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ASTM-C829 2010

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C829-81(2010) Standard Practices for Measurement of Liquidus Temperature of Glass by the Gradient Furnace Method

Published By Publication Date Number of Pages
ASTM 2010 9
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1.1 These practices cover procedures for determining the liquidus temperature (Note 1) of a glass (Note 1) by establishing the boundary temperature for the first crystalline compound, when the glass specimen is held at a specified temperature gradient over its entire length for a period of time necessary to obtain thermal equilibrium between the crystalline and glassy phases.

Note 1These terms are defined in Terminology C162 .

1.2 Two methods are included, differing in the type of sample, apparatus, procedure for positioning the sample, and measurement of temperature gradient in the furnace. Both methods have comparable precision. Method B is preferred for very fluid glasses because it minimizes thermal and mechanical mixing effects.

1.2.1 Method A employs a trough-type platinum container (tray) in which finely screened glass particles are fused into a thin lath configuration defined by the trough.

1.2.2 Method B employs a perforated platinum tray on which larger screened particles are positioned one per hole on the plate and are therefore melted separately from each other.

1.3 This standard does not purport to address all of the safety concerns, if any, associated with its use. It is the responsibility of the user of this standard to establish appropriate safety and health practices and determine the applicability of regulatory limitations prior to use.

PDF Catalog

PDF Pages PDF Title
1 Scope
Referenced Documents
Significance and Use
Apparatus
2 FIG. 1
FIG. 2
FIG. 3
3 FIG. 4
FIG. 5
FIG. 6
4 Preparation of Test Specimens
Procedure
FIG. 7
5 FIG. 8
FIG. 9
6 FIG. 10
FIG. 11
7 Surface Crystallization
Report
Precision and Bias
Keywords
A1. DESCRIPTION OF LIQUIDUS FURNACE COMPONENTS
A1.1 Components for Liquidus Furnace Used in Method A (see
FIG. 12
9 A2. CARE OF THE PLATINUM TRAYS
A2.1
A2.2
A2.3
A2.4
A2.5
A2.6
ASTM-C829 2010
$40.63