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cm^-1
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0.7172
The Vibrational Spectroscopy Calculator computes the fundamental vibrational frequency, energy levels, and zero-point energy for a diatomic molecule modeled as a quantum harmonic oscillator. Vibrational spectroscopy (infrared and Raman spectroscopy) is one of the most widely used analytical techniques in chemistry, providing molecular fingerprints for identification, structural analysis, and quantitative measurements.
The quantum harmonic oscillator model gives vibrational energy levels E_v = (v + 1/2) * h * nu, where v = 0, 1, 2... is the vibrational quantum number and nu = (1/2*pi) * sqrt(k/mu) is the fundamental frequency (k is the force constant, mu is the reduced mass). The IR selection rule requires a change in dipole moment (delta_v = ±1 for harmonic oscillator), while Raman spectroscopy requires a change in polarizability.
The fundamental vibrational frequency in wavenumbers (cm^-1) directly identifies functional groups: O-H and N-H stretches near 3200-3600 cm^-1, C-H near 2800-3100 cm^-1, C=O near 1700-1750 cm^-1, C-C near 800-1200 cm^-1. The fingerprint region (400-1500 cm^-1) contains complex combinations of bending and stretching modes unique to each molecule.
The harmonic oscillator is an approximation. Real bonds are anharmonic: the potential energy curve is not perfectly parabolic, leading to anharmonicity constants that make higher overtone transitions slightly different in energy and allowing dissociation at high vibrational levels. Nevertheless, the harmonic approximation works excellently for the lowest few vibrational levels.
Isotope effects in vibrational spectroscopy (comparing H vs D, 12C vs 13C) are calculable from the reduced mass ratio, providing mechanistic information in chemical kinetics and confirming structural assignments in complex molecules.
Fundamental frequency: nu = (1/2*pi)*sqrt(k/mu) Hz. In wavenumbers: nu_bar = nu/c (cm^-1). Vibrational energy: E_v = (v+1/2)*h*nu eV. Zero-point energy: E_0 = (1/2)*h*nu. Isotope effect (H to D substitution): nu_D/nu_H = sqrt(mu_H/mu_D).
C-H stretch: k ~ 450-530 N/m, nu_bar ~ 2800-3100 cm^-1 (IR active, strong). C=O stretch: k ~ 1100-1200 N/m, nu_bar ~ 1650-1750 cm^-1 (very strong IR). O-H stretch in water: k ~ 780 N/m, nu_bar ~ 3600 cm^-1 (broad due to H-bonding). Doubling k increases frequency by sqrt(2) ~ 1.41x. Doubling mass decreases frequency by sqrt(2).
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HCl fundamental stretch at ~2991 cm^-1 (literature: 2991 cm^-1). ZPE = 0.185 eV. DCl would absorb at 2991/1.372 ~ 2179 cm^-1, consistent with observed DCl stretch.
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The C=O stretch in CO (k~1855 N/m) appears at ~2143 cm^-1. Using k=1150 gives v=1 level at 0.532 eV. Carbonyl groups in organic molecules appear at 1700-1750 cm^-1 with lower force constants.
A vibration is IR-active if it involves a change in dipole moment. Asymmetric stretches and bends of polar bonds are IR-active. Symmetric stretches of homonuclear diatomics (N2, O2) are IR-inactive because they do not change the dipole moment.
A vibration is Raman-active if it involves a change in polarizability. Symmetric stretches are often Raman-active but IR-inactive. The mutual exclusion rule: in molecules with a center of symmetry, no vibration can be both IR and Raman active simultaneously.
Real bonds deviate from the ideal harmonic oscillator potential at large displacements. Anharmonicity causes overtone transitions at frequencies slightly below 2*nu_bar, 3*nu_bar, allows dissociation at high v, and causes hot bands to appear at room temperature.
The 400-1500 cm^-1 region in IR spectra where complex combinations of bending, stretching, and skeletal vibrations occur, unique to each molecule. It is used for identification like a molecular fingerprint, even though individual peaks are harder to assign.
O-H groups involved in hydrogen bonding vibrate over a range of frequencies because H-bond strengths vary. This gives broad absorption bands at 2500-3300 cm^-1 for carboxylic acids and 3200-3550 cm^-1 for alcohols.
Replacing H with D (deuterium, ~twice the mass) reduces the reduced mass and lowers the vibrational frequency by a factor of sqrt(2) ~ 1.41. This shifts O-H stretches (~3400 cm^-1) to O-D (~2500 cm^-1), useful for confirming assignments.
A collective vibration of all atoms in a molecule that oscillate in phase with the same frequency. A molecule with N atoms has 3N-6 vibrational normal modes (3N-5 for linear molecules). Each normal mode has its own frequency and symmetry.
Raman spectroscopy provides complementary information to IR: it is sensitive to symmetric, nonpolar vibrations (C=C, C-C, S-S stretches), works well in aqueous solution (water has weak Raman signal), and can be used for in vivo biomedical imaging.
Stronger bonds (higher bond order) have larger force constants. For carbon: C-C k~450 N/m, C=C k~950 N/m, C-C triple bond k~1650 N/m. Measuring k from IR spectroscopy gives direct experimental evidence for bond strength.
Fourier Transform Infrared spectroscopy uses a Michelson interferometer to measure all IR frequencies simultaneously, then Fourier transforms the interferogram to a spectrum. It is faster, more sensitive, and higher resolution than dispersive IR instruments.
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