Solid state NMR – Part 2 · 2013-04-10 · then connected to the input pulley of the NMR probe as...

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Solid state NMR – Part 2 - Chapter 14, on web site: http://www.chem.ubc.ca/faculty/straus/c518_09.html A) Averaging – Magic angle sample spinning B) Polarization transfer - CP

Transcript of Solid state NMR – Part 2 · 2013-04-10 · then connected to the input pulley of the NMR probe as...

Page 1: Solid state NMR – Part 2 · 2013-04-10 · then connected to the input pulley of the NMR probe as shown in (A). (C) The drawing containing only the pulling assembly in (B) for changing

Solid state NMR –Part 2

- Chapter 14, on web site: http://www.chem.ubc.ca/faculty/straus/c518_09.html

A) Averaging – Magic angle sample spinning

B) Polarization transfer - CP

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Interactions in solid state

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Chemical shift:

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Spherical tensor notation:

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where

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Dipolar interaction:

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How averaging of CSA works under MAS:

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average A20

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In the LAB frame:

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Or rewritten in a different way:

FT

signal at isotropic chemical shift, with sidebands due to theterm

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e.g. 13C spectrum ofalanine

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Alternative methods: Magic angle hopping and Magic angle turning

MAS continuous rotation, averaging over a full rotation

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Given

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Final result:

= 0

How is this achieved experimentally?

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Analogous approach: magic angle turning

rotor is synchronized so that signal is detected at the appropriate angles (120° apart) requires slow spinning

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A quick look at MAS and quadrupolar nuclei:

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To average the P4 term completely dynamic angle spinning (DAS) ordouble rotation (DOR)

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B) Cross-polarization

Why use it? To enhance sensitivity (analogous to INEPT in solution state)

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oscillations proportional todipolar coupling constant

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Dipolar oscillations PISEMA