Engineering Chemistry. Module 3, module 3.

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Module - 3

Molecular Spectroscopy and Analytical Techniques

SPECTROSCOPY :

It is the branch of science which describes interaction of electromagnetic radiation with matter (ions, atoms, molecules).

↪\hookrightarrow Due to the interaction, the spectrum is formed. The spectrum are classified into two :

  1. Absorption spectrum
  2. Emission spectrum

ABSORPTION SPECTRUM

Energy level diagram for absorption spectrum

  • A molecule undergoes tramition from lowest energy level to highest energy level by absorbing energy from electromagnetic - netic radiation.
  • Then absorption spectrum is obtained.
  • Eg: UV-visible spectroscopy; InfraRed spectroscopy; NMR spectroscopy.

EMISSION SPECTRUM :

Energy level diagram for emission spectrum

  • A molecule undergoes transition from highest energy level to lowest energy level with an emission of energy in the form of photon, then emission opectrum is obtained.

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• Eg: Raman Spectroscopy ; Atomic force spectroscopy.

DIFFERENT TYPES OF MOLECULAR ENERGY LEVELS:

  1. Electronic energy level (EeleE_{\text{ele}})
  2. Vibrational energy level (EvibE_{\text{vib}})
  3. Rotational energy level (ErotE_{\text{rot}})
  4. Translational energy level (EtransE_{\text{trans}})

ELECTRONIC ENERGY LEVEL : ↳ Associated with electrons present in a molecule. ↳ The energy gap between electronic energy level fall in uv-visible region.

VIBRATIONAL ENERGY LEVEL : ↳ Associated with vibrational movement of molecule . ↳ The energy gap between vibrational energy level fall in infra red region.

ROTATIONAL ENERGY LEVEL : ↳ Associated with rotational movement of molecule. ↳ The energy gap between rotational energy level fall in microwave region.

TRANSLATIONAL ENERGY LEVEL : ↳ Associated with translational movement of molecule. ↳ The energy gap between tramolational energy level is considered negligibly small.

• Total energy = Eele+Evib+Erot+EtransE_{\text{ele}} + E_{\text{vib}} + E_{\text{rot}} + E_{\text{trans}} Eele>Evib>Erot>>>EtransE_{\text{ele}} > E_{\text{vib}} > E_{\text{rot}} >>> E_{\text{trans}}


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Electronic, vibrational, and rotational energy levels in an excited state

Electronic, vibrational, and rotational energy levels in a ground state

Parameters related to light

Transmittance (T)

Transmittance is the ratio of transmitted-light intensity to incident-light intensity. It has no unit.

T=II0T=\frac{I}{I_0}

Here, II is the intensity of transmitted light and I0I_0 is the intensity of incident light.

Absorbance (A)

Absorbance is the logarithm of the ratio of incident-light intensity to transmitted-light intensity. It has no unit.

A=log⁡(I0I)=log⁡(1T)=−log⁡TA=\log\left(\frac{I_0}{I}\right)=\log\left(\frac{1}{T}\right)=-\log T

Beer–Lambert's law

Beer-Lambert's Law setup showing a cuvette containing a coloured solution


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4 The law states that, when a parallel beam of monochromatic electromagnetic radiation is passed through a coloured, dilute and homogeneous solution of known concentration, then absorbance 'A' is directly proportional to concentration of solution and thickness of the medium.

i.e A∝cxA \propto c x A=εcxA = \varepsilon c x, where A→AbsorbanceA \rightarrow \text{Absorbance} ε→molar absorption coefficient\varepsilon \rightarrow \text{molar absorption coefficient} c→concentration of solutionc \rightarrow \text{concentration of solution} x→Thickness of the cuvettex \rightarrow \text{Thickness of the cuvette}

∴ε=Acx\therefore \varepsilon = \frac{A}{c x}

unit of AA - no unit unit of CC - mol/L or mol/dm3\text{mol/L or mol/dm}^3 (M) unit of xx - dm\text{dm} ∴unit of ε=mol−1dm2\therefore \text{unit of } \varepsilon = \text{mol}^{-1}\text{dm}^2

Q. Define Beer - Lambert's law and deduce integrated form. Discuss the plot of Absorbance versus concentration. What does the slope of the graph represent.

ans.

Cuvette diagram showing incident intensity I0 and transmitted intensity I with path length dx and concentration c

Beer lambert's law states that when a parallel beam of monochromatic electromagnetic radiation is passed through a coloured, dilute and homogeneous solution, the rate of decrease in decrease intensity of radition (dIdI) with the thickness of sourtion (dxdx) is directly proportional to intensity of the radiation and concentration of the solution.


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i.e., −dIdxoIC-\frac{dI}{dx} o I C

−dIdx=kIC-\frac{dI}{dx} = k I C where kok o proportionality constant

−dII=kCdx-\frac{dI}{I} = k C dx

Integrating both sides,

∫I0I−dII=∫0xkCdx\int_{I_0}^I \frac{-dI}{I} = \int_0^x k C dx

ln⁡I0I=kCx\ln \frac{I_0}{I} = k C x

2.303log⁡I0I=kCx2.303 \log \frac{I_0}{I} = k C x

log⁡I0I=kCx2.303\log \frac{I_0}{I} = \frac{k C x}{2.303}

∴log⁡I0I=A\therefore \log \frac{I_0}{I} = A and k2.303=ε\frac{k}{2.303} = \varepsilon

A=εCxA = \varepsilon C x

Plot of absorbance versus concentration showing a straight line passing through the origin with slope equal to Ex

  • The plot of absorbance versus concentration should be a straight line passing through the origin for a cell of thickness xx and slope is given by εx\varepsilon x.

Q. The percentage transmittance of 0.01M0.01M dye solution in ethanol is 2020. In a 2 cm2\text{ cm} cell for a light of wavelength 5000 A˚5000\text{ \AA}. Find the absorbance and molar absorption coefficient.

Ans. Concentration C=0.01M=0.01 mol/dm3C = 0.01M = 0.01 \text{ mol}/\text{dm}^3

Thickness x=2 cm=0.2 dmx = 2\text{ cm} = 0.2\text{ dm}


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I0=100  ,  I=20(%T=20 means when 100% light is incident,20% is transmitted).I_0 = 100 \; , \; I = 20 \quad \quad (\% T = 20 \text{ means when } 100\% \text{ light is incident}, 20\% \text{ is transmitted}).

  • A=log⁡I0IA = \log \frac{I_0}{I} =log⁡(10020)= \log \left(\frac{100}{20}\right) =log⁡(5)= \log (5) =0.6989‾= \underline{0.6989}

  • ε=Acx\varepsilon = \frac{A}{cx} =0.69890.01×0.2= \frac{0.6989}{0.01 \times 0.2} =349.45‾ mol−1dm2= \underline{349.45}\text{ mol}^{-1}\text{dm}^2

APPLICATIONS OF BEER - LAMBERT'S LAW:

↳ If two solutions of concentration c1c_1 and c2c_2, where c1c_1 concentration is known and c2c_2 concentration is unknown, then absorbance of both solutions measured under same condition are :

A1=εc1xandA2=εc2xA_1 = \varepsilon c_1 x \quad \text{and} \quad A_2 = \varepsilon c_2 x

∴c1c2=A1A2\therefore \frac{c_1}{c_2} = \frac{A_1}{A_2}

↳ Absorbance is measured in terms of transmittance, A=−log⁡TA = -\log T −log⁡T1=εc1xand−log⁡T2=εc2x-\log T_1 = \varepsilon c_1 x \quad \text{and} \quad -\log T_2 = \varepsilon c_2 x ∴c1c2=log⁡T1log⁡T2\therefore \frac{c_1}{c_2} = \frac{\log T_1}{\log T_2}


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Q. Dye solution of concentration 0.04 M0.04\text{ M} shows absorbance of 0.0450.045 at 530 nm530\text{ nm} while test solution of same dye solution shows 0.0220.022 absorbance.

⇒\Rightarrow

C1=0.04 MC_1 = 0.04\text{ M} A1=0.045A_1 = 0.045 A2=0.022A_2 = 0.022

C2=C1A2A1C_2 = \frac{C_1 A_2}{A_1}

=0.04×0.0220.045= \frac{0.04 \times 0.022}{0.045}

=0.04×2245= \frac{0.04 \times 22}{45}

=4×2245001125= \frac{4 \times 22}{\frac{4500}{1125}}

=221125= \frac{22}{1125}

=0.0195 M= 0.0195\text{ M}

Q. A 50 ppm50\text{ ppm} standard solution of Fe3+\text{Fe}^{3+} after developing red colour with ammonium thiocyanate shows a transmittance of 0.20.2 at 620 nm620\text{ nm} while an unknown solution of Fe3+\text{Fe}^{3+} after developing red colour with same amount of ammonium thiocyanate gives a transmittance of 0.40.4. Find the concentration of the unknown Fe3+\text{Fe}^{3+} solution.

⇒\Rightarrow

C1=50 ppmC_1 = 50\text{ ppm} T1=0.2T_1 = 0.2 T2=0.4T_2 = 0.4

C2=C1log⁡T2log⁡T1C_2 = \frac{C_1 \log T_2}{\log T_1}


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=50×log⁡(0.4)log⁡(0.2)=50 \times \frac{\log(0.4)}{\log(0.2)} =50×0.56932=50 \times 0.56932 =28.46 ppm=28.46\text{ ppm}

LIMITATIONS OF BEER-LAMBERT'S LAW:

  • The law is applicable to only dilute, coloured and homogeneous solution.
  • It does not obey, if the light is not monochromatic.
  • Deviations may occur, if impurity is present.
  • Deviation may occur if temperature varies.

UV - VISIBLE SPECTROSCOPY:

  • It is an absorption spectroscopy.
  • Principle: UV-visible spectrum or electronic spectrum arises due to transition of electrons from lower energy level to higher energy level by absorbing UV-visible radiation in the range of 200−800 nm200 - 800\text{ nm}.
  • The two groups which are responsible for UV-visible radiation absorption are chromophore and auxochrome.

CHROMOPHORE:

  • It provides colour to a compound.
  • It contains unsaturation in their structure (C=C,C=O,NO2,N=NC=C, C=O, NO_2, N=N).

AUXOCHROME:

  • It does not produce colour, but it can enhance colour of a compound.
  • It contains lone pair of electrons in their structure (OH,NH2,NR2OH, NH_2, NR_2).

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λmax⁡\lambda_{\max} : The wavelength at which maximum absorbance occurs.

Eg: CH2=CH2\text{CH}_2=\text{CH}_2 ; CH2=CH−CH=CH2\text{CH}_2=\text{CH}-\text{CH}=\text{CH}_2 ; CH2=CH−CH=CH−CH=CH2\text{CH}_2=\text{CH}-\text{CH}=\text{CH}-\text{CH}=\text{CH}_2 ;

Benzene ring chemical structure

\text{Ethene} & < & 1,3\text{-butadiene} & < & 1,3,5\text{-hexatriene} & < & \text{benzene} \\ \lambda_{\max}=169\text{nm} & & \lambda_{\max}=217\text{nm} & & \lambda_{\max}=247\text{nm} & & \lambda_{\max}=255\text{nm} \end{array}$ ROLE OF CONJUGATION IN ABSORPTION MAXIMUM: - As more and more double bonds come into conjugation, the absorption comes to the visible region. - In case of lycopene, a red coloured natural dye in tomatoes, there are 11 double bonds in conjugation. Therefore, $\lambda_{\max}$ is observed at $505\text{nm}$. DIFFERENT TYPES OF ELECTRONIC TRANSITION: 1. $\sigma \rightarrow \sigma^*$ transition 2. $\pi \rightarrow \pi^*$ transition 3. $n \rightarrow \pi^*$ transition 4. $n \rightarrow \sigma^*$ transition. ![Electronic energy levels and transitions diagram](/notes/cse/s1/chemistry/module-3/assets/page-010-image-2-source.png) 1. $\sigma \rightarrow \sigma^*$ transition : - Observed in all saturated hydrocarbons. - This transition absorbs radiations below $150\text{nm}$. So this transition is uv-visible inactive. 2. $\pi \rightarrow \pi^*$ transition : - This type of transition is observed in unsaturated hydrocarbons. - It absorbs radiation in the range of $200 - 800\text{nm}$. So this transition is uv-visible active. - This transition is known as allowed transition. So the intensity is very high. ---

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  1. noπ∗n o \pi^* transition :
  • observed in aldehydes and ketones.
  • This transition absorbs radiation in the range of 200−800nm200-800\text{nm}.
  • This is a forbidden transition. So the intensity is very low.
  • This transition is uv-visible active.
  1. noσ∗n o \sigma^* transition :
  • observed in compounds containing nitrogen, oxygen, sulphur.
  • This transition absorbs radiation below 200nm200\text{nm}. This transition is uv-visible inactive.

Q. Draw the possible electronic transition in (i) ethane.

Ans. CH3−CH3\text{CH}_3-\text{CH}_3 ethane

Electronic energy levels and transition for ethane

(ii) CH2=CH−CH=CH2\text{CH}_2=\text{CH}-\text{CH}=\text{CH}_2 1,3-butadiene

Electronic energy levels and transitions for 1,3-butadiene

(iv) Benzoic acid

Electronic energy levels and transitions for benzoic acid

(iii) benzene

Electronic energy levels and transitions for benzene

(v) Salicylic acid

Electronic energy levels and transitions for salicylic acid


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(vi) Benzaldehyde : \text{-CHO}

Energy level transitions for benzaldehyde showing sigma, pi, n, pi star, and sigma star orbitals.

(vii) Ethanol : \text{CH}_3-\text{CH}_2-\text{OH}

Energy level transitions for ethanol showing sigma, pi, n, pi star, and sigma star orbitals alongside an absorption curve.

(viii) Propanol : \text{CH}_3-\text{CO}-\text{CH}_3

Energy level transitions for propanol showing sigma, pi, n, pi star, and sigma star orbitals.

UV - VISIBLE SPECTROPHOTOMETER:

flowchart LR S["Source"] --> M["Monochromator"] --> B["Beam splitter"] B --> R["Reference cell — I₀"] B --> C["Sample cell — I"] R --> D["Detector"] C --> D D --> O["Output: A = log(I₀/I)"]
  • Commonly used sources are H filament lamp, tungsten filament lamp or Xe filament lamp.
  • Prism or grating is used as monochromator. It disperses the light into desired wavelength.
  • Beam splitter splits wave into two having same intensity.
  • Reference cell or sample cell : It is made up of quartz. It must be inert and highly transparent.

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↳ Photo multiplier tube used as detector. It converts light signal to electrical signal. ↳ Output is a plot of Absorbance versus wavelength (UV-visible spectrum).

Plot of Absorbance versus Wavelength (UV-visible spectrum)

WORKING: ↳ A dilute solution of sample prepared in suitable solvent and taken in a cuvette, which is called sample. A pure solvent taken in another cuvette is called reference. ↳ Source produce UV visible radiation which is allowed to prism, and it makes it monochromatic light. ↳ Beam splitter splits monochromatic light into two beams having same intensity. ↳ One beam is allowed to pass through sample and the other through reference. ↳ Reference doesn't absorb radiation, so intensity of radiation is considered as intensity of incident light. ↳ Sample absorbs radiation, so intensity of radiation is considered as intensity of transmitted light. ↳ Detector detects both radiation and compares. The difference is analysed and recorded. ↳ UV visible spectrum is produced.


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APPLICATIONS OF UV-VISIBLE SPECTROSCOPY:

↳ Determination of unknown concentration of a solution. ↳ Determination of unknown compound. ↳ Used to study kinetics of reaction. ↳ Used to characterise dyes. ↳ Used in quantitative estimation of blood sugar and cholestrol.

INFRARED SPECTROSCOPY: ↳ It is an absorption spectrum. ↳ Vibrational spectrum or IR spectrum arises due to transition of a molecule from lower vibrational energy level to higher vibrational energy level by absorbing IR radiation in the range of 400−5000 cm−1400-5000\text{ cm}^{-1}. ↳ The essential criteria for a molecule to show IR spectrum - dipole moment must change during vibration. ↳ Homonuclear diatomic molecules have no dipole moment, so they are IR inactive. Eg: H2,N2,Cl2,O2\text{H}_2, \text{N}_2, \text{Cl}_2, \text{O}_2. ↳ Heteronuclear diatomic or polyatomic molecules have dipole moment, so they are IR active. Eg: HCl,CO2,HCN,H2O\text{HCl}, \text{CO}_2, \text{HCN}, \text{H}_2\text{O}.

CALCULATION OF NUMBER OF MODES OF VIBRATION: ↳ For a linear molecule, number of modes of vibration is 3n−53n-5, where nn is the number of atoms.

Eg: • carbon dioxide −CO2-\text{CO}_2 O=C=O\text{O}=\text{C}=\text{O} n=3n=3 (3imes3)−5(3 imes3)-5 =9−5=9-5 =4=4

• HCl\text{HCl} H−Cl\text{H}-\text{Cl} n=2n=2 (3imes2)−5(3 imes2)-5 =6−5=6-5 =1=1

• HCN\text{HCN} H−C extequivN\text{H}-\text{C}\text{ extequiv}\text{N} n=3n=3 (3imes3)−5(3 imes3)-5 =9−5=9-5 =4=4


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For a non-linear molecule, number of modes of vibration is 3n−63n - 6.

Eg: H2O\text{H}_2\text{O}

Water molecule structure

n &= 3\\ (3 \times 3) - 6 &= 9 - 6 = 3 \end{aligned}$ $\, \cdot \text{C}_6\text{H}_6$ Benzene ![Benzene ring structure](/notes/cse/s1/chemistry/module-3/assets/page-015-image-2-structured.svg) $\begin{aligned} n &= 12\\ (3 \times 12) - 6 &= 36 - 6 = 30 \end{aligned}$ $\, \cdot \text{CH}_4$ methane ![Methane molecule structure](/notes/cse/s1/chemistry/module-3/assets/page-015-image-3-structured.svg) $\begin{aligned} n &= 5\\ (3 \times 5) - 6 &= 15 - 6 = 9 \end{aligned}$ --- FUNDAMENTAL VIBRATION ```mermaid flowchart TD F["Fundamental vibrations"] --> S["Stretching"] F --> B["Bending"] S --> SS["Symmetric stretching"] S --> AS["Asymmetric stretching"] B --> IP["In-plane bending"] B --> OP["Out-of-plane bending"] ``` Q. Calculate number of vibration modes in $\text{CO}_2$, draw the possible vibration and find out IR active vibration. $\Rightarrow \text{O} = \text{C} = \text{O}$ $n = 3$ $(3 \times 3) - 5 = 4$ The possible vibration are symmetric stretching vibration, assymmetric stretching vibration, in plane bending vibration, out plane bending vibration. 1. Symmetric stretching vibration: ![Symmetric stretching of CO2](/notes/cse/s1/chemistry/module-3/assets/page-015-image-5-structured.svg) : No change in dipole moment $\therefore$ IR inactive 2. Asymmetric stretching vibration: ![Asymmetric stretching of CO2](/notes/cse/s1/chemistry/module-3/assets/page-015-image-6-structured.svg) : Change in dipole moment $\therefore$ IR active. ---

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  1. In plane bending vibration :

In plane bending vibration of CO2 showing O=C=O with arrows indicating in-plane bending.

: change in dipole moment ∴\therefore IR active.

  1. Out plane bending vibration :

Out of plane bending vibration of CO2 showing O=C=O with arrows indicating out-of-plane movement.

: change in dipole moment ∴\therefore IR active.

In CO2CO_2 , out of 4 vibrations , 3 vibrations are IR active but 2 signals are observed in IR spectrum because in plane and out plane bending vibrations are degenerate (i.e, same energy).

(ii) HCN

Linear structure of HCN.

n=3n = 3

(3×3)−5=4(3 \times 3) - 5 = 4

In HCN, four vibrations are IR active.

(iii) H2OH_2 O

Bent structure of H2O.

n=3n = 3

(3×3)−6=3(3 \times 3) - 6 = 3

Three vibrations are : symmetric, asymmetric and inplane bending vibrations.

  1. Symmetric stretching vibration

Symmetric stretching vibration of H2O.

: Change in dipole moment ∴\therefore IR active.

  1. Asymmetric stretching vibration

Asymmetric stretching vibration of H2O.

: change in dipole moment ∴\therefore IR active


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3. In-plane bending vibration

H2O molecule bending vibration showing oxygen moving up and hydrogens moving down with double-sided arrows

The dipole moment changes during this vibration, so it is IR active. The source notes show three IR signals for H₂O.

Calculation of force constant (K)

Vibrational frequency depends on bond length and atomic masses. The wavenumber is

νˉ=12πcKμ\bar\nu=\frac{1}{2\pi c}\sqrt{\frac{K}{\mu}}

where cc is the speed of light, KK is the force constant, and μ\mu is the reduced mass:

μ=m1m2m1+m2\mu=\frac{m_1m_2}{m_1+m_2}

Squaring and rearranging gives

νˉ2=K4π2c2μ\bar\nu^2=\frac{K}{4\pi^2c^2\mu}

K=4π2c2μνˉ2K=4\pi^2c^2\mu\bar\nu^2

Use consistent units for cc and νˉ\bar\nu; with SI units, KK is in N m⁻¹.

Question: A CO molecule absorbs infrared radiation at 2140 cm⁻¹. Calculate its force constant, given atomic masses C = 12 amu and O = 16 amu. The solution continues on the next page.


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μ=12×1612+16=12×1628\mu = \frac{12 \times 16}{12 + 16} = \frac{12 \times 16}{28}
=487=6.857×1.66×10−27 kg= \frac{48}{7} = 6.857 \times 1.66 \times 10^{-27}\text{ kg}
=1.138×10−26 kg= 1.138 \times 10^{-26}\text{ kg}

u}^2$ $= 4 \times (3.14)^2 \times 9 \times 10^{16} \times 6.857 \times 1.66 \times 10^{-27} \times (214000)^2$ $= 4 \times (3.14)^2 \times 9 \times 10^{16} \times 1.138 \times 10^{-26} \times (214000)^2$ $= 1849\text{ Nm}^{-1}$ Question: Calculate the force constant of HCl for an IR absorption wavenumber of 3050 cm⁻¹. Given atomic masses: H = 1 amu (m₁), Cl = 35 amu (m₂). $\mu = \frac{1 \times 35}{36}$ $= 0.972 \times 1.66 \times 10^{-27}$ $= 1.6139 \times 10^{-27}\text{ kg}$ $K = 4 \pi^2 c^2 \mu \bar{ u}^2$ $= 4 \times (3.14)^2 \times 9 \times 10^{16} \times 1.6139 \times 10^{-27} \times (3050 \times 100)^2$ $= 4 \times (3.14)^2 \times 9 \times 10^{16} \times 1.6139 \times 10^{-27} \times (305000)^2$ $= 532.89\text{ Nm}^{-1}$ ---

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APPLICATIONS OF IR SPECTROSCOPY:

  • Determination of force constant of a molecule.

  • Identification of functional groups in organic compounds.

    Eg:

    Functional GroupsStretching frequency
    1. C=OC=O1700−1750 cm−11700 - 1750\text{ cm}^{-1}
    2. NH2NH_23200−3300 cm−13200 - 3300\text{ cm}^{-1}
    3. −OH-OH3300−3500 cm−13300 - 3500\text{ cm}^{-1}
    4. C=CC=C in alkene1620−1650 cm−11620 - 1650\text{ cm}^{-1}
    5. C−HC-H2900−3000 cm−12900 - 3000\text{ cm}^{-1}
  • Determination of unknown compounds.

  • Determination of purity of a compound.

  • To distinguish inter-molecular and intra-molecular hydrogen bonding.

INTER-MOLECULAR HYDROGEN BONDING

o-hydroxy phenol

Intermolecular hydrogen bonding between para-hydroxyphenol molecules (source figure)

INTRAMOLECULAR HYDROGEN BONDING

p-hydroxy phenol

Intramolecular hydrogen bonding between adjacent hydroxyl groups (source figure)

  • −OH-OH stretching frequency does not change on dilution in the case of intermolecular hydrogen bonding.

  • In pp-hydroxy phenol, there exist intramolecular hydrogen bonding. The molecule gets separated on dilution and intramolecular hydrogen bond weakens and there is shift of absorption frequency with dilution.

  • In oo-hydroxy phenol, HH bonding is intramolecular which is not affected by dilution.


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DIELECTRIC THERMAL ANALYSIS (DETA)

  • DETA is used to study dielectric and thermal properties of samples.
  • It can give information about dielectric changes with temperature.
  • In this technique, the change in dielectric properties of a material under an applied voltage is recorded with change in temperature.

Principle of DETA:

  • In DETA technique, the sample under study is subjected to an electric field.

  • The applied sinusoidal voltage (alternating current) will polarise the sample which forces the charge carriers inside the sample to move (positively charged particle migrate to negative pole and vice-versa).

  • This movement results in a sinusoidal current with phase shift which is being measured.

  • Here, the polarisation change of the material under varying temperature is measured at a fixed frequency.

  • PERMITTIVITY (E′\text{E}'): It is the ability of a material to store electrical energy under an applied electric field.

  • DIELECTRIC LOSS (E′′\text{E}''): It is the energy dissipated as heat when a material is subjected to electric field.

  • DISSIPATION FACTOR (tan⁡δ\tan \boldsymbol{\delta}) : It represents efficiency of a material to convert electrical energy to heat energy under an electric field.


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↪\hookrightarrow Material with lower value of tan⁡δ\tan \delta is preferred as thermal insulator and capacitor applications.

↪tan⁡δ=ε′′ε′\hookrightarrow \tan \delta = \frac{\varepsilon''}{\varepsilon'}

INSTRUMENTATION OF DETA:

flowchart LR FG["Frequency generator"] --> E["Electrodes and sample in programmable furnace"] ENV["Environmental control"] --> E TC["Temperature controller"] --> E TS["Thermocouple / temperature sensor"] --> TC E --> DA["Dielectric analyser"] --> REC["Recorder"]
  • Sample Holder : sample is placed between two parallel metal plates (electrodes).

  • Temperature programmable furnace : Furnace with temperature programming facility is used to ramp up and down the temperature of the sample.

  • Frequency Generator : Sinusoidal voltage (ac) is provided through the frequency generator.

  • Temperature control unit / equipment : Prevents over heating of the sample.

  • Environmental control equipment : It is used to provide suitable atmosphere (air or inert gas) for the sample as per requirement.


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  • Thermocouple / Temperature sensor: Used to measure temperature changes of sample.
  • Dielectric Analyser: Key component of DETA instrumentation which acts as detector and detects permittivity and dielectric loss with change in temperature.
  • Recorder: Computer will record the data and DETA curve is obtained as a plot between permittivity versus temperature or dielectric loss versus temperature.

WORKING:

  • Sample in the form of thin film, powder, pellet, etc is placed between two electrodes and then electric field is applied.
  • The temperature of the sample is increased at a controlled rate using temperature programmable furnace under suitable environmental condition.
  • The response signal is detected and analysed using dielectric analyser.
  • The dielectric response is recorded for every change in temperature under a constant frequency.
  • Temperature of the sample is monitored by thermocouple.
  • DETA plot is obtained between ε′\varepsilon' vs TT or ε′′\varepsilon'' vs TT.

APPLICATIONS:

  • Used to study dielectric and thermal properties of material.
  • It is used to analyse polymers, plastics, glasses, ceramic, etc.
  • Used to identify phase transition temperature like glass transition temperature of polymers.

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↪\hookrightarrow used to study curing profile of thermosets. ↪\hookrightarrow used to study epoxy curing process. ↪\hookrightarrow Study of dielectric properties at different temperature is used for the development of new insulating material and energy storage material.

SCANNING ELECTRON MICROSCOPE (SEM)

↪\hookrightarrow SEM produce image of a sample by scanning the surface of the sample usingby\underset{\text{by}}{\text{using}} high energy electron beam. ↪\hookrightarrow The interaction of electron beam with the atoms near the surface of the sample produce different signals - backscattered electrons, secondary electrons and X-ray. ↪\hookrightarrow These signals are detected by suitable detectors and can be used to obtain information about surface topography (size, shape and texture) and elemental composition

SECONDARY ELECTRONS: ↪\hookrightarrow These are directly knocked out from the atom of the sample by incidental electron.

BACK SCATTERED ELECTRON: ↪\hookrightarrow These are incidental electrons that are reflected backwards.

X-RAYS: ↪\hookrightarrow Emitted from the sample


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INSTRUMENTATION

Diagram of a Scanning Electron Microscope (SEM) instrumentation

  • source : electron source generates high energy electron beam. Thermionic gun or field emission guns are used as electron source.
  • Anode : Positively charged anodes are used. It can accelerate the electron beam.
  • condenser lens : It is a electromagnetic lens. can be used to focus the electron beam into small, thin and coherent beam.
  • scan coil : Deflects the electron beam horizontally and vertically over the surface of the sample and scan the surface in rectangular fashion.
  • Objective lens : It is also an electromagnetic lens used to focus electron beam to the surface of the sample.
  • Detectors : There are suitable detectors to detect secondary electrons and x-rays.
  • sample : should be conductive and dehydrated.

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WORKING:

↳ Electron gun generates high energy electron beam which are accelerated by anode.

↳ Accelerated electron beam is focused by condenser lens.

↳ Objective lens focus the beam onto sample where the solid sample is placed.

↳ Scan coil scan the surface in raster fashion.

↳ Secondary electrons and x-rays are produced from the sample and detected by suitable detectors.

↳ Black and white three dimensional image of the sample is obtained after processing.

APPLICATIONS:

↳ Used to characterise nanomaterials.

↳ Used to detect and analyse surface fracture and contamination.

↳ Used as an essential research tool in fields like lifescience, nanoscience, medical and forensic science.


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[Non-content page]


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module - 3

Spectroscopy and analytical technique

Advantages of spectroscopy technique

  • ⇒\Rightarrow less sample quantities required.
  • ⇒\Rightarrow sample material remain unchanged during analysis and resuse.
  • ⇒\Rightarrow requires very less time.
  • ⇒\Rightarrow They give acurate result.
  • →\rightarrow spectroscopy deals with the interaction of atoms or molecules or matter with the electromagnetic radiation.
flowchart LR I["Interacting radiation"] --> S["Atom / molecule (sample)"] --> T["Transmitted radiation"] --> D["Detector"]

Electromagnetic spectrum

  • ⇒\Rightarrow electromagnetic radiation arranged by wavelength or frequency
  • ⇒\Rightarrow It includes radiowaves, microwaves, IR, VL, UV, X-Ray and gamma ray.
  • ⇒\Rightarrow wavelength decreases and frequency increases from radio waves to gamma rays
  • ⇒\Rightarrow Energy of radiation increases from low-frequency to high frequency.

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Different energy levels in a molecule.

Different energy levels in a molecule diagram showing electronic, vibrational, and rotational levels

  1. Electronic energy level (EelE_{el})

⇒\Rightarrow Energy levels associated with the electrons present in the molecules

⇒\Rightarrow These energy levels falls in uv visible region

⇒\Rightarrow The spectrum associated with electronic energy level [uncertain: ...]


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is called uv visible spectroscopy.

  1. vibrational energy level (EvbE_{vb})

=> The energy level associated with vibration is called vibrational energy.

=> Atoms in a molecule can vibrate by keeping the position of center of mass constant.

=> The energy gap betw EvbE_{vb} falls in infrared region.

  1. Rotational energy levels (EROTE_{ROT})

=> The energy level associated with rotation is called rotational energy level.

=> If a molecule rotate in space about an axis passing through its centre of mass.

=> The energy gaps between rotational energy level falls in microwave region.

  1. Translational Energy Level (ETEE_{TE})

=> The energy level associated with translational energy is called translational energy level.

=> If the position of centre of mass changes with time the molecule is said to possess the translational energy.

=> Translational energy of a molecule is usually not quantised.

Etotal=Eele+Evb+ERT+ETEE_{total} = E_{ele} + E_{vb} + E_{RT} + E_{TE}

Eel>Evb>ERT⟩⟩ETEE_{el} > E_{vb} > E_{RT} \rangle\rangle E_{TE} can be neglected.


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Etotal=Eele+Evib+ErotE_{total} = E_{ele} + E_{vib} + E_{rot}

Types of spectrum

  1. Based on the nature of interaction.
Emmision spectrumAbsorption spectrum

Emission spectrum diagram showing transition from higher to lower energy level with emission of photon

|

Absorption spectrum diagram showing transition from lower to higher energy level with absorption of photon

| | →\rightarrow when an atom or molecule undergoes transition from higher energy level to lower energy level with a absorption of photon [uncertain: emission] of energy hνh\nu is emmision spectrum. | →\rightarrow when an atom or molecule undergoes transition from lower energy level to higher energy with an absorption of a photon is called absorption spectrum. | | →\rightarrow Hydrogen spectrum, atomic emmision spectrum, fluorescence spectrum etc... belongs to it. | →\rightarrow It includes uv-visible, IR, Microwave and NMR. |

  1. Based on interacting species.
Atomic spectramolecular spectra

Atomic spectra diagram showing atomic energy levels

|

Molecular spectra diagram

|


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⇒\Rightarrow which arise from the transition of electrons between atomic energy levels.

⇒\Rightarrow which arise from the transition of electrons between different molecule energy levels.

⇒\Rightarrow UV visible, IR, microwave, NMR belongs in it.

IMP Beer-lamberts law.

Diagram illustrating Beer-Lambert's law with a light beam passing through a medium of thickness x

−dIdx∝Ic\frac{-dI}{dx} \propto I c

−dIdx=kIc\frac{-dI}{dx} = k I c

−dII=kc dx\frac{-dI}{I} = k c \, dx

∫I0I−dII=∫0xkc dx\int_{I_0}^{I} \frac{-dI}{I} = \int_{0}^{x} k c \, dx

ln⁡I0I=kcx\ln \frac{I_0}{I} = k c x

2.303log⁡I0I=kcx2.303 \log \frac{I_0}{I} = k c x

log⁡I0I=k2.303cx\log \frac{I_0}{I} = \frac{k}{2.303} c x

log⁡I0I=εcx\log \frac{I_0}{I} = \varepsilon c x

\log \frac{I_0}{I} &= \varepsilon c x = A \\ A &= -\log \frac{I}{I_0} \\ &= -\log T \\ &= \log \frac{1}{T} \end{aligned}$ $\boxed{\log \frac{I_0}{I} = \varepsilon c x}$ $\boxed{\log \frac{1}{T}}$ ---

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=> When a parallel beam of monochromatic electromagnetic radiation is pass through an absorbing medium of given conc. cc, the rate of decrease is intensity, [−dIdx][-\frac{dI}{dx}] of radiation, with thickness of the solution (dx)(dx) is proportional to the intensity of incident radiation at that point and also the concentration of the solution.

log⁡I0I=εcx\log \frac{I_0}{I} = \varepsilon c x

Absorbance

=> It is the logarithmic ratio of intensity of incident radiation to the transmitted radiation.

Transmittance

=> It is the ratio of transmitted radiation to the incident radiation.

I0→I_0 \rightarrow intensity of incident radiation.

I→I \rightarrow transmitted radiation.

ε→\varepsilon \rightarrow molar absorption coefficient/absorbivity/extinction\text{coefficient} / \text{absorbivity} / \text{extinction}.

c→c \rightarrow conc. in mol/L→unit−mol/dm3\text{mol}/L \rightarrow \text{unit} - \text{mol}/\text{dm}^3.

x→x \rightarrow Thickness in decimeter.

A→A \rightarrow Absorbance.

T→T \rightarrow Transmittance.


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What is molar absorbtion coefficient (ε\varepsilon) write it's unit.

A=εcxA = \varepsilon c x

ε=Acx=\varepsilon = \frac{A}{c x} =

unit=mol−1dm2\text{unit} = \text{mol}^{-1} \text{dm}^2

How can you determine the unknown concentration using Beer Lamberts law (by graphical method).

Graph of Absorbance vs Concentration showing graphical method to determine unknown concentration

⇒\Rightarrow graph derived from unknown concentration.

⇒\Rightarrow Based on the graph derived from know concentration and absorbance, we can find out the unknown concentration using it's unk- absorbance value.

The percentage transmittens of 0.01M0.01 \text{M} dye solution in ethanol is 2020. In a 2cm2 \text{cm} cell for a light of wavelength 5000A˚5000 \mathring{\text{A}}.

Find the absorbance and molar absoption constant.


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C=0.01 MC = 0.01\text{ M}

I=20I = 20

I0=100I_0 = 100

λ=5000 A˚=5000×10−10\lambda = 5000\text{ \AA} = 5000 \times 10^{-10}

A=εcx=log⁡I0IA = \varepsilon cx = \log \frac{I_0}{I}

A=log⁡10020=log⁡(5)=0.69\phantom{A} = \log \frac{100}{20} = \log(5) = 0.69

ε=Acx=0.690.01×2×100=[illegible]≃343 mol−1dm3\varepsilon = \frac{A}{cx} = \frac{0.69}{0.01 \times 2 \times 10^0} = \text{[illegible]} \simeq 343\text{ mol}^{-1}\text{dm}^3

  1. A dye solution of concentration 0.04 M0.04\text{ M} shows absorbance of 0.0450.045 at 530 nm530\text{ nm} while a test solution of same dye shows absorbance of 0.0220.022 under same conditions. Find the concentration of test solutions.

C1=0.04 MC_1 = 0.04\text{ M}.

A1=0.045A_1 = 0.045

λ=530 nm\lambda = 530\text{ nm}

A2=0.022A_2 = 0.022

A1=ε1c1x∴A1A2=c1c2A_1 = \varepsilon_1 c_1 x \quad \therefore \frac{A_1}{A_2} = \frac{c_1}{c_2}

A2=ε2c2xA_2 = \varepsilon_2 c_2 x

=0.0450.022=0.04c2= \frac{0.045}{0.022} = \frac{0.04}{c_2}

c2=0.022×0.040.045=0.019 Mc_2 = \frac{0.022 \times 0.04}{0.045} = 0.019\text{ M}


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A 50 ppm50\text{ ppm} standard solution of Fe3+\text{Fe}^{3+} after developing red colour with ammonium thiocyanate shows a transmittance of 0.20.2 at 640 nm640\text{ nm}, while an unknown solution of Fe3+\text{Fe}^{3+} after developing colour with same amount ammonium thiocyanate gives transmittance of 0.40.4. Find the conc. of Fe3+\text{Fe}^{3+} solution?

T1=0.2T_1 = 0.2

T2=0.4T_2 = 0.4

C1=50 ppmC_1 = 50\text{ ppm}.

−log⁡T1=ε1c1l-\log T_1 = \varepsilon_1 c_1 l

−log⁡T2=ε1c2l-\log T_2 = \varepsilon_1 c_2 l

−log⁡T1−log⁡T2=C1C2=−log⁡0.2−log⁡0.4=50C2\frac{-\log T_1}{-\log T_2} = \frac{C_1}{C_2} = \frac{-\log 0.2}{-\log 0.4} = \frac{50}{C_2}

C2=+log⁡0.4×50+log⁡0.2=[illegible]  28.4 ppmC_2 = \frac{+\log 0.4 \times 50}{+\log 0.2} = \text{[illegible]} \; 28.4\text{ ppm}


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UV-visible spectroscopy IMP

  • 0−200 nm0 - 200\text{ nm} - Far UV / vacuum UV.
  • 200−400 nm200 - 400\text{ nm} - neer UV
  • 400−800 nm400 - 800\text{ nm} - visible region

Principle:

  • If a material blue in colour it absorb the orange red visible line.
  • When a molecule interacts with UV-visible radiation, electronic transition will occur between electronic energy levels by absorbing the radiation.
  • It is also called electronic spectrum - transition occurs between electronic energy level.
  • It is a plot of absorbance or intensity vls λ\lambda in nm\text{nm}.

Absorption spectrum and electronic energy level transition diagram

Different transition observed in UV-visible spectroscopy

Electronic transitions energy level diagram


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In a molecule there are three types of electrons

  • σ\sigma electrons - bonding
  • π\pi electrons - bonding
  • nn " - lone pairs - non bonding

→\to σ−σ∗\sigma - \sigma^*

→\to It is mainly observed in molecule with sigma bonds. →\to Hydrocarbons can shows this prop signal. →\to It mainly occur at uv region, below 150 nm150\text{ nm}

eg: CH4,CH3−CH3,cyclohexane\text{eg: } \text{CH}_4, \text{CH}_3-\text{CH}_3, \text{cyclohexane}

→\to π−π∗\pi - \pi^*

→\to mainly it is observed by molecules containing double bond or tripple bond.

→\to it can be used for determine the organic functional grp.

→\to The value depends upon the conjugation of the molecule.

eg: alkene (CH2=CH2),alkyne (CH≡CH),benzene\text{eg: alkene } (CH_2=CH_2), \text{alkyne } (CH\equiv CH), \text{benzene}.

→\to n−π∗n - \pi^*

→\to mainly observed by molecules with lone pairs of electron and multiple bond

→\to It can be used for determinem the functional groop

eg: carboxylic acid group,aldehydes,ketone,amide,ester\text{eg: carboxylic acid group}, \text{aldehydes}, \text{ketone}, \text{amide}, \text{ester}


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⇒n−σ∗‾\Rightarrow \underline{n-\sigma^*}

→\rightarrow mainly observed by molecule with nn electrons and sigma bond. →\rightarrow It contains hetero atoms. such as, oxygen, [uncertain: ni...]

e.g: CH3NH2CH_3NH_2, Alcohol, ether

Effect of conjugation in UV-visible spectroscopy

⇒\Rightarrow On increasing the conjugation, stability of the molecule increases. So ΔE\Delta E decreases and λmax\lambda_{max} increases.

ΔE=hcλ\Delta E = \frac{hc}{\lambda}

  1. CH2=CH2→CH_2 = CH_2 \rightarrow ethene (169nm169nm)

  2. Buta-1,3-diene - N\mathbb{N} (217nm217nm)

  3. hex-1,3,5-triene - NN\mathbb{NN} (247nm247nm).

  4. benzene - ⟨⟩\langle \rangle - (255nm255nm).

  5. ethene

Energy level diagram for ethene transition showing \\psi_1 and \\psi_2 levels and 169 nm transition


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  1. buta-1, 3-diene

Energy level diagram for buta-1,3-diene with 4 molecular orbitals

  1. hexa-1, 3, 5-triene.

Energy level diagram for hexa-1,3,5-triene with 6 molecular orbitals

  1. benzene.

Energy level diagram for benzene with 6 molecular orbitals

  • Arrange the increasing order of uv-visible absorption or λmax\lambda_{max} (or reverse to ΔE\Delta E).

Structural formulas comparing conjugated systems in increasing order of UV-visible absorption


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  1. List out the allowed transition observed in the following molecule ?

Chemical structures of acetone and aniline

Chemical structure of phenol

Chemical structure of 1-butyne

Chemical structure of pentane

Chemical structure of ethanol

Chemical structure of methoxymethane

Table of compounds, main functional groups and transitions

compoundMain functional grptransition
AcetoneC=OC=O (carbonyl)n→π∗n \rightarrow \pi^*, π→π∗\pi \rightarrow \pi^* [uncertain: ...]
aniline−NH2-NH_2 (aromatic ring)π→π∗\pi \rightarrow \pi^*, n→π∗n \rightarrow \pi^*, [uncertain: ...]
phenol−OH-OH (aromatic ring)π→π∗\pi \rightarrow \pi^*, n→π∗n \rightarrow \pi^*, [uncertain: ...]
1-butyneC≡CC \equiv C (alkyne)π→π∗\pi \rightarrow \pi^*, σ→σ∗\sigma \rightarrow \sigma^*
pentanealkaneσ→σ∗\sigma \rightarrow \sigma^*
ethanol−OH-OHn→σ∗n \rightarrow \sigma^*, σ→σ∗\sigma \rightarrow \sigma^*
methoxymethaneEthern→σ∗n \rightarrow \sigma^*, σ→σ∗\sigma \rightarrow \sigma^*

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Instrumentation of UV-visible spectroscopy

block diagram

flowchart LR S["Radiation source"] --> M["Monochromator"] --> B["Beam divider"] B --> R["Blank / reference cell"] --> DR["Reference detector"] B --> C["Sample cell"] --> DC["Sample detector"] DR --> A["Amplifier"] DC --> A A --> REC["Recorder"] --> O["Absorbance vs wavelength"]

Components In UV-visible spectroscopy

  • Radiation source.   ⟹  \implies Tungsten filament lamp. or HH-discharge lamp. or xenon flash lamp.
  • Monochromator.
  • Beam divider.
  • Cuvette For reference and sample.
  • Blank detector, sample detector.
  • Amplifier.
  • Recorder.

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monochromator →\rightarrow prism or grating

beam divider →\rightarrow split in to two, one through reference & other through sample

cuvette →\rightarrow container →\rightarrow sample →\rightarrow molecule dissolved in suitable solvent. reference →\rightarrow solvent only

blank detector }→\left.\begin{matrix}\\ \\ \end{matrix}\right\}\rightarrow Generally electronic detectors are used. sample detector

A beam of light split in to two equal beams one is pass through sample (II) and other through reference (I0I_0). Then the intensity of these light beam are measured after passing through sample and reference by using electronic detectors and compared.

If I0=I→I_0 = I \rightarrow light does not absorbed by sample

If I0>I→I_0 > I \rightarrow light absorbed by sample and it's recorded in the plot of absorbance v/s wavelength in nm.


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Applications of uv-visible spectroscopy

  • ⇒\Rightarrow [illegible] different transitions absorbed
  • ⇒\Rightarrow Identifications of materials.
  • ⇒\Rightarrow To study about the molecules and materials by using its λ\lambda max value.
  • ⇒\Rightarrow Identification of functional groups using n−π∗n-\pi^* & π−π∗\pi-\pi^* transitions.
  • ⇒\Rightarrow To study about coloured materials and dyes
  • ⇒\Rightarrow To identifies the impurities present in a material by comparing the uv-visible absorption.
  • ⇒\Rightarrow To study about the kinetics of a reaction.
  • ⇒\Rightarrow To find out the unknown concentration by graphical representation.

IR-spectroscopy / vibrational spectroscopy

  • ⇒\Rightarrow It is a plot of percentage transmittence v/s wave numbers (cm−1cm^{-1})
  • ⇒\Rightarrow The range 500cm−1⟶400cm−1500 cm^{-1} \longrightarrow 400 cm^{-1}

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-> Principle

When a molecule interact with IR radiation vibrational transition will occur between vibrational energy level by absorbing IR-Radiation. It is also called vibration spectrum, since transition occur between vibrational energy level.

IR spectrum graph showing transmittance versus wave number

-> The photons of IR radiations are not energetic enough to cause electronic transition.

-> By absorbing IR radiation by a molecule, vibrations will occur (either stretching or bending).


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vibrations.

Flowchart showing classification of vibrations into stretching and bending, with their further subdivisions and molecular illustrations.

  • Different types of bonds & different functional groups can be identified by this vibrational methods modes.

  • The absorption is followed, νˉ=12πcKμ\bar{\nu} = \frac{1}{2\pi c} \sqrt{\frac{K}{\mu}} μ=m1m2m1+m2\mu = \frac{m_1 m_2}{m_1 + m_2}

K=K = Force constant (strength of a bond).

μ=\mu = reduced mass.

Here, m₁ and m₂ are the masses of the connected atoms.


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→\rightarrow no. of vibrational bands modes in IR spectroscopy.

→\rightarrow Then for a molecule of with 'n' no. of atoms, no. of degrees of freedom = 3n3n.

Linear molecule

→\rightarrow no. of translational modes = 33

→\rightarrow no. of rotational modes = 22

→\rightarrow no. of vibrational modes = 3n−53n - 5

Example,

→\rightarrow HCl, n=2n = 2, linear molecule.

no. of vibrational modes = 3×2−53 \times 2 - 5 =6−5=1//= 6 - 5 = 1 //.

→\rightarrow HCl have only symmetric strething

→\rightarrow Dipole moment will be change so IR active.

⇒\Rightarrow H2H_2 n=2n = 2.

no. of vibrational modes = 2×3−5=1//2 \times 3 - 5 = 1 //.

symmetric streching.

→\rightarrow no change in dipole moment. IR inactive.


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Homonuclear diatomic molecules are IR inactive.

eg: H2,O2,Cl2,N2H_2, O_2, Cl_2, N_2.

→\rightarrow No change in dipole moment during vibration.

Heteronuclear diatomic molecules are IR active.

eg: HCl,HBr,HIHCl, HBr, HI

→\rightarrow Change in dipole moment during vibration.

polynuclear molecules - all are IR active

eg: CO2,HCN,H2O,CH4,C6H6CO_2, HCN, H_2O, CH_4, C_6H_6

→\rightarrow Change in dipole moment during vibration.

Non-linear molecules - No. of vibrational modes

→\rightarrow No. of translational modes = 3.

→\rightarrow No. of vibrational modes = 3n−63n - 6.

→\rightarrow No. of rotational modes = 3.

eg:

→H2O\rightarrow H_2O - non-linear.

→\rightarrow No. of vibrational modes.

=3n−6= 3n - 6

=3×3−6= 3 \times 3 - 6

=3//= 3 \text{//}.


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Vibrational modes of CO₂

CO₂ is a linear molecule with n = 3 atoms, so it has

3n−5=3(3)−5=43n-5=3(3)-5=4

vibrational modes.

1. Symmetric stretching

Symmetric stretching of CO2 with arrows pointing away from the center or inwards

The dipole moment does not change during this vibration. Symmetric stretching is IR inactive.

2. Asymmetric stretching

Asymmetric stretching of CO2

The dipole moment changes during this vibration, so asymmetric stretching is IR active.

3. In-plane bending

In-plane bending mode of CO2

This vibration changes the dipole moment and is IR active. The second bending mode continues on the next page.


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CO2 out of plane bending molecular diagram showing central C atom and two O atoms with directional arrows

  • out of plane bending.
  • IR absorption at ∼650 cm−1\sim 650\text{ cm}^{-1}
  • change in dipole moment.
  • IR inactive.

conclusion

  • for CO2\text{CO}_2 4 vibrational modes - 3 are active but only 2 signals.
  1. H2O\text{H}_2\text{O}
  • non linear molecules.

n=3n = 3

No. of vibrational mode

=3n−6= 3n - 6

=3×3−6=3//= 3 \times 3 - 6 = 3 //.

(1)

H2O symmetric stretching molecular diagram showing central O atom and two H atoms with directional arrows

  • change in dipole moment.
  • symmetric stretching.
  • IR active.

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(2).

Asymmetric stretching vibration of a molecule

→\rightarrow assymetric stretching.

→\rightarrow IR active.

→\rightarrow change in dipole moment.

(3).

Bending vibration of a molecule

→\rightarrow IR active.

→\rightarrow Bending vibration.

→\rightarrow change in dipole moment.

  • Predict the following based on IR activity and give reason?
  1. CO2CO_2 →\rightarrow poly nuclear molecule.

→\rightarrow IR active.

  1. cyclohexane (C6H12C_6H_{12}) →\rightarrow poly nuclear molecule

→\rightarrow IR active.

→\rightarrow change in dipole moment.

  1. F2F_2 →\rightarrow IR inactive.

→\rightarrow no change in [illegible]


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[illegible] ⟶\longrightarrow poly nuclear. ⟶\longrightarrow IR active.

  • How can you distinguish C−CC-C & C=CC=C.
  1. C−CC-C, C=CC=C by using IR spectroscopy.

νˉ=12πckμ\bar{\nu} = \frac{1}{2\pi c} \sqrt{\frac{k}{\mu}}

\mu - \text{same}\\ k - \text{diff} \end{matrix}\right\} \text{IR absorption will be different.}$ 2) $C-C$, $C=C$ $\bar{\nu} = \frac{1}{2\pi c} \sqrt{\frac{k}{\mu}}$ $\left.\begin{matrix} k - \text{same}\\ \mu - \text{diff} \end{matrix}\right\} \text{IR absorption will be different.}$ <u>Applications</u> * To study about molecules, materials by using IR absorption value $(\text{cm}^{-1})$ * Identification of Functional grps. $\begin{aligned} OH & \simeq 3400 \text{ cm}^{-1} - 3600 \text{ cm}^{-1} \\ C=O & \simeq 1700 \text{ cm}^{-1} - 1800 \text{ cm}^{-1} \end{aligned}$ ---

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NH≈3200 cm−1−3400 cm−1NH \approx 3200 \text{ cm}^{-1} - 3400 \text{ cm}^{-1} C=C≈1560 cm−1−1650 cm−1C = C \approx 1560 \text{ cm}^{-1} - 1650 \text{ cm}^{-1}

⇒\Rightarrow To identify the impurities present in a sample by comparing the IR absorption value of pure component.

⇒\Rightarrow To study about the kinetics of chemical reaction.

⇒\Rightarrow To study about intra & inter molecular hydrogen bonding.

⇒\Rightarrow ortho hydroxy phenol →\rightarrow →\rightarrow Intra molecular hydrogen bonding on dilution no change in the strength of O-H bond and hydrogen bonding because IR absorption remain unchanged.

Chemical structure of ortho-hydroxy phenol showing intramolecular hydrogen bonding


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Para hydroxy phenol

  • intermolecular hydrogen bonding.
  • on dilution changes in strength of OH bond and IR absorption.

Intermolecular hydrogen bonding in para-hydroxy phenol showing vertical alignment of two phenol rings

Intramolecular hydrogen bonding in ortho-substituted phenol

  • Compare ortho nitrophenol & para nitrophenol with solution?

application => To study about force constant or the strength of the bond

C−C<C=C<C≡CC-C < C=C < C\equiv C 1300165021501300 \quad 1650 \quad 2150


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SEM (Scanning electron microscopy) IMP

-> It's a powerful magnification tool that utilises focused beam of electrons to obtain informations. -> It has high resolving power or resolution (1nm), high depth of field (30μm) and high magnification (300kx). -> It provides topography, morphologic, compositional and crystallographic informations.

Principle

-> SEM scanes a Focus electron beam over a suin to create an image. The electrons in the beam interact with the sample, producing various signals that can be used to obtain information about the surface of the material. -> There mainly two types of electrons are genner


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secondary electron

Secondary electron generation diagram showing an atom with concentric shells, an incoming electron beam, and an ejected secondary electron.

SE is generated by a inelastic interactions.

Widely used for imaging the sample.

Good topographic inform^n with good resolution.

BSE (Back scattered electron)

BSE (Back scattered electron) diagram showing an atom with concentric shells and a primary electron bouncing back out.

⇒\Rightarrow BSE is generated by a inelastic interactions.

⇒\Rightarrow It can also be used for imaging.

⇒\Rightarrow mainly it is generated by heavier elements.

⇒\Rightarrow It gives the information of composition and topography of the sample.

Instrumentation

Components.

  1. Electron source.

  2. Electro magnetic and/or electrostatic lenses [struckout: vacuum] chamber.

  3. computer.

  4. SE detector

  5. BSE detector.

  6. vacuum champer.


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Schematic diagram of a Scanning Electron Microscope (SEM)

Electron source.

Anode.

Condenser lens.

Scan coils.

Objective lens.

Secondary electron detector.

Sample.

Applications

  • SEM helps in the characterisation of solid materials.
  • It can detect and analyse surface structures, surface contamination, and provide information in microstructures.
  • It helps to reveal spacial variation in chemical compositions and to identify crystalline structures.
  • It used as an essential research tool in fields such as life science, nanoscience, medical, gemology and forensic science.

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Dielectric Thermal Analysis (DETA) IMP.

  • It is also known as dielectric analysis (DEA).
  • The technique used to study dielectric property of materials as they undergo changes in temperature.
  • It is mainly used to study about dielectric behaviours of polymers, resins, and adhesives.
  • mainly for polar or semipolar [uncertain: properties].

Principle

  • When applying an electric field to a sample placed between two electrodes and monitoring how samples dielectric properties change with temperature.
  • The mobile charge carrier (ions/dipoles) within the sample align with the electric field, resulting in a [illegible] which can be measured.
  • These responses are directly proportional to sample [uncertain: related] permittivity parameters.

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Instrumentation.

Components of DEA:

  • Dielectric analyzer
  • Furnace
  • Sample holder
  • Frequency generator
  • Data acquisition system

Diagram of furnace and sample holder setup for dielectric analysis

without external electrical field.

Diagram of dipoles inside a material without external electrical field

with external electrical field.

Diagram of dipoles inside a material with external electrical field

You’ve reached the end of S1 CSE Chemistry · Module 3.

Source: KTU GXCYT122 study notes, imported from the provided complete study pack. Check the original material if a step looks unclear.