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Long-range correlations ( n j C,H n > 3 ) in the HMBC spectra of 3-(4-oxo-4H-chromen-3-YL)-acrylic acid ethyl esters

Abstracts

A systematic study about the long-range correlations observed in the HMBC spectra of a series of cis and trans 3-(4-oxo-4H-chromen-3-yl)-acrylic acid ethyl esters, and 5-hydroxy derivatives, was carried out. The results were compared with those observed in IMPEACH-MBC and CIGARHMBC spectra. An uncommon 5J C,H between the methyl protons and the Ca to the carbonyl group was observed in these systems as well as in ethyl chrotonate. The complete assignments of the ¹H and 13C NMR spectra are provided.

¹H and 13C NMR; HMBC; CIGAR-HMBC; IMPEACH-MBC; 5J C,H, acrylic acid ethyl esters; chromone


Um estudo sistemático das correlações de longo alcance em espectros de HMBC foi feito para uma série de ésteres etílicos do ácido cis- e trans-3-(4-oxo-4H-chromen-3-il) acrílico e os derivados 5-hydroxilados. Os resultados foram comparados com os já observados para espectros IMPEACH-MBC e CIGAR-HMBC. Um acoplamento incomum do tipo 5J C,H entre prótons metilicos e o Ca do grupo carbonilico foi observado nesses sistemas, assim como no crotonato etílico. A atribuição completa dos espectros ¹H e 13C RMN foi realizada.


SHORT REPORT

Long-range correlations ( nj C,H n > 3 ) in the HMBC spectra of 3-(4-oxo-4H-chromen-3-YL)-acrylic acid ethyl esters

Ramiro Araya-MaturanaI,* * e-mail: raraya@ciq.uchile.cl ; José A. Gavín-SazatornilII; Jorge Heredia-MoyaI; Hernán Pessoa-MahanaI; Boris Weiss-LópezIII

IDepartamento de Química Orgánica y Fisicoquímica, Facultad de Ciencias Químicas y Farmacéuticas, Universidad de Chile, Casilla 233, Santiago 1, Chile

IIInstituto Universitario de Bio-Orgánica, Universidad de La Laguna, Spain

IIIDepartamento de Química, Facultad de Ciencias Universidad de Chile

ABSTRACT

A systematic study about the long-range correlations observed in the HMBC spectra of a series of cis and trans 3-(4-oxo-4H-chromen-3-yl)-acrylic acid ethyl esters, and 5-hydroxy derivatives, was carried out. The results were compared with those observed in IMPEACH-MBC and CIGARHMBC spectra. An uncommon 5JC,H between the methyl protons and the Ca to the carbonyl group was observed in these systems as well as in ethyl chrotonate. The complete assignments of the 1H and 13C NMR spectra are provided.

Keywords:1H and 13C NMR , HMBC, CIGAR-HMBC, IMPEACH-MBC, 5J C,H, acrylic acid ethyl esters, chromone

RESUMO

Um estudo sistemático das correlações de longo alcance em espectros de HMBC foi feito para uma série de ésteres etílicos do ácido cis- e trans-3-(4-oxo-4H-chromen-3-il) acrílico e os derivados 5-hydroxilados. Os resultados foram comparados com os já observados para espectros IMPEACH-MBC e CIGAR-HMBC. Um acoplamento incomum do tipo 5JC,H entre prótons metilicos e o Ca do grupo carbonilico foi observado nesses sistemas, assim como no crotonato etílico. A atribuição completa dos espectros 1H e 13C RMN foi realizada.

Introduction

The Heteronuclear Multiple Bond Correlation (HMBC)1,2 NMR experiment has probably been the most widely used 2D heteronuclear NMR method in the field of structural elucidation of complex organic molecular structures. Nowadays, it has become one of the most popular techniques for multiple-bond (or long-range) heteronuclear chemical shift correlation. It provides a wealth of structural information, and eventually the full assignment, through long-range correlation signals for 13C,1H spin pairs. It can span quaternary carbons or heteronuclei, providing a way to link different molecular fragments into a complete structure.3-5 The use of HMBC together with Heteronuclear Multiple Quantum Coherence, HMQC,6 or Heteronuclear Single Quantum Correlation, HSQC,7 has proved to be extremely useful in the total structure elucidation and NMR spectral assignments of numerous complex organic molecules.

The HMBC experiment was highly improved since the application of pulsed field gradients (PFG) in the early 1990's. High quality spectra, without artefacts, are obtained in standard conditions, allowing the analysis of very small but informative cross peaks. Today the advantages offered by the incorporation of pulsed field gradients into high-resolution NMR pulse sequences, combined with advanced software tools available to acquire and process multidimensional NMR experiments, has allowed to record and process the HMBC sequence with PFG just by clicking a button or executing a predefined macro, making it available to the non-experienced NMR user.8

Despite the widely recognized structural elucidation capabilities of HMBC, it is usually described as a technique that allows the assignment of structural fragments through the correlation between protons and carbons separated by two or three bonds.3-5 However, the early observation of a crucial four bond C,H correlation in the HMBC spectrum of antibiotic distamicyn A9, along with another examples of this kind of correlations ( nJ C,H n > 3 ) subsequently reported, validate HMBC as a technique that allow to obtain more valuable structural information.10 Moreover, a frequent source of contradictions in computer-assisted structure elucidation programs, has been the observation of correlations in COSY and in long-range heteronuclear shift-correlation experiments, which corresponds to four or more bonds.11

With regard to the observation of nJC,H n>3, two extreme opinions have been argued: the first position emphasizes the disadvantages associated with the increase in the number of H,C correlation peaks for which the number of bonds is uncertain, even worst if the cross-peaks intensities are low, as usually occurs. Because of this, the valuable information that might be obtained through heteronuclear long-range correlations, across four or more bonds, has been generally discarded. It is important to mention, even though it is obvious, that if the number of intervening bonds assigned to a cross-peak is different from the actual value, wrong connectivities will be made. Moreover, these correlations can be crucial in structural elucidation.9,12,13 The other position focuses on the large amount of structural information that can be obtained with a larger number of long-range correlation peaks, which can be translated to bonding network, despite the lack of discrimination. The pulse sequences: D-HMBC,14 3D-HMBC,15 CT-HMBC,16 ACCORD-HMBC,17 IMPEACH-MBC18 and CIGAR-HMBC,19 which sample a great number of long-range coupling constants, were developed based on the last point of view.

The tuning of the HMBC experiment is achieved by setting the D2 preparation period, the so called long-range delay, to a sufficiently long time to allow the small long-range proton-carbon couplings to evolve and produce the antiphase displacement of vectors required for the subsequent generation of heteronuclear multiple quantum coherence, and is calculated from D2 = 1 / (2 nJC,H).5 Since molecules have a range of nJCH values, typically from 2 to 15 Hz,4,5D2 should be at least 100ms. In practice a delay shorter than the theoretical value is employed in order to avoid the 1H magnetization to decay during this delay, particularly for large molecules. For routine applications D2 is usually set from 60 to 80 ms.3-5 This delay significantly attenuate cross-peaks intensities arising from values of nJCH which are far away from the average value.

Since small molecules tend to have slower relaxation rates, longer delays can be successfully used in the search for connectivities through smaller couplings. A maximum of 200 ms has been recommended to detect cross-peaks arising from four bonds correlations, which are described as most likely to occur when the coupling pathway contains unsaturations or when it has the planar zig-zag (W coupling) configuration,4 as commonly observed in long-range proton-proton coupling. However these generalizations might induce to confusion. For example values of D2 between 50 to 400 ms to record HMBC spectra of phenolic compounds, has been reported,20 moreover the observation of five bonds correlations by using standard value of D2 (65 or 80 ms) in HMBC spectra of quinones has also been reported.12,13,21 In a similar way, several examples of 4JCH has been observed in a great variety of molecules and coupling pathways.10

Generally the choice of D2 is made on arbitrary basis rather than from knowledge of the actual value of the couplings. On this basis, a first approximation to observe a greater number of long-range correlations is to perform several HMBC experiments with different long-range delays and using a deeper threshold in the contour plot. Hereby new correlations could be observed and some of the already observed ones might disappear. Alternatively, some of the new pulse sequences focused on long-range delay optimisation, of which CIGAR-HMBC has been described as the best,5 can be used.

In order to explore this subject in a systematic way and hence to obtain further information that can be used for a more effective choice of D2 values, we selected compounds 1-4 (Figure 1) to study the long range correlations that can be observed at different D2 values. The selection of these structures was made considering that the oxygen atom of the heterocyclic moiety and the quaternary carbons impose an assignment relying on long-range correlations. Additionally, it is interesting because the chromone system has received attention due to the possibility of aromatic character of the heterocyclic moiety.22 On the other hand, from a synthetic point of view, the p system of the acrylic ester conjugated with heterocyclic double bond conform an attractive push-pull diene with E or Z configuration that has been used in cycloadditions.23 In this paper we present a study to obtain a criterion that allows a more appropriate choice of D2 in this type of molecular systems. For this purpose, several HMBC experiments increasing D2 long-range delays were carried out to observe the necessary nJCH correlations for the assignments. In this manner we have assigned the 13C NMR spectra of these compounds by the concerted use of 1H-detected one bond heteronuclear multiple quantum coherence HMQC,6 or HSQC,7 and long-range heteronuclear multiple bond connectivity, HMBC.1,2


Experimental

General procedure for preparation of chromones 1-4

The chromones 1-4 were prepared starting from the corresponding 3-formylchromone,24 through a Wittig reaction according to the following experimental conditions: one equivalent of carboethoxymethylenetriphenylphosphorane was added to a solution of 0.5 g of the corresponding 3-formylchromone in 10 mL of toluene and the mixture heated to reflux for 2h. The triphenylphosphine oxide formed in the reaction was removed through vacuum filtration and then rotatory evaporation of the solvent from the filtrate affords a mixture of cis and trans acrylic acid ethyl esters derivatives. Purification by column chromatography through silica gel using ethyl acetate/hexane 1: 2 as eluent and further crystallization from a mixture of ethyl acetate/hexane yields the corresponding pure compounds 1-4 as white needles. trans-5-hydroxy-3-(4-oxo-4H-chromen-3-yl) -acrylic acid ethyl ester 1 was obtained with 55% yield (m.p. 158.5-159.5 ºC), Anal. Calc. For C14H12O5: C, 64.61; H, 4.65 Found: C, 64.40; H, 4.42. IR (KBr) nmax/cm-1: 3442, 1706, 1652, 1296, 1267, 1170. cis-5-hydroxy-3-(4-oxo-4H-chromen-3-yl)-acrylic acid ethyl ester 3 was obtained with 40% yield (m.p. 69.5-70 ºC). Anal. Calc. For C14H12O5: C, 64.61; H, 4.65 Found: C, 64.10; H, 4.47. IR (KBr) nmax/cm-1: 3440, 1703, 1655, 1265, 1196, 1158. trans-3-(4-oxo-4H-chromen-3-yl)-acrylic acid ethyl ester 2 was obtained with a 50% yield (m.p. 111.5-112.5 ºC lit. 96-98 ºC23). cis-3-(4-oxo-4H-chromen-3-yl)-acrylic acid ethyl ester 4 was obtained with a 49 % yield (m.p. 66,5 - 67.5 ºC).

NMR Spectra

1H and 13C NMR spectra were recorded using a Bruker AVANCE 300 and a Bruker AVANCE 400 spectrometers operating at 300.13 and 400 MHz (1H) or 75.47 and 100 MHz (13C) respectively. All measurements were carried out at a probe temperature of 300 K, using solutions of 1-4 (20-30 mg mL-1 in CDCl3 containing tetramethylsilane as internal standard). All two dimensional spectra were acquired, in both spectrometers, with a Bruker inverse 5 mm Z gradient probe. HMQC spectra were recorded using the standard Bruker software. These spectra were collected with 512 x 512 data points, with eight scans acquired for every 256 increments in t1, and the D1 delay was set to 3.45 ms. Spectral widths of 3000 Hz and 18000 Hz were used in the F2 (1H) and F1 (13C) domains, respectively. HMBC, CIGAR-HMBC and IMPEACH-MBC spectra were obtained using the standard pulse sequence from the Bruker software. The spectral widths were 3900 Hz (F2) and 18000Hz (F1). The D2 delay in the HMBC pulse sequence was varied from 65 to 390 ms. Data was processed using an exponential decay window in F2, with 1b = 5Hz, and a qsine window function in F1.

Results and Discussion

The 1H-NMR spectra of compounds 1 and 3 display two doublets corresponding to an AB system with J 15.9 Hz, characteristics of trans double bond (1), and J 12.8 Hz for the cis compound (3). The H-10 proton doublet, d 7.21 for compound 1, is shifted to lower field respect to compound 3 (d 6.12), probably due to the anisotropic effect of C-4 carbonyl group in the s-trans conformation of the diene moiety. Both compounds exhibit three signals for the aromatic protons: two doublets and an apparent triplet, besides the two characteristic triplet and quartet of the ethyl chain. The singlet corresponding to the heterocyclic proton appears at very low field, as reported before for this class of heterocyclic systems,23,25 due to oxygen substitution and the conjugation effect of the carbonyl group (C-4), although the postulated aromatic character of heterocyclic ring of the chromone22 may also contribute. The absolutes magnetic shielding at the rings centers and at the carbon nuclei has been previously reported.22 The H-2 resonance in compound 3 (d 9.10) is shifted to low field with respect to compound 1 (d 8.10), probably due to the anisotropic effect of the carbonyl ester group in the s-cis conformation.

The protonated carbons can be easily assigned through an HMQC or HSQC experiments, except in the case of C-6 and C-8 because H-6 and H-8 exhibit similar chemical shifts and multiplicities. Therefore, these carbons together with the quaternary centers must be assigned through long-range correlations.

The HMBC spectra of both compounds obtained with a 300 MHz spectrometer and using a standard long-range delay of 65 ms, displayed a three bond correlation between the hydroxyl proton and C-6, and did not correlate with C-8, allowing the discrimination between them. A three bond correlation between the same proton and C-4a is also observed allowing discrimination between C-4a and C-3. The 3JC,H between H-10 with C-3 and the 2JC,H between this carbon with H-2 assures these assignments.

The HMBC spectrum of compound cis (3), with D2 = 65 ms, shows seven 4JC,H correlations, of which only four of them take place through a W coupling path: H-10 with C2, H-6 with C-4, H-8 with C-4 and OH with C-7. The other three correlations occur between a proton and the carbon located at the para position: H-6 with C-8a, H-7 with C-4a and H-8 with C-5. With the purpose of confirming that these cross-peaks are real and not artifacts, we performed duplicate experiments in a 400 MHz spectrometer. The HMBC spectrum for the cis compound 3 displays the same cross-peaks in both spectrometers. The 300 MHz HMBC spectrum with D2 = 65 ms of compound trans 1 shows only four 4JC,H correlations: the hydroxyl proton with C-7, H-7 with C-4a, OH with C-4 and H-8 with C-4. However in the spectrum recorded at 400 MHz the correlation between OH and C-4 is not observed. However other four correlations were observed: H-6 with C-8a, H-8 with C-5, H-10 with C-2 and H-9 with C-4a. At present we have no explanation for these differences.

The 300 MHz spectra of both compounds, with a little increment in D2 (130 ms), lead to observation of several additional 4JC,H correlations, (12 cross-peaks). Interestingly, a long-range correlation across five bonds between the methyl protons with C-10 is also observed. This is a very long-range correlation through a coupling path with a high degree of conformational freedom. As far as we know10 this kind of long-range correlation has not been reported before.

In the 400 MHz HMBC spectrum of compound 1, with D2 = 130 ms, only the same correlations obtained using D2 = 65 ms were observed. However the HMBC spectrum of compound 3 showed a 4JC,H correlation between the OH and C-4, but the cross-peaks due to H-7 with C-4a and H-8 with C-5 disappeared. In the spectra of both compounds, 1 and 3, the 5JC,H correlations were not observed, but in the 400 MHz spectra of both compounds with D2 = 195 ms the 5JC,H correlations between CH3 and C-10 can be observed, beside eleven 4JC,H other correlations. In the 300 MHz HMBC spectrum (D2 = 195 ms) of compound 1 thirteen 4JC,H correlations are shown, in addition to a 5JC,H correlation. For compound cis twelve 4JC,H correlations are observed, beside two 5JC,H: CH3 with C-10 and H-10 with C-4a.

The IMPEACH-MBC experiment (D2 = 50-200 ms, J 2.5-10 Hz) of compound trans shows several although not all correlations observed in the series of HMBC experiments. This experiment shows the 4JC,H correlations between the aromatic protons with carbon atoms in the para positions: H-8 with C-4, H-10 with C-2 and H-9 with C-4, but is unable to show correlations of the ethyl chain with Ca. A CIGAR-HMBC (D2 = 50-200 ms, J 2.5-10 Hz) of the same compound shows two additional 5JC,H: CH3 with C-10 and OH with C-8 , but several artifacts are obtained, mainly for H-2.

The 1H spectra of compounds 2 and 4 display the known AB system for olefinic protons with coupling constants of 12.8 and 15.9 Hz for compounds cis (4) and trans (2) respectively. For compound 2, H-5 appears as broad doublet with coupling constant of 8.3 Hz, at d 8.28, H-8 appears as broad doublet with J 8.3 Hz at d 7.45. For compound 4, H-5 appears at d 8.26 as doublet of doublet, with coupling constants of 9.4 and 1.6 Hz, and H-8 appears at d 7.49 as a broad doublet with J 8.5 Hz.

The conjugation of the carbonyl group shifts the aromatic protons H-5 and H-7 to low field and the conjugation of the heterocyclic oxygen atom shifts the H-6 and H-8 to high field. In this way was possible to discriminate between H-5 and H-8 or H-6 and H-7, together with the reported chemical shifts of chromone derivatives.

H-2 appears at 8.12 ppm and 9.13 ppm for molecules 2 and 4 respectively, in a similar way as compounds 1 and 3. The standard HMBC spectrum (D2 = 65 ms) of compound 2 displays only one 4JC,H correlation (H-8 with C-4), however the HMBC spectrum of compound 4 shows four 4JC,H correlations: H-8 with C-4, H-6 with C-8a, H-2 with C-10, and H-10 with C-2. Increments of D2 allows to observe a bigger number of these 4JC,H as discussed previously for compounds 1 and 3. Using D2 = 130 ms or larger, the 5JC,H correlation between the methyl protons with C-10 is observed for both compounds, in a similar way as compounds 1 and 3.

The HMBC spectrum of ethyl chrotonate shows the correlation between the methyl protons (d 1.89) and Ca to carbonyl with D2 = 65 ms, indicating that this very long-range coupling is a general characteristic for the unsaturated ester moiety.

Conclusions

From this study, an additional HMBC spectrum using a long D2 delay (200 – 300 ms) is recommended in order to obtain valuable structural information through long range correlations (nJC,H n > 3).

An uncommon 5JC,H between the methyl protons and Ca to carbonyl, as well as several 4JC,H through no W coupling paths, were observed in these systems.

Acknowledgments

The authors are pleased to acknowledge financial assistance from FONDECYT grant 1030916 and CYTED (RIDEST). J.H.-M. is gratefull to DAAD for his fellowship.

Received: December 8, 2003

Published on the web: March 15, 2005

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  • Publication Dates

    • Publication in this collection
      09 Aug 2005
    • Date of issue
      June 2005

    History

    • Accepted
      15 Mar 2005
    • Received
      08 Dec 2003
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