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What is Nuclear Magnetic Resonance?
Nuclear Magnetic Resonance (NMR) measures the absorption of electromagnetic radiation in the radio-frequency region (~4-900 MHz)
o Nuclei (instead of outer electrons) are involved in absorption process
o Sample needs to be placed in magnetic field to cause different energy states
- NMR was first experimentally observed by Bloch and Purcell in 1946 (received Nobel Prize in 1952) and quickly became commercially available and widely used.
- Probe the Composition, Structure, Dynamics and Function of the Complete Range of Chemical Entities: from small organic molecules to large molecular weight polymers and proteins
- NMR is routinely and widely used as the preferred technique to rapidly elucidate the chemical structure of most organic compounds.
- One of the MOST Routinely used Analytical Techniques
NMR History
First NMR Spectra: on Water
-Electrons spin clock-wise or counter-clockwise
-Nucleus also has nuclear-spin. So, like a magnet, it will be attracted to one part of the field
-Back to spectroscopy
-Proved that nuclei had spin
-Then discovered chemical shift when doing NMR of Ethanol
-Every molecule absorbs differently based on different chemical environments
-Results in different peaks
-Each chemical has a fingerprint
Typical Applications of NMR: Structural (chemical) elucidation
a. Natural product chemistry
b. Synthetic organic chemistry
i. Analytical tool of choice of synthetic chemists
ii. Used in conjunction with MS and IR
Typical Applications of NMR: Study of Dynamic Processes
a. Reaction kinetics
b. Study of equilibrium (chemical or structural)
Typical Applications of NMR: Drug Design
Structure Activity Relationships by NMR
Typical Applications of NMR: Others
1.) Medicine-MRI
2.) Metabolomics-disease biomarkers
Information in an NMR Spectrum: Absorption
electromagnetic (light) energy is transferred to atoms, ions, or molecules in the sample. Results in the transition to a higher energy state.
Information in an NMR Spectrum: Wave model
Represented by a sinusoidal wave traveling space with an oscillating electric field and perpendicular magnetic field (NMR responds to magnetic field)
What is Electromagnetic Theory?
- A perpendicular external magnetic field will induce an electric current in a closed loop
- Magnetic field produced by circulating electron
- An electric current in a closed loop will create a perpendicular magnetic field
Theory of NMR: Quantum Description
- Nuclear Spin (think Electron Spin)
a) Nucleus rotates about its axis (spin
b) Nuclei with spin have angular momentum
-Quantized, spin quantum number I
-2I + 1 states: I, I-1, I-2
-idenitcal energyies in absence of external magnetic field
c) NMR “active” Nuclear Spin (I)= ½
1H, 13C, 15N, 19F, 31P
Odd atomic mass
I= +1/2 & -1/2
NMR “inactive” Nuclear Spin (I)=0
12C,16O
Even atomic mass and Number
Quadrupole Nuclei Nuclear Spin (I)>1/2
What is a magnetic moment?
spinning charged nucleus creates a magnetic field
Similar to magnetic field created by electric current flowing in a coil
a) Magnetic moment is created along axis of nuclear spin
a. U=yp
Where:
p-angular momentum
y-gyromagnetic ratio (different value for each type of nucleus)
b) Magnetic moment is quantized (m)
a. M=I, I-1, I-2…, -I
For common nuclei of interest:
M=1/2 & -1/2
What is Magnetic Alignment?
Without magnetic field the nucleus does not prefer any particular alignment.
· Add a strong external field (Bo). and the nuclear magnetic moment aligns with (low energy) against (high-energy)
· To sense these magnetic moments, we have to put it into a magnetic field
o Can’t detect a signal if there is no change in energy
Zeeman Effect
Magnetic moments are oriented in one of two directions in a magnetic field
Energy Levels in a Magnetic Field
Transition from the low energy to high energy spin state occurs through an absorption of a photon of radio-frequency (RF) energy
NMR Theory: Classical Description
Spinning particle precesses around an applied magnetic field
a) Angular velocity of this motion is given by:
ωo=γBo
Net Magnetization in A Magnetic Field: Classic View
Nuclei either align with or against external magnetic field along the z-axis
- Since more nuclei align with field, not magnetization (Mo) exists parallel to external magnetic field
Net Magnetization in A Magnetic Field: Quantum Description
- Nuclei either populate low energy (α, aligned with field) or high energy (β, aligned against field)
- Net population in α energy level.
- Absorption of radio-frequency promotes nuclear spins from α-β
Resonant conditions
frequency (ω1) of B1 matches Lamor frequency (ωo) energy is absorbed and population of α and β states are perturbed
And/or
Mo, now precess about B1 (similar to Bo) for as long as the B1 field is applied
Classical Description: Observe NMR Signal
o Need to perturb system from equilibrium
§ B1 field (radio frequency pulse with γBo/2π frequency
o Net magnetization (Mo) now precesses about Bo and B1
§ Mx and My are non-zero
§ Mx and My rotate at Larmor frequency
§ System absorbs energy with transitions between aligned and unaligned states
o Precession about B1 stopped when B1 is turned off
The B1 field is turned off and Mxy continues to precess about Bo at a frequency ωo
The oscillation of Mxy generates a fluctuating magnetic field which can be used to generate a current in a receiver coil to detect the NMR signal
- A magnetic field perpendicular to a circular loop will induce a current in the loop.
NMR Signal Detection- Fourier Transform
So, the NMR signal is collected in the Time-domain
Fourier Transform is a mathematical procedure that transforms time domain data into frequency domain
After the NMR signal is generated and the B1 field is removed, the net magnetization will relax back to equilibrium aligned along the Z-axis
V1/2 = 1/πT2
Two types of relaxation processes, on in the x, y plane and one along the x-axis
Peak shape also affected by magnetic field homogeneity or shimming
NMR Relaxation
No spontaneous reemission of photons to relax down to ground state
Probability too low- cube of the frequency
NMR Relaxation: Spin-lattice or longitudinal relaxation (T1)
i. Transfer energy to the lattice or solvent material
ii. Coupling of nuclei magnetic field with magnetic fields created by the ensemble of vibrational and rotational motion of the lattice or solvent
iii. Results in a minimal temperature increase in sample
Mz=Mo (1-e-t/T1)
NMR Relaxation: Spin-Spin or transverse relaxation (T2)
i. Exchange of energy between excited nucleus and low energy state nucleus
i. Randomization of spins or magnetic moment in x,y-plane
ii. Related to NMR peak line width
Mx=My=Moexp(-t/T2)