Seventeen RDCs were meticulously measured thanks to the narrow spectral line, resulting in 1 D CH values within a range of between 3.0 and −6.7 Hz. RDC data were fitted on an experimentally constrained ensemble of conformers for both plausible configurations as in the RCSA analysis (See Figure 7). accuracy of the 1 DCH values was enhanced as there was almost no interference from deuterated polymer background signals.
Seventeen RDCs were meticulously measured thanks to the narrow spectral line, resulting in 1 DCH values within a range of between 3.0 and −6.7 Hz. RDC data were fitted on an experimentally constrained ensemble of conformers for both plausible configurations as in the RCSA analysis (See Figure 7). Fitting the 1 D CH data, determining and aligning the tensor, and calculating Cornilescu's quality factor Q were carried out through single-tensor approximation on the MSpin-RDC software. Configuration (3R*,7S*,11R*)-1b showed a Q of 0.134, while (3S*,7S*,11R*)-1b had a Q of 0.328, the discrimination presenting a degree of linearity between experimental and back-calculated values (see Figure 7b). By using 1 D CH -RDC, configuration (3S*,7S*,11R*)-1b was removed from consideration with ease, showing the efficacy of the RDC methodology for establishing relative orientations of two distant stereoclusters of meroditerpene 1b.
Absolute configuration of 1b. Finally, we resorted to chiroptical methods (ECD/OR) to assign the absolute configuration (AC) of 1b. We used the empirical chromane helicity rule [47,48] and compared the experimental chiroptical data with predicted ECD/ORD from ab initio time-dependent DFT (TD-DFT). Currently, chiroptical methodologies associated with quantum chemical calculations are some of the most powerful tools for elucidating stereochemistry and examining even minute changes in the geometry of chiral molecules [49][50][51]. Determining the AC of this framework is also possible by following a chromane helicity rule [47,48]. This rule, established by Crabbé and related to 1 L b excitation of the chromophore, relates the sign of the ECD band with the helicity of the trisubstituted dihydropyran ring [48] at around 270-290 nm. An extra requirement for the application of the rule is that the largest substituent at the C3 carbon atom should favorably occupy an equatorial position. This rule was exhaustively studied in 2014 by Górecki and Frelek, who revised both the scope and limitations of comparing the experimental ECD spectra with those simulated by TD-DFT, and should, therefore, be used with great caution [52,53]. In our case, following Crabbé's rule, the ECD curve strongly depends on the population ratio of 1b conformers with the methyl group at C3 either in axial or equatorial positions.
Both the experimental and calculated ECD spectra as well as the OR value were applied to establish the AC of the stereoisomeric pairs exhibiting opposite ECD and OR. Two different levels of theory were chosen to calculate ECD curves: PBE0/Def2TVZ/W06 and HSE06/6-311+G(2d,p)/DGA1 basis sets, with 50 and 38 transition states, respectively, and COSMO-IEFPCM as solvent models (CH 2 Cl 2 ). Populations were calculated through Q factor minimization by NMR anisotropy constraints [54][55][56]. Calculations at two levels of theory clearly reproduced the 240-290 nm range of the ECD of 1b, demonstrating an equilibrium between conformers with M-(68%) and P-helicities (32%) with an excellent agreement towards the (3R,7S,11R) AC for 1b (see Figure 8). Figure 8a depicts the conformers found for the correct configuration of 1b along with their populations, derived from the analysis of NMR anisotropic parameters.
The specific optical rotation ([α] 25 D ) of 1b was experimentally measured, −11.67 (c 0.12, CH 2 Cl 2 ), and then computed at CAM-B3LYP/6-311++G(2d,2p)/DGA1 DFT level. The IEFPCM (CH 2 Cl 2 ) solvation effect model and the conformer population were the same as with the ECD calculation ( Figure 8). After comparing the experimental results with the DFT computed values, the sign was well reproduced, although the [α] 25 D was overestimated for (3R,7S,11R)-1b −49.4 (see Table S8). The absolute signs indicate that our approach is suitable for correlating the absolute configuration of molecules with rather restricted flexibility to the sign of the [α] 25 D . Both the ECD and the optical rotation approaches agree with the same identifications of 1b as 3R,7S,11R [57]. The specific optical rotation ( ) of 1b was experimentally measured, −11.67 (c 0.12, CH2Cl2), and then computed at CAM-B3LYP/6-311++G(2d,2p)/DGA1 DFT level. The IE-FPCM (CH2Cl2) solvation effect model and the conformer population were the same as with the ECD calculation ( Figure 8). After comparing the experimental results with the DFT computed values, the sign was well reproduced, although the was overestimated for (3R,7S,11R)-1b −49.4 (see Table S8). The absolute signs indicate that our approach is suitable for correlating the absolute configuration of molecules with rather restricted flexibility to the sign of the 25 . Both the ECD and the optical rotation approaches agree with the same identifications of 1b as 3R,7S,11R [57].

General
ECD and UV spectra were recorded on a JASCO J-815 CD spectrometer. The ECD spectrum of 1b was recorded in the region from 225 to 470 nm at a concentration of 0.2 mg/mL (2.88 × 10 −4 M) in CH 2 Cl 2 in a 1 mm cell, totaling five accumulations at a scan rate of 20 nm/min and a temperature of 25 • C. Specific optical rotation (OR) of 1b was recorded on a Jasco DIP-1000 polarimeter at 589 nm (Na lamp) at a concentration of 0.12 g/100 mL in CH 2 Cl 2 in a 1 dm/SiO 2 cuvette (25 • C). NMR spectra were recorded on either a 950, 900, 800, or a 700 MHz Bruker, all the signals being referenced to 13 C (54.00 ppm) and 1 H (5.320 ppm) signals of CD 2 Cl 2 . HR-MS were obtained on a Thermo Scientific LTQ Orbitrap XL mass spectrometer (Thermo Fisher Scientific, Waltham, MA, USA). Semipreparative HPLC was performed on an Agilent column (RP-C18 column 10 × 100 mm; 4.6 mL/min). TLC was performed on silica gel (Merck, Kieselgel 60 F 254 ) plates; the spots were visualized by exposure to UV light (254 nm). Column chromatography was carried on silica gel (Merck, Kieselgel 60).

Data Processing
Experimental and calculated ECD and UV data were handled with SpecDis V 1.7.1 developed by T. Bruhn [58]. NMR data were processed and analyzed by Bruker TopSpin Software V 4.1.1. Graphics were carried out on Microsoft Excel 365. Geometrical optimization and TDSCF calculation were carried out with the Gaussian 16 Suite. Molecular structures were drawn in ChemDraw V 12.0 and Avogadro V 1.0 [59]. Orbitrap files were processed using Xcalibur™ V 3.0 Software-Thermo Fisher Scientific-and its chemical molecular generator module was employed to provide elemental formulas. Conformer weighing by isotropic constraints was handled by the StereoFitter module nested in MNova Suite [39,40]. Anisotropic NMR and J-coupling data processing were performed using MSpin-RDC V 2.6.1.

Raw Material
The seaweed Sargassum muticum (SM) was collected on a rocky shore on the southern coast of Galicia, Praia da Mourisca (Alcabre, Spain) during the summer of 2011. Specimens were washed carefully with water and then oven-dried at 50 • C for 72 h to preserve them until use. Dried algae were milled to facilitate sample handling and provide higher extraction yields by increasing the contact surface. First, it was milled in a cutting mill up to a particle size of 1-2 cm length and then further milled to obtain a coarse powder.

Computational Section
Conformational searches for J-DP4 and CASE-3D analyses were performed by employing MAESTRO software, using an energy window of 5 kcal/mol. Energy cut-off (5 kcal/mol) for CASE-3D was based on calculations at B3LYP/6-31G(d,p), solvent model = IEFPCM (CH 2 Cl 2 ). Conformational searches for NMR anisotropy analyses were carried out on relevant rotatable bounds ρ1, ρ2, ρ3, and ρ4 (See Figures S21-S27) using the grid search module in PCModel V10. Both Pand Mhelicities were considered. Conformers used on NMR anisotropy analyses were optimized with DFT calculations at B3LYP/ 6-31+G(d) level, with vibrational frequency calculations confirming the presence of minima, using the Gaussian16 program. Chemical shielding tensors (CST) were computed at the GIAO/MPW1PW9/6-311+G(2d,p) (in gas phase). J-couplings were computed either at DFT level or by using Karplus-like equations [61,62]. All chiroptical properties were calculated as Boltzmann averages, weighted with conformer population factors obtained from NMR anisotropic Q factor minimization. Time-dependent DFT calculations were performed for each configuration using the combinations PBE0/Def2TZV/W06, solvent model: COSMO, 50 excited states and HSE06/6-311+G(2d,p)/DGA1; solvent model: IEFPCM, 38 excited states. In both, solvent CH 2 Cl 2 parameters were used. ECD spectra were generated using the program SpecDis by applying a Gaussian band shape with a 0.18 eV width and 25 blue shifts to facilitate comparison to the experimental data. OR values were computed, for both configurations, at CAM-B3LYP/6-311++G(2d,2p)/DGA1 (IEFPCM = CH 2 Cl 2 ) level of theory at 589 nm.

J-Coupling Calculation
(-)-(α)-santonin and strychnine were purchased at Sigma-Aldrich and both molecular models were optimized based on RCSA/RDC and NOE, respectively, as described before [22]. For strychnine, two conformers were taken into account as found by Butts et al. [24] for 2,3 J CH benchmarking at different levels of theory. J-coupling data were handled using the CST module nested in MSpin (See SI).

13 C-RCSA Measurements
A first attempt to establish the relative configuration of meroditerpene 1b by 13 C RCSA involved the use of a 4 mg sample in protonated PMMA swollen in CD 2 Cl 2 and using a conventional 5 mm outer diameter compression device. A number of resonances were obscured by the polymer background signal (see Figures S35-S43 and Table S6). Therefore, 2.2 mg of 1b was dissolved in CD 2 Cl 2 and swollen into a deuterated chemically crosslinked poly(methylmethacrylate) (PMMA-d 8 ) gel in an in-house made 3 mm compression device. RCSA were extracted as the difference in the referenced chemical shift between signals at maximum and minimum compression ( 13 C-RCSA i = ∆δ i,max − ∆δ i,min ) [63]. Due to the inherent properties of the compression device, the gel was surrounded by a layer of isotropic solution; carbon signals were phenomenologically observed from within (∆δ i,min ) and without (∆δ i,iso ) the gel (asterisk marked in Figure 9) [16]. After compressing the gel, the analyte concentration inside the gel increased, changing the isotropic contribution of the chemical shifts, and hindering the precise extraction of RCSAs without compensating for these isotropic shift contributions [16]. Therefore, an isotropic shift contribution of gel, expressed as free parameter c, was computed by applying an automatic linear correction [64] (Equation (1)). A quality factor computed without using this means is considered as uncorrected (Qu); it tends to have less discriminating power or even give ambiguous results. ∆δ i represents the referenced chemical shift with respect to a selected resonance at the corresponding conditions. Whenever possible, a nucleus with low associated anisotropy, a methylene group, for instance, was taken (Equation (2)). Data were fitted in units of ppm to obtain reasonable weight [63]. The quality of the fitting is scored in terms of quality factor Q. When carbon chemical shift variations due to analyte concentration changes are not considered, the uncorrected quality factor is named as QU. To yield minimum Q factor [65], free parameter c was minimized simultaneously along with the alignment tensor during the fitting procedure, and RCSA was fitted by singular value decomposition [63,66]. Conformers were fitted using a multiconformer single tensor approach and distances among the heavy atoms were minimized. The unscaled quality factor (Q) and the chemical shift anisotropic weighted quality factor (QCSA) were computed using Equations (3) and (4), respectively [16].
Data robustness was addressed by either bootstrapping analysis or Jackknife resampling as implemented in MSpin software and Excel [67]. Some significant variations in carbon chemical shifts in the oriented media were observed (see Figure 9). A certain amount of isotropic analyte was always detected because the gel in the compression device did not completely fill the entire sample space, even under maximum compression [68]. As before, the isotropic signals were easily distinguishable from their anisotropic counterparts, as their intensities diminished upon compression.

Conclusions
We demonstrated that the use of an integrated approach combining isotropic and anisotropic NMR means and incorporating chiroptical methods is a perfect toolbox to deduce the three-dimensional structure containing stereoclusters that cannot be connected through local correlations.
We also detected, through 3 JHH, 2 JCH, 3 JCH, coupling constants and RDC, flip-flop conformational changes around the C1′-O-C3-C2 dihedral. Using this approach, the structure The quality of the fitting is scored in terms of quality factor Q. When carbon chemical shift variations due to analyte concentration changes are not considered, the uncorrected quality factor is named as Q U . To yield minimum Q factor [65], free parameter c was minimized simultaneously along with the alignment tensor during the fitting procedure, and RCSA was fitted by singular value decomposition [63,66]. Conformers were fitted using a multiconformer single tensor approach and distances among the heavy atoms were minimized. The unscaled quality factor (Q) and the chemical shift anisotropic weighted quality factor (Q CSA ) were computed using Equations (3) and (4), respectively [16].
Data robustness was addressed by either bootstrapping analysis or Jackknife resampling as implemented in MSpin software and Excel [67]. Some significant variations in carbon chemical shifts in the oriented media were observed (see Figure 9). A certain amount of isotropic analyte was always detected because the gel in the compression device did not completely fill the entire sample space, even under maximum compression [68]. As before, the isotropic signals were easily distinguishable from their anisotropic counterparts, as their intensities diminished upon compression.

Conclusions
We demonstrated that the use of an integrated approach combining isotropic and anisotropic NMR means and incorporating chiroptical methods is a perfect toolbox to deduce the three-dimensional structure containing stereoclusters that cannot be connected through local correlations.
We also detected, through 3 J HH , 2 J CH , 3 J CH , coupling constants and RDC, flip-flop conformational changes around the C1 -O-C3-C2 dihedral. Using this approach, the structure of the tetraprenyltoluquinol chromane meroterpenoids 1b isolated from Sargassum muticum was corrected to the trans fusion dimethylbicyclo [4.3.0]nonane system; and the distant stereocenter at C3 was related to C7 and C11 with the use of DP4, iJ-DP4,