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Nuclear Magnetic Resonance (NMR). for beginners. 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 ( 13 C NMR) or (rarely) other elements. Spin States.
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Nuclear Magnetic Resonance (NMR) for beginners
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
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
Spin States • In the absence of a magnetic field the spin states are degenerate • The “spinning” nucleus generates its own magnetic field
Spin States • In a magnetic field the states have different energies B’ B’ Bo
Spin states in a magnetic field • Energy difference linearly depends on field strength = magnetic moment of H (2.7927N or +14.106067x10-27J/T)
Spin states in a magnetic field • Even in a very large field (1-20T) the energy difference is small (~0.1cal/mol)
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 60-500MHz)
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
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
Sample must be spun to average out magnetic field inhomogeneity
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
NMR data collection CW NMR of isopropanol
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
Chemical shift • Protons in different environments absorb at different field strengths (for the same frequency) • Different environment = different electron density around the H
Chemical shift positions High field, shielded Low field, deshielded PPM of applied field () from reference Reference (tetramethylsilane)
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
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
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
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
Anisotropy • “Anisotropy”: any characteristic that varies with direction (asymmetric) • Applied to the shielding/deshielding characteristics of electrons in some systems
Anisotropy • Aromatic hydrogens are in the deshielding region of the magnetic field generated by circulating electrons
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
Coupling constants • Separation between peaks is the “coupling constant” • Symbol: J • Measured in Hz • It is the same for both coupled protons
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
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)
Spin coupling example • Chloroethane CH3CH2Cl
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
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)
Alcoholic protons and coupling 1H NMR spectrum of methanol at various temperatures
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
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
Ternary systems • AaMmXx systems exhibit simple splitting with two coupling constants
Chemical and magnetic equivalence NMR spectrum of butane