Chapter 3 Infrared Spectroscopy Each interatomic bond may vibrate in several different motions...

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Chapter 3 Infrared Spectroscopy Each interatomic bond may vibrate in several different motions (stretching or bending) - vibrational, rotational energy level Absorption of radiation by a typical organic molecule results in the excita tion of vibrational, rotational and be nding modes would be between 0.75 – 20 0 μ, or infrared region

Transcript of Chapter 3 Infrared Spectroscopy Each interatomic bond may vibrate in several different motions...

Page 1: Chapter 3 Infrared Spectroscopy Each interatomic bond may vibrate in several different motions (stretching or bending) - vibrational, rotational energy.

Chapter 3 Infrared Spectroscopy

Each interatomic bond may vibrate in several different motions (stretching or bending) - vibrational, rotational energy level

Absorption of radiation by a typical organic molecule results in the excitation of vibrational, rotational and bending modes would be between 0.75 – 200 μ, or infrared region

Page 2: Chapter 3 Infrared Spectroscopy Each interatomic bond may vibrate in several different motions (stretching or bending) - vibrational, rotational energy.

IR Theory & Principles• IR energy lower than visible

Page 3: Chapter 3 Infrared Spectroscopy Each interatomic bond may vibrate in several different motions (stretching or bending) - vibrational, rotational energy.

Infrared Region

Near IR 0.75 ~ 2.5 μ (12820 – 4000 cm-1)

reciprocal centimeters, cycle per cm,

wavenumber

IR 2.5 ~ 25 μ (4000 – 400 cm-1 )

Useful region for organic analysis

Far IR 25 ~ 1000 μ (400 – 10 cm-1 )

Page 4: Chapter 3 Infrared Spectroscopy Each interatomic bond may vibrate in several different motions (stretching or bending) - vibrational, rotational energy.
Page 5: Chapter 3 Infrared Spectroscopy Each interatomic bond may vibrate in several different motions (stretching or bending) - vibrational, rotational energy.

•Infrared energy absorbed as vibrations of polar molecules (thermal energy) when sample is placed in IR beam -

Page 6: Chapter 3 Infrared Spectroscopy Each interatomic bond may vibrate in several different motions (stretching or bending) - vibrational, rotational energy.

•Vibration frequencies are quantized and depend on atom masses, bond strengths, and change in dipole.

Page 7: Chapter 3 Infrared Spectroscopy Each interatomic bond may vibrate in several different motions (stretching or bending) - vibrational, rotational energy.

StretchingBending

TwistingWaggingRocking

VibrationMotions

can be SymmetricAsymmetric

can be

Page 8: Chapter 3 Infrared Spectroscopy Each interatomic bond may vibrate in several different motions (stretching or bending) - vibrational, rotational energy.
Page 9: Chapter 3 Infrared Spectroscopy Each interatomic bond may vibrate in several different motions (stretching or bending) - vibrational, rotational energy.

•Spectrum is transmission of IR light plotted against frequency in wavenumbers (cm-1).

Page 10: Chapter 3 Infrared Spectroscopy Each interatomic bond may vibrate in several different motions (stretching or bending) - vibrational, rotational energy.

Structural Information from IR

• Good for confirming certain functional groups - especially: -O-H C=O -CN and CC

• Not good for carbon backbone.• Intensities vary so not normally quantitative. electronegativity, vibration mode, conjugation, etc• NOT GREAT FOR FIGURING OUT STRUCTURE• USED FOR VERIFYING OR ELIMINATING POSSIBLE STR

UCTURES.

Page 11: Chapter 3 Infrared Spectroscopy Each interatomic bond may vibrate in several different motions (stretching or bending) - vibrational, rotational energy.
Page 12: Chapter 3 Infrared Spectroscopy Each interatomic bond may vibrate in several different motions (stretching or bending) - vibrational, rotational energy.
Page 13: Chapter 3 Infrared Spectroscopy Each interatomic bond may vibrate in several different motions (stretching or bending) - vibrational, rotational energy.

IR Interpretation Chart

Page 14: Chapter 3 Infrared Spectroscopy Each interatomic bond may vibrate in several different motions (stretching or bending) - vibrational, rotational energy.

2.2 Structural Group Analysis

• Extensive correlations exist between absorption peak positions and structural units of organic molecules

stretching (υ) and bending (δ, γ)

Page 15: Chapter 3 Infrared Spectroscopy Each interatomic bond may vibrate in several different motions (stretching or bending) - vibrational, rotational energy.

Alkanes (1)

• The most prominent peaks in IR spectra of saturated hydrocarbons are due to C-H stretching and bending.

1. υ C-H appears in 2975 to 2845 cm-1 regions, it’s due to symmetric and asymmetric stretching vibration of CH3, CH2 and CH groups. They can be applied to identify alkanes (< 3000 cm-1 ) from unsaturated compounds

Page 16: Chapter 3 Infrared Spectroscopy Each interatomic bond may vibrate in several different motions (stretching or bending) - vibrational, rotational energy.
Page 17: Chapter 3 Infrared Spectroscopy Each interatomic bond may vibrate in several different motions (stretching or bending) - vibrational, rotational energy.

Alkanes (2)

2. δC-H appears in ~1460 and ~1380 cm-1. The first one is attribute to δas of CH3 and CH2, the later is due to δ s of C-H of CH3. δ s is an evidence of the existence of CH3 in unknown compound.

The exact positions of these as well as the stretching frequencies depend upon the nature of adjacent atoms.

Page 18: Chapter 3 Infrared Spectroscopy Each interatomic bond may vibrate in several different motions (stretching or bending) - vibrational, rotational energy.
Page 19: Chapter 3 Infrared Spectroscopy Each interatomic bond may vibrate in several different motions (stretching or bending) - vibrational, rotational energy.

Alkanes (3)

• υ c-c are within 1250 ~ 800 cm-1, and are weak peaks. Usually they are not specific for compounds and can not be used in IR analysis.

Page 20: Chapter 3 Infrared Spectroscopy Each interatomic bond may vibrate in several different motions (stretching or bending) - vibrational, rotational energy.

Alkenes (1)

• The big difference of IR spectra between alkanes and alkenes are due to the vibration of =C-H and C-C. The specific peaks of Olefin are:

1. υ C=C-H generally appear in the region 3100 to 3000 cm-1, thus differentiating saturated and unsaturated hydrocarbons.

Page 21: Chapter 3 Infrared Spectroscopy Each interatomic bond may vibrate in several different motions (stretching or bending) - vibrational, rotational energy.
Page 22: Chapter 3 Infrared Spectroscopy Each interatomic bond may vibrate in several different motions (stretching or bending) - vibrational, rotational energy.

Alkenes (2)

2. The out-of-plane bending vibrations in the 1000 to 650 cm-1 region γC=C-H are often useful in predicting the substitution pattern of the double bond.

Page 23: Chapter 3 Infrared Spectroscopy Each interatomic bond may vibrate in several different motions (stretching or bending) - vibrational, rotational energy.

Olefinic C-H out-of-plane bending frequencies

Olefin Frequency range (cm-1 )

R-CH=CH2 1000-960 and 940-900

R2C=CH2 915-870

Trans-RCH=CHR 990-940

cis-RCH=CHR 790-650

R2C=CHR 850-790

Page 24: Chapter 3 Infrared Spectroscopy Each interatomic bond may vibrate in several different motions (stretching or bending) - vibrational, rotational energy.
Page 25: Chapter 3 Infrared Spectroscopy Each interatomic bond may vibrate in several different motions (stretching or bending) - vibrational, rotational energy.

Alkenes (3)

3. The C=C stretching frequency υC=C in the 1600 to 1675 cm-1 region also varies with substitution but to a lesser degree

Page 26: Chapter 3 Infrared Spectroscopy Each interatomic bond may vibrate in several different motions (stretching or bending) - vibrational, rotational energy.
Page 27: Chapter 3 Infrared Spectroscopy Each interatomic bond may vibrate in several different motions (stretching or bending) - vibrational, rotational energy.
Page 28: Chapter 3 Infrared Spectroscopy Each interatomic bond may vibrate in several different motions (stretching or bending) - vibrational, rotational energy.

Alkynes (1)

• It’s not difficult to distinguish alkynes from IR spectra based on the following specific band:

1. The C-H stretching vibration of terminal acetyenes (νC≡C-H )generally appears at 3300 to 3100 cm-1 as a strong sharp band.

The peak of νN-H is also in this region, but can be recognized with its broad band

Page 29: Chapter 3 Infrared Spectroscopy Each interatomic bond may vibrate in several different motions (stretching or bending) - vibrational, rotational energy.
Page 30: Chapter 3 Infrared Spectroscopy Each interatomic bond may vibrate in several different motions (stretching or bending) - vibrational, rotational energy.

Alkynes (2)

2. The C≡C stretching band is found in the region 2150 to 2100 cm-1 if the alkyne is monosubstituted and at 2270 to 2150 cm-1 if disubstituted. The latter are usually quite weak absorptions

Page 31: Chapter 3 Infrared Spectroscopy Each interatomic bond may vibrate in several different motions (stretching or bending) - vibrational, rotational energy.
Page 32: Chapter 3 Infrared Spectroscopy Each interatomic bond may vibrate in several different motions (stretching or bending) - vibrational, rotational energy.

Alkynes (3)

• The C≡C-H out-of-plane bending vibration (γC≡C-H ) is found in the region 680 to 610 cm-1

Page 33: Chapter 3 Infrared Spectroscopy Each interatomic bond may vibrate in several different motions (stretching or bending) - vibrational, rotational energy.

Aromatic compounds (1)

1. Aromatic C-H stretching absorption appears in the region 3100-3000 cm-1, close to that of olefinic C-H stretching

2. Aromatic C-H out-of-plane bending bands ( γC=C-

H)in the 900 to 690 cm-1 region are reasonably well determined by the substitution pattern of the benzene ring as indicated. These strong, usually sharp bands can be used in distinguishing positional isomers of substituted benzenes.

Page 34: Chapter 3 Infrared Spectroscopy Each interatomic bond may vibrate in several different motions (stretching or bending) - vibrational, rotational energy.

Aromatic γC=C-H Frequencies

Substitution Frequency range (cm-1 )

mono 775-730 and 710-690

1,2-di 765-730

1,3-di 800-750 and 710-690

1,4-di 840-800

1,2,3-tri 800-760 and 740-700

1,2,4-tri 880-860 and 820-800

Page 35: Chapter 3 Infrared Spectroscopy Each interatomic bond may vibrate in several different motions (stretching or bending) - vibrational, rotational energy.
Page 36: Chapter 3 Infrared Spectroscopy Each interatomic bond may vibrate in several different motions (stretching or bending) - vibrational, rotational energy.

Aromatic compounds (2)

3. Sharp peaks at ~1600 and ~1500 cm-1 are very characteristic of all benzenoid compounds; a band at 1580 cm-1 appears when the ring is conjugated with a substituent.

Page 37: Chapter 3 Infrared Spectroscopy Each interatomic bond may vibrate in several different motions (stretching or bending) - vibrational, rotational energy.
Page 38: Chapter 3 Infrared Spectroscopy Each interatomic bond may vibrate in several different motions (stretching or bending) - vibrational, rotational energy.
Page 39: Chapter 3 Infrared Spectroscopy Each interatomic bond may vibrate in several different motions (stretching or bending) - vibrational, rotational energy.

Alcohols and phenols (1)

1. The very characteristic infrared band due to O-H stretching appears at 3650 to 3600 cm-1 in dilute solution. In spectra of neat liquids or solids intermolecular hydrogen banding broadens the band and shifts its position to lower frequency (3500 – 3200 cm-1 )

Page 40: Chapter 3 Infrared Spectroscopy Each interatomic bond may vibrate in several different motions (stretching or bending) - vibrational, rotational energy.
Page 41: Chapter 3 Infrared Spectroscopy Each interatomic bond may vibrate in several different motions (stretching or bending) - vibrational, rotational energy.

Alcohols and phenols (2)

2. Strong bands due to O-H bending and C-O stretching are observed at 1500 to 1300 cm-1 and 1220 to 1000 cm-1 , respectively. In simple alcohols and phenols the exact position of the latter is useful in classification of the hydroxyl group.

Phenol 1230 cm-1 tertiary 1200 cm-1 secondary 1125 cm-1 primary 1050 cm-1

Page 42: Chapter 3 Infrared Spectroscopy Each interatomic bond may vibrate in several different motions (stretching or bending) - vibrational, rotational energy.
Page 43: Chapter 3 Infrared Spectroscopy Each interatomic bond may vibrate in several different motions (stretching or bending) - vibrational, rotational energy.
Page 44: Chapter 3 Infrared Spectroscopy Each interatomic bond may vibrate in several different motions (stretching or bending) - vibrational, rotational energy.

Ether

• The asymmetric C-O stretching absorption of ethers appears in the region 1280 to 1050 cm-1 . As in alcohols, the exact position of this strong peak is dependent on the nature of the attached groups. Phenol and enol ethers generally absorb at 1275 to 1200 cm-1 , dialkyl ethers at 1150 to 1050 cm-1 . Alcohols, acids, esters may interfere the identification.

Page 45: Chapter 3 Infrared Spectroscopy Each interatomic bond may vibrate in several different motions (stretching or bending) - vibrational, rotational energy.
Page 46: Chapter 3 Infrared Spectroscopy Each interatomic bond may vibrate in several different motions (stretching or bending) - vibrational, rotational energy.

Aldehydes and Ketones

• The C=O stretching frequencies of saturated aldehydes and acyclic ketones are observed at 1735 to 1710 cm-1 and 1720 to 1700 cm-1 , respectively. Aldehydes are also recognizable by the C-H stretching vibration which appears as two peaks in the 2850 to 2700 cm-

1 region.

Page 47: Chapter 3 Infrared Spectroscopy Each interatomic bond may vibrate in several different motions (stretching or bending) - vibrational, rotational energy.
Page 48: Chapter 3 Infrared Spectroscopy Each interatomic bond may vibrate in several different motions (stretching or bending) - vibrational, rotational energy.
Page 49: Chapter 3 Infrared Spectroscopy Each interatomic bond may vibrate in several different motions (stretching or bending) - vibrational, rotational energy.

Carboxylic acids

• The most characteristic absorption of carboxylic acids is a broad peak extending from 3300 to 2500 cm-1 due largely to hydrogen bonded O-H stretching. The C-H stretching vibrations appear as small peaks on top of this band.

• The C=O stretching band appears from 1725 to 1700 cm-1 and is shifted to 1690~1680 cm-1 by adjacent unsaturation. It’s a strong band.

Page 50: Chapter 3 Infrared Spectroscopy Each interatomic bond may vibrate in several different motions (stretching or bending) - vibrational, rotational energy.

Carboxylic acids

• C-O stretching band appears from 1440~1395 cm-1 , and usually weak peak.

Page 51: Chapter 3 Infrared Spectroscopy Each interatomic bond may vibrate in several different motions (stretching or bending) - vibrational, rotational energy.
Page 52: Chapter 3 Infrared Spectroscopy Each interatomic bond may vibrate in several different motions (stretching or bending) - vibrational, rotational energy.

Carboxylic esters

• Saturated ester carbonyl stretching is observed at 1740 to 1720 cm-1. Unsaturation adjacent to the carbonyl group lowers the frequency by 10 to 15 cm-1 .

• The C-O-C stretching of esters appears as two bands in the 1280 to 1050 cm-1 region. The asymmetric stretching peak at 1289 to 1150 cm-1 is usually strong.

Page 53: Chapter 3 Infrared Spectroscopy Each interatomic bond may vibrate in several different motions (stretching or bending) - vibrational, rotational energy.
Page 54: Chapter 3 Infrared Spectroscopy Each interatomic bond may vibrate in several different motions (stretching or bending) - vibrational, rotational energy.

Anhydrieds

• Acid anhydrides are readily recognized by the presence of two high frequency (1830 to 1800 cm-1 and 1775 to 1740 cm-1 carbonyl absorptions. As with other carbonyl stretching vibrations, the frequency is increased by incorporating the group in a ring and decreased by adjacent unsaturation. Cylic anhydrides differ from acyclic anhydrides also in that the lower frequency band is stronger in the former, while the reverse is true of the latter.

Page 55: Chapter 3 Infrared Spectroscopy Each interatomic bond may vibrate in several different motions (stretching or bending) - vibrational, rotational energy.

Amines (1)

• Primary and secondary amines show N-H stretching vibrations in the 3500 to 3300 cm-1 region. Primary amines generally have two bands approximately 70 cm-1 apart due to asymmetric and symmetric stretching modes. Secondary amines show only one band. Inter- or intramolecular hydrogen bonding broadens the absorptions and lowers the frequency.

Page 56: Chapter 3 Infrared Spectroscopy Each interatomic bond may vibrate in several different motions (stretching or bending) - vibrational, rotational energy.

Amines (2)

• In general the intensities of N-H bands are less than of O-H bands. The N-H bending and C-N stretching absorptions are not as strong as the corresponding alcohol bands and occur at approximately 100 cm-1 higher frequencies

Page 57: Chapter 3 Infrared Spectroscopy Each interatomic bond may vibrate in several different motions (stretching or bending) - vibrational, rotational energy.

Amines (3)

• In addition, NH2 groups give an additional broad band at 900 to 700 cm-1 due to out-of-plane bending

Page 58: Chapter 3 Infrared Spectroscopy Each interatomic bond may vibrate in several different motions (stretching or bending) - vibrational, rotational energy.
Page 59: Chapter 3 Infrared Spectroscopy Each interatomic bond may vibrate in several different motions (stretching or bending) - vibrational, rotational energy.

Amides

• Amide carbonyl stretching is observed in the 1670 to 1640 cm-1 region. In contrast to other carbonyl groups, both adjacent unsaturation and ring formation cause the absorption to shift to higher frequencies. Primary and secondary amides also show N-H stretching at 3500 to 3100 cm-1 and N-H bending at 1640 to 1550 cm-1

Page 60: Chapter 3 Infrared Spectroscopy Each interatomic bond may vibrate in several different motions (stretching or bending) - vibrational, rotational energy.

Analysis procedure

• Qualitative analysis

Compare with standard

Database:

Sadtler, Catalog of Infrared Standard Spectra;

Documentation of Molecular Spectroscopy;

American Petroleum Institute Infrared Spectral Data;

IR Data Committee

Page 61: Chapter 3 Infrared Spectroscopy Each interatomic bond may vibrate in several different motions (stretching or bending) - vibrational, rotational energy.

Degree of unsaturation

Page 62: Chapter 3 Infrared Spectroscopy Each interatomic bond may vibrate in several different motions (stretching or bending) - vibrational, rotational energy.

Interpretation of IR spectra

Page 63: Chapter 3 Infrared Spectroscopy Each interatomic bond may vibrate in several different motions (stretching or bending) - vibrational, rotational energy.

2.3 Interpretation of IR Spectra

Page 64: Chapter 3 Infrared Spectroscopy Each interatomic bond may vibrate in several different motions (stretching or bending) - vibrational, rotational energy.

2.3 Interpretation of IR Spectra

• The 7 important region of IR spectra

1. Most organic compounds are composed of C, H, O and N.

2. Most chemical groups have specific absorption with 4000 – 670 cm-1 . This region can be divided into 7 regions as:

Page 65: Chapter 3 Infrared Spectroscopy Each interatomic bond may vibrate in several different motions (stretching or bending) - vibrational, rotational energy.

7 important region

No. Wavenumber Bond and vibration

1 3750 ~ 3300 νO-H, νN-H

2 3300 ~ 3000 νC-H (-C≡C-H, >C=C-H, Ar-H)

3000 ~ 2700 νC-H(CH3, CH2, CH, CHO)

3 2400 ~ 2100 νC ≡C, νC ≡N

4 1900 ~ 1650 νC=O

5 1675 ~ 1500 νC=C, νC=N

6 1475 ~ 1000 δCH, ν C-O, ν C-C

7 1000 ~ 650 γC=C-H, Ar-H, γ CH2

Page 66: Chapter 3 Infrared Spectroscopy Each interatomic bond may vibrate in several different motions (stretching or bending) - vibrational, rotational energy.

Interpretation (part 1)O-H, N-H stretching (3750-3000

cm-1 )• νO-H at 3700-3200 cm-1 is an important evide

nce of the existence of OH

• Free OH group (dilute CCl4 solution) shows sharp peak. H-bond and intermolecular association broad and lower the wavenumbers (3450-3200 cm-1 )

Page 67: Chapter 3 Infrared Spectroscopy Each interatomic bond may vibrate in several different motions (stretching or bending) - vibrational, rotational energy.
Page 68: Chapter 3 Infrared Spectroscopy Each interatomic bond may vibrate in several different motions (stretching or bending) - vibrational, rotational energy.

Interpretation 1

• The peak numbers of νN-H depend on the number of substituents of N atom. Primary amines and primary amides have two peaks with almost the same strength. Amide can be distinguished by the strong νC=O peak around 1600 cm-1

Page 69: Chapter 3 Infrared Spectroscopy Each interatomic bond may vibrate in several different motions (stretching or bending) - vibrational, rotational energy.
Page 70: Chapter 3 Infrared Spectroscopy Each interatomic bond may vibrate in several different motions (stretching or bending) - vibrational, rotational energy.

Interpretation 1

• Secondary amines and amides have only one weak νN-H peak at 3500 –3100 cm-1 . Secondary aromatic amines have strong absorption at 3450 –3490 cm-1 .

• No peak for tertiary amines and amides in the corresponding νN-H region.

IR is a simple way to distinguish primary, secondary and tertiary amines and amides

Page 71: Chapter 3 Infrared Spectroscopy Each interatomic bond may vibrate in several different motions (stretching or bending) - vibrational, rotational energy.

Interpretation (part 2)C-H stretching (3300-2700)

• Distinguish saturated hydrocarbons from unsaturated

• Alkynes,

• aromatic (3030 cm-1 , weak and sharp)

Page 72: Chapter 3 Infrared Spectroscopy Each interatomic bond may vibrate in several different motions (stretching or bending) - vibrational, rotational energy.
Page 73: Chapter 3 Infrared Spectroscopy Each interatomic bond may vibrate in several different motions (stretching or bending) - vibrational, rotational energy.

Interpretation (2)

• Besides the C=O stretching frequencies of saturated aldehydes at 1735 to 1710 cm-

1,Aldehydes are also recognizable by the C-H stretching vibration which appears as two peaks in the 2850 to 2700 cm-1 region.

Page 74: Chapter 3 Infrared Spectroscopy Each interatomic bond may vibrate in several different motions (stretching or bending) - vibrational, rotational energy.

Interpretation (part 3)C ≡ C, C ≡ N etc. 2400-2100

Page 75: Chapter 3 Infrared Spectroscopy Each interatomic bond may vibrate in several different motions (stretching or bending) - vibrational, rotational energy.

Interpretation (part 4)C=O (1900-1650 cm-1 )

• The C=O stretching band (1755-1670 cm-1) is a very strong peak, it can be a good evidence for the existence of C=O groups in the unknown compound.

• The adjacent group may affect the position of υC=O

Page 76: Chapter 3 Infrared Spectroscopy Each interatomic bond may vibrate in several different motions (stretching or bending) - vibrational, rotational energy.
Page 77: Chapter 3 Infrared Spectroscopy Each interatomic bond may vibrate in several different motions (stretching or bending) - vibrational, rotational energy.

Interpretation (part 5)Double bond stretching (1690-1500 cm-

1 )• Stretching vibration of C=C, C=N, N=N, N

=O and C=C of benzene ring

• Usually weak peak. Asymmetric structure enhances the absorption

• Sharp peaks at ~1600 and ~1500 cm-1 are very characteristic of all benzenoid compounds;

Page 78: Chapter 3 Infrared Spectroscopy Each interatomic bond may vibrate in several different motions (stretching or bending) - vibrational, rotational energy.
Page 79: Chapter 3 Infrared Spectroscopy Each interatomic bond may vibrate in several different motions (stretching or bending) - vibrational, rotational energy.
Page 80: Chapter 3 Infrared Spectroscopy Each interatomic bond may vibrate in several different motions (stretching or bending) - vibrational, rotational energy.

Interpretation (part 5)

• Besides, δNH2 of amines are also in this region. Primary amine 1650 – 1580 (m-s) with a broad peak at 900-650 cm-1. (maybe interfered with the peaks of aromatic ring). There isn’t any peaks for secondary peaks.

• Primary amide δNH2 at 1640-1600 cm-1 is a strong and sharp peak(1/3-1/2 of C=O). Secondary amide δNH2 at 1550-1530 cm-1

Page 81: Chapter 3 Infrared Spectroscopy Each interatomic bond may vibrate in several different motions (stretching or bending) - vibrational, rotational energy.

Interpretation (part 6)X-H and X-Y (1475-1000 cm-1 )

• The absorption bands include C-H in plane bending, stretching vibration of C-O and C-X, and C-C vibration

Page 82: Chapter 3 Infrared Spectroscopy Each interatomic bond may vibrate in several different motions (stretching or bending) - vibrational, rotational energy.
Page 83: Chapter 3 Infrared Spectroscopy Each interatomic bond may vibrate in several different motions (stretching or bending) - vibrational, rotational energy.

Interpretation

• 1460 cm-1 is the specific peak for CH3 and CH2

• Can be identified with the peak at 1380 cm-1 • 1380 cm-1 peak can split into 2 peaks with same str

ength.

Example: isopropyl group has two peaks at 1389-1381 and 1372-1368 cm-1. It can be verified with C-C stretching of isopropyl at 1170 and 1150 cm-1 dual peaks

Page 84: Chapter 3 Infrared Spectroscopy Each interatomic bond may vibrate in several different motions (stretching or bending) - vibrational, rotational energy.
Page 85: Chapter 3 Infrared Spectroscopy Each interatomic bond may vibrate in several different motions (stretching or bending) - vibrational, rotational energy.

Interpretation

• δs(C-H) of tert-butyl group splits into 1401-1395 and 1374-1360 cm-1. The low frequency peak is stronger than the former one

Page 86: Chapter 3 Infrared Spectroscopy Each interatomic bond may vibrate in several different motions (stretching or bending) - vibrational, rotational energy.
Page 87: Chapter 3 Infrared Spectroscopy Each interatomic bond may vibrate in several different motions (stretching or bending) - vibrational, rotational energy.

Interpretation

• The strong stretching vibration peak of C-O appears in the spectra of alcohol, ether and ester as an evidence of OH group

• Alcohol: 1410-1050 cm-1, reflect the structure of alcohols.

• Ether: 1250-1100 cm-1

• Ester: most of them 1200-1190 cm-1

Page 88: Chapter 3 Infrared Spectroscopy Each interatomic bond may vibrate in several different motions (stretching or bending) - vibrational, rotational energy.

Interpretation (part 7)C-H out-of-plane bending(1000-650 cm-1 )

• Mainly of γC-H of alkenes and aromatic compounds

Page 89: Chapter 3 Infrared Spectroscopy Each interatomic bond may vibrate in several different motions (stretching or bending) - vibrational, rotational energy.

Aromatic compound

• Two bands were applied to identify the structure of aromatic compound: 900-650 cm-1 (γC-H ) and 2000-1660 cm-1 (υC=C)

Page 90: Chapter 3 Infrared Spectroscopy Each interatomic bond may vibrate in several different motions (stretching or bending) - vibrational, rotational energy.
Page 91: Chapter 3 Infrared Spectroscopy Each interatomic bond may vibrate in several different motions (stretching or bending) - vibrational, rotational energy.
Page 92: Chapter 3 Infrared Spectroscopy Each interatomic bond may vibrate in several different motions (stretching or bending) - vibrational, rotational energy.

Aromatic compound

• The absorption bands at 900-650 cm-1 are strong and specific for substitution structure of aromatic. They can also be used for quantitation.

Page 93: Chapter 3 Infrared Spectroscopy Each interatomic bond may vibrate in several different motions (stretching or bending) - vibrational, rotational energy.

Example

Page 94: Chapter 3 Infrared Spectroscopy Each interatomic bond may vibrate in several different motions (stretching or bending) - vibrational, rotational energy.
Page 95: Chapter 3 Infrared Spectroscopy Each interatomic bond may vibrate in several different motions (stretching or bending) - vibrational, rotational energy.
Page 96: Chapter 3 Infrared Spectroscopy Each interatomic bond may vibrate in several different motions (stretching or bending) - vibrational, rotational energy.
Page 97: Chapter 3 Infrared Spectroscopy Each interatomic bond may vibrate in several different motions (stretching or bending) - vibrational, rotational energy.

C8H10O

Page 98: Chapter 3 Infrared Spectroscopy Each interatomic bond may vibrate in several different motions (stretching or bending) - vibrational, rotational energy.

C12H26O

Page 99: Chapter 3 Infrared Spectroscopy Each interatomic bond may vibrate in several different motions (stretching or bending) - vibrational, rotational energy.

C9H7NO

Page 100: Chapter 3 Infrared Spectroscopy Each interatomic bond may vibrate in several different motions (stretching or bending) - vibrational, rotational energy.
Page 101: Chapter 3 Infrared Spectroscopy Each interatomic bond may vibrate in several different motions (stretching or bending) - vibrational, rotational energy.
Page 102: Chapter 3 Infrared Spectroscopy Each interatomic bond may vibrate in several different motions (stretching or bending) - vibrational, rotational energy.
Page 103: Chapter 3 Infrared Spectroscopy Each interatomic bond may vibrate in several different motions (stretching or bending) - vibrational, rotational energy.

Procedure for obtaining IR spectra

• Liquid Samples: The simplest method for mounting the sample consists of placing a thin film of the liquid between two transparent windows. The most common material used for the windows is NaCl(transparent within 10000 to 650 cm-1)

Page 104: Chapter 3 Infrared Spectroscopy Each interatomic bond may vibrate in several different motions (stretching or bending) - vibrational, rotational energy.

Procedure for obtaining IR spectra

• Solid Samples: As an alternative to measuring the spectrum of a liquid solution of a solid compound, a solid solution or dispersion in KBr is usually more convenient.

1-2 mg of sample is mixed with 50-100 mg of dry KBr powder. The mixing powder is formed into a transparent pellet by pressure in a small die.