The largest database of trusted experimental protocols

Jnm eca 600ii nmr spectrometer

Manufactured by JEOL
Sourced in Japan

The JNM-ECA 600II NMR spectrometer is a high-performance nuclear magnetic resonance (NMR) instrument designed for analytical and research applications. It features a 600 MHz superconducting magnet and advanced electronics for acquiring and processing NMR data. The spectrometer is capable of performing various NMR experiments to analyze the molecular structure and properties of chemical samples.

Automatically generated - may contain errors

3 protocols using jnm eca 600ii nmr spectrometer

1

Synthetic Characterization of Novel Compounds

Check if the same lab product or an alternative is used in the 5 most similar protocols
All reagents were purchased from Merck (Sigma-Aldrich, St. Louis, MO, USA) or Alfa (Alfa-Aesar, Ward Hill, MA, USA). Reactions were performed using a CEM Discover SP microwave reactor (CEM, Matthews, NC, USA). Melting points were determined on an apparatus Stuart SMP10 (Stone, UK) and are uncorrected. Infrared (IR) spectra were recorded on an ATR Zn/Se for a Nicolet™ iS 5 FT-IR spectrometer (Thermo Fisher Scientific, West Palm Beach, FL, USA). The spectra were obtained by the accumulation of 64 scans with 4 cm−1 resolution in the region of 4000–400 cm−1. All 1H- and 13C-NMR spectra were recorded on a JEOL JNM-ECA 600II NMR spectrometer (600 MHz for 1H and 150 MHz for 13C, Jeol, Tokyo, Japan) in dimethyl sulfoxide-d6 (DMSO-d6); 1H and 13C chemical shifts (δ) are reported in ppm. High-resolution mass spectra were measured using a high-performance liquid chromatograph Dionex UltiMate® 3000 (Thermo Scientific, West Palm Beach, FL, USA) coupled with an LTQ Orbitrap XLTM Hybrid Ion Trap-Orbitrap Fourier Transform Mass Spectrometer (Thermo Scientific) equipped with a HESI II (heated electrospray ionization) source in the negative mode.
+ Open protocol
+ Expand
2

Synthesis and Characterization of Novel Compounds

Check if the same lab product or an alternative is used in the 5 most similar protocols
All reagents were purchased from Merck (Sigma-Aldrich, St. Louis, MO, USA) and Alfa (Alfa-Aesar, Ward Hill, MA, USA). Reactions were performed using a CEM Discover SP microwave reactor (CEM, Matthews, NC, USA). Melting points of 16 and 18 were determined on an apparatus STA 449 F1 Jupiter (NETZSCH, Selb, Germany). Infrared (IR) spectra were recorded on an UATR Zn/Se for a Spectrum Two™ Fourier-transform IR spectrometer (PerkinElmer, Waltham, MA, USA). The spectra were obtained by the accumulation of 32 scans with 4 cm−1 resolution in the region of 4000–400 cm−1. All 1H- and 13C-NMR spectra were recorded on a JEOL JNM-ECA 600II NMR spectrometer (600 MHz for 1H and 150 MHz for 13C, Jeol, Tokyo, Japan) in dimethyl sulfoxide-d6 (DMSO-d6). 1H and 13C chemical shifts (δ) are reported in ppm. High-resolution mass spectra were measured using a high-performance liquid chromatograph Dionex UltiMate® 3000 (Thermo Scientific, West Palm Beach, FL, USA) coupled with an LTQ Orbitrap XLTM Hybrid Ion Trap-Orbitrap Fourier Transform Mass Spectrometer (Thermo Scientific) equipped with a HESI II (heated electrospray ionization) source in the positive mode.
+ Open protocol
+ Expand
3

Optimizing 180° Pulse Widths for fp-RFDR NMR

Check if the same lab product or an alternative is used in the 5 most similar protocols
All NMR experiments were performed on a 600 MHz JNM-ECA600II NMR spectrometer (JEOL RESONANCE Inc., Tokyo, Japan) equipped using a 0.75 mm ultrafast MAS probe. Powder samples of U-13C,15N-L-alanine and glycine were purchased from Isotec and were used without any modification. N-acetyl-15N-L-valyl-15N-L-leucine (NAVL) was prepared as explained elsewhere[16 , 17 ]. Samples were packed in a 0.75 mm zirconia rotor and all experiments were performed at room temperature (ca. 24 °C). Experiments were performed to optimize the width of the 180° pulse so that the loss of net magnetization after fp-RFDR can be minimized. The 180° pulse width that gave the maximal signal intensity after fp-RFDR irradiation was used in the subsequent experiments reported in this study. The experimentally optimized 180° pulse width was 5 μs for 110 kHz RF-field strength, 2.7 μs for 231 kHz, and 1.3 μs for 467 kHz. It should be noted that these 180° pulse widths are longer than that calculated from the respective RF field strength, because of the transients at the rising and falling edges of the pulses. All other experimental conditions used in this study are given in figure captions.
+ Open protocol
+ Expand

About PubCompare

Our mission is to provide scientists with the largest repository of trustworthy protocols and intelligent analytical tools, thereby offering them extensive information to design robust protocols aimed at minimizing the risk of failures.

We believe that the most crucial aspect is to grant scientists access to a wide range of reliable sources and new useful tools that surpass human capabilities.

However, we trust in allowing scientists to determine how to construct their own protocols based on this information, as they are the experts in their field.

Ready to get started?

Sign up for free.
Registration takes 20 seconds.
Available from any computer
No download required

Sign up now

Revolutionizing how scientists
search and build protocols!