Fundamentals of Magnetic Resonance Flashcards

1
Q

What is the nuclear spin quantum number

A

I - describes the intrinsic spin of the nuclei

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2
Q

What is the nuclear spin quantum number associated with the z-component?

A

m - values range from +I to -I in steps of 1

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3
Q

What types of nuclei have spin magnetic moment?

A

Nuclei with nuclear spin > 0

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4
Q

What is the Zeeman interaction?

A

The nuclear magnetic moment will interact with any applied magnetic field. The energy of this interaction can be described by the Zeeman Hamiltonian

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5
Q

What can be used to determine the transition frequency from one spin state to another

A

𝛥E between spin states

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6
Q

Limitations of the energy level picture of NMR

A

NMR is not emission/ absorption spectroscopy, it is a resonance technique

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7
Q

What are vectors

A

Vectors are quantities with both magnitude and a direction defined in terms of a coordinate system

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8
Q

What is torque

A

A twisting force that acts perpendicular to interacting vectors - this causes M to precess around B

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9
Q

Net magnestisation

A

vector sum of all magnetic moments of all spins in sample

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10
Q

In absence of magnetic field what is what is the net magnetisation?

A

zero - no net magnetisation as there is no preference for direction so they all cancel out

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11
Q

What happens when 2 magnetic moments are out of phase?

A

Mostly cancel each other out - destructive interference

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12
Q

What happens when 2 magnetic moments are in phase?

A

The magnetic moments add up - constructive interference

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13
Q

When can there only be net magnetisation in Mxy plane

A

if there is phase coherence - when nuclear magnetic moments precess in sync with one another at same frequency and same initial phase

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14
Q

What is the net magnetisation in Mxy plane at thermal equilibrium?

A

At thermal eqm all spins point in arbitrary directions so Mxy = 0 as there is no phase coherence

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15
Q

What happens when we rotate net magnetisation (Mo) into xy plane

A

Magnetic moments are precessing in sync so add up in xy plane Mxy > 0
Destroy longitudinal magnetisation Mz now = 0 equal popn between energy states
Mo precesses around Bo at Larmor frequency

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16
Q

How do we rotate Mo into xy plane?

A

Generate RF pulse - an oscillating voltage passed through a coil of wire will generate oscillating magnetic field
Radio frequency pulse at Larmor frequency to induce transitions between 2 energy states.
New magnetic field B1 oscillates at larmor frequency perpendicular to Bo

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17
Q

What does applying a second magnetic field B1 on x axis perpendicular Bo do?

A

This causes Mo net magnetisation to precess around B1 in the rotating frame. If we apply the pulse for exactly the right amount of time we can rotate magnetisation from z into xy plane

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18
Q

What is NMR receptivity?

A

NMR receptivity is a measure of how easy it is to detect the NMR signal of a given nucleus - it is quoted relatitive to another nucleus e.g. 1H or 13C

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19
Q

Longitudinal relaxation

A

T1
This process generates the eqm population difference across zeeman energy levels and establishes Mo along z axis

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20
Q

Transverse relaxation

A

T2
process that causes xy magnetisation to decay to zero. Mxy comes from phase coherence so relaxation must be due to loss of phase coherence - randomisation of phase

21
Q

What is the rate of change of longitudinal magnetisation proportional to?

A

Proportional to the difference between current magnetisation and equilibrium magnetisation

22
Q

what is it called if Mz is larger than equilibrium magnetisation?

A

Hyperpoarisation
Mz will decay time due to T1 relaxation

23
Q

what is the rate of transverse relaxation proportional to?

A

magnetisation in xy plane, Mxy

24
Q

What is the rate of longitudinal relaxation proportional to?

A

The difference between current magnetisation and eqm magnetisation

25
Q

What is effective transverse relaxation T2*?

A

the rate at which transverse magnetisation decays faster than expected in NMR experiments
Mxy can also decay due to reversible dephasing - this comes from nuclei experiencing different larmor frequencies (e.g. bubble in NMR tube)
If nuclei in different parts of sample will experience different fields so precess at different frequencies and dephase as time goes on

26
Q

What effect does short T2* have on NMR spectra?

A

Short T2* (fast relaxation) leads to broad peaks in NMR spectrum - reduced resolution and signal to noise ratio

27
Q

What effect does long T2* have on NMR spectra

A

This means slow relaxation which leads to narrow peaks with higher signal

28
Q

What is shimming?

A

Shimming is the process of improving the homogeneity of Bo by applying small additional fields to cancel out small variations across the sample

29
Q

What causes T1 relaxation?

A

Exchange of energy with the environment re-establishing the equilibrium population difference across the nuclear spin energy levels

30
Q

What causes T2 relaxation?

A

Interaction between spins and the environment - doesn’t require exchange of energy.
Causes loss of phase coherence between precessing spins

31
Q

What is dipole-dipole coupling?

A

direct magnetic spin-spin interaction between nuclei, occurs through space
the size of the interaction is determined by the coupling constants
As it is an anisotropic interaction it averages out in liquids

32
Q

What is J coupling

A

indirect magnetic spin-spin interaction mediated by the electrons, occurs through chemical bonds

33
Q

What is Quadrupolar interactions?

A

Electronic interaction of electric quadrupole moment (eQ) of spins with I > 1/2 with surrounding electric field
The more anisotropic the distribution of charge the larger the eQ

34
Q

What are hyperfine interactions?

A

Interaction between a nuclear spin and an unpaired electron spin, similar in origin to J coupling

35
Q

What makes an interaction an isotropic interaction?

A

The size of the interaction is independent of the relative orientation of the molecule and the magnetic field

36
Q

Some examples of isotropic interactions?

A

J coupling
Hyperfine
Zeeman interaction
isotropic chemical shift

37
Q

what makes an interaction an anisotropic interaction

A

The size of the interaction depends on the orientation of the molecule with respect to the magnetic field

38
Q

Example of anisotropic interaction

A

Dipole-dipole coupling
Quadrupole coupling
Chemical shift anisotropy

39
Q

What are the effects of anisotropic interactions on NMR spectra

A

Cause different frequency shifts depending on orientation of molecule relative to Bo
(Not observed in liquid due to molecular tumbling - anisotropic interactions average to zero)

40
Q

What does the size of J-Coupling depend on?

A

Gyromagnetic ratio of each nucleus
number of bonds/ bond angle between nuclei

41
Q

What is chemical equivalence?

A

Where 2 spins have the same chemical shift, appears as a singlet, no coupling between A and B is observed

42
Q

when are two nuclei magnetically inequivalent?

A

if they couple differently to a 3rd nucleus.
For example in an octahedral complex one H couples cis to a P spin up nuclei and one H couples trans to the same P spin up nuclei

43
Q

If the difference in chemical shift of 2 nuclei is much bigger than the J coupling

A

get weak coupling
standard multiplets

44
Q

If the difference in chemical shift is approximately the same as the J value

A

Means there is strong coupling
Lots of roofing

45
Q

If 2 nuclei have the same chemical shift?

A

they are chemically equivalent - see a singlet

46
Q

What is chemical shift anisotropy

A

in the presence of a strong applied field, the electrons in the molecule give rise to a small induced field at the nucleus that opposes Bo

47
Q

What do hyperfine interactions cause in NMR spectroscopy?

A

causes fast T2 relaxation meaning NMR spectra can often not be obtained for paramagnetic species

48
Q

What is magic angle spinning

A

Technique used in solid state NMR to average out anisotropic interactions to simplify spectra and recover isotropic chem shift info
Averages out anisotropic interactions in a similar way to motional averaging but not random, it is at a fixed rotation frequency at a single specific axis.
Rotation axis oriented at 54.7 bc due to symmetry the dipole dipole and CSA interactions are zero at this angle