High-Resolution Research FTIR Spectrometer
Equipped with a globar mid-IR ceramic source, Ge-coated KBr beam splitter, and liquid-nitrogen-cooled MCT (mercury cadmium telluride) detector delivering 0.25 cm⁻¹ optical resolution.
Determine the fundamental vibrational frequency (ν̃₀ = 2885.90 cm⁻¹), vibration-rotation coupling constant (α_e = 0.3072 cm⁻¹), and harmonic bond force constant (k = 481.0 N/m) of gas-phase hydrogen chloride (H³⁵Cl) using high-resolution FTIR spectroscopy. Explore interactive analytical gravimetry, Class A volumetric glassware and density determination.
Ready to dispense 3.0 of liquid.
Adjust m V, then weigh the dispensed aliquot.
Mass observations are determined by the high-precision thermodynamic equation of state for pure liquid water. Readings reflect thermal equilibrium and analytical balance force restoration.
['The harmonic oscillator force constant k is extracted from the fundamental band origin ν̃₀, which includes minor anharmonic correction terms (ν̃₀ = ω_e − 2ω_e x_e).', 'At sample pressures exceeding 50 Torr, self-broadening obscures the narrow rotational lines, precluding baseline deconvolution of the ³⁵Cl and ³⁷Cl isotopologue peaks.', 'Centrifugal distortion constants (D_e ≈ 5.3 × 10⁻⁴ cm⁻¹) introduce minor high-J deviations (J > 8) that are neglected in the truncated quadratic model.'] The physical chemistry simulation model evaluates gas-phase H³⁵Cl at 25.0 °C (sample pressure 25.0 Torr, 100.0 mm path length). System parameters: reduced mass μ(H³⁵Cl) = 1.626652 × 10⁻²⁷ kg; fundamental band origin ν̃₀ = 2885.90 cm⁻¹; equilibrium rotational constant B_e = 10.5934 cm⁻¹; vibration-rotation coupling constant α_e = 0.3072 cm⁻¹; ground state rotational constant B₀ = 10.4398 cm⁻¹; excited state rotational constant B₁ = 10.1326 cm⁻¹. Across the six rotational pairs m = [1, 2, 3, 4, 5, 6], measured mean transition wavenumbers are ν̃_mean = [2885.593, 2884.671, 2883.135, 2880.985, 2878.220, 2874.841] cm⁻¹. Plotting ν̃_mean against m² = [1, 4, 9, 16, 25, 36] yields a linear slope of −α_e = −0.30719 cm⁻¹ (α_e = 0.3072 cm⁻¹) and Y-intercept ν̃₀ = 2885.900 cm⁻¹ with R² = 1.0000000. Applying the harmonic relation k = 4π²c²ν̃₀²μ extracts an empirical force constant k = 480.68 N/m (difference = 0.0660% from the 481.0 N/m literature benchmark), confirming quantum mechanical harmonic and anharmonic oscillator models.
Equipped with a globar mid-IR ceramic source, Ge-coated KBr beam splitter, and liquid-nitrogen-cooled MCT (mercury cadmium telluride) detector delivering 0.25 cm⁻¹ optical resolution.
Stainless steel or Pyrex cylindrical gas cell (100.0 ± 0.1 mm internal path length) fitted with water-insoluble, cleaved single-crystal sodium chloride (NaCl) windows transparent from 4000 to 650 cm⁻¹.
Pyrex vacuum manifold evacuated by a turbomolecular pump to < 10⁻⁴ Torr, equipped with capacitive capacitance manometer and chemical traps for synthesis and cryogenic transfer of anhydrous HCl gas.
Generates pure, anhydrous hydrogen chloride gas by controlled dropwise addition of concentrated sulfuric acid (18 M H₂SO₄) to analytical grade ammonium chloride or sodium chloride, followed by cryogenic trap distillation.
Continuously purges the FTIR interferometer and sample compartment at 25 L/min with dry, CO₂-free air (dew point < −70 °C) to eliminate atmospheric H₂O and CO₂ ro-vibrational absorption bands.
Measures gas cell fill pressure with 0.1 Torr readability; standard measurements are recorded at 25.0 ± 0.5 Torr HCl to achieve optimal peak absorbance without pressure-broadening artifacts.
Determine the fundamental vibrational frequency (ν̃₀ = 2885.90 cm⁻¹), vibration-rotation coupling constant (α_e = 0.3072 cm⁻¹), and harmonic bond force constant (k = 481.0 N/m) of gas-phase hydrogen chloride (H³⁵Cl) using high-resolution FTIR spectroscopy. Suggested independent volumetric settings: 1.0, 2.0, 3.0, 4.0, 5.0, 6.0 .
Initiate dry nitrogen purge of the FTIR optical bench at 25 L/min for 60 minutes. Fill the MCT detector dewar with liquid nitrogen and allow 20 minutes of thermal stabilization. Record a 64-scan background single-beam spectrum of the evacuated sample compartment across 4000 to 2000 cm⁻¹ at 0.5 cm⁻¹ resolution.
Mount the 100 mm NaCl-window gas cell onto the vacuum manifold. Evacuate to below 0.05 Torr. Admit anhydrous HCl gas through a cryogenic dry ice-acetone trap until the cell pressure reaches 25.0 ± 0.5 Torr. Close the PTFE isolation valves, dismount the cell, and position it securely in the spectrometer sample compartment.
Collect 64 co-added interferograms of the filled gas cell at 0.5 cm⁻¹ resolution with Blackman-Harris 3-term apodization and 2× zero filling. Transform the interferogram into an absorbance spectrum spanning 3100 to 2600 cm⁻¹, resolving the fundamental vibration-rotation band of HCl.
Identify the characteristic doublet structure of each rotational transition corresponding to H³⁵Cl and H³⁷Cl (3:1 natural abundance ratio). Using second-derivative peak centroid algorithms, determine the exact peak wavenumbers for the six pairs of R-branch lines (R(0) through R(5)) and P-branch lines (P(1) through P(6)) for H³⁵Cl.
For each rotational running index m from 1 to 6 (where R(m−1) has index +m and P(m) has index −m), compute the mean transition wavenumber: ν̃_mean(m) = [ν̃_R(m−1) + ν̃_P(m)] / 2. Verify that ν̃_mean decreases quadratically from 2885.593 cm⁻¹ at m = 1 to 2874.841 cm⁻¹ at m = 6.
Plot ν̃_mean(m) on the Y-axis against m² on the X-axis across the six experimental pairs. Perform ordinary least-squares linear regression to extract the slope (−α_e) and Y-intercept (ν̃₀). From the fundamental band origin ν̃₀ = 2885.90 cm⁻¹ and reduced mass μ = 1.62665 × 10⁻²⁷ kg, calculate the harmonic bond force constant: k = 4π²c²ν̃₀²μ.
Points are your recorded gravimetric observations. The regression line validates the linear mass-volume proportionality and extracts density.
| # | Rotational Transition Quantum Index m () | Mean Branch Transition Wavenumber ν̃_mean (cm⁻¹) | Squared Rotational Index m² | Mean Transition Wavenumber ν̃_mean (cm⁻¹) | Remove |
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