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Mercury 400 mhz nmr instrument

Manufactured by Agilent Technologies

The Mercury 400 MHz NMR instrument is a nuclear magnetic resonance (NMR) spectrometer designed for analytical applications. It operates at a frequency of 400 MHz and is capable of providing high-resolution NMR data for the identification and structural analysis of chemical compounds.

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2 protocols using mercury 400 mhz nmr instrument

1

Synthesis and Characterization of Metal Complexes

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All materials listed below were of research grade or a spectro grade in the highest purity available and were generally used without purification except 2-pyridinecarboxaldehyde, which was distilled, and acrylonitrile, which was passed through a plug of basic alumina. 1H and proton-decoupled 13C NMR were obtained using a Varian Mercury 400 MHz NMR instrument, and chemical shifts are reported in ppm relative to the deuterated solvent used. Elemental analysis was performed by Atlantic Microlabs (Atlanta, GA, USA). Mass spectral data were obtained on a Bruker AmaZon SL ion trap LC/MS (Northwestern University). X-ray crystallography was performed on a Bruker APEX-II CCD Diffractometer (UC San Diego). Potentiometric titrations were performed using a 785 DMP Titrino equipped with an Accumet double injection pH electrode and thermally regulated titration vessel. Formation-constant data were evaluated using the Hyperquad2008 program suite [28 ]. The fluorescence spectra were recorded using a Cary Eclipse fluorescence spectrophotometer with 3 cm3 quartz cuvette (1 cm pathlength).
Caution! Perchlorates of metal complex cations have been known to explode. No explosions occurred during this work.
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2

2D NMR Spectroscopy of Acetylated Wood

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Two-dimensional Heteronuclear Single Quantum Coherence spectra were run in DMSO-d 6 on acetylated wood samples. The inverse detected 1 H- 13 C correlation spectra were measured on a Varian Mercury 400 MHz NMR instrument at 308 K. The spectral width was set at 5 kHz in F2 and 25 kHz in F1. Altogether 128 transients in 256 time increments were collected. The polarization transfer delay was set at the assumed coupling of 140 Hz and a relaxation delay of 2 s was used. The spectra were processed using Π/2 shifted squared sinebell functions in both dimensions before Fourier transformation.
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