81.060.20 陶瓷制品 标准查询与下载

JIS T 0330-4:2012 生物陶瓷.第4部分:磷酸钙骨泥物理化学特性

Bioceramics -- Part 4: Physico-chemical characterization of calcium phosphate bone paste

DB13/T 1583-2012 陶制耐热炊具

Porcelain Heat Resistant Cookware

DB13/T 1585-2012 陶制烧烤炊具

Earthen BBQ Cookware

DB43/T 679-2012 中国红日用瓷器

Chinese Red Daily Porcelain

ASTM C949-80(2012) 孔隙度的标准测试方法

Standard Test Method for Porosity  in  Vitreous  Whitewares  by  Dye  Penetration

DB44/T 999-2012 涂膜陶质砖

本标准规定了涂膜陶质砖的术语和定义、等级、要求、试验方法、检验规则、标志、使用说明书、包装、运输及贮存。 本标准适用于内墙用的涂膜陶质砖。

Coated ceramic tiles

ASTM C738-94(2011) 从釉面陶瓷表面提取的铅和镉的标准测试方法

Standard Test Method for Lead and Cadmium Extracted from Glazed Ceramic Surfaces

ASTM C773-88(2011) 燃烧白色材料的压缩（粉碎）强度的标准测试方法

Standard Test Method for Compressive (Crushing) Strength of Fired Whiteware Materials

ASTM C848-88(2011) 用共振法测定陶瓷洁具的杨氏模量、剪切模量和泊松比的标准试验方法

1.1 This test method covers the determination of the elastic properties of ceramic whiteware materials. Specimens of these materials possess specific mechanical resonance frequencies which are defined by the elastic moduli, density, and geometry of the test specimen. Therefore the elastic properties of a material can be computed if the geometry, density, and mechanical resonance frequencies of a suitable test specimen of that material can be measured. Young’s modulus is determined using the resonance frequency in the flexural mode of vibration. The shear modulus, or modulus of rigidity, is found using torsional resonance vibrations. Young’s modulus and shear modulus are used to compute Poisson’s ratio, the factor of lateral contraction. 1.2 All ceramic whiteware materials that are elastic, homogeneous, and isotropic may be tested by this test method.2 This test method is not satisfactory for specimens that have cracks or voids that represent inhomogeneities in the material; neither is it satisfactory when these materials cannot be prepared in a suitable geometry. NOTE 1—Elastic here means that an application of stress within the elastic limit of that material making up the body being stressed will cause an instantaneous and uniform deformation, which will cease upon removal of the stress, with the body returning instantly to its original size and shape without an energy loss. Many ceramic whiteware materials conform to this definition well enough that this test is meaningful. NOTE 2—Isotropic means that the elastic properties are the same in all directions in the material. 1.3 A cryogenic cabinet and high-temperature furnace are described for measuring the elastic moduli as a function of temperature from −195 to 1200°C. 1.4 Modification of the test for use in quality control is possible. A range of acceptable resonance frequencies is determined for a piece with a particular geometry and density. Any specimen with a frequency response falling outside this frequency range is rejected. The actual modulus of each piece need not be determined as long as the limits of the selected frequency range are known to include the resonance frequency that the piece must possess if its geometry and density are within specified tolerances. 1.5 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.

Standard Test Method for Young's Modulus, Shear Modulus, and Poisson's Ratio For Ceramic Whitewares by Resonance

ASTM F109-11 与陶瓷表面缺陷相关的标准术语

1.1 This terminology describes and illustrates imperfections observed on whitewares and related products. For additional definitions of terms relating to whitewares and related products, refer to Terminology C242. To observe these defects, examination shall be performed visually, with or without the aid of a dye penetrant, as described in Test Method C949. Agreement by the manufacturer and the purchaser regarding specific techniques of observation is strongly recommended.

Standard Terminology Relating to Surface Imperfections on Ceramics

ASTM C1678-10 陶瓷和玻璃中的断裂镜面尺寸的断裂面显微镜图像分析的标准实施规程

Fracture mirror size analysis is a powerful tool for analyzing glass and ceramic fractures. Fracture mirrors are telltale fractographic markings in brittle materials that surround a fracture origin as discussed in Practices C1256 and C1322. Fig. 1 shows a schematic with key features identified. Fig. 2 shows an example in glass. The fracture mirror region is very smooth and highly reflective in glasses, hence the name “fracture mirror.” In fact, high magnification microscopy reveals that, even within the mirror region in glasses, there are very fine features and escalating roughness as the crack advances away from the origin. These are submicrometer in size and hence are not discernable with an optical microscope. Early investigators interpreted fracture mirrors as having discrete boundaries including a “mirror-mist” boundary and also a “mist-hackle” boundary in glasses. These were also termed “inner mirror” or “outer mirror” boundaries, respectively. It is now known that there are no discrete boundaries corresponding to specific changes in the fractographic features. Surface roughness increases gradually from well within the fracture mirror to beyond the apparent boundaries. The boundaries were a matter of interpretation, the resolving power of the microscope, and the mode of viewing. In very weak specimens, the mirror may be larger than the specimen or component and the boundaries will not be present. Figs. 3-5 show examples in ceramics. In polycrystalline ceramics, the qualifier “relatively” as in “relatively smooth” must be used, since there is an inherent roughness from the microstructure even in the area immediately surrounding the origin. In coarse-grained or porous ceramics, it may be impossible to identify a mirror boundary. In polycrystalline ceramics, it is highly unlikely that a mirror-mist boundary can be detected due to the inherent roughness created by the crack-microstructure interactions, even within the mirror. The word “systematic” in the definition for “mirror-hackle boundary in polycrystalline ceramics” requires some elaboration. Mirror boundary hackle lines are velocity hackle lines created after the radiating crack reaches terminal velocity. However, premature, isolated hackle can in some instances be generated well within a ceramic fracture mirror. It should be disregarded when judging the mirror boundary. Wake hackle from an isolated obstacle inside the mirror (such as a large grain or agglomerate) can trigger early “premature” hackle lines. Steps in scratches or grinding flaws can trigger hackle lines that emanate from the origin itself. Sometimes the microstructure of polycrystalline ceramics creates severe judgment problems in ceramic matrix composites (particulate, whisker, or platelet) or self-reinforced ceramics whereby elongated and interlocking grains impart greater fracture resistance. Mirrors may be plainly evident at low magnifications, but accurate assessment of their size can be difficult. Th......

Standard Practice for Fractographic Analysis of Fracture Mirror Sizes in Ceramics and Glasses

ASTM C1678-10(2015) 陶瓷和玻璃中断裂镜面尺寸断口分析的标准实施规程

5.1 Fracture mirror size analysis is a powerful tool for analyzing glass and ceramic fractures. Fracture mirrors are telltale fractographic markings in brittle materials that surround a fracture origin as discussed in Practices C1256 and C1322. Fig. 1 shows a schematic with key features identified. Fig. 2 shows an example in glass. The fracture mirror region is very smooth and highly reflective in glasses, hence the name “fracture mirror.” In fact, high magnification microscopy reveals that, even within the mirror region in glasses, there are very fine features and escalating roughness as the crack advances away from the origin. These are submicrometer in size and hence are not discernable with an optical microscope. Early investigators interpreted fracture mirrors as having discrete boundaries including a “mirror-mist” boundary and also a “mist-hackle” boundary in glasses. These were also termed “inner mirror” or “outer mirror” boundaries, respectively. It is now known that there are no discrete boundaries corresponding to specific changes in the fractographic features. Surface roughness increases gradually from well within the fracture mirror to beyond the apparent boundaries. The boundaries were a matter of interpretation, the resolving power of the microscope, and the mode of viewing. In very weak specimens, the mirror may be larger than the specimen or component and the boundaries will not be present. σ   =   stress at the origin (MPa or ksi), R   =   fracture mirror radius (m or in), A   =   fracture mirror constant (MPa√m or ksi√in). Eq 1 is hereafter referred to as the “empirical stress – fracture mirror size relationship,” or “stress-mirror size relationship” for short. A review of the history of Eq 1, and fracture mirror analysis in general, may be found in Refs8201;1 and 2. 5.5 A, the “fracture mirror constant” (sometimes also known as the “mirror constant”) has units of stress intensity (MPa√m or ksi√in) and is considered by many to be a material property. As shown in Figs. 1 and 2, it is possible to discern separate mist and hackle regions and the apparent boundaries between them in glasses. Each has a corresponding mirror constant, A. The most common notation is to refer to the mirror-mist boundary as the inner mirror boundary, and its mirror constant is designated Ai. The mist-hackle boundary is referred to as the outer mirror boundary, and its mirror constant is designated Ao. The mirror-mist boundary is usually not perceivable in polycrystalline ceramics. Usually, only the mirror-hackle boundary is measured and only an Ao for the mirror-hackle boundary is calculat......

Standard Practice for Fractographic Analysis of Fracture Mirror Sizes in Ceramics and Glasses

KS L 1598-2009(2019) 高温高性能陶瓷弹性模量试验方法

Testing method for elastic modulus of high performance ceramics at elevated temperature

KS L 1209-2009(2019) 陶瓷材料45°镜面光泽试验方法

Testing method for 45° specular gloss of ceramic materials

KS L 1210-2009(2019) 测试方法抗性的釉上彩装饰品袭击清净剂

Testing method for resistance of overglaze decorations to attack by detergents

KS L 1210-2009 陶瓷装饰物的耐洗涤剂试验方法

1.1 이 표준은 일반 가정에서 사용하는 비누 및 세척액에 대한 도자기 장식물의 내세제성

Testing method for resistance of overglaze decorations to attack by detergents

KS L 1209-2009 陶瓷餐具45℃镜向光泽度试验方法

이 시험 방법은 유약을 시유한 자기류 시험편의 광택도에 대하여 규정하고 있으며 비슷한 반사

Testing method for 45° specular gloss of ceramic materials

KS L 1598-2009 精细陶瓷高温弹性模量试验方法

이 표준은 기계 부품, 구조 재료 등의 고강도 재료로 사용되는 파인 세라믹스의 고온에서의

Testing method for elastic modulus of high performance ceramics at elevated temperature

KS L 1202-2009(2019) 卫生陶瓷的热导率

Thermal conductivity of whiteware ceramics

KS L 1202-2009 陶瓷热传导率测定方法

이 표준은 40∼150 ℃의 온도 범위에서 도자기에 대한 열 전도도 측정 방법에 대하여 규

Thermal conductivity of whiteware ceramics