IR-Spectroscopy Introduction Theory Instrumentation Sample preparation Table and charts.

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IR-Spectroscopy Introduction Theory Instrumentation Sample preparation Table and charts

Transcript of IR-Spectroscopy Introduction Theory Instrumentation Sample preparation Table and charts.

Page 1: IR-Spectroscopy Introduction Theory Instrumentation Sample preparation Table and charts.

IR-Spectroscopy

Introduction

Theory

Instrumentation

Sample preparation

Table and charts

Page 2: IR-Spectroscopy Introduction Theory Instrumentation Sample preparation Table and charts.

IntroductionVibrational spectrocopy

Spectral area : 4000 – 400 cm-1

Wave number: ν̃! = 1/λ

Even simple molecules can give complex spectra.Advantage: identification when authentic sample is known. Large

databases available for comparison.

Unknown sample: Analysis of functional groups. Functional groups have characteristic absorptions in an IR-spectrum.

Page 3: IR-Spectroscopy Introduction Theory Instrumentation Sample preparation Table and charts.

Theory

Harmonic oscillator

r(t) = r0 + Asin(2πν̃t)

r0

IR-radiation is absorped by organic molecules and converted to molecular vibrational energy. This absorption is quantized,but for every vibrational energy change, there are manyrotational energy changes resulting in band spectra.

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The absorption frequency is dependent on the relative mass of the atoms,the force constant of the chemical bonds and the geometry of the atoms.The frequency can be approximated:

Force constant

Reduced mass

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Page 6: IR-Spectroscopy Introduction Theory Instrumentation Sample preparation Table and charts.

Force constants

Approximation: the value of the force constant doubles from a single bond to a double bond and increases three times from a single to a triple bond.

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The intensity is reported in semi quantitative termes: vs = very strongs = strong, m = medium, w = weak

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Two types of molecular vibrations: bending and stretching

Stretch: rythmic motionalong the binding axis

Bend: Change in the bonding-angle

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Selection rules

1. Absorption of electromagnetic radiation when ν̃(IR) = ν̃(vib)

2. When the dipole moment fluctuates within a vibrational periode.

Consequence: Symmetrical molecules are IR-inactive for symmetrical stretching frequencies. No change in dipole moment.For instance: H2 og CO2

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Degrees of freedom

A non linear molecule with n atoms have 3n – 6 delocalized vibrational modes. The theoretical number of fundamental

vibrational frequencies will rarely be observed. It’s often a good approximation to use localized vibrations. Conequence:

The frequency ν̃ gives a fingerprint of functional groups.

Even though the IR-spectrum is a function of the whole molecule, functional groups will give absorption bands with almost the same frequency independent of the structure of the rest of the molecule.

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Overtones and combination tones

Overtones occur as multiples of a given frequency

ν̃ = nν̃fund

It’s common with only one overtone (n = 2) for strong abs.because the intensitiy drops off rapidly f.eks. C=O strekk (3400)

Combinations bands occur at frequencies which are the sum of two other vibrational frequencies.

ν̃ = ν̃1fund + ν̃2

fund

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”Characteristic frequencies should be recognizedC=O stretch (ca. 1740) and weak overtone (ca 3480)ca. 2850 – 3000, 1465, 1150- 1350 for C-H

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Hydrogen bonding

Hydrogen bonding can occur in a system with aproton donor (X-H) and a proton acceptor Y:. X og Y: are electronegative elements and Y: has an available free elektron pair.

Common proton donors: carboxyl, hydroxyl, amine, amide.

Common acceptor atoms: oxygen, nitrogen og halogens.

Hydrogen bonding changes the force constant to both the donor and the acceptor. X-H stretch moves towards lower frequencies with increasing intensity and band with. The stretching frequency of the acceptor group will also be reduced, but often to a smaller degree.

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The difference in frequency between ”free” and H-bondet OH-absorption is a measure of the strenght of the H-bondingen.

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FTIR

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Advantages with FTIR

1. Electromagnetic radiation covering the entire frequency area passes through the sample at the same time. Saves tid.

2. Digital spectra are easily manipulated.

3. Multiple scans give good S/N ratio.

4. FTIR gives very high resolution.

5. Substraction of reference spectra or solvents is possible.

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Sample preparation

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Enterpretation of spectra

Three impotant areas: 4000 – 1300, 1300 – 900 and 900 – 650 cm-1

4000 – 1300 cm-1 : Functional group area. For instance:OH-, NH- og C=O stretch. Overtones from C=O .

1300 – 900 cm-1 : ”Fingerprint” area. Often very complexabsorption patterns which are unique for every different molecule.

900 – 650 cm-1 : Aromatic stuctures absorb strongly in this area.

Cross check between the three different areas.

Page 19: IR-Spectroscopy Introduction Theory Instrumentation Sample preparation Table and charts.

Next class

- Functional groups and characteristic features

- Tables and charts