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Nuclear Magnetic Resonance (NMR)
for beginners
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Overview NMR is a sensitive, non-destructive method for elucidating the structure of organic molecules Information can be gained from the hydrogens (proton NMR, the most common), carbons (13C NMR) or (rarely) other elements
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Spin States All nuclei have a spin state (I )
Hydrogen nuclei have a spin of I = ±½ (like electrons) Spin number gives number of ways a particle can be oriented in a magnetic field: 2I + 1
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Spin States In the absence of a magnetic field the spin states are degenerate The “spinning” nucleus generates its own magnetic field
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Spin States In a magnetic field the states have different energies Bo
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Spin states in a magnetic field
Energy difference linearly depends on field strength = magnetic moment of H (2.7927N or x10-27J/T)
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Spin states in a magnetic field
Even in a very large field (1-20T) the energy difference is small (~0.1cal/mol)
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Spin states in a magnetic field
A small excess of protons will be in the lower energy state These can be promoted to the higher state by zapping them with EM radiation of the proper wavelength Wavelength falls in the radio/TV band (frequency of MHz)
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Spin states in a magnetic field
Stronger magnetic field necessitates shorter wavelength (higher frequency) After low energy protons are promoted to the higher energy state they relax back to the lower state
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Making NMR work Not all protons absorb at the same field values
Either magnetic field strength or radio frequency must be varied Frequency/field strength at which the proton absorbs tells something about the proton’s surroundings
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Making NMR work
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Sample must be spun to average out magnetic field inhomogeneity
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NMR data collection Continuous wave data collection (CW):
Magnetic field value is varied Intensity of emitted RF compared to RF at detector Absorption is plotted on graph
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NMR data collection CW NMR of isopropanol
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NMR data collection Pulsed Fourier transform data collection:
Short bursts of RF energy are shot at sample Produces a decay pattern FT done by computer produces spectrum
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Simple FT FID and spectrum
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More complex FT FID and spectrum
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Even more complex FT FID
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FT NMR Spectrum
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Pulsed FT NMR of isopropanol
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Chemical shift Protons in different environments absorb at different field strengths (for the same frequency) Different environment = different electron density around the H
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Chemical shift positions
High field, shielded Low field, deshielded PPM of applied field () from reference Reference (tetramethylsilane)
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Chemical shift positions
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NMR reference Tetramethylsilane ((CH3)4Si) Advantages: Makes one peak
12 equivalent H, so little is needed Volatile, inert, soluble in organic solvents Absorbs upfield of hydrogens in most organic compounds
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Shielding/deshielding
Electron density affects chemical shift Electrons generate a magnetic field opposed to the applied field H in high electron density absorbs upfield (toward TMS, 0ppm) from H in low electron density
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Shielding/deshielding
Effect of electronegativity: electronegative atom nearby removes electron density and causes deshielding TMS protons are extremely shielded because Si is electropositive compared to C
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Shielding/deshielding
Few protons absorb upfield of TMS Alkyl groups are electron donating, so alkanes absorb around 0-2ppm () Hydrogens near electronegative atoms are deshielded Absorption is around 3-4
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Anisotropy “Anisotropy”: any characteristic that varies with direction (asymmetric) Applied to the shielding/deshielding characteristics of electrons in some systems
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Anisotropy Aromatic hydrogens are in the deshielding region of the magnetic field generated by circulating electrons
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Typical chemical shifts
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Spin-spin coupling Magnetic field felt by a proton is affected by the spin states of nearby protons – either shielding or deshielding Case 1: neighboring single protons These H can either be the same or opposite spins – equal probability Makes doublets of two equal peaks at both absorptions
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NMR spectrum of dichloroacetaldehyde
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Coupling constants Separation between peaks is the “coupling constant”
Symbol: J Measured in Hz It is the same for both coupled protons
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Spin-spin coupling Case 2: Single proton next to a pair
Single proton splits the pair into a doublet Spin state possibilities for pair: Integration ratio: 1:2:1 Bo Equal energy
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Spin-spin coupling Single proton is split into a triplet
Any group of n protons will split its neighbors into n + 1 peaks Intensity follows Pascal’s triangle (Fibonacci series)
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Spin coupling example Chloroethane CH3CH2Cl
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Protons on Heteroatoms
Protons on N or O often give broad uncoupled peaks of uncertain chemical shift Protons on nitrogen are broad due to coupling with nitrogen nucleus (spin # = 1) Chemical shift can depend on concentration Peaks will be sharp and coupled if there is no acid or water present
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Protons on heteroatoms
Split into doublet by NH – reciprocal splitting is not seen Proton on nitrogen: broad due to interaction with nitrogen (spin number = 1)
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Phenolic Protons and Concentration
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Alcoholic protons and coupling
1H NMR spectrum of methanol at various temperatures
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Chemical Shift Differences and Coupling
Equivalent protons do not split each other Adjacent protons (“vicinal”) exhibit simple coupling if their chemical shifts are very different (/J >10) Designated an “AaXx” system (“AaMmXx” for three widely separated sets) Subscripts designate the number of protons involved
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Chemical Shift Differences and Coupling
Sets of protons close to each other are “AaBb” or “AaBbCc” The closer two sets are the more the peaks are distorted AX system becoming an AB system
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Chemical Shift Differences and Coupling
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AX system with some distortion
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Ternary systems AaMmXx systems exhibit simple splitting with two coupling constants
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Ternary Systems
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Ternary systems
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Chemical and magnetic equivalence
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Chemical and magnetic equivalence
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Chemical and magnetic equivalence
NMR spectrum of butane
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Chemical Shift Differences and Coupling
AaBbXx systems are approximately first order (simple splitting) AaBbCc systems are complex
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