Gay-Lussac Calibrated Pycnometer (25.000 cm³)
Precision borosilicate glassware featuring ground glass capillary stopper designed to maintain an invariant volumetric capacity of 25.000 ± 0.003 cm³ under controlled thermal equilibrium.
To determine the density of a series of binary ethanol-water mixtures using high-precision Gay-Lussac pycnometry at 25.0 °C, compute the apparent molar volume (\phi_V) of ethanol as a function of molality, and evaluate the limiting partial molar volume of ethanol at infinite dilution (\bar{V}_2^\infty) and excess thermodynamic properties via linearized extrapolation. Explore interactive analytical gravimetry, Class A volumetric glassware and density determination.
Ready to dispense 1.5 mol/kg of liquid.
Adjust ethanol molality 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.
Gay-Lussac pycnometry assumes that ambient room temperature does not diverge significantly from the bath setpoint (25.00 °C) during the brief weighing period, minimizing capillary expansion overflow. At higher ethanol concentrations (> 3 mol/kg or > 15 wt%), non-linear higher-order solute-solute clustering effects require quadratic terms in the molality expansion. The physical simulation calculates binary solution densities and apparent molar volumes at 25.00 °C governed by φ_V = (1/m) · [ (1000 + m·M₂)/ρ − 1000/ρ₀ ], where solvent is Millipore water (M₁ = 18.015 g/mol, ρ₀ = 0.997047 g/cm³) and solute is anhydrous ethanol (M₂ = 46.069 g/mol, pure molar volume V₂* = 58.68 cm³/mol). In the dilute regime (m = 0.50 to 3.00 mol/kg), non-electrolyte hydrophobic hydration dictates linear apparent volume expansion: φ_V(m) = φ_V° + b_V·m, with limiting partial molar volume at infinite dilution φ_V° = V̄₂^∞ = 54.20 cm³/mol and slope b_V = +0.250 cm³·kg·mol⁻². For a calibrated 25.000 cm³ Gay-Lussac pycnometer with dry tare mass m₀ = 18.4250 g, filled pycnometer masses span 43.2529 g (m = 0.50 mol/kg, ρ = 0.99312 g/cm³) down to 42.7912 g (m = 3.00 mol/kg, ρ = 0.97465 g/cm³). Ordinary least-squares linear regression extracts the intercept b = 54.20 cm³/mol with R² = 0.99998, validating limiting partial molar volume without bias and demonstrating volumetric contraction of 4.48 cm³/mol due to interstitial cavity accommodation.
Precision borosilicate glassware featuring ground glass capillary stopper designed to maintain an invariant volumetric capacity of 25.000 ± 0.003 cm³ under controlled thermal equilibrium.
Dual-range electronic analytical balance with 0.0001 g resolution, automated internal calibration, and draft-shielded pan for gravimetric measurement of pycnometer tare and filled masses.
Constant-temperature bath regulated to 25.00 ± 0.01 °C with continuous fluid circulation to equilibrate pycnometers and eliminate thermal expansion density drift.
Set of 100 mL airtight borosilicate volumetric and glass flasks with PTFE stopcocks used to synthesize precise binary ethanol-water solutions across 0.5 to 3.0 mol/kg.
Specialized lintless optical paper used to wipe external pycnometer surfaces and blot meniscus overflow at the capillary tip without wicking interior liquid.
High-purity anhydrous ethanol (M₂ = 46.069 g/mol) and vacuum-degassed Type 1 deionized water (M₁ = 18.015 g/mol, ρ₀ = 0.997047 g/cm³ at 25.0 °C).
To determine the density of a series of binary ethanol-water mixtures using high-precision Gay-Lussac pycnometry at 25.0 °C, compute the apparent molar volume (\phi_V) of ethanol as a function of molality, and evaluate the limiting partial molar volume of ethanol at infinite dilution (\bar{V}_2^\infty) and excess thermodynamic properties via linearized extrapolation. Suggested independent volumetric settings: 0.5, 1.0, 1.5, 2.0, 2.5, 3.0 mol/kg.
Thoroughly clean the 25 mL Gay-Lussac pycnometer with chromic acid substitute, rinse repeatedly with deionized water and acetone, dry with warm filtered nitrogen, and record the dry tare mass m₀ on the analytical balance to ±0.0001 g.
Fill pycnometer with freshly boiled, degassed deionized water, seat capillary stopper allowing excess to overflow, equilibrate in the 25.00 °C bath for 20 minutes, wipe dry, weigh (m_water), and calculate exact internal volume V_pyc = (m_water - m₀) / ρ₀.
Prepare six binary solutions of exact ethanol molalities m = 0.50, 1.00, 1.50, 2.00, 2.50, and 3.00 mol/kg solvent by weighing degassed water into flasks followed by anhydrous ethanol, sealing promptly to prevent volatile evaporation.
Rinse pycnometer twice with 3 mL aliquots of the test solution, fill to the brim, insert capillary stopper firmly, and immerse in the 25.00 °C water bath for 20 minutes to reach thermal and volumetric equilibrium.
Carefully remove pycnometer from bath, swiftly touch capillary apex with lint-free paper to bring meniscus flush with the ground rim without capillary draw, wipe exterior dry, and record mass m_soln on the analytical balance to ±0.0001 g.
Repeat duplicate trials for each concentration, compute solution density ρ = (m_soln - m₀) / V_pyc, determine apparent molar volume φ_V = [M₂/ρ − 1000(ρ − ρ₀)/(m·ρ·ρ₀)], and perform linear regression to obtain limiting partial molar volume.
Points are your recorded gravimetric observations. The regression line validates the linear mass-volume proportionality and extracts density.
| # | Ethanol molality m (mol/kg solvent) (mol/kg) | Filled pycnometer total mass m_filled (g) | Ethanol molality m (mol/kg) | Apparent molar volume φ_V (cm³/mol) | Remove |
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No readings yet. Dispense and weigh a volumetric aliquot to record it.