Topic 1: Motional averaging of NMR interactions Flashcards

1
Q
  • NMR interactions: …, … and
  • interactions depend on the of the with respect to
  • Anisotropic interactions depend on the geometry of molecules
  • Motion changes of molecules and parts of molecules influencing the of anisotropic interactions measured with NMR
A
  • Anisotropic NMR interactions: CSA, dipolar and quadrupolar couplings
  • Anisotropic interactions depend on the orientation of the molecule with respect to B0
  • Anisotropic interactions depend on the geometry of molecules
  • Motion changes orientation of molecules and parts of molecules influencing the magnitude of anisotropic interactions measured with NMR
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2
Q
  • Sketch the NMR spectra of an isotropic solution and a solid-state sample
A
  • In isotropic, all anisotropic interactions averaged to 0
  • In solid-state, all anisotropic interactions still present
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3
Q
  • How does dipolar coupling between 2 molecules vary with angle with respect to a magnetic field of a smaple in solution?
A
  • If molecule samples all values of θ in a short time will result in an average of values –> isotropic tumbling (as can move in solution)
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4
Q
  • What is the overall average of anisotropic interactions in solution NMR? Use an equation to support your answer (don’t need to know equation, just output number)
A
  • Interactions at all orientations cancel each other out with respect to magnetic field
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5
Q
  • In an isotropic solution only interactions (don’t depend on ) are retained leaving only and coupling
  • Anisotropic interaction ( , dipolar/ coupling) only influence spectra through but not directly observable via
A
  • In an isotropic solution only isotropic interactions (don’t depend on B0) are retained leaving only isotropic CS and J coupling
  • Anisotropic interaction (CSA, dipolar/quadrupolar coupling) only influence spectra through relaxation but not directly observable via modulation
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6
Q
  • Using a sketch to describe molecular motion, describe the differences of solution and solid-state NMR
A
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7
Q
  • Describe the interaction in solid-state NMR and sketch the resulting powder spectra that results
A
  • No overall tumbling present in solution as in static powders all orientations are present but no interchange present between them
  • Pake pattern forms as sum of all orientations instead of an average
  • Dc is the dipolar coupling constant
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8
Q
  • What can lead to averaging in solid-state NMR? How id the powder spectra effected?
A
  • Local/internal motion will lead to averaging as forms an overall motion of molecules giving residual dipolar coupling (RDC)
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9
Q
  • Describe a method for selectively isolating interactions in solid-state NMR
A
  • Magic angle spinning (MAS) simulates tumbling by spinning the sample, removing anisotropic interactions in doing so
  • Recoupling uses pulses to interfere with MAS to bring back interactions of interest
  • Motional averaging cannot be undone as random in nature
  • RDCs can be measured under MAS
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10
Q
  • What parameter can be assigned to the measurement of amplitude of motion of a molecule?
A
  • Order parameter (OP) is an expression for amplitude of motion which relates to how big the motion is.
  • Static/rigid limit is the absence of motion (Dc), calculated from a known distance
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11
Q
  • An NH coupling has a measured dipolar coupling of 9230 Hz and a one-bond NH rigid limit of 11477 Hz. What is the order parameter associated with this coupling and the correlation time (τ­c) associated with it?
A
  • S2 = (9230/11477)2 = 0.67
  • Only motion faster than the inverse of the dipolar coupling can average this coupling and contribute to the OP
  • Inverse of dipolar coupling is correlation time; 1/(2π*11477) = 13 µs
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12
Q
  • Describe the scale of restriction of motion when varying the order parameter from one limit to the other
A
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13
Q
  • How can the use of deuterium help infer dynamics of systems that have indistinguishable hydrogens?
A
  • Deuterium is a quadrupolar nucleus 2H (I = 1)
  • Quadrupolar line shapes probe dynamics of a system, which can be compared to Hydrogen data
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14
Q
  • How does the source of residual dipolar coupling (RDC) vary from solid-state to solution NMR?
A
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15
Q
  • Is there a way to overall motion is present but not all orientations are sampled
A
  • Yes, via an anisotropic solution, where molecules rotate around some but not whole 360o axis
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16
Q
  • How can molecules be partially aligned to obtain solution RDCs?
A
  • Different media can be used to enforce different alignment
  • E.g. bicelles can be inserted to restrict the motion of proteins in a solution
  • Not all orientations are samples so anisotropic interactions average to 0
  • RDCs that are +ve/ -ve depending on media and direction of B0, relate to amplitude of motions in a molecule
17
Q
  • Overall motion averages … … so we observe only a fraction of
  • Amplitude of motion (… ) determines what fraction of is measured
A
  • Overall motion averages dipolar coupling so we observe only a fraction of Dc
  • Amplitude of motion (S2) determines what fraction of dipolar coupling is measured
18
Q
  • How does the size of a motion relate to its order parameter?
A
  • A bigger S2 has a smaller amplitude of motion
19
Q
  • What motions would contribute to the averaging of coupling in a system with a 13C-13C Dc ~ 2100 Hz) and a 1H-13C (Dc ~ 24000 Hz) bond present? Would a motion of τ­c = 30 µs average dipolar coupling?
A
  • Only if frequency (1/ τ­c) of motion is greater than coupling size will it contribute to averaging of coupling
  • 13C-13C; only motions faster than 1/(2π*2100 Hz) = 76 µs will average
  • 1H-13C; only motions faster than 1/(2π*24000 Hz) = 13 µs will average
  • A motion of τ­c = 30 µs will average 13C-13C but not 1H-13C dipolar coupling
  • RDCs yield the amplitude of motions but only an upper bound for their timescales
20
Q

Summary of topic 1

  • Motions average interactions
  • () give cumulative amplitude of motions faster than inverse of the coupling
  • Need … … in anisotropic liquids to get RDC in solution
  • S2 – order parameter gives generalised … … … , S2 = 1, ; S2 = , unrestricted motion; the rest is between 0-1
A

Summary of topic 1

  • Motions average anisotropic interactions
  • Residual dipolar coupling (RDC) give cumulative amplitude of motions faster than inverse of the coupling
  • Need partial alignment in anisotropic liquids to get RDC in solution
  • S2 – order parameter gives generalised amplitude of motion, S2 = 1, rigid; S2 = 0, unrestricted motion; the rest is between 0-1