<rss version="2.0" xmlns:atom="http://www.w3.org/2005/Atom" xmlns:media="http://search.yahoo.com/mrss/"><channel><title>JEOL Resources</title><link>https://www.jeolusa.com/RESOURCES/Analytical-Instruments/Documents-Downloads</link><item><title>Introduction of a method to analyze 3D structures using homonuclear couplings_NM210004E</title><link>https://www.jeolusa.com/RESOURCES/Analytical-Instruments/Documents-Downloads/introduction-of-a-method-to-analyze-3d-structures-using-homonuclear-couplingsnm210004e</link><category>NMR Applications</category><pubDate>Mon, 29 Nov 2021 10:14:39 GMT</pubDate><summary>Structural analysis by NMR can provide not only a planar molecular structure but also three-dimensional structural information. In this Note, we describe a method for obtaining information on dihedral angles by using 1H-1H coupling constants (JHH values). For example, hydrogen atoms attached to a cyclohexane ring are either located in axial or equatorial positions in respect to the cyclohexane ring (Fig. 1). The dihedral angles between vicinal protons are known to be ∠Hax-C-C-Hax ≈ 180°, ∠Hax-C-Heq ≈ 60°, and ∠Heq-C-C-Heq ≈ 60°. If we look at the Karplus curve shown in Fig. 2, we can see that 3JHH of around 4 Hz can be expected in the case of the dihedral angle of 60°, while 3JHH of around 13 Hz corresponds to the dihedral angle of 180°. In reality, 3JHH values depend on substituents attached to the cyclohexane ring in substituted cyclohexanes, so the analysis is not straightforward, but the basic trend of having a larger J-value for a 180° dihedral angle compared to a 60° dihedral angle remains unchanged. Therefore, from the value of 3JHH of the methylene protons, it is possible to differentiate between the dihedral angle of 60° or 180°.</summary><description>&lt;p&gt;Structural analysis by NMR can provide not only a planar molecular structure but also three-dimensional structural information. In this Note, we describe a method for obtaining information on dihedral angles by using &lt;sup&gt;1&lt;/sup&gt;H-&lt;sup&gt;1&lt;/sup&gt;H coupling constants (&lt;em&gt;J&lt;/em&gt;&lt;sub&gt;HH&lt;/sub&gt; values). For example, hydrogen atoms attached to a cyclohexane ring are either located in axial or equatorial positions in respect to the cyclohexane ring (Fig. 1). The dihedral angles between vicinal protons are known to be ∠H&lt;sub&gt;ax&lt;/sub&gt;-C-C-H&lt;sub&gt;ax&lt;/sub&gt; ≈ 180°, ∠H&lt;sub&gt;ax&lt;/sub&gt;-C-H&lt;sub&gt;eq&lt;/sub&gt; ≈ 60°, and ∠H&lt;sub&gt;eq&lt;/sub&gt;-C-C-H&lt;sub&gt;eq&lt;/sub&gt; ≈ 60°. If we look at the Karplus curve shown in Fig. 2, we can see that &lt;sup&gt;3&lt;/sup&gt;&lt;em&gt;J&lt;/em&gt;&lt;sub&gt;HH&lt;/sub&gt; of around 4 Hz can be expected in the case of the dihedral angle of 60°, while &lt;sup&gt;3&lt;/sup&gt;&lt;em&gt;J&lt;/em&gt;&lt;sub&gt;HH&lt;/sub&gt; of around 13 Hz corresponds to the dihedral angle of 180°. In reality, &lt;sup&gt;3&lt;/sup&gt;&lt;em&gt;J&lt;/em&gt;&lt;sub&gt;HH&lt;/sub&gt; values depend on substituents attached to the cyclohexane ring in substituted cyclohexanes, so the analysis is not straightforward, but the basic trend of having a larger &lt;em&gt;J&lt;/em&gt;-value for a 180° dihedral angle compared to a 60° dihedral angle remains unchanged. Therefore, from the value of &lt;sup&gt;3&lt;/sup&gt;&lt;em&gt;J&lt;/em&gt;&lt;sub&gt;HH&lt;/sub&gt; of the methylene protons, it is possible to differentiate between the dihedral angle of 60° or 180°.&lt;/p&gt;

&lt;h3&gt;Please click below to download and read more.&lt;/h3&gt;
</description></item><item><title>Separation of 13C spectra of polyurethane soft and hard segments by ROSY_NM200013E</title><link>https://www.jeolusa.com/RESOURCES/Analytical-Instruments/Documents-Downloads/separation-of-13c-spectra-of-polyurethane-soft-and-hard-segments-by-rosy</link><category>Experimental Possibilities</category><pubDate>Tue, 09 Mar 2021 16:22:11 GMT</pubDate><summary>The ROSY (Relaxation Ordered SpectroscopY) is a method in which the 13C CPMAS spectrum of a mixture is classified by a longitudinal relaxation time of 1H, and the 13C CPMAS spectrum is displayed separately for each substance. In solution NMR, each peak in the 1H spectrum has its own longitudinal relaxation time. In solid-state NMR, however, spin diffusion occurs due to the dipolor interaction between 1H, and all 1H have the same longitudinal relaxation in the domain within a certain distance. The 13C spectrum can be separated for each domain by using this difference in relaxation time of 1H. The longitudinal relaxation time (T1H) obtained by the saturation recovery method as shown in Fig.1a is usually used to separate the 13C spectrum of the mixture. The size of the domain that can be separated by this method is about 100 nm. To separate domains smaller than this, a measurement using the relaxation time at rotational flame (T1ρH) obtained by the spinlock method as shown in Fig.1b is effective. The domain size that can be separated by T1ρH is about several nm, and it is possible to determine the phase separation structure of block copolymers and the molecular compatibility.</summary><description>&lt;h2 data-key="2010" id="key_title"&gt;Separation of &lt;sup&gt;13&lt;/sup&gt;C spectra of polyurethane soft and hard segments by ROSY&lt;/h2&gt;

&lt;div&gt;
&lt;section&gt;
&lt;p&gt;The ROSY (Relaxation Ordered SpectroscopY) is a method in which the &lt;sup&gt;13&lt;/sup&gt;C CPMAS spectrum of a mixture is classified by a longitudinal relaxation time of &lt;sup&gt;1&lt;/sup&gt;H, and the &lt;sup&gt;13&lt;/sup&gt;C CPMAS spectrum is displayed separately for each substance. In solution NMR, each peak in the &lt;sup&gt;1&lt;/sup&gt;H spectrum has its own longitudinal relaxation time. In solid-state NMR, however, spin diffusion occurs due to the dipolor interaction between &lt;sup&gt;1&lt;/sup&gt;H, and all &lt;sup&gt;1&lt;/sup&gt;H have the same longitudinal relaxation in the domain within a certain distance. The &lt;sup&gt;13&lt;/sup&gt;C spectrum can be separated for each domain by using this difference in relaxation time of &lt;sup&gt;1&lt;/sup&gt;H. The longitudinal relaxation time (&lt;em&gt;T&lt;/em&gt;&lt;sub&gt;1&lt;/sub&gt;&lt;sup&gt;H&lt;/sup&gt;) obtained by the saturation recovery method as shown in Fig.1a is usually used to separate the &lt;sup&gt;13&lt;/sup&gt;C spectrum of the mixture. The size of the domain that can be separated by this method is about 100 nm. To separate domains smaller than this, a measurement using the relaxation time at rotational flame (&lt;em&gt;T&lt;/em&gt;&lt;sub&gt;1ρ&lt;/sub&gt;&lt;sup&gt;H&lt;/sup&gt;) obtained by the spinlock method as shown in Fig.1b is effective. The domain size that can be separated by &lt;em&gt;T&lt;/em&gt;&lt;sub&gt;1ρ&lt;/sub&gt;&lt;sup&gt;H&lt;/sup&gt; is about several nm, and it is possible to determine the phase separation structure of block copolymers and the molecular compatibility.&lt;/p&gt;
&lt;/section&gt;
&lt;/div&gt;
</description></item><item><title>Analysing complex mixtures using Pure shift DOSY_NM190018E</title><link>https://www.jeolusa.com/RESOURCES/Analytical-Instruments/Documents-Downloads/analysing-complex-mixtures-using-pure-shift-dosynm190018e</link><category>Experimental Possibilities</category><pubDate>Tue, 15 Sep 2020 10:43:42 GMT</pubDate><summary>Diffusion-ordered spectroscopy (DOSY) is a powerful NMR method for the analysis of mixtures. In DOSY, signals in the NMR spectrum are resolved according to the measured diffusion coefficient for each signal, yielding a 2D spectrum which has chemical shift along the x-axis and diffusion coefficient along the y-axis.</summary><description>&lt;h1&gt;Please click below to view the full article.&lt;/h1&gt;
</description></item><item><title>Observation of NOE by HSQC-NOESY_NM200005E</title><link>https://www.jeolusa.com/RESOURCES/Analytical-Instruments/Documents-Downloads/observation-of-noe-by-hsqc-noesynm200005e</link><category>Experimental Possibilities</category><pubDate>Mon, 14 Sep 2020 16:53:22 GMT</pubDate><summary>NOE (Nuclear Overhauser Effect) correlations  comprise important information to estimate internuclear distance and determine structure.
However, NOE correlation peaks are very weak compared with diagonal peaks in 2D NOESY. For this reason, it is difficult to observe NOE correlation peaks in the vicinity of much larger diagonal peaks.</summary><description>&lt;h1&gt;Please click below to view the full app notes.&lt;/h1&gt;
</description></item><item><title>On Accurate Measurements of Diffusion Coefficients by PGSE NMR Methods</title><link>https://www.jeolusa.com/RESOURCES/Analytical-Instruments/Documents-Downloads/on-accurate-measurements-of-diffusion-coefficients-by-pgse-nmr-methods</link><category>Experimental Possibilities</category><pubDate>Tue, 28 Jul 2020 10:02:16 GMT</pubDate><summary>In this article, we will show the accurate measurements of the diffusion coefficients (D) by using room-temperature ionic liquids (RTIL, IL) as examples.</summary><description>&lt;p&gt;In this article, we will show the accurate measurements of the diffusion coefficients (&lt;em&gt;D&lt;/em&gt;) by using room-temperature ionic liquids (RTIL, IL) as examples.&lt;/p&gt;
</description></item><item><title>Need for high resolution 2D spectra</title><link>https://www.jeolusa.com/RESOURCES/Analytical-Instruments/Documents-Downloads/need-for-high-resolution-2d-spectra1</link><category>Experimental Possibilities</category><pubDate>Tue, 28 Jul 2020 09:59:38 GMT</pubDate><summary>13C NMR spectra provide wide range chemical shift, and it suggests that can easily distinguish each signals. But carbon resolution of 2D spectra such as HSQC and HMBC is worse than 1D 13C spectra due to small data points. In order to analyze a compound with close 13C chemical shifts, a high resolution 2D spectrum is required frequently. In this document, some improvements to distinguish each signals on 13C axis of 2D hetero nuclear experiments are presented.</summary><description>&lt;p&gt;&lt;sup&gt;13&lt;/sup&gt;C NMR spectra provide wide range chemical shift, and it suggests that can easily distinguish each signals. But carbon resolution of 2D spectra such as HSQC and HMBC is worse than 1D &lt;sup&gt;13&lt;/sup&gt;C spectra due to small data points. In order to analyze a compound with close &lt;sup&gt;13&lt;/sup&gt;C chemical shifts, a high resolution 2D spectrum is required frequently. In this document, some improvements to distinguish each signals on &lt;sup&gt;13&lt;/sup&gt;C axis of 2D hetero nuclear experiments are presented.&lt;/p&gt;
</description></item><item><title>High sensitivity and quantitative 13C measurements using "Q-POMMIE"</title><link>https://www.jeolusa.com/RESOURCES/Analytical-Instruments/Documents-Downloads/high-sensitivity-and-quantitative-13c-measurements-using-q-pommie</link><category>Experimental Possibilities</category><pubDate>Tue, 28 Jul 2020 09:54:20 GMT</pubDate><summary>POMMIE (Phase Osacillations to Maximize Editing) is a 13C experiment that, like the more familiar DEPT experiment, utilizes polarization transfer to enhance the intensities of the 13C signals. However, unlike DEPT, POMMIE edits the spectrum by varying pulse phase rather than adjusting pulse flip angle.</summary><description>&lt;p&gt;POMMIE (Phase Osacillations to Maximize Editing) is a &lt;sup&gt;13&lt;/sup&gt;C experiment that, like the more familiar DEPT experiment, utilizes polarization transfer to enhance the intensities of the &lt;sup&gt;13&lt;/sup&gt;C signals. However, unlike DEPT, POMMIE edits the spectrum by varying pulse phase rather than adjusting pulse flip angle.&lt;/p&gt;
</description></item><item><title>Sample tube grade affects resolution</title><link>https://www.jeolusa.com/RESOURCES/Analytical-Instruments/Documents-Downloads/sample-tube-grade-affects-resolution</link><category>Experimental Possibilities</category><pubDate>Mon, 29 Jun 2020 09:15:49 GMT</pubDate><summary>Some low-grade, inexpensive NMR sample tubes have large warpage, low wall thickness uniformity, and large distortion, which may adversely affect the resolution.  The effect of low-grade sample tubes, such as disposable ones, on the resolution is small in low-field NMR, but it may be noticeable in high-field NMR.  In addition, some disposable sample tubes are thicker or thinner than the nominal value and will not fit in the sample holder.</summary><description>&lt;p&gt;Some low-grade, inexpensive NMR sample tubes have large warpage, low wall thickness uniformity, and large distortion, which may adversely affect the resolution.  The effect of low-grade sample tubes, such as disposable ones, on the resolution is small in low-field NMR, but it may be noticeable in high-field NMR.  In addition, some disposable sample tubes are thicker or thinner than the nominal value and will not fit in the sample holder.&lt;br /&gt;
	 &lt;/p&gt;

&lt;section&gt;
	&lt;h2&gt;Good resolution cannot be expected with low grade sample tubes in high-field NMR&lt;/h2&gt;

	&lt;p&gt;To examine the effect of disposable sample tubes on resolution, data measured on 400 MHz and 600 MHz spectrometers were compared.  The sample solution was prepared in advance and dispensed into 10 disposable sample tubes.  The gradient shim was performed with two iterations of magnetic field correction.&lt;br /&gt;
		The resolution of one out of ten samples was poor on the 400 MHz spectrometer (shown in Figure A).  On the other hand, when these ten samples were measured with the 600 MHz spectrometer, four of the ten samples showed good resolution, but five did not have very good resolution and one had poor resolution (shown in Figure B).  The distortion of the static magnetic field resulting from the distortion of a sample tube is proportional to the magnetic field strength.  Note that as the magnetic field strength increases, the effect of sample tube distortion on the resolution increases.&lt;/p&gt;
	&lt;img alt="Low grade sample tubes" class="img-responsive" src="/Portals/2/images/AI/1955e_01.png" /&gt;
	&lt;p&gt;&lt;strong&gt;Resolution of 10 identical samples&lt;/strong&gt;&lt;br /&gt;
		Results of gradient shimming on (A) 400 MHz and (B) 600 MHz NMR.&lt;br /&gt;
		 &lt;/p&gt;
&lt;/section&gt;

&lt;p&gt;If good resolution is not achieved, it may be possible to improve the resolution by increasing the number of iterations of the magnetic field correction or by adding the magnetic field correction with auto shim or FID shim after gradient shimming, but this may not be possible.  In other words, using a highly accurate sample tube depending on the magnetic field strength of the NMR will lead to stable and high resolution data.  If the sample tube is not suitable for the magnetic field strength, it cannot be said that the resolution will definitely increase.&lt;br /&gt;
	If a sample is measured with a 400 MHz NMR and the resolution is good, but not good when the same sample is measured with a higher field NMR, it may be due to the grade of the sample tube as mentioned above.  However, a low-grade sample tube does not necessarily impair the resolution.  After sample preparation, the grade of the sample tube tends to be unknown.  If the sample tube grade is suspected to be the cause of the poor resolution, it is recommended to consider changing the sample tube.&lt;br /&gt;
	 &lt;/p&gt;

&lt;section&gt;
	&lt;h2&gt;Resolution when using a scratched sample tube&lt;/h2&gt;

	&lt;p&gt;Even if the sample tube is highly accurate, scratches can cause localized distortion of the magnetic susceptibility, resulting in poor resolution.  The spectrum in the center of the figure below is the data obtained by measuring with a scratched sample tube.  Gradient shim conditions are the same as those without scratches (left in the figure below), but resolution did not improve.  If you use the Gradient Shim Tool for shimming, you can see the magnetic field map at the time of magnetic field correction (lower part of the figure below).  In this figure, you can see that the magnetic field map is distorted where there are scratches.  Even if the number of iterations was increased until the magnetic field correction results converged, the resolution did not improve (right figure below).  It is strongly recommended to replace the sample tube if it becomes scratched.  In order to always achieve good resolution, it is important to be careful not to mix low-precision or scratched sample tubes with high-precision ones.&lt;br /&gt;
		 &lt;/p&gt;
	&lt;img alt="Effect of scratches on resolution" class="img-responsive" src="/Portals/2/images/AI/1955e_02.png" /&gt;
	&lt;p&gt;&lt;strong&gt;Effect of scratches on resolution&lt;/strong&gt;&lt;br /&gt;
		Spectra shown in the upper row and the magnetic field maps in the bottom row.  Left; No scratch, 2 iterations.  Center; After measuring the data on the left, the sample tube was scratched.  The number of magnetic field-corrected iterations is two, which is the same as without a scratch.  Right; The same sample as the central data.  The number of magnetic field-corrected iterations was judged by automatic convergence to increase the number of iterations.&lt;br /&gt;
		 &lt;/p&gt;
&lt;/section&gt;
</description></item><item><title>NOAH-NMR Supersequences with Nested Acquisition for Small Molecules</title><link>https://www.jeolusa.com/RESOURCES/Analytical-Instruments/Documents-Downloads/noah-nmr-supersequences-with-nested-acquisition-for-small-molecules</link><category>Experimental Possibilities</category><pubDate>Fri, 12 Jun 2020 12:48:15 GMT</pubDate><summary>NOAH (NMR by Ordered Acquisition using 1H-detection)[1] is a group of nested NMR experiments combining several conventional two-dimensional (2D) NMR pulse sequences, such as COSY, HSQC and HMBC, into one supersequence. Therefore, two or more 2D NMR data can be obtained from a single NOAH experiment. By using a single relaxation delay, the NOAH method significantly reduces the total data collection time and increases the throughput of an NMR instrument in structure elucidation of small organic molecules.</summary><description>&lt;p&gt;NOAH (&lt;strong&gt;N&lt;/strong&gt;MR by &lt;strong&gt;O&lt;/strong&gt;rdered &lt;strong&gt;A&lt;/strong&gt;cquisition using &lt;sup&gt;1&lt;/sup&gt;&lt;strong&gt;H&lt;/strong&gt;-detection)[1] is a group of nested NMR experiments combining several conventional two-dimensional (2D) NMR pulse sequences, such as COSY, HSQC and HMBC, into one supersequence. Therefore, two or more 2D NMR data can be obtained from a single NOAH experiment. By using a single relaxation delay, the NOAH method significantly reduces the total data collection time and increases the throughput of an NMR instrument in structure elucidation of small organic molecules.&lt;/p&gt;
</description></item><item><title>High Resolution 2D spectra</title><link>https://www.jeolusa.com/RESOURCES/Analytical-Instruments/Documents-Downloads/need-for-high-resolution-2d-spectra</link><category>Experimental Possibilities</category><pubDate>Fri, 12 Jun 2020 12:46:00 GMT</pubDate><summary>13C NMR spectra provide wide range chemical shift, and it suggests that can easily distinguish each signals. But carbon resolution of 2D spectra such as HSQC and HMBC is worse than 1D 13C spectra due to small data points. In order to analyze a compound with close 13C chemical shifts, a high resolution 2D spectrum is required frequently. In this document, some improvements to distinguish each signals on 13C axis of 2D hetero nuclear experiments are presented.</summary><description>&lt;p&gt;&lt;sup&gt;13&lt;/sup&gt;C NMR spectra provide wide range chemical shift, and it suggests that can easily distinguish each signals. But carbon resolution of 2D spectra such as HSQC and HMBC is worse than 1D &lt;sup&gt;13&lt;/sup&gt;C spectra due to small data points. In order to analyze a compound with close &lt;sup&gt;13&lt;/sup&gt;C chemical shifts, a high resolution 2D spectrum is required frequently. In this document, some improvements to distinguish each signals on &lt;sup&gt;13&lt;/sup&gt;C axis of 2D hetero nuclear experiments are presented.&lt;/p&gt;
</description></item></channel></rss>