Molecular Spectroscopy and Analytical Techniques

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34 Terms

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Molecular Spectroscopy

The branch of science dealing with the interaction of matter (atoms or molecules) with electromagnetic radiation, involving the production, measurement, and interpretation of absorption or emission spectra.

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<p>Absorption Spectrum</p>

Absorption Spectrum

A spectrum consisting of dark lines formed when an atom or molecule transitions from a lower energy level to a higher energy level by absorbing a photon of energy hνh\nu equal to the energy difference.

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<p>Emission Spectrum</p>

Emission Spectrum

A spectrum consisting of bright lines obtained when an atom or molecule transitions from a higher energy level to a lower energy level with the emission of a photon of energy hνh\nu, requiring the higher energy state to be more populated.

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Atomic Spectra

Spectra obtained due to the interaction of isolated atoms with electromagnetic radiation, characterized by sharp individual lines (line spectra) originating from electronic transitions.

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Molecular Spectra

Spectra obtained from the interaction of molecules with electromagnetic radiation, consisting of bands (band spectra) where each band contains closely spaced lines from associated vibrational and rotational transitions.

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Electronic Energy Levels

Quantized molecular energy states where electrons occupy bonding, non-bonding, or antibonding molecular orbitals; transitions between these levels fall in the UV-Visible region (200 to 800 nm200\text{ to }800\,nm).

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Vibrational Energy Levels

Quantized energy levels associated with the to-and-fro motion of nuclei in a molecule about their equilibrium positions while the center of mass remains constant; transitions between them fall in the infrared (IR) region.

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Rotational Energy Levels

Quantized energy levels arising from the rotation of a molecule about an axis perpendicular to its internuclear axis passing through the center of mass; transitions between them fall in the microwave region.

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Translational Energy Levels

Energy levels of a molecule whose center of mass changes with time; these levels are negligibly small and only quantized when the molecule is enclosed in a box of nano-dimensions.

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Beer-Lambert's Law

The law stating that the rate of decrease in radiation intensity with path length (−dIdx-\frac{dI}{dx}) through an absorbing solution is directly proportional to the incident intensity (II) and the solute concentration (CC).

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Molar Absorption Coefficient

A constant (ϵ\epsilon) dependent on the nature of the absorbing molecule and absorption wavelength, given by ϵ=ACx\epsilon = \frac{A}{Cx} with units of mol−1 dm2mol^{-1}\,dm^2.

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<p>Absorbance</p>

Absorbance

The logarithm of the ratio of incident light intensity (I0I_0) to transmitted light intensity (II), defined as A=log⁡(I0I)=−log⁡(T)=ϵCxA = \log\left(\frac{I_0}{I}\right) = -\log(T) = \epsilon C x.

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<p>Transmittance</p>

Transmittance

The ratio of transmitted light intensity (II) to incident light intensity (I0I_0), represented as T=II0=e−ϵCxT = \frac{I}{I_0} = e^{-\epsilon C x}, which decreases exponentially with increasing concentration.

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UV-Visible Spectroscopy

An electronic spectroscopy method based on promoting valence electrons from ground state to higher energy molecular orbitals via absorption of ultraviolet (200 to 400 nm200\text{ to }400\,nm) or visible (400 to 800 nm400\text{ to }800\,nm) radiation.

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<p>Electronic Transitions</p>

Electronic Transitions

Promotions of electrons between bonding (σ\sigma, π\pi), non-bonding (nn), and antibonding (σ∗\sigma^*, π∗\pi^*) orbitals upon the absorption of UV or visible light.

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σ→σ∗\sigma \rightarrow \sigma^* Transition

A high-energy electronic transition in saturated hydrocarbons (e.g., methane, ethane) exciting a bonding σ\sigma electron to an antibonding σ∗\sigma^* orbital at wavelengths shorter than 150 nm150\,nm.

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π→π∗\pi \rightarrow \pi^* Transition

An electronic transition observed in unsaturated systems (alkenes, alkynes) from HOMO to LUMO, shifting by approximately 30 nm30\,nm to longer wavelengths with each additional conjugated double bond.

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n→π∗n \rightarrow \pi^* Transition

A low-intensity, symmetry-forbidden electronic transition occurring in molecules containing both heteroatoms with non-bonding lone pairs and π\pi bonds, such as aldehydes and ketones.

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n→σ∗n \rightarrow \sigma^* Transition

A low-intensity electronic transition observed in saturated compounds with non-bonding lone pairs on heteroatoms (SS, NN, OO), such as alcohols and haloalkanes, requiring less energy than $$\sigma \rightarrow \sigma^*$.

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<p>Double-Beam Spectrophotometer</p>

Double-Beam Spectrophotometer

An optical instrument where monochromatic light selected by a slit is divided into two beams passing simultaneously through sample and reference cells before reaching photocell detectors.

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Infrared Spectroscopy

A vibrational spectroscopy technique studying the absorption of IR radiation (500 nm to 4000 cm−1500\,nm\text{ to }4000\,cm^{-1}) to identify functional groups and establish the structural fingerprint of a molecule.

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Infrared Active Molecules

Molecules that experience a net change in dipole moment during vibrational motion, permitting the absorption of IR radiation (e.g., H2OH_2O, SO2SO_2, NH3NH_3, HCNHCN, HBrHBr, HClHCl, HFHF, COCO).

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Infrared Inactive Molecules

Molecules that undergo no change in dipole moment during vibration and consequently do not absorb IR radiation (e.g., Br2Br_2, Cl2Cl_2, N2N_2, H2H_2, O2O_2, F2F_2).

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Fundamental Vibrational Frequency

The characteristic oscillation frequency (ν0\nu_0) of a diatomic molecule treated as a simple harmonic oscillator, calculated by ν0=12πkμ\nu_0 = \frac{1}{2\pi}\sqrt{\frac{k}{\mu}}.

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Reduced Mass

The effective inertial mass (μ\mu) of a two-particle vibrating system, defined as μ=m1m2m1+m2\mu = \frac{m_1 m_2}{m_1 + m_2}.

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Force Constant

A parameter (kk) measuring the bond strength between two bonded atoms, derived from vibrational frequency as k=4π2c2μνˉ2k = 4\pi^2 c^2 \mu \bar{\nu}^2, where kk increases from single to triple bonds (C−C<C=C<C≡CC-C < C=C < C\equiv C).

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Vibrational Degrees of Freedom (Non-linear Molecule)

The number of fundamental vibrational modes in a non-linear molecule of nn atoms, equal to 3n−63n - 6 because 3 degrees correspond to translation and 3 to rotation.

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Vibrational Degrees of Freedom (Linear Molecule)

The number of fundamental vibrational modes in a linear molecule of nn atoms, equal to 3n−53n - 5 because 3 degrees correspond to translation and 2 to rotation.

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Vibrational Modes of Carbon Dioxide

The four fundamental vibrational modes (3×3−5=43\times 3 - 5 = 4) of linear CO2CO_2: one symmetric stretching mode (IR inactive) and three IR active modes (one asymmetric stretch and two bending vibrations).

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<p>Vibrational Modes of Water</p>

Vibrational Modes of Water

The three fundamental modes of non-linear H2OH_2O (3×3−6=33\times 3 - 6 = 3)—antisymmetric stretch, symmetric stretch, and scissoring bend—all of which cause a net dipole moment change and are IR active.

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<p>Intramolecular Hydrogen Bonding</p>

Intramolecular Hydrogen Bonding

Hydrogen bonding occurring internally within a single molecule (e.g., o-hydroxy phenol) whose characteristic −OH-OH stretching absorption frequency does not shift upon dilution.

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<p>Intermolecular Hydrogen Bonding</p>

Intermolecular Hydrogen Bonding

Hydrogen bonding formed between adjacent molecules (e.g., p-hydroxy phenol) that weakens and dissociates upon dilution, causing a detectable shift in the −OH-OH absorption frequency.

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<p>Dielectric Thermal Analysis</p>

Dielectric Thermal Analysis

A thermal analysis technique (DETA) measuring changes in dielectric properties (conductance GG and capacitance CC) of a material placed under an alternating electric field across varying temperatures.

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Dielectric Loss Tangent

The dissipation factor ($$\tan(\delta) = \frac{\epsilon_{11}}{\epsilon_