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1.1 Porphyrins - Friedrich-Alexander-Universität Erlangen-Nürnberg

1.1 Porphyrins - Friedrich-Alexander-Universität Erlangen-Nürnberg

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3 Discussion and Results<br />

3.2.3.2 NMR Investigations at Room Temperature<br />

The 1 H NMR spectrum of free base system 53 shows up quite complex in comparison to the<br />

precursor systems as those have appeared pseudo-symmetrical leading to a reduced<br />

number of detected resonances. In this case, the C1 symmetry gives rise to a large number of<br />

partly overlaid resonance signals as it is shown in Figure 17.<br />

46<br />

2<br />

18<br />

7<br />

8<br />

17<br />

O<br />

12+13<br />

9.0 8.8 8.6 8.4 8.2 8.0 7.8 7.6 7.4<br />

CDCl 3<br />

N<br />

NH HN<br />

102/6<br />

15 2/6<br />

N<br />

53<br />

10 2/6 ,15 2/6<br />

m-ArH<br />

20 2/6<br />

3 2 in<br />

5 3<br />

3 2 out<br />

5 5<br />

1.60 1.55 1.50<br />

9 8 7 6 5 4 3 2 1 0 -1 δ [ppm] -3<br />

Figure 17. 1 H NMR spectrum of 53, 400 MHz, CDCl3, rt. All signals are numbered according to<br />

IUPAC recommendations.<br />

The seven β-pyrrolic protons give rise to a set of one singlet and six doublets ( 3 J = 4.9 Hz)<br />

most downfield between 9.0 and 8.5 ppm as it is to be expected for a C1 symmetric system<br />

with one β-substituent. These signals can be nearly all assigned via COSY (Correlated<br />

Spectroscopy) and NOE (Nuclear Overhauser Effect) experiments 46 as they appear well<br />

resolved. In contrast, the ones for the arylic protons in between 8.5 and 7.3 ppm show a<br />

significant line-broadening and thus are overlaid making a definite assignment impossible.<br />

Only the protons on the tethered phenyl ring (5 3 and 5 5 ) are an exception as they give rise to<br />

two doublets at 7.68 and 7.35 ppm ( 4 J = 1.7 Hz). This behavior corroborates the assumption<br />

that the porphyrin system is bent as then the rotational barriers for the meso-aryl<br />

5 2<br />

15 4<br />

10 4<br />

20 4<br />

NH<br />

5 4

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