12. Structure Determination: Mass Spectrometry and
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Transcript 12. Structure Determination: Mass Spectrometry and
12. Structure Determination:
Mass Spectrometry and
Infrared Spectroscopy
Based on McMurry’s Organic Chemistry, 7th edition
Determining the Structure of an
Organic Compound
The analysis of the outcome of a reaction requires
that we know the full structure of the products as well
as the reactants
In the 19th and early 20th centuries, structures were
determined by synthesis and chemical degradation
that related compounds to each other
Physical methods now permit structures to be
determined directly. We will examine:
mass spectrometry (MS)
infrared (IR) spectroscopy
nuclear magnetic resonance spectroscopy (NMR)
ultraviolet-visible spectroscopy (VIS)
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Why this Chapter?
Finding structures of new molecules
synthesized is critical
To get a good idea of the range of structural
techniques available and how they should be
used
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12.1 Mass Spectrometry of Small
Molecules:Magnetic-Sector Instruments
Measures molecular weight
Sample vaporized and subjected to bombardment by
electrons that remove an electron
Creates a cation radical
Bonds in cation radicals begin to break (fragment)
Charge to mass ratio is measured
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The Mass Spectrum
Plot mass of ions (m/z) (x-axis) versus the intensity of
the signal (roughly corresponding to the number of
ions) (y-axis)
Tallest peak is base peak (100%)
Other peaks listed as the % of that peak
Peak that corresponds to the unfragmented radical
cation is parent peak or molecular ion (M+)
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12.2 Interpreting Mass Spectra
Molecular weight from the mass of the molecular ion
Double-focusing instruments provide high-resolution
“exact mass”
0.0001 atomic mass units – distinguishing specific
atoms
Example MW “72” is ambiguous: C5H12 and C4H8O
but:
C5H12 72.0939 amu exact mass C4H8O 72.0575 amu
exact mass
Result from fractional mass differences of atoms 16O =
15.99491, 12C = 12.0000, 1H = 1.00783
Instruments include computation of formulas for each
peak
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Other Mass Spectral Features
If parent ion not present due to electron
bombardment causing breakdown, “softer” methods
such as chemical ionization are used
Peaks above the molecular weight appear as a result
of naturally occurring heavier isotopes in the sample
(M+1) from 13C that is randomly present
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Interpreting Mass-Spectral
Fragmentation Patterns
The way molecular ions break down can produce
characteristic fragments that help in identification
Serves as a “fingerprint” for comparison with
known materials in analysis (used in forensics)
Positive charge goes to fragments that best can
stabilize it
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Mass Spectral Fragmentation of
Hexane
Hexane (m/z = 86 for parent) has peaks at m/z = 71,
57, 43, 29
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12.3 Mass Spectrometry of Some
Common Functional Groups
Alcohols:
Alcohols undergo -cleavage (at the bond next
to the C-OH) as well as loss of H-OH to give
C=C
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Mass Spectral Cleavage of
Amines
Amines undergo -cleavage, generating
radicals
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Fragmentation of Carbonyl
Compounds
A C-H that is three atoms away leads to an internal
transfer of a proton to the C=O, called the McLafferty
rearrangement
Carbonyl compounds can also undergo cleavage
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12.4 Mass Spectrometry in Biological
Chemistry: Time-of-Flight (TOF)
Instruments
Most biochemical analyses by MS use:
- electrospray ionization (ESI)
- Matrix-assisted laser desorption ionization
(MALDI)
• Linked to a time-of-flight mass analyzer
(See figure 12.9)
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12.5 Spectroscopy and the
Electromagnetic Spectrum
Radiant energy is proportional to its frequency
(cycles/s = Hz) as a wave (Amplitude is its height)
Different types are classified by frequency or
wavelength ranges
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Absorption Spectra
Organic compound exposed to electromagnetic
radiation, can absorb energy of only certain
wavelengths (unit of energy)
Transmits energy of other wavelengths.
Changing wavelengths to determine which are
absorbed and which are transmitted produces an
absorption spectrum
Energy absorbed is distributed internally in a distinct
and reproducible way (See Figure 12-12)
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12.6 Infrared Spectroscopy
IR region lower energy than visible light (below red –
produces heating as with a heat lamp)
2.5 106 m to 2.5 105 m region used by organic
chemists for structural analysis
IR energy in a spectrum is usually measured as
wavenumber (cm-1), the inverse of wavelength and
proportional to frequency
Specific IR absorbed by organic molecule related to
its structure
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Infrared Energy Modes
IR energy absorption corresponds to specific modes,
corresponding to combinations of atomic movements,
such as bending and stretching of bonds between
groups of atoms called “normal modes”
Energy is characteristic of the atoms in the group and
their bonding
Corresponds to vibrations and rotations
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12.7 Interpreting Infrared Spectra
Most functional groups absorb at about the same
energy and intensity independent of the molecule
they are in
Characteristic higher energy IR absorptions in Table
12.1 can be used to confirm the existence of the
presence of a functional group in a molecule
IR spectrum has lower energy region characteristic of
molecule as a whole (“fingerprint” region)
See samples in Figure 12-14
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Regions of the Infrared Spectrum
4000-2500 cm-1 N-H,
C-H, O-H (stretching)
3300-3600 N-H, O-H
3000 C-H
2500-2000 cm-1 CC and C
N (stretching)
2000-1500 cm-1 double
bonds (stretching)
C=O 1680-1750
C=C 1640-1680 cm-1
Below 1500 cm-1
“fingerprint” region
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Differences in Infrared Absorptions
Molecules vibrate and rotate in normal modes, which
are combinations of motions (relates to force
constants)
Bond stretching dominates higher energy modes
Light objects connected to heavy objects vibrate
fastest: C-H, N-H, O-H
For two heavy atoms, stronger bond requires more
energy: C C, C N > C=C, C=O, C=N > C-C, C-O,
C-N, C-halogen
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12.8 Infrared Spectra of Some
Common Functional Groups
Alkanes, Alkenes, Alkynes
C-H, C-C, C=C, C
C have characteristic peaks
absence helps rule out C=C or C C
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IR: Aromatic Compounds
Weak C–H stretch at 3030 cm1
Weak absorptions 1660 - 2000 cm1 range
Medium-intensity absorptions 1450 to 1600 cm1
See spectrum of phenylacetylene, Figure 12.15
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IR: Alcohols and Amines
O–H 3400 to 3650 cm1
Usually broad and intense
N–H 3300 to 3500 cm1
Sharper and less intense than an O–H
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IR: Carbonyl Compounds
Strong, sharp C=O peak 1670 to 1780 cm1
Exact absorption characteristic of type of carbonyl
compound
1730 cm1 in saturated aldehydes
1705 cm1 in aldehydes next to double bond or
aromatic ring
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C=O in Ketones
1715 cm1 in six-membered ring and acyclic ketones
1750 cm1 in 5-membered ring ketones
1690 cm1 in ketones next to a double bond or an aromatic ring
C=O in Esters
1735 cm1 in saturated esters
1715 cm1 in esters next to aromatic ring or a double bond
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