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ASTM D1015-05 (Reapproved 2015) specifies a precise procedure for measuring the freezing points of high-purity hydrocarbons. The method relies on the interpretation of time-temperature freezing or melting curves to determine an accurate freezing point, which is then used with Test Method D1016 to calculate the molal purity of the sample.
This test method covers the precise measurement of the freezing points of high-purity hydrocarbons, with SI units regarded as the standard. The measured freezing point, when interpreted with the physical constants found in Test Method D1016, allows for the calculation of the material’s purity. This knowledge is vital for controlling manufacturing processes and determining suitability for use as reagent chemicals, chemical intermediates, or finished products (Section 4).
The required apparatus includes a specialized freezing tube, a metal sheath with specific venting, Dewar flasks for both cooling and warming baths, a stirring mechanism, and absorption tubes. The outer walls of the Dewar flasks should be taped to reduce the hazard of broken glass. The critical instrument for measurement is the resistance bridge.
| 🟦 Component | 📏 Specification / Requirement |
|---|---|
| Resistance Bridge | Mueller Type |
| Measurement Range | 0.0001 Ω to 50 Ω |
| Reading Resolution | 0.001 Ω |
| Cooling / Warming Baths | Dewar Flasks |
The test method also relies on several key companion standards for sampling and data analysis.
| 📐 Referenced Standard | 🎯 Title / Application |
|---|---|
| D1016 | Purity of Hydrocarbons from Freezing Points |
| D1265 | Practice for Sampling Liquefied Petroleum (LP) Gases |
| D4057 | Practice for Manual Sampling of Petroleum Products |
The primary measurement is the precise freezing point, derived from a carefully constructed time-temperature curve. The flatness of the melting or freezing plateau is a direct indicator of the sample’s purity. Using the cryoscopic constants and procedures detailed in Test Method D1016, this freezing point measurement is converted into a precise molal purity value.
The standard precisely measures the freezing points of high-purity hydrocarbons. This measurement is the critical step for calculating the molar purity of the sample using the companion standard, Test Method D1016.
High-purity hydrocarbons exhibit very sharp freezing points. A Mueller bridge offers the extremely high sensitivity (0.001 Ω resolution) over a wide range (0.0001 Ω to 50 Ω) needed to construct the detailed time-temperature curves required for accurate purity calculation.
Section 5.1 warns of a potential explosive breakage hazard when using liquid nitrogen without a properly vented metal sheath. The sheath must have side and bottom openings to prevent liquefied oxygen from accumulating and becoming sealed by ice.
Accuracy is ensured by strict adherence to the specified apparatus (Mueller bridge, Dewar flasks), controlled thermal conditions, proper sampling techniques (D1265, D4057), and mathematically rigorous data analysis using the cryoscopic constants provided in Test Method D1016.