NMR data were obtained as previously reported following standard procedures [27 ]. Spectra were recorded at 290 and 298 K on a Bruker Avance III 600 MHz spectrometer (Bruker, Billerica, MA, USA) equipped with a cryoprobe. Crude venom samples were prepared in 90% H2O/10% D2O (v/v) (99.9%, Cambridge Isotope Labs, Tewksbury, Massachusetts, United States of America), vortexed, and centrifuged prior to transfer to an NMR tube (Wilmad, 5 mm). One‐dimensional (1D) and two‐dimensional (2D) spectra were collected using standard Bruker pulse programs, and referenced to external 4,4‐dimethyl‐4‐silapentane‐1‐sulfonic acid (DSS; Cambridge Isotope Laboratories). The 1D data included a cpmgpr1d experiment to suppress the larger peptide and protein signals. The 2D spectra included TOCSY, NOESY, COSY, HMBC, 13C‐HSQC, and 15N‐HSQC experiments with TOCSY and NOESY mixing times of 80 and 500 ms, respectively. Spectra of crude SvV were also collected in 100% MeOD (Cambridge Isotope Labs, methanol‐d4) to observe peaks otherwise obscured by the water suppression. Spectra were analyzed with
Nmr tube
NMR tubes are specialized containers used in nuclear magnetic resonance (NMR) spectroscopy. They are designed to hold samples for analysis in NMR instruments.
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NMR Analysis of Fish Venom Composition
NMR data were obtained as previously reported following standard procedures [27 ]. Spectra were recorded at 290 and 298 K on a Bruker Avance III 600 MHz spectrometer (Bruker, Billerica, MA, USA) equipped with a cryoprobe. Crude venom samples were prepared in 90% H2O/10% D2O (v/v) (99.9%, Cambridge Isotope Labs, Tewksbury, Massachusetts, United States of America), vortexed, and centrifuged prior to transfer to an NMR tube (Wilmad, 5 mm). One‐dimensional (1D) and two‐dimensional (2D) spectra were collected using standard Bruker pulse programs, and referenced to external 4,4‐dimethyl‐4‐silapentane‐1‐sulfonic acid (DSS; Cambridge Isotope Laboratories). The 1D data included a cpmgpr1d experiment to suppress the larger peptide and protein signals. The 2D spectra included TOCSY, NOESY, COSY, HMBC, 13C‐HSQC, and 15N‐HSQC experiments with TOCSY and NOESY mixing times of 80 and 500 ms, respectively. Spectra of crude SvV were also collected in 100% MeOD (Cambridge Isotope Labs, methanol‐d4) to observe peaks otherwise obscured by the water suppression. Spectra were analyzed with
Rhodium-Catalyzed Hydrogenation of Unsaturated Substrates
NMR Serum Sample Preparation
Vanillin Isotopic Characterization
purchased from Cambridge Isotope Laboratories (Andover, MA, USA).
Chromium acetylacetonate Cr(Acac)3, 99% and HPLC/Spectro
grade acetone were obtained from Sigma-Aldrich (Oakville, ON, Canada).
IRMS reference materials IAEA-CH-6, USGS65, IAEA-600, NBS22, USGS61,
IAEA-603, IAEA-610, IAEA-611, and IAEA-612 were obtained from the
International Atomic Energy Agency. NMR tubes (5 mm diameter) were
obtained from Wilmad LabGlass (Buena, New Jersey, USA). Five vanillin
materials, VANA-1, VANB-1 (NMR analysis in previous study4 (link)), VAN-1, VAN-4, and VAN-8 (NMR analysis in this
study; GC-IRMS of all five vanillin samples in this study), are all
synthetic materials of high chemical purity (≥99%) obtained
from Fisher Scientific (Waltham, MA, USA), Sigma-Aldrich (St. Louis,
MO, USA), Alfa Aesar (product of USA), and Sigma-Aldrich (product
of China), respectively.
Diffusion Measurements of Hydrogel Solutions
hydrogel solutions are pipetted into NMR tubes (Wilmad-LabGlass, Vineland,
New Jersey) and allowed to cure in a 37 °C oven for 20 min. The
samples are kept at 25 °C until measurements are made. Diffusion
measurements were made at 25, 30, and 37 °C. The samples are
allowed to equilibrate in the instrument (600 MHz Varian NMR spectrometer,
Agilent Technologies, Santa Clara, California) at 25 °C for 10
min and at 30 and 37 °C for 1 h before measurements at each respective
temperature are started. For each temperature, the π/2 pulse
time is determined before making measurements. A stimulated spin-echo
pulse sequence, based on the sequence described by Wu et al., was
used for diffusion coefficient measurements.20 (link),21 (link) The expected signal for this measurement is a function of the Stejskal–Tanner
variable, X, defined in terms of the pulse–sequence
parameters as Experiments used gradient-pulse amplitudes, g, that varied from 0 to 61.5 G/cm with a fixed gradient-pulse
duration (δ = 2 ms) and gradient-pulse separation time (Δ
= 100 ms). The variable-time delay, τ, was computed to ensure
proper timings for a measurement and was typically 1.5 ms. A diffusion
coefficient, D, can then be calculated using where S(X) is the signal for a given value of X and S(0) is the signal without a gradient pulse. The signal
is taken from the water peak in the 1H NMR spectrum, around
4.0 ppm.
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