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Sampling spinning sample

Place 0.2-pm filters into 0.5-mL centrifuge tubes. Load with 50 pL of sample. Spin sample through the filters at low speed ( 2000 rpm). [Pg.174]

In most cases we adjust the shims along the z-axis, but sometimes we will also shim in the xy plane without sample spinning. Sample... [Pg.28]

Thennal equilibrium produees a Boltzmann distribution between these energy levels and produees the bulk mielear magnetization of the sample tlirough the exeess population whieh for a sample eontaining a total of N spins is Nytj B lkT. For example for Si in an applied magnetie field of 8.45 T the exeess in the... [Pg.1468]

Motion, and in particular diffiision, causes a further limit to resolution [14,15]. First, there is a physical limitation caused by spins diflfiising into adjacent voxels durmg the acquisition of a transient. For water containing samples at room temperature the optimal resolution on these grounds is about 5 pm. However, as will be seen in subsequent sections, difhision of nuclei in a magnetic field gradient causes an additional... [Pg.1529]

Figure Bl.14.6. J -maps of a sandstone reservoir eore whieh was soaked in brine, (a), (b) and (e), (d) represent two different positions in the eore. For J -eontrast a saturation pulse train was applied before a standard spin-eeho imaging pulse sequenee. A full -relaxation reeovery eiirve for eaeh voxel was obtained by inerementing the delay between pulse train and imaging sequenee. M - ((a) and (e)) and r -maps ((b) and (d)) were ealeulated from stretehed exponentials whieh are fitted to the magnetization reeovery eurves. The maps show the layered stnieture of the sample. Presumably -relaxation varies spatially due to inliomogeneous size distribution as well as surfaee relaxivity of the pores. (From [21].)... Figure Bl.14.6. J -maps of a sandstone reservoir eore whieh was soaked in brine, (a), (b) and (e), (d) represent two different positions in the eore. For J -eontrast a saturation pulse train was applied before a standard spin-eeho imaging pulse sequenee. A full -relaxation reeovery eiirve for eaeh voxel was obtained by inerementing the delay between pulse train and imaging sequenee. M - ((a) and (e)) and r -maps ((b) and (d)) were ealeulated from stretehed exponentials whieh are fitted to the magnetization reeovery eurves. The maps show the layered stnieture of the sample. Presumably -relaxation varies spatially due to inliomogeneous size distribution as well as surfaee relaxivity of the pores. (From [21].)...
The C-H spin couplings (Jen) have been dealt with in numerous studies, either by determinations on samples with natural abundance (122, 168, 224, 231, 257, 262, 263) or on samples specifically enriched in the 2-, 4-, or 5-positions (113) (Table 1-39). This last work confirmed some earlier measurements and permitted the determination for the first time of JcH 3nd coupling constants. The coupling, between a proton and the carbon atom to which it is bonded, can be calculated (264) with summation rule of Malinovsky (265,266), which does not distinguish between the 4- and 5-positions, and by use of CNDO/2 molecular wave functions the numerical values thus - obtained are much too low, but their order agrees with experiment. The same is true for Jch nd couplings. [Pg.79]

Another form of radiationless relaxation is internal conversion, in which a molecule in the ground vibrational level of an excited electronic state passes directly into a high vibrational energy level of a lower energy electronic state of the same spin state. By a combination of internal conversions and vibrational relaxations, a molecule in an excited electronic state may return to the ground electronic state without emitting a photon. A related form of radiationless relaxation is external conversion in which excess energy is transferred to the solvent or another component in the sample matrix. [Pg.425]

Another automated approach to kinetic analyses is the centrifugal analyzer, a partial cross section of which is shown in Figure 13.9. In this technique the sample and reagents are placed in separate wells oriented radially around a circular transfer disk attached to the rotor of a centrifuge. As the centrifuge spins, the... [Pg.634]


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See also in sourсe #XX -- [ Pg.113 , Pg.114 ]




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CPMAS sample spinning

Carbon-13 spin system, solid sample

Cross-polarization and magic angle sample spinning

Electron spin resonance doped samples

Electron spin resonance polycrystalline samples

High speed spinning of samples

High-resolution magic angle spinning sample preparation

Magic Angle Spinning and Static Experiments on Powdered Samples

Magic-angle sample spinning

Magic-angle spinning sample preparation

Magic/angle sample spinning nuclear

Magic/angle sample spinning nuclear magnetic resonance spectroscopy

Magic/angle sample spinning nuclear multiple pulse techniques

Manual vs Robotic Instrumentation for Sample Preparation and Acquiring Spin Column Eluates

Nuclear magnetic resonance , solids magic angle sample spinning

Sample Prepared Under Equilibrium Conditions Prior to Spin Column Treatment

Sample rotor magic-angle spinning

Sample spinning

Sample spinning

Sample spinning frequencies

Sample spinning shimming

Sample spinning sidebands

Sample spinning, NMR

Spinning of samples

Switching-angle sample spinning—

Variable-angle sample spinning

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