Chapter 13 Flashcards

1
Q

Nuclear Magnetic Resonance (NMR) Spectroscpoy

A

a stectroscopic technique that gives information about the number and types of atoms in a molecule

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2
Q

nuclear spin states

A
  • an electron has a spin quantum number of 1/2 (can be +1/2 or -1/2)
  • a moving charge has an associated magnetic field
  • nuclei need multiple spin states to be NMR active, which include those with an odd mass and /or atomic number
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3
Q

orientation of nuclear spin in an applied magnetic field

A
  • placing nuclei in a strong magnetic field aligns their molecular spin with (+1/2 = lower energy) and against (-1/2 =higher energy) the field
  • the difference in energy between these states is on the order of radio waves and is of the magnet
  • stronger magnets have greater sensitivity and require higher radio frequency
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4
Q

nuclear magnetic resonance

A
  • irradiating the nuclei with a radio frequency equal to the difference in energy between the spin states excites the spin from +1/2 to -1/2
  • upon return to the ground state, the nuclei emit radio waves equal in energy to that absorbed, which is measured and recorded as signal
  • a nucleus is in resonance when absorption occurs
  • an applied magnetic field causes electrons to circulate, and the orientation of this field dictates the direction of circulation
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5
Q

deshielding

A

electron density circulation adds to the applied magnetic field, thus requiring higher energy to cause resonance

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6
Q

chemical shift

A

the difference in resonance frequencies caused by shielding/deshielding of nuclei

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7
Q

NMR Spectrometer

A

-NMR samples are prepared by dissolving the compound of interest in a deuterated solvent, to avoid H resonances from the solvent that would saturate the signal

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8
Q

equivalent hydrogens

A

hydrogens that have the same chemical environment, and thus show up as a single signal in H-NMR

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9
Q

rules to determine equivalency

A
  1. bonded to the same sp3 hybridized carbon that can rotate freely
  2. a plane or point of symmetry in a molecule exists and hydrogens equidistant from the plane or point are the same
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10
Q

signal area

A
  • the area under the signal is proportional to the number of equivalent hydrogens giving rise to that signal
  • integrating the peaks in a H-NMR spectrum tells you the relative number of hydrogens represented by each peak
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11
Q

chemical shift

A
  • incredibly valuable in determining structure since the “electronic environment” around the H influences its chemical shift
  • influenced by electronegativity, hybridization of nearby atoms, and magnetic induction within an adjacent pi bond
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12
Q

electronegativity of nearby atoms

A

-EN atoms pull electron density away from atoms bonded to it, thus deshielding them, and causing a downfield shift in resonance

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13
Q

hybridization of adjacent atoms

A

-more s character for sp2 and sp hybridized carbon than sp3, making it more EN

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14
Q

diamagnetic effects from pi-Bonds

A

-shielding vs. E.N=> “deshielding”

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15
Q

ring current

A

circulation of pi-electrons on an aromatic ring under an applied magnetic field
-this current induces a strong magnetic field that opposes the applied field in the middle of the ring, but reinforces it outside the ring

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16
Q

signal splitting

A

spin-spin coupling with adjacent nuclei split NMR signals depending on the extent of coupling and the number of adjacent nuclei

17
Q

(n+1) rule

A

if a hydrogen has n hydrogens nonequivalent to it, but equivalent among themselves on the same or adjacent atoms, its H-NMR signal is split into (n=1) peaks
-for molecules that can freely rotate, sp3 hybridized, the rule simplifies to m+n+1 peaks

18
Q

vicinal coupling

A

spin-spin coupling involving the H atoms on two C atoms that are bonded to each other

19
Q

germinal coupling

A

spin-spin coupling that occurs between nonequivalent H atoms bonded to the same C atom (often due to restricted bond rotation, such as on a terminal double bond

20
Q

13C-NMR

A
  • 13C-NMR active, and 13C has a natural abundance of 1%
  • (n+1) rule applies, but splitting is not observed due to the nearly negligible probability of two 13C isotopes being adjacent to each other in a molecule
  • 1H will split 13C signals resulting in complex splitting patterns, which is why H signals are decoupled and no splitting is observed, resulting in relative clear spectra