Thermal Analysis Freezing Point Glass Cell
Double-walled vacuum-jacketed glass tube with internal PTFE mechanical paddle stirrer for controlled cooling.
Construct the solid-liquid equilibrium (SLE) phase diagram for a binary naphthalene-biphenyl organic eutectic mixture using thermal analysis cooling curves across solute mole fractions x_B from 0.04 to 0.24, evaluate freezing point depression ΔT_f, determine the cryoscopic limiting slope, and extract the eutectic point coordinates. Explore interactive transport phenomena, unit operations simulation, and chemical engineering telemetry.
Ready to sample with Solute Mole Fraction x_B = 0.12 mol/mol.
Adjust Solute Mole Fraction x_B, then execute chemical process trial.
Chemical and process engineering telemetry is evaluated rigorously using 64-bit IEEE 754 precision. Residuals reflect ordinary least-squares regression across successive observations. Continuous data structures support high-fidelity transport phenomena and unit operations modeling.
The transport and thermodynamic models apply within the specified calibrated operating window (0.04 to 0.24 mol/mol). Evaluated using an automated thermal analysis cooling cell with 4-wire Pt100 RTD sensor (±0.02 °C) and programmable air-jacketed cooling mantle. Pure naphthalene: T_mA = 80.20 °C, ΔH_fus,A = 18.98 kJ/mol; pure biphenyl: T_mB = 69.20 °C, ΔH_fus,B = 18.58 kJ/mol.
Double-walled vacuum-jacketed glass tube with internal PTFE mechanical paddle stirrer for controlled cooling.
Measures melt temperature with 0.01 °C resolution and 5 Hz sampling rate to record cooling curve inflection points.
Melts organic mixtures up to 100.0 °C and maintains uniform liquid temperature before cooling.
Provides steady, reproducible convective heat removal rate of 1.5 to 2.0 °C/min during solidification.
Maintains continuous 120 RPM vertical agitation to eliminate thermal stratification and minimize supercooling.
Weighs naphthalene and biphenyl components gravimetrically to establish exact synthetic mole fractions.
Construct the solid-liquid equilibrium (SLE) phase diagram for a binary naphthalene-biphenyl organic eutectic mixture using thermal analysis cooling curves across solute mole fractions x_B from 0.04 to 0.24, evaluate freezing point depression ΔT_f, determine the cryoscopic limiting slope, and extract the eutectic point coordinates. Standardized parameter settings: 0.04, 0.08, 0.12, 0.16, 0.2, 0.24 mol/mol.
Calibrate the Pt100 RTD sensor against distilled ice point (0.00 °C) and boiling water (100.00 °C); record cooling curve of pure naphthalene to verify T_mA = 80.20 °C.
Weigh exactly 10.000 g of naphthalene and add calculated mass of biphenyl to synthesize x_B = 0.04 into the freezing tube.
Immerse sample tube in 95.0 °C silicone oil bath until solids are completely melted; stir gently to ensure homogeneous liquid mixing.
Transfer tube to the air-jacketed cooling assembly; start reciprocating stirrer at 120 RPM and begin logging temperature versus time at 2 Hz.
Identify the liquidus freezing point T_f from the cooling curve slope change (inflection from sensible cooling to crystal latent heat plateau); compute ΔT_f = T_mA - T_f.
Add subsequent increments of biphenyl to achieve x_B = 0.08, 0.12, 0.16, 0.20, and 0.24, repeating the melt-cool protocol to determine cryoscopic slope S.
Points are your recorded observations. The solid regression line validates SLE Eutectic Phase Diagram mathematical scaling.
| # | Biphenyl Solute Mole Fraction x_B (mol/mol) | Freezing Point Depression ΔT_f (°C) | Biphenyl solute mole fraction x_B (mol/mol) | Freezing point depression ΔT_f (°C) | Remove |
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Solid-liquid equilibrium (SLE) phase diagrams are foundational to chemical engineering crystallization, melt purification, pharmaceutical co-crystal formulation, metallurgy, and thermal energy storage phase-change materials (PCMs). When two chemical species are completely miscible in the liquid melt but mutually immiscible in the solid crystalline state, they form a simple binary eutectic system. The classic chemical engineering model system is the binary mixture of naphthalene (component A, pure melting point T_mA = 80.20 °C) and biphenyl (component B, pure melting point T_mB = 69.20 °C). In this system, adding solute B to pure liquid A depresses the liquidus temperature—the temperature at which the first pure crystal of component A nucleates from the melt. According to the Schröder–van Laar equation derived from chemical potential equality between pure solid A and liquid solution A: ln(γ_A · x_A) = -[ΔH_fus,A / R] · [1/T - 1/T_mA], where ΔH_fus,A is the standard enthalpy of fusion (18.98 kJ/mol for naphthalene) and γ_A is the liquid-phase activity coefficient. In the dilute solute regime (x_B = 1 - x_A << 1), the liquid behaves nearly ideally (γ_A ≈ 1.00), and expanding the reciprocal temperature term in a first-order series yields the linear cryoscopic freezing point depression relation: ΔT_f = T_mA - T = S · x_B, where the cryoscopic limiting slope is given by S = R · T_mA^2 / ΔH_fus,A = 58.5000 °C (K). Continued addition of solute B depresses the liquidus until it intersects the second liquidus curve of component B at the eutectic point (T_eutectic ≈ 39.4 °C, x_B,eutectic ≈ 0.45), where both solid A and solid B crystallize simultaneously at a unique invariant temperature. In this laboratory experiment, an instrumented thermal analysis freezing point apparatus records time-temperature cooling curves across biphenyl mole fractions from 0.04 to 0.24 to identify the liquidus break temperatures, confirm the linear cryoscopic slope S = 58.5000 °C, and construct the complete SLE phase boundary.
Evaluated using an automated thermal analysis cooling cell with 4-wire Pt100 RTD sensor (±0.02 °C) and programmable air-jacketed cooling mantle. Pure naphthalene: T_mA = 80.20 °C, ΔH_fus,A = 18.98 kJ/mol; pure biphenyl: T_mB = 69.20 °C, ΔH_fus,B = 18.58 kJ/mol.