NMR in Medicine and Biology MRI- Magnetic Resonance Imaging (water) In-vivo spectroscopy (metabolites) Solid-state NMR (large structures) Solution NMR.

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NMR in Medicine and Biology MRI- Magnetic Resonance Imaging (water) In-vivo spectroscopy (metabolites) Solid-state NMR (large structures) Solution NMR –Bioanalytical, primary structure –Three-dimensional structure –Molecular motions –Molecular interactions- binding, reactions Ligand screening (Pharma)

Nuclear Spin Nuclear spin angular momentum is a quantized property of the nucleus in each atom, which arises from the sub-atomic properties of neutrons and protons The nuclear spin angular momentum of each atom is represented by a nuclear spin quantum number (I) All nuclei with odd mass numbers have I=1/2,3/2... Nuclei with even mass numbers and an even number of protons have I=0 Nuclei with even mass numbers and an odd number of protons have I=1,2,3… Biomolecular NMR: primarily spin 1/2 nuclei ( 1 H, 13 C, 15 N, 31 P)

Nuclei With Non-Zero Spin Align in Magnetic Fields HoHo anti-parallel parallel Alignment Energy  E = h  H o Efficiency factor- nucleus ConstantsStrength of magnet

NMR: The Bar Magnet Analogy +-+- H o = force non-alignment2. release p ap p p

Resonance: Perturb Equilibrium HoHo h  E H1H1 2. pump in energy  E = h  H o Efficiency factor- nucleus ConstantsStrength of magnet p ap 1. equilibrium EE p ap 3. non-equilibrium

Return to Equilibrium (Relax): Read Out Signals p ap 5. equilibrium h  E 4. release energy (detect) p ap EE 3. Non-equilibrium

Magnetic Resonance Sensitivity  E is small At room temp.,  N ~ 1:10 5 Intrinsically low sensitivity  Need lots of sample  E = h  H o Efficiency factor- nucleus ConstantsStrength of magnet N p N ap = e -  E/kT Sensitivity (S) ~  population) S ~  N = Increase sensitivity by increasing magnetic field strength

Intrinsic Sensitivity of Nuclei Nucleus  Natural Relative Abundance Sensitivity 1 H2.7 x C6.7 x N -2.7 x P1.1 x

The Classical Treatment: Nuclear Spin Angular Momentum HoHo anti-parallel parallel  Torque + int. motion = precession  Precession around Z axis  Larmor frequency (  ):  E = h  H o   E = h  =  H 0 =  Two spins All spins  Sum Bulk Magnetization excess facing down