Mass Spectrometry and Infrared Spectroscopy

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Transcript Mass Spectrometry and Infrared Spectroscopy

John E. McMurry
Chapter 12
Structure Determination: Mass
Spectrometry and Infrared
Paul D. Adams • University of Arkansas
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
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
The Mass Spectrum
Plot mass of ions (m/z) (x-axis) versus the intensity of the
signal (roughly corresponding to the number of ions) (yaxis)
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+)
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
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
Mass Spectral Fragmentation of
Hexane (m/z = 86 for parent) has peaks at m/z = 71, 57,
43, 29
12.3 Mass Spectrometry of Some
Common Functional Groups
 Alcohols undergo -cleavage (at the bond next to the COH) as well as loss of H-OH to give C=C
Mass Spectral Cleavage of
Amines undergo -cleavage, generating
Fragmentation of Carbonyl
A C-H that is three atoms away leads to an internal
transfer of a proton to the C=O, called the McLafferty
Carbonyl compounds can also undergo  cleavage
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
Absorption Spectra
An 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
12.6 Infrared Spectroscopy
IR region lower energy than visible light (below red –
produces heating as with a heat lamp)
IR energy in a spectrum is usually measured as
wavenumber (cm-1), the inverse of wavelength and
proportional to frequency
Specific IR absorbed by an organic molecule is related to
its structure
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”
Corresponds to vibrations and rotations
12.7 Interpreting Infrared
Most functional groups absorb at about the same energy
and intensity independent of the molecule they are in
IR spectrum has lower energy region characteristic of
molecule as a whole (“fingerprint” region)
Figure 12.14
Regions of the Infrared
4000-2500 cm-1 N-H,
C-H, O-H (stretching)
3300-3600 N-H, O-H
3000 C-H
2500-2000 cm-1 CC 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
Differences in Infrared
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
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
IR: Aromatic Compounds
Weak C–H stretch at 3030 cm1
Weak absorptions 1660 - 2000 cm1 range
Medium-intensity absorptions 1450 to 1600 cm1
See spectrum of phenylacetylene, Figure 12.15
IR: Alcohols and Amines
O–H 3400 to 3650 cm1
 Usually broad and intense
N–H 3300 to 3500 cm1
 Sharper and less intense than an O–H
IR: Carbonyl Compounds
Strong, sharp C=O peak 1670 to 1780 cm1
Exact absorption characteristic of type of carbonyl
 1730 cm1 in saturated aldehydes
 1705 cm1 in aldehydes next to double bond or
aromatic ring
C=O in Ketones
1715 cm1 in six-membered ring and acyclic ketones
1750 cm1 in 5-membered ring ketones
1690 cm1 in ketones next to a double bond or an aromatic ring
C=O in Esters
1735 cm1 in saturated esters
1715 cm1 in esters next to aromatic ring or a double bond
Let’s Work a Problem
Propose structures for a compound that fits the
following data: It is an alcohol with M+ = 88 and
fragments at m/z = 73, m/z = 70, and m/z = 59
Answer: We must first decide on the the formula of an alcohol that could
undergo this type of fragmentation via mass spectrometry. We know
that an alcohol possesses an O atom (MW=16), so that leads us to the
formula C5H12O for an alcohol with M+ = 88, with a structure of:
One fragmentation peak at 70 is due to the loss of water, and alpha
cleavage can result in m/z of 73 and 59.