Glasses with improved tempering capabilities

Information

  • Patent Grant
  • 11485673
  • Patent Number
    11,485,673
  • Date Filed
    Friday, August 24, 2018
    6 years ago
  • Date Issued
    Tuesday, November 1, 2022
    2 years ago
Abstract
The disclosure relates to glass compositions having improved thermal tempering capabilities. The disclosed glass compositions have high coefficients of thermal expansion and Young's moduli, and are capable of achieving high surface compressions. A method of making such glasses is also provided.
Description
FIELD OF DISCLOSURE

The disclosure relates to highly temperable glass compositions. More particularly, the disclosure relates to glasses having improved tempering when compared to common soda lime glasses. Even more particularly, the disclosure relates to glass compositions with high coefficients of thermal expansion and high Young's moduli for use with a thermal tempering process.


BACKGROUND

In thermal tempering, a glass product is heated to near the softening temperature and then rapidly quenched. As a result, the glass will possess a lower surface temperature than the interior during cooling. The temperature difference is maintained until the surface of the glass cools to room temperature. As the center of the glass cools more slowly to room temperature it contracts to a smaller specific volume while the high specific volume of the surface layer remains unchanged. This leads to a surface compressive layer that gives tempered glass its strength. The difference in specific volume is in majority due to differences in the thermal expansion of the glass upon cooling, while to a lesser extent from a fictive temperature difference between the surface and the bulk. To a first approximation, the stress distribution in thermally tempered glass can be represented by a simple parabola, with the magnitude of the surface compressive stress approximately equal to twice the center tension.


Thermally tempered glass, sometimes called safety glass, is often applied in situations where safe fracture behavior is required to prevent injury in the case of failure, being used to strengthen automobile side and rear windows, as well as object such as shower doors. It is desired that when thermally tempered glass breaks, unlike annealed glass, it shatters into rock-salt like pieces which do not have sharp edges or needle-like shapes. It is for this reason that characterizing the fracture behavior of thermally tempered glass is of paramount importance. The desired fracture behavior is called “dicing” and occurs when the glass has achieved full temper.


In addition to the safety aspect of thermally tempered glass, tempering strengthens the glass, making it more damage resistant and durable. Because of the increased durability, tempered glass can be used in applications where normal glass would quickly break—for example, automotive windshields, where the glass may impacted by rocks or other hard materials. Due to the increase in glass use in architectural, automotive, and electronic device applications, there is a continued need for strengthened glasses having improved tempering capabilities.







BRIEF DESCRIPTION OF THE FIGURE

FIG. 1 is a graph of transmittance as a function of wavelength for compositions disclosed herein.


DETAILED DESCRIPTION

In the following description, whenever a group is described as comprising at least one of a group of elements and combinations thereof, it is understood that the group may comprise, consist essentially of, or consist of any number of those elements recited, either individually or in combination with each other. Similarly, whenever a group is described as consisting of at least one of a group of elements or combinations thereof, it is understood that the group may consist of any number of those elements recited, either individually or in combination with each other. Unless otherwise specified, a range of values, when recited, includes both the upper and lower limits of the range as well as any ranges therebetween. As used herein, the indefinite articles “a,” “an,” and the corresponding definite article “the” mean “at least one” or “one or more,” unless otherwise specified. It also is understood that the various features disclosed in the specification and the drawings can be used in any and all combinations.


Where a range of numerical values is recited herein, comprising upper and lower values, unless otherwise stated in specific circumstances, the range is intended to include the endpoints thereof, and all integers and fractions within the range. It is not intended that the scope of the claims be limited to the specific values recited when defining a range. Further, when an amount, concentration, or other value or parameter is given as a range, one or more preferred ranges or a list of upper preferable values and lower preferable values, this is to be understood as specifically disclosing all ranges formed from any pair of any upper range limit or preferred value and any lower range limit or preferred value, regardless of whether such pairs are separately disclosed. Finally, when the term “about” is used in describing a value or an end-point of a range, the disclosure should be understood to include the specific value or end-point referred to. When a numerical value or end-point of a range does not recite “about,” the numerical value or end-point of a range is intended to include two embodiments: one modified by “about,” and one not modified by “about.”


As used herein, the term “about” means that amounts, sizes, formulations, parameters, and other quantities and characteristics are not and need not be exact, but may be approximate and/or larger or smaller, as desired, reflecting tolerances, conversion factors, rounding off; measurement error and the like, and other factors known to those of skill in the art. It is noted that the terms “substantially” may be utilized herein to represent the inherent degree of uncertainty that may be attributed to any quantitative comparison, value, measurement, or other representation. These terms are also utilized herein to represent the degree by which a quantitative representation may vary from a stated reference without resulting in a change in the basic function of the subject matter at issue. Thus, a glass that is “free of Al2O3” is one in which Al2O3 is not actively added or batched into the glass, but may be present in very small amounts as a contaminant (e.g., 500, 400, 300, 200, or 100 parts per million (ppm) or less or).


Unless otherwise specified, all compositions are expressed in terms of mole percent (mol %). Coefficients of thermal expansion (CTE) are expressed in terms of 10−7/° C. and represent a value measured over a temperature range from 25° C. to 300° C., unless otherwise specified. The low temperature CTE (LTCTE) is measured at 25° C. and expressed in terms of 10−7/° C. The high temperature CTE (HTCTE) is measured at 300° C. and expressed in terms of 10−7/° C. The sum of the LTCTE and the HTCTE is expressed in terms of 10−7/° C. The density in terms of grams/cm3 was measured via the Archimedes method (ASTM C693). Young's modulus, shear modulus, and Poisson's Ratio were measured via the ASTM C623 standard.


Glass Compositions

In thermal tempering, a glass product is heated to near the softening temperature and then rapidly quenched. As a result, the glass will possess a lower surface temperature than the interior during cooling. The temperature difference is maintained until the surface of the glass cools to room temperature. As the center of the glass cools more slowly to room temperature it contracts to a smaller specific volume while the high specific volume of the surface layer remains unchanged. This leads to a surface compressive layer that gives tempered glass its strength. The difference in specific volume is due to a combination of differences in the thermal expansion of the glass upon cooling and from a fictive temperature difference between the surface and the bulk. To a first approximation, the stress distribution in thermally tempered glass can be represented by a simple parabola, with the magnitude of the surface compressive stress approximately equal to twice the center tension.


When thermally tempered glass breaks, unlike annealed glass, it shatters into rock-salt like pieces which do not have sharp edges or needle-like shapes. This behavior is particularly useful for situations where safe fracture behavior is necessary and it is for this reason that characterizing the fracture behavior of thermally tempered glass is of paramount importance. The desired fracture behavior is called “dicing” and occurs when the glass has achieved full temper. The dicing threshold of tempered glass is an arbitrarily defined fracture behavior which can be considered “safe” to the user in the event of glass failure. Standards exist worldwide such as ASTM C1048 and ANSI Z97.1 in the United States, EN12150-1 in Europe, GOST 5727-88 in Russia, JIS R 3206 in Japan, and GB 15763.2 in China (all of which are hereby incorporated by reference). The standards are nearly identical across countries in that a fragmented piece of tempered soda-lime glass is required to contain at least 30-40 fragments in an area of 50 mm×50 mm (1.6 fragments/cm2) for thick glasses >3 mm, while Japanese standards in particular require at least 60 fragments in the case of thinner glass.


It is of interest to predict the ability of a glass composition to produce stresses during thermal tempering. The simplest approximation one can make in forming a more general expression is to assume that for any chosen combination of glass thickness and quenching rate, the stress formed due to thermal strain is a fraction of the maximum possible. Therefore a general expression for the compressive tempering stress formed when quenched from a constant viscosity can be expressed as:

σCs−C(h,t,η)+Ψ(E,αCTE3CTEL,Tsoft,Tstrain)

where αs is the CTE of the glass in solid form, αL is the CTE of the glass in liquid form, Tsoft is the softening point temperature, Tstrain is the strain point temperature, and the constant, Ψ, is a material property called the “temperability parameter” and is representative of the maximum thermal strain that can be formed if the surface was frozen upon quenching. The maximum thermal strain can be roughly estimated by a 2-step integration of the thermal expansion as a function of temperature and general glass properties. The thermal expansion coefficient (CTE) is assumed to be a constant from room temperature to the strain point, and then constant again from the strain point to softening. With this in mind and with the assumption that room temperature is close to 0° C., a more general “temperability parameter” can be expressed as:

Ψ=E*[TstrainCTEsCTEL*(Tsoft−Tstrain)]

where E is in GPa, temperatures are given in ° C., and α is in ° C.−1. It can be seen that this expression contains a more general form of the volumetric strain calculated using the strain point of the glass between glassy and liquid behavior.


By measuring a few standard properties for a given glass, it is possible to estimate the temper stresses that would be expect to form if the constant, C(h,t,η), is known. This constant has been evaluated using modeling for a wide range of known compositions, and from the calculation of Ψ, the relative temperability of various glass compositions can be quickly compared to one another. When the temperabilities of a variety glass compositions are calculated, the results show that various combinations of properties can reach a similar endpoint and that glasses vast differences in the compositions and properties can be nearly indistinguishable in terms of temperability.


The glasses disclosed herein have high coefficients of thermal expansion and high Young's moduli and can be used with a thermal tempering process to obtain improved tempering when compared to commercially available glasses. The glasses described herein are needed to satisfy a growing demand for stronger but thinner thermally strengthened glasses for commercial electronics, automotive and architectural applications where durability and/or scratch resistance are desired along with a “safe” break pattern. As glass becomes thinner, it becomes harder to produce any thermal tempering stresses at all and the central tension required for a safe ‘dicing” fracture pattern increases—producing a compound challenge. Developing glasses which produce enhanced temper stresses can help to meet this challenge. Additionally, the glasses must also retain a significant chemical durability, as they will likely be exposed to the elements for extended periods of time.


It has been found that glasses having temperability parameters, Ψ, of 0.8 or higher, 0.85 or higher, or even 0.9 or higher, are capable of increased thermal tempering. In some embodiments, to improve temperability, it has been found that the low temperature coefficient of thermal expansion (LTCTE) should be 5.5×10−7/° C. or greater. In some embodiments, it has been found that the high temperature coefficient of thermal expansion (HTCTE) should be 27×10−7/° C. or greater. In some embodiments, it has been found that in order to improve temperability, the sum of the LTCTE and HTCTE should be greater than 35×10−7/° C., 37×10−7/° C., or 40×10−7/° C. The invention is a novel glass composition space that has high coefficients of thermal expansion and Young's modulus. In some embodiments, it has been found that glass compositions have improved temperability when the Young's modulus is greater than 67 GPa and the temperability factor is greater than or equal to 0.75 (The approximate value of commercially available soda-lime glass).


In some embodiments, the glass comprises a combination of SiO2, Na2O or K2O, Al2O3, B2O3 or ZnO, and alkaline earth oxides. For example, embodiments may comprise from 60 mol % to 72 mol % SiO2 (60 mol %≤SiO2≤72 mol %); from greater than 0 mol % Al2O3 (0 mol %<Al2O3); from greater than 0 mol % MgO (0 mol %<MgO); from greater than 0 mol % CaO (0 mol %<CaO); 6-16 mol % Na2O+K2O (6 mol %≤Na2O+K2O≤16 mol %); 0-16 mol % Na2O (0 mol %≤Na2O≤16 mol %); 0-16 mol % K2O (0 mol %≤K2O≤16 mol %); and one or more of B2O3 or ZnO, wherein B2O3, when present, comprises 1-10 mol % (1 mol %≤B2O3≤10 mol %); and ZnO, when present, comprises 3-8 mol % (3 mol %≤ZnO≤8 mol %). Additional aspects of the various constituents that can make up the embodied compositions are detailed below.


In some embodiments, the glass comprises a combination of SiO2, Na2O or K2O, Al2O3, B2O3, and alkaline earth oxides. For example, embodiments may comprise from 60 mol % to 65 mol % SiO2 (60 mol %≤SiO2≤65 mol %); from 5 mol % to 10 mol % Al2O3 (5 mol %≤Al2O3≤10 mol %); from 3 mol % to 10 mol % MgO (3 mol %≤MgO≤10 mol %); from 5 mol % to 15 mol % CaO (5 mol %≤CaO≤15 mol %); 8-15 mol % Na2O+K2O (8 mol %≤Na2O+K2O≤15 mol %); 0-15 mol % Na2O (0 mol %≤Na2O≤15 mol %); 0 mol % to 15 mol % K2O (0 mol %≤K2O≤15 mol %); and 1.5 mol % to 6 mol % B2O3 (1.5 mol %≤B2O3≤6 mol %).


Alternative embodiments may comprise from 65 mol % to 70 mol % SiO2 (65 mol %≤SiO2≤70 mol %); from >0 mol % to 5 mol % Al2O3 (>0 mol %≤Al2O3≤5 mol %); from 4 mol % to 8 mol % MgO (4 mol %≤MgO≤8 mol %); from 7 mol % to 11 mol % CaO (7 mol %≤CaO≤11 mol %); 9-14 mol % Na2O+K2O (9 mol %≤Na2O+K2O≤14 mol %); 0-14 mol % Na2O (0 mol %≤Na2O≤14 mol %); 0 mol % to 14 mol % K2O (0 mol %≤K2O≤14 mol %); and 1 mol % to 6 mol % B2O3 (1 mol %≤B2O3≤6 mol %).


Still other embodiments may comprise from 65 mol % to 70 mol % SiO2 (65 mol %≤SiO2≤70 mol %); from >0 mol % to 5 mol % Al2O3 (>0 mol %≤Al2O3≤5 mol %); from 5 mol % to 10 mol % MgO (5 mol %≤MgO≤10 mol %); from 6 mol % to 13 mol % CaO (6 mol %≤CaO≤13 mol %); 10-16 mol % Na2O+K2O (10 mol %≤Na2O+K2O (16 mol %); 2-16 mol % Na2O (2 mol %≤Na2O≤16 mol %); 0 mol % to 8 mol % K2O (0 mol %≤K2O≤8 mol %); and 1 mol % to 6 mol % B2O3 (1 mol %≤B2O3≤6 mol %).


Still other embodiments may comprise from 65 mol % to 72 mol % SiO2 (65 mol %≤SiO2≤72 mol %); from 4 mol % to 10 mol % Al2O3 (4 mol %≤Al2O3≤10 mol %); from 3 mol % to 10 mol % MgO (3 mol %≤MgO≤10 mol %); from >0 mol % to 13 mol % CaO (0 mol %≤CaO≤13 mol %); 10-16 mol % Na2O+K2O (10 mol %≤Na2O+K2O≤16 mol %); 10-16 mol % Na2O (10 mol %≤Na2O≤16 mol %); 0 mol % to 6 mol % K2O (0 mol %≤K2O≤6 mol %); and 1.5 mol % to 8 mol % B2O3 (1.5 mol %≤B2O3≤8 mol %).


SiO2, along with Al2O3, B2O3, P2O5, ZrO2 and SnO2, are network formers when present in the glass. SiO2, which is the largest oxide component of the glass, may be included to provide high temperature stability and chemical durability. In some embodiments, the glass can comprise from 60 to 72 mol % SiO2. In some embodiments, the glass can comprise from 60 to 65 mol % SiO2. In some embodiments, the glass can comprise from 65 to 72 mol % SiO2. In some embodiments, the glass can comprise from 65-70 mol % SiO2. In some embodiments, the glass can comprise 60 to 72 mol %, 63 to 72 mol %, 65 to 72 mol %, 68 to 72 mol %, 60 to 70 mol %, 63 to 70 mol %, 65 to 70 mol %, 68 to 70 mol %, 60 to 68 mol %, 63 to 68 mol %, 65 to 68 mol %, 60 to 65 mol %, 63 to 65 mol %, or 60 to 63 mol % SiO2. In some embodiments, the glass comprises 60, 61, 62, 63, 64, 65, 66, 67, 68, 69, 70, 71, or 72 mol % SiO2.


Al2O3 may influence the structure of the glass and, additionally, lower the liquidus temperature and coefficient of thermal expansion, or enhance the strain point. In some embodiments, the glass can comprise greater than 0 mol % Al2O3. In some embodiments, the glass can comprise from >0 to 12 mol % Al2O3. In some embodiments, the glass can comprise from >0 to 5 mol %, 4 to 10 mol %, 5 to 10 mol % Al2O3 or >0 to 3 mol % Al2O3. In some embodiments, the glass can comprise from 0.5 to 4 mol % Al2O3. In some embodiments, the glass can comprise from >0 to 12 mol %, >0 to 10 mol %, >0 to 8 mol %, >0 to 6 mol %, >0 to 4 mol %, >0 to 2 mol %, 1 to 12 mol %, 1 to 10 mol %, 1 to 8 mol %, 1 to 6 mol %, 1 to 4 mol %, 1 to 2 mol %, 3 to 8 mol %, 3 to 6 mol %, 3 to 10 mol %, 3 to 12 mol %, 5 to 8 mol %, 5 to 10 mol %, 5 to 12 mol %, 7 to 12 mol %, 7 to 10 mol %, or 8 to 10 mol % Al2O3. In some embodiments, the glass can comprise about >0, 1, 2, 3, 4, 5, 6, 7, 8, 9, 10, 11 or 12 mol % Al2O3.


Without being bound by theory, it is believed that incorporating B2O3 into the glasses described herein impacts the coefficient of thermal expansion, especially at high temperatures, and improves the temperability of the glasses. In some embodiments, the glass can comprise 1 mol % to 10 mol % B2O3. In some embodiments, the glass can comprise from 1 mol % to 8 mol % or from 1 mol % to 6 mol % B2O3. In some embodiments, the glass can comprise from about 1.5 to 8 mol % B2O3 or 1.5 to 6 mol % B2O3. In some embodiments, the glass can comprise from 1 to 4 mol % B2O3. In some embodiments, the glass can comprise from 1 to 10 mol %, 1.5 to 10 mol %, 2 to 10 mol %, 4 to 10 mol %, 1 to 8 mol %, 1.5 to 8 mol %, 2 to 8 mol %, 4 to 8 mol %, 1 to 6 mol %, 1.5 to 6 mol %, 2 to 6 mol %, 4 to 6 mol %, 1 to 4 mol %, 1.5 to 4 mol %, 2 to 4 mol %, 1.5 to 3 mol %, or 1 to 3 mol % B2O3. In some embodiments, the glass can comprise about 0, >0, 1, 2, 3, 4, or 5 mol % B2O3.


Zinc oxide, ZnO, may be present and influence the glass properties, including the Young's modulus. In some embodiments, when ZnO is present, the glass can comprise 3 to 8 mol % ZrO2 or, in some embodiments, from 3 to 5 mol % ZnO. In some embodiments, the glass can comprise 3, 4, 5, 6, 7, or 8 mol % ZnO.


Without wanting to be bound by theory, it is believed that in some embodiments, the both ZnO and B2O3 may have similar effects on the material properties. In some embodiments, when B2O3 is present in the glass, the glass is free of ZnO. Alternatively, in some embodiments, when ZnO is present in the glass, the glass is free of B2O3.


Alkaline earth oxides may improve desirable properties in the materials, including influencing the Young's modulus and the coefficient of thermal expansion. In some embodiments, the glass comprises from >0 mol % to about 20 mol % MO (0 mol %≤MO≤20 mol %), where M is the sum of the alkaline earth metals Mg, Ca, Sr, and Ba, in the glass. In some embodiments, the glass can comprise from >0 to 18 mol % MO. In some embodiments, the glass can comprise from >0 to 16 mol % MO. In some embodiments, the glass can comprise about >0, 1, 2, 3, 4, 5, 6, 7, 8, 9, 10, 11, 12, 13, 14, 15, 16, 17, 18, 19, or 20 mol % MO.


In some embodiments, the glasses comprise MgO, CaO, or SrO. In some embodiments, the glass can comprise greater than 0 mol % MgO. In some embodiments, the glass can comprise from >0 to 10 mol % MgO. In some embodiments, the glass can comprise from 3 to 10 mol %, 5 to 10 mol %, 5 to 8 mol % MgO. In some embodiments, the glass can comprise from >0 to 10 mol %, >0 to 8 mol %, >0 to 6 mol %, >0 to 4 mol %, >0 to 2 mol %, 1 to 10 mol %, 1 to 8 mol %, 1 to 6 mol %, 1 to 4 mol %, 1 to 2 mol %, 3 to 8 mol %, 3 to 6 mol %, 3 to 10 mol %, 5 to 8 mol %, 5 to 10 mol %, 7 to 10 mol %, or 8 to 10 mol % MgO. In some embodiments, the glass can comprise about >0, 1, 2, 3, 4, 5, 6, 7, 8, 9, or 10 mol % MgO.


In some embodiments, the glass can comprise greater than 0 mol % CaO. In some embodiments, the glass can comprise from >0 to 15 mol % CaO. In some embodiments, the glass can comprise from >0 to 5 mol %, 6 to 13 mol %, 5 to 15 mol %, 7 to 13 mol %, 7 to 11 mol %, 8 to 12 mol % CaO. In some embodiments, the glass can comprise from >0 to 15 mol %, >0 to 13 mol %, >0 to 11 mol %, >0 to 9 mol %, >0 to 7 mol %, >0 to 5 mol %, 1 to 15 mol %, 1 to 13 mol %, 1 to 11 mol %, 1 to 9 mol %, 1 to 7 mol %, 1 to 5 mol %, 3 to 15 mol %, 3 to 13 mol %, 3 to 11 mol %, 3 to 9 mol %, 3 to 7 mol %, 3 to 5 mol %, 5 to 15 mol %, 5 to 13 mol %, 5 to 11 mol %, 5 to 9 mol %, 5 to 7 mol %, 7 to 15 mol %, 7 to 13 mol %, 7 to 11 mol %, 7 to 9 mol %, 9 to 15 mol %, 9 to 13 mol %, 9 to 11 mol %, 11 to 15 mol %, or 11 to 13 mol % CaO. In some embodiments, the glass can comprise about >0, 1, 2, 3, 4, 5, 6, 7, 8, 9, 10, 11, 12, 13, 14, or 15 mol % CaO.


SrO may be present in some embodiments and in such embodiments, the glass can comprise from 0 to 5 mol % SrO. In some embodiments, the glass can comprise from >0 to 5 mol % SrO. In some embodiments, the glass can comprise from about >0 to 3.5 mol % SrO or 0.2 to 3 mol % SrO. In some embodiments, the glass can comprise from 1 to 4 mol % SrO. In some embodiments, the glass can comprise from 0.2 to 5 mol %, 0.2 to 4 mol %, 0.2 to 3 mol %, 0.2 to 2 mol %, >0 to 5 mol %, >0 to 4 mol %, >0 to 3 mol %, >0 to 2 mol %, 1 to 5 mol %, 1 to 4 mol %, or 1 to 3 mol % SrO. In some embodiments, the glass can comprise about 0, >0, 1, 2, 3, 4, or 5 mol % SrO.


Na2O and K2O may improve the temperability of the glass and influence the coefficient of thermal expansion, especially at low temperatures. In some embodiments, the glass can comprise from 0 to 16 mol % Na2O. In some embodiments, the glass can comprise >0 to 15 mol % Na2O. In some embodiments, the glass can comprise 10 to 16 mol % Na2O. In some embodiments, the glass can comprise 2 to 16 mol % Na2O. In some embodiments, the glass can comprise from 0 to 16 mol %, 0 to 15 mol %, 0 to 14 mol %, 0 to 10 mol %, 0 to 8 mol %, 0 to 5 mol %, >0 to 16 mol %, >0 to 15 mol %, >0 to 14 mol %, >0 to 10 mol %, >0 to 8 mol %, >0 to 5 mol %, 2 to 16 mol %, 2 to 15 mol %, 2 to 14 mol %, 2 to 10 mol %, 2 to 8 mol %, 2 to 5 mol %, 5 to 16 mol %, 5 to 15 mol %, 5 to 14 mol %, 5 to 10 mol %, 5 to 8 mol %, 8 to 16 mol %, 8 to 15 mol %, 8 to 14 mol %, 8 to 10 mol %, 10 to 16 mol %, 10 to 15 mol %, or 10 to 14 mol % Na2O. In some embodiments, the glass can comprise 0, >0, 1, 2, 3, 4, 5, 6, 7, 8, 9, 10, 11, 12, 13, 14, 15, or 16 mol % Na2O.


In some embodiments, the glass can comprise from 0 to 16 mol % K2O. In some embodiments, the glass can comprise >0 to 15 mol % K2O. In some embodiments, the glass can comprise 0 to 8 mol % K2O. In some embodiments, the glass can comprise 0 to 6 mol % K2O. In some embodiments, the glass can comprise from 0 to 16 mol %, 0 to 15 mol %, 0 to 14 mol %, 0 to 10 mol %, 0 to 8 mol %, 0 to 5 mol %, >0 to 16 mol %, >0 to 15 mol %, >0 to 14 mol %, >0 to 10 mol %, >0 to 8 mol %, >0 to 5 mol %, 2 to 16 mol %, 2 to 15 mol %, 2 to 14 mol %, 2 to 10 mol %, 2 to 8 mol %, 2 to 5 mol %, 5 to 16 mol %, 5 to 15 mol %, 5 to 14 mol %, 5 to 10 mol %, 5 to 8 mol %, 8 to 16 mol %, 8 to 15 mol %, 8 to 14 mol %, 8 to 10 mol %, 10 to 16 mol %, 10 to 15 mol %, or 10 to 14 mol % K2O. In some embodiments, the glass can comprise 0, >0, 1, 2, 3, 4, 5, 6, 7, 8, 9, 10, 11, 12, 13, 14, 15, or 16 mol % K2O.


In some embodiments, the total amount of the alkalis Na2O and K2O is important to the glass properties. In some embodiments, the glass can comprise 6 to 16 mol % Na2O+K2O. In some embodiments, the glass can comprise 8 to 16 mol % Na2O+K2O. In some embodiments, the glass can comprise 8 to 15 mol % Na2O+K2O. In some embodiments, the glass can comprise 10 to 16 mol % Na2O+K2O. In some embodiments, the glass can comprise 9 to 14 mol % Na2O+K2O. In some embodiments, the glass can comprise from 6 to 16 mol %, 8 to 16 mol %, 10 to 16 mol %, 6 to 15 mol %, 8 to 15 mol %, 10 to 15 mol %, 6 to 14 mol %, 8 to 14 mol %, 10 to 14 mol %, 6 to 12 mol %, 8 to 12 mol %, 10 to 12 mol %, 6 to 10 mol %, 8 to 10 mol %, or 6 to 8 mol % Na2O+K2O. In some embodiments, the glass can comprise 6, 7, 8, 9, 10, 11, 12, 13, 14, 15, or 16 mol % Na2O+K2O.


Na2O can be useful in the glass for ion exchange and chemical tempering. In some embodiments, the glass comprises from 0 mol % to about 5 mol % Na2O (0 mol %≤Na2O≤5 mol %). In some embodiments, the glass can comprise from greater than 0 to 5 mol % Na2O. In some embodiments, the glass can comprise from about 0 to 3 mol % Na2O or >0 to 3 mol % Na2O. In some embodiments, the glass can comprise from 0.5 to 4 mol % Na2O. In some embodiments, the glass can comprise from 0 to 5 mol %, 0 to 4 mol %, 0 to 3 mol %, 0 to 2 mol %, >0 to 5 mol %, >0 to 4 mol %, >0 to 3 mol %, >0 to 2 mol %, 1 to 5 mol %, 1 to 4 mol %, or 1 to 3 mol % Na2O. In some embodiments, the glass can comprise about 0, >0, 1, 2, 3, 4, or 5 mol % Na2O.


K2O may also be useful in ion exchange and may be present in the glass at amounts from 0 mol % to about 10 mol % K2O (0 mol %≤K2O≤10 mol %). In some embodiments, the glass can comprise from >0 to 10 mol % K2O. In some embodiments, the glass can comprise from about 0 to 5 mol % K2O or >0 to 3 mol % K2O. In some embodiments, the glass can comprise from 0.5 to 4 mol % K2O. In some embodiments, the glass can comprise from 0 to 10 mol %, 0 to 8 mol %, 0 to 5 mol %, 0 to 4 mol %, 0 to 3 mol %, >0 to 10 mol %, >0 to 8 mol %, >0 to 5 mol %, >0 to 3 mol %, 1 to 10 mol %, 1 to 8 mol %, 1 to 5, 1 to 4 mol %, 1 to 3 mol %, 2 to 10 mol %, 2 to 8 mol %, or 2 to 4 K2O. In some embodiments, the glass can comprise about 0, >0, 1, 2, 3, 4, 5, 6, 7, 8, 9, or 10 mol % K2O.


Alkaline earth oxides may provide advantages for ion exchange in the glass, along with improving other properties in the materials. In some embodiments, the glass comprises from 0 mol % to about 10 mol % MO (0 mol %≤MO≤10 mol %), where M is the sum of the alkaline earth metals Mg, Ca, Sr, and Ba, in the glass. In some embodiments, the glass can comprise from 0 to 8 mol % MO. In some embodiments, the glass can comprise from 0 to 5 mol % MO. In some embodiments, the glass can comprise from 1 to 8 mol % MO. In some embodiments, the glass can comprise from 0 to 10 mol %, 0 to 8 mol %, 0 to 6 mol %, 0 to 4 mol %, 1 to 10 mol %, 1 to 8 mol %, 1 to 6 mol % 2 to 10 mol %, 2 to 8 mol %, or 2 to 6 mol % MO. In some embodiments, the glass can comprise about >0, 1, 2, 3, 4, 5, 6, 7, 8, 9, or 10 mol % MO.


In some embodiments, the glasses above further comprise a coloring component. The coloring component may comprise, for example, Fe2O3, V2O5, Cr2O3, TiO2, MnO2, NiO, ZnO, CuO, NiO, Co3O4, rare earth oxides, and combinations thereof. In some cases, the total mol % of coloring component is from 0 to 4 mol %, 0 to 3 mol %, 0 to 2 mol %, 0 to 1 mol %, >0 to 0.1, >0 to 0.5, >0 to 1, >0 to 2, >0 to 3, or >0 to 4 mol %.


Additional components can be incorporated into the glass to provide additional benefits or may be incorporated as contaminants typically found in commercially-prepared glass. For example, additional components can be added as fining agents (e.g., to facilitate removal of gaseous inclusions from melted batch materials used to produce the glass) and/or for other purposes. In some embodiments, the glass may comprise one or more compounds useful as ultraviolet radiation absorbers. In some embodiments, the glass can comprise 3 mol % or less MnO, Nb2O5, MoO3, Ta2O5, WO3, SnO2, Fe2O3, As2O3, Sb2O3, Cl, Br, or combinations thereof. In some embodiments, the glass can comprise from 0 to about 3 mol %, 0 to about 2 mol %, 0 to about 1 mol %, 0 to 0.5 mol %, 0 to 0.1 mol %, 0 to 0.05 mol %, or 0 to 0.01 mol % MnO, ZnO, Nb2O5, MoO3, Ta2O5, WO3, SnO2, Fe2O3, As2O3, Sb2O3, Cl, Br, or combinations thereof. In some embodiments, the glass can comprise from 0 to about 3 mol %, 0 to about 2 mol %, 0 to about 1 mol %, 0 to about 0.5 mol %, 0 to about 0.1 mol %, 0 to about 0.05 mol %, or 0 to about 0.01 mol % SnO2 or Fe2O3, or combinations thereof. The glasses, according to some embodiments, can also include various contaminants associated with batch materials and/or introduced into the glass by the melting, fining, and/or forming equipment used to produce the glass.


Non-limiting examples of precursor glasses for forming the embodied glasses are listed in Table 1, wherein the values of the components are listed in mol %.











TABLE 1









Sample
















Glaverbel










soda-lime
A
B
C
D
E
F
G





SiO2 (mol %)
70.06
68.10
67.22
65.43
67.11
69.03
68.48
60.40


B2O3 (mol %)
0.00
1.77
3.41
5.34
4.31
3.13
5.06
1.98


Al2O3 (mol %)
1.17
0.95
0.96
0.96
0.99
1.01
0.97
8.71


MgO (mol %)
6.49
6.77
6.56
6.54
6.69
6.78
4.03
6.63


CaO (mol %)
8.69
9.06
9.01
8.98
9.21
9.44
8.95
9.11


SrO (mol %)
0.00
0.00
0.00
0.00
0.00
0.00
0.00
0.00


Na2O (mol %)
13.33
12.86
12.40
12.32
6.39
0.02
12.11
12.60


K2O (mol %)
0.25
0.50
0.43
0.43
5.30
10.60
0.40
0.47


ZnO (mol %)
0.00
0.00
0.00
0.00
0.00
0.00
0.00
0.00


SnO2 (mol %)
0.22
0.02
0.00
0.00
0.01
0.00
0.01
0.09


LTCTE (10−7/° C.)
8.8
8.65
8.47
8.42
8.47
8.16
8.20
8.4


HTCTE (10−7/° C.)
27.0
33.80
39.20
44.60
43.50
31.90
43.00
32.40


Young's Modulus
72.0
76.2
77.2
79.2
76.0
78.8
78.3
78.4


(GPa)


Shear Modulus

31.2
31.9
32.2
31.0
32.3
32.1
32.0


(GPa)


Poisson's Ratio

0.219
0.212
0.229
0.225
0.222
0.219
0.226


Strain Point (° C.)
507
512
521
522
532
598
526
557


Anneal Point (° C.)
549
550
557
557
569
643
563
598


Softening Point (° C.)
728
714
713
705
733
829
716
774


Density (g/cm3)
2.540
2.519
2.528
2.535
2.509
2.471
2.519
2.539


SOC (TPa−1)
2.720
2.730
2.698
2.696
2.728
2.820
2.769
2.868


Refractive Index
1.520
1.5236
1.5267
1.5292
1.5247
1.5172
1.5260
1.5272


VFT - a

−1.469
−1.103
−1.086
−1.601
−1.736
−1.234
−1.881


VFT - b

3794.1
3054.6
2868.8
3916.3
4270.5
3207.9
4625.2


VFT - T0

301.9
367.7
379.2
313.1
376.8
352.2
286.4


Liquidus Viscosity

11088
7677
4886
20712
40459
29243



(Poise)


Temperability, ψ
0.75
0.86
0.92
0.99
1.01
0.96
0.98
0.94


HTCTE + LTCTE
35.8
42.45
47.67
53.02
51.97
40.06
51.2
40.8


(10−7/° C.)












Sample
















Glaverbel










soda-lime
H
I
J
K
L
M
N





SiO2 (mol %)
70.06
58.76
56.86
57.23
57.70
59.66
70.39
70.50


B2O3 (mol %)
0.00
3.73
5.52
5.24
5.03
5.53
7.77
9.76


Al2O3 (mol %)
1.17
9.05
9.13
9.19
9.18
9.01
5.99
3.98


MgO (mol %)
6.49
6.52
6.50
6.52
6.45
3.94
7.23
7.03


CaO (mol %)
8.69
9.09
9.00
9.16
9.02
8.75
0.06
0.06


SrO (mol %)
0.00
0.00
0.00
0.00
0.00
0.00
0.00
0.00


Na2O (mol %)
13.33
12.32
12.44
6.52
0.10
12.54
8.47
8.57


K2O (mol %)
0.25
0.46
0.45
6.06
12.44
0.48
0.01
0.01


ZnO (mol %)
0.00
0.00
0.00
0.00
0.00
0.00
0.00
0.00


SnO2 (mol %)
0.22
0.09
0.09
0.09
0.09
0.09
0.05
0.05


LTCTE (10−7/° C.)
8.8
8.32
8.36
8.93
8.89
8.25
5.89
5.79


HTCTE (10−7/° C.)
27.0
34.00
27.90
36.00
27.00
42.00
28.07
32.70


Young's Modulus
72.0
78.3
78.3
75.8
68.0
77.6
69.71
70.74


(GPa)


Shear Modulus

31.9
31.8
30.6
27.6
31.6
28.89
29.44


(GPa)


Poisson's Ratio

0.226
0.232
0.238
0.229
0.229
0.206
0.202


Strain Point (° C.)
507
543
536
541
589
537
543
532


Anneal Point (° C.)
549
584
576
583
634
577
587
575


Softening Point (° C.)
728
757
740
758

742
812
766


Density (g/cm3)
2.540
2.536
2.535
2.52
2.486
2.521
2.363
2.363


SOC (TPa−1)
2.720
2.783
2.792
2.843
2.861
2.737
3.398
3.345


Refractive Index
1.520
1.5289
1.5298
1.5266
1.5212
1.5264
1.4951
1.4964


VFT - a

−1.514
−1.345
−1.994
−2.387
−1.441
−3.154
−2.402


VFT - b

3916.1
3518.8
4730.7
5460.2
3873
9067.9
7058.4


VFT - T0

335.4
354.3
271.2
296
319.3
−54.2
44.4


Temperability, ψ
0.75
0.94
0.94
0.81
0.99
0.82
0.75
0.76


HTCTE + LTCTE
35.8
42.32
36.26
44.93
35.89
50.25
33.96
38.49


(10−7/° C.)












Sample
















Glaverbel










soda-lime
O
P
Q
R
S
T
U





SiO2 (mol %)
70.06
70.53
70.70
70.71
70.55
63.11
62.26
63.12


B2O3 (mol %)
0.00
7.80
9.67
7.62
7.77
0
0
0


Al2O3 (mol %)
1.17
6.02
4.01
3.99
4.00
11.58
11.41
10.58


MgO (mol %)
6.49
4.97
5.06
7.01
8.98
0.00
0.00
0.00


CaO (mol %)
8.69
0.04
0.04
0.06
0.07
0.00
0.00
0.00


SrO (mol %)
0.00
0.00
0.00
0.00
0.00
0.00
0.00
0.00


Na2O (mol %)
13.33
10.54
10.42
10.51
8.54
16.43
16.81
16.41


K2O (mol %)
0.25
0.01
0.01
0.01
0.01
1.88
1.94
1.89


ZnO (mol %)
0.00
0.00
0.00
0.00
0.00
1.93
3.12
1.94


SnO2 (mol %)
0.22
0.05
0.05
0.05
0.05
0.05
0.05
0.05


LTCTE ((10−7/° C.)
8.8
6.47
6.39
6.57
5.88
10.3
10.31
10.19


HTCTE (10−7/° C.)
27.0
34.44
34.01
35.99
32.70
17.62
18.82
17.30


Young's Modulus
72.0
70.05
71.50
72.19
71.91
66.19
67.78
65.22


(GPa)


Shear Modulus

29.23
29.79
29.99
29.85
27.44
27.99
27.03


(GPa)


Poisson's Ratio

0.198
0.201
0.203
0.203
0.206
0.21
0.207


Strain Point (° C.)
507
532
522
531
545
615
605
628


Anneal Point (° C.)
549
576
564
573
584
672
661
688


Softening Point (° C.)
728
778
748
758
780
912
927
911


Density (g/cm3)
2.540
2.379
2.383
2.393
2.379
2.432
2.459
2.414


SOC (TPa−1)
2.720
3.287
3.284
3.225
3.289
3.104
3.108
3.107


Refractive Index
1.520
1.497
1.4982
1.4991
1.4982
1.4902
1.4948
1.4862


VFT - a

−2.120
−1.385
−2.166
−2.528
−2.656
−2.515
−1.732


VFT - b

6504.5
4601.5
6190.8
7167.1
7560.6
7279.9
5405.9


VFT - T0

89.2
231.8
112.9
62.2
90.7
109.2
273.5


Temperability, ψ
0.75
0.84
0.79
0.84
0.78
0.77
0.83
0.75


HTCTE + LTCTE
35.8
40.91
40.4
42.56
38.58
27.92
29.13
27.49


(10−7/° C.)













Sample

















Glaverbel









soda-lime
V
W
X
Y
Z







SiO2 (mol %)
70.06
63.29
60.87
65.43
62.23
62.53



B2O3 (mol %)
0.00
0.00
0.00
16.86
5.90
5.98



Al2O3 (mol %)
1.17
9.58
11.52
3.7
0.96
0.96



MgO (mol %)
6.49
0.00
0.00
0.00
6.49
6.37



CaO (mol %)
8.69
0.00
0.00
0.00
9.07
8.96



SrO (mol %)
0.00
0.00
0.00
3.06
0.00
0.00



Na2O (mol %)
13.33
16.34
16.63
6.47
12.79
12.64



K2O (mol %)
0.25
1.90
1.87
0
0.47
0.46



ZnO (mol %)
0.00
2.93
2.94
0
0.00
0.00



SnO2 (mol %)
0.22
0.05
0.05
0.05
0.11
0.11



Fe2O3 (mol %)




0.03
0.05



TiO2 (mol %)




1.96
1.93



LTCTE (10−7/° C.)
8.8
10.45
10.08
6.22



HTCTE (10−7/° C.)
27.0
17.02
18.00
39.36



Young's Modulus
72.0
65.64
65.84
78.53



(GPa)



Shear Modulus

27.37
27.17
32.41



(GPa)



Poisson's Ratio

0.199
0.213
0.212



Strain Point (° C.)
507
638
612
492



Anneal Point (° C.)
549
700
671
527



Softening Point (° C.)
728
931
907
673



Density (g/cm3)
2.540
2.425
2.442
2.432



SOC (TPa−1)
2.720
3.149
3.149
3.105



Refractive Index
1.520
1.4867
1.4903
1.5116



VFT - a

−0.116
−2.665
−0.779



VFT - b

2364
7338.2
2734.7



VFT - T0

629.2
118.9
347.9



Temperability, ψ
0.75
0.78
0.76
0.79



HTCTE + LTCTE
35.8
27.47
28.08
45.58



(10−7/° C.)










In addition to having high fracture toughness, the glasses described herein can have color and transparency/translucency properties that make them advantageous for a number of applications. The glasses of one or more embodiments may exhibit a substantially white, white-clear, gold or amber color, or other colors as well. In some embodiments, the glasses exhibit a color presented in SCE color space coordinates (determined from reflectance spectra measurements using a spectrophotometer, with illuminant D65 and specular reflectance excluded), of the following ranges: a*=from about −5 to about −1; b*=from about 5 to about 18; and L*>83. In some applications, the glasses are transparent and quantitatively white to yellow-brown in color and are of particular interest in photovoltaic applications.


Color examples are shown in Table 2. The first four columns of the table have the color coordination of thin-line PV cell, and the color coordination when the glass is on the top of the PV cell (thickness of the glass is 2 mm or 4 mm). The last four columns are the color coordination for the glass itself.





















SCE color coordination
L*
a*
b*
SCE color coordination
L*
a*
b*





PV cell thin lines
19.09
8.43
−14.12


Comp. Y (2 mm w/cell)
15.03
6.14
−8.62
Comp. Y (2 mm)
86.76
−2.51
9.14


Comp. Y (4 mm w/cell)
13.69
4.48
−5.54
Comp. Y (4 mm)
82.63
−4.48
15.11


Comp. Z (2 mm w/cell)
14.96
7
−10.28
Comp. Z (2 mm)
88.07
−1.72
6.72


Comp. Z (4 mm w/cell)
13.73
5.56
−7.65
Comp. Z (4 mm)
84.43
−3.32
12.21





SCI color
L*
a*
b*
SCI color coordination
L*
a*
b*





PV cell thin lines
19.25
7.99
−13.28


Comp. Y (2 mm w/cell)
38.56
1.66
−2.85
Comp. Y (2 mm)
91.89
−2.4
8.72


Comp. Y (4 mm w/cell)
37.43
0.66
−0.52
Comp. Y (4 mm)
87.81
−4.3
14.47


Comp. Z (2 mm w/cell)
38.04
1.23
−1.72
Comp. Z (2 mm)
93.2
−1.61
6.31


Comp. Z (4 mm w/cell)
38.76
2.11
−4
Comp. Z (4 mm)
89.63
−3.19
11.59










Wherein L* indicates lightness, a* is the red/green coordinate, and b* is the yellow/blue coordinate. Deltas for L* (ΔL*), a* (Δa*) and b* (Δb*) may be positive (+) or negative (−). From specular component excluded (SCE) color coordination, all the glasses make the PV cell darker, and move the color to less red and less blue. Less blue color is more aesthetically desirable for the appearance when combined with the PV cell.


As shown in FIG. 1, the transmittance of visible light (390-700 nm) is above 60% for all glasses and generally over 80% at the center (˜550 nm). Generally, solar cells are made out of N-type and P-type semiconductor materials that use the visual light wavelengths of 380 nm to 750 nm to generate electricity. Therefore, these glasses with the embodied color components (e.g, the darkest color, being Comp. Z, 4 mm) won't reduce the efficiency of solar cell significantly.


In some embodiments, the glass can be strengthened to include compressive stress (CS) that extends from a surface thereof to a depth of compression (DOC). The compressive stress regions are balanced by a central portion exhibiting a tensile stress. At the DOC, the stress crosses from a positive (compressive) stress to a negative (tensile) stress.


As an alternative to thermal tempering, the glasses disclosed herein may be ion exchanged by immersion in at least one ion exchange bath containing molten salts (e.g., nitrates, sulfides, halides, or the like) of at least one alkali metal such as lithium, sodium, or potassium. Ion exchange is commonly used to chemically strengthen glasses. In one particular example, alkali cations within a source of such cations (e.g., a molten salt, or “ion exchange,” bath) are exchanged with smaller alkali cations within the glass to achieve a layer under a compressive stress (CS) extending from the surface of the glass to a depth of compression (DOC) within the glass phase. For example, potassium ions from the cation source are often exchanged with sodium and/or lithium ions within the glass phase, and the K+ concentration profile correlates with the compressive stress and depth of layer. The ion exchange bath may contain a salt (or salts) of a single alkali metal (e.g., sulfides, nitrates, or halides of Li, Na, or K) or salts of two or more alkali metals (e.g., sulfides, nitrates, or halides of Li and Na, or sulfides, nitrates, or halides of Na and K). Ion exchange is carried out in the ion exchange bath at temperatures ranging from about 390° C. to about 550° C. for times ranging from about 0.5 hour to about 24 hours.


The glass, in some embodiments, is ion exchanged and has a compressive layer extending from a surface to a depth of compression (DOC) of at least about 10 μm or, in some embodiments, at least about 30 μm into the glass, or in some embodiments up to about 10, 15, 20 or 25% into the glass as measured by thickness (surface to center). In some embodiments, the compressive layer extends from the surface of the glass to a depth of up to about 20% of the thickness of the glass. In some embodiments, the glass may be strengthened to exhibit a surface compressive stress in a range from 250 MPa to 800 MPa or greater.


In the strengthened glass, the depth of the compressive layer may be determined by electron microprobe, glow-discharge optical emission spectroscopy (GDOES, which is a technique for measuring depth profiles of constituent elements in a solid sample by detecting emissions from atoms accommodated in plasma by sputtering), or similar techniques that can provide composition data as a function of depth, where data would show incorporation of Na (where Na+ replaces Li+ in the glass phase) and/or K at the surfaces. The DOC of a precursor glass may be measured by surface stress meter (FSM) using commercially available instruments such as the FSM-6000, manufactured by Orihara Industrial Co., Ltd. (Japan). Surface stress measurements rely upon the accurate measurement of the stress optical coefficient (SOC), which is related to the birefringence of the glass. SOC in turn is measured by those methods that are known in the art, such as fiber and four point bend methods, both of which are described in ASTM standard C770-98 (2013), entitled “Standard Test Method for Measurement of Glass Stress-Optical Coefficient,” the contents of which are incorporated herein by reference in their entirety, and a bulk cylinder method. CS may also be measured by measured by FSM. As used herein CS may be the “maximum compressive stress” which is the highest compressive stress value measured within the compressive stress layer. In some embodiments, the maximum compressive stress is located at the surface of the glass. In other embodiments, the maximum compressive stress may occur at a depth below the surface, giving the compressive profile the appearance of a “buried peak.”


The thermally or chemically strengthened glasses or articles disclosed herein may be incorporated into another article such as an article with a display (or display articles) (e.g., consumer electronics, including mobile phones, tablets, computers, navigation systems, and the like), architectural articles (e.g., windows, skylights, shingles), transportation articles (e.g., automotive, trains, aircraft, sea craft, etc.), appliance articles, or any article that would benefit from transparency, scratch-resistance, abrasion resistance or a combination thereof. In other embodiments, the glass forms a portion of a consumer electronic product, such as a cellular phone or smart phone, laptop computer, tablet, or the like. Such consumer electronic products typically comprise a housing having front, back, and side surfaces, and include electrical components such as a power source, a controller, a memory, a display, and the like, which are at least partially internal to the housing. In some embodiments, the glass described herein comprises at least a portion of a protective element, such as, but not limited to, the housing and/or display of a consumer electronic product.


Processes for Making Glasses

Glasses having the oxide contents listed in Table 1 can be made via traditional methods. For example, in some embodiments, the precursor glasses can be formed by thoroughly mixing the requisite batch materials (for example, using a turbular mixer) in order to secure a homogeneous melt, and subsequently placing into silica and/or platinum crucibles. The crucibles can be placed into a furnace and the glass batch melted and maintained at temperatures ranging from 1250-1650° C. for times ranging from about 6-16 hours. The melts can thereafter be poured into steel molds to yield glass slabs. Subsequently, those slabs can be transferred immediately to an annealer operating at about 500-650° C., where the glass is held at temperature for about 1 hour and subsequently cooled overnight. In another non-limiting example, precursor glasses are prepared by dry blending the appropriate oxides and mineral sources for a time sufficient to thoroughly mix the ingredients. The glasses are melted in platinum crucibles at temperatures ranging from about 1100° C. to about 1650° C. and held at temperature for about 16 hours. The resulting glass melts are then poured onto a steel table to cool. The precursor glasses are then annealed at appropriate temperatures.


Tempering of the embodied glasses was achieved using conventional processes wherein the glasses were heated in a radiant energy furnace or a convection furnace (or a “combined mode” furnace using both techniques) to a predetermined temperature, then gas cooling (“quenching”), typically via convection by blowing large amounts of ambient air against or along the glass surface.


Examples

Embodied glasses can be made as described herein. The properties of Glaverbel soda lime glass (SLG) are compared to the properties of the embodied glasses. Properties of the glasses are shown in Table 1. In addition, the surface compression composition C is compared to Glaverbel SLG for 1 mm thick glass slabs in Table 3. Composition C shows a temperability value of 0.99, approximately 32% higher than SLG and is capable of obtaining a surface compression of 145 MPa vs 105 MPa for SLG under equivalent tempering conditions.














TABLE 2










Surface




H
T0
Thickness
Compression


Glass
ψ
(cal/(cm2-s-K))
(° C.)
(mm)
(MPa)







Glaverbel
0.75
0.039
690
1.05
105


Comp. C
0.99
0.039
680
1.03
145









While typical embodiments have been set forth for the purpose of illustration, the foregoing description should not be deemed to be a limitation on the scope of the disclosure or appended claims. Accordingly, various modifications, adaptations, and alternatives may occur to one skilled in the art without departing from the spirit and scope of the present disclosure or appended claims.

Claims
  • 1. A glass composition comprising: 60-72 mol % SiO2;greater than 0 mol % Al2O3;greater than 0 mol % MgO;greater than 0 mol % CaO;8-16 mol % Na2O+K2O;0-16 mol % Na2O;0-16 mol % K2O;3-8 mol % ZnO; andfree of B2O3.
  • 2. The glass composition of claim 1, comprising >0-10 mol % MgO.
  • 3. The glass composition of claim 1, comprising >0-12 mol % Al2O3.
  • 4. The glass composition of claim 1, comprising >0-15 mol % CaO.
  • 5. The glass composition of claim 1, comprising >0-15 mol % Na2O.
  • 6. The glass composition of claim 1, wherein the glass composition has a low temperature coefficient of thermal expansion (LTCTE) measured at 25° C. and a high temperature coefficient of thermal expansion (HTCTE) measured at 300° C., and wherein the sum of the LTCTE and the HTCTE is 35×10−7/° C. or greater.
  • 7. The glass composition of claim 6, wherein the sum of the LTCTE and the HTCTE is 37×10−7/° C. or greater.
  • 8. The glass composition of claim 6, wherein the sum of the LTCTE and the HTCTE is 40×10−7/° C. or greater.
  • 9. The glass composition of claim 1, wherein the glass composition has a temperability, Ψ, and the temperability, Ψ, is equal to or greater than 0.80.
  • 10. The glass composition claim 9, wherein the temperability, Ψ, is equal to or greater than 0.85.
  • 11. The glass composition claim 9, wherein the temperability, Ψ, is equal to or greater than 0.90.
  • 12. A glass composition comprising: 60-72 mol % SiO2;greater than 0 mol % Al2O3;greater than 0 mol % MgO;greater than 0 mol % CaO;6-16 mol % Na2O+K2O;0-16 mol % Na2O;0-16 mol % K2O;3-8 mol % ZnO;a coloring component; andfree of B2O3.
  • 13. The glass composition of claim 12, wherein the coloring component comprises Fe2O3, V2O5, Cr2O3, TiO2, MnO2, NiO, ZnO, CuO, NiO, Co3O4, or combinations thereof.
  • 14. The glass composition of claim 12, wherein the total mol % of coloring components is from 0 to 4 mol %.
  • 15. The glass composition of claim 12, wherein the glass composition exhibits a color presented in SCE color space coordinates with the following values: a*=from about −5 to about −1; b*=from about 5 to about 18; and L*>83.
  • 16. The glass composition of claim 12, wherein the glass composition when rolled into a 2 mm thick slab has a transmission and wherein the transmission is greater than 80% at 575 nm.
  • 17. The glass composition of claim 12, comprising 8-16 mol % Na2O+K2O.
Parent Case Info

This application claims the benefit of priority under 35 U.S.C. § 371 of International Application No. PCT/US2018/047859, filed on Aug. 24, 2018, which claims the benefit of priority under 35 U.S.C. § 119 of U.S. Provisional Application Ser. No. 62/549,507 filed on Aug. 24, 2017, the content of each of which is relied upon and incorporated herein by reference in their entirety.

PCT Information
Filing Document Filing Date Country Kind
PCT/US2018/047859 8/24/2018 WO
Publishing Document Publishing Date Country Kind
WO2019/040818 2/28/2019 WO A
US Referenced Citations (226)
Number Name Date Kind
2145119 Littleton Jan 1939 A
2177336 Shaver et al. Oct 1939 A
3107196 Acloque Oct 1963 A
3169900 Ermlich Feb 1965 A
3174839 Long Mar 1965 A
3223499 Cypher et al. Dec 1965 A
3223501 Fredley et al. Dec 1965 A
3223549 Fredley et al. Dec 1965 A
3225349 Thor Dec 1965 A
3279906 Baker Oct 1966 A
3293015 Fredley et al. Dec 1966 A
3332759 McMaster et al. Jul 1967 A
3374078 Wright Mar 1968 A
3409422 Gulotta Nov 1968 A
3449102 Nedelec et al. Jun 1969 A
3497340 Dennison et al. Feb 1970 A
3558415 Rieser et al. Jan 1971 A
3637453 Simmons Jan 1972 A
3673049 Giffen et al. Jun 1972 A
3679388 Giddings et al. Jul 1972 A
3744921 Weller et al. Jul 1973 A
3753674 Ohlberg et al. Aug 1973 A
3776712 Wilde Dec 1973 A
3793127 Wartenberg Feb 1974 A
3794476 Michalik et al. Feb 1974 A
3830540 Sperry Aug 1974 A
3844758 Wartenberg Oct 1974 A
3883339 Michalik et al. May 1975 A
3890128 Melling et al. Jun 1975 A
3902884 Harrison Sep 1975 A
3929442 Neely, Jr. Dec 1975 A
3931438 Beall et al. Jan 1976 A
3936291 McMaster Feb 1976 A
3973943 Seymour Aug 1976 A
3994711 McMaster Nov 1976 A
4081254 Matsumoto et al. Mar 1978 A
4128690 Boardman et al. Dec 1978 A
4194898 Marsh et al. Mar 1980 A
4198226 Marsh et al. Apr 1980 A
4198463 Greenhalgh Apr 1980 A
4204845 Shields et al. May 1980 A
4214886 Shay et al. Jul 1980 A
4300936 Quillevere et al. Nov 1981 A
4314836 Seymour Feb 1982 A
4319907 Pike Mar 1982 A
4372774 Cross et al. Feb 1983 A
4400193 Cross et al. Aug 1983 A
4470838 McMaster et al. Sep 1984 A
4471024 Pargamin et al. Sep 1984 A
4494972 Marsh et al. Jan 1985 A
4516999 Kiefer et al. May 1985 A
4662926 Aratani et al. May 1987 A
4744676 Lind May 1988 A
4773926 Letemps et al. Sep 1988 A
4913720 Gardon et al. Apr 1990 A
5009694 Nishitani et al. Apr 1991 A
5071796 Jones et al. Dec 1991 A
5121329 Crump Jun 1992 A
5236488 Vehmas Aug 1993 A
5340433 Crump Aug 1994 A
5626911 Bertin et al. May 1997 A
5654057 Kitayama et al. Aug 1997 A
5676722 Seidel et al. Oct 1997 A
5735923 Hisaeda Apr 1998 A
5885316 Sato et al. Mar 1999 A
5931981 McMaster et al. Aug 1999 A
5938808 McMaster et al. Aug 1999 A
6053011 Lisec Apr 2000 A
6079227 Yoshizawa et al. Jun 2000 A
6094943 Okuda et al. Aug 2000 A
6183565 Granneman et al. Feb 2001 B1
6200665 Seto Mar 2001 B1
6295842 McMaster Oct 2001 B1
6336775 Morita et al. Jan 2002 B1
6353283 Ghosh et al. Mar 2002 B1
6370917 Kato et al. Apr 2002 B1
6412309 Kajii et al. Jul 2002 B1
6442017 Ewing et al. Aug 2002 B1
6461439 Granneman et al. Oct 2002 B1
6472800 Goda et al. Oct 2002 B2
6598427 Douche et al. Jul 2003 B1
6613685 Granneman et al. Sep 2003 B1
6642017 Weiser Nov 2003 B2
6656597 Takahara Dec 2003 B2
6713180 Torr et al. Mar 2004 B1
6722160 Nemugaki et al. Apr 2004 B1
6770851 Granneman et al. Aug 2004 B2
6805749 Granneman et al. Oct 2004 B2
6826929 Boaz Dec 2004 B2
6877250 Granneman et al. Apr 2005 B2
6881485 Kato et al. Apr 2005 B2
6881931 Vehmas et al. Apr 2005 B2
6977710 Akiyama et al. Dec 2005 B2
7022627 Granneman et al. Apr 2006 B2
7048488 Kuznetsov et al. May 2006 B1
7153798 Bordeaux et al. Dec 2006 B2
7215262 Suzuki et al. May 2007 B2
7306848 Tominaga et al. Dec 2007 B2
7312156 Granneman et al. Dec 2007 B2
7341968 Yoda et al. Mar 2008 B2
7367205 Boaz May 2008 B1
7410355 Granneman et al. Aug 2008 B2
7666511 Ellison et al. Feb 2010 B2
7694532 Boaz Apr 2010 B1
7867932 Beall Jan 2011 B2
8074473 Nitschke et al. Dec 2011 B2
8233433 Kalhan Jul 2012 B2
8234883 Krall et al. Aug 2012 B2
8289342 Matsumoto Oct 2012 B2
8415013 Barefoot et al. Apr 2013 B2
8524804 Kitano et al. Sep 2013 B2
8713967 Danielson et al. May 2014 B2
8713972 Lakota et al. May 2014 B2
8728961 Lautenschlaeger et al. May 2014 B2
8769990 Saito et al. Jul 2014 B2
8916013 Hong et al. Dec 2014 B2
8997521 Vehmas et al. Apr 2015 B2
9003835 Lock Apr 2015 B2
9039886 Gong et al. May 2015 B2
9073291 Bookbinder et al. Jul 2015 B2
9137892 Bando et al. Sep 2015 B2
9296638 Lezzi et al. Mar 2016 B2
9478449 Vermont et al. Oct 2016 B2
9522836 Gulati et al. Dec 2016 B2
9552836 Ramakrishnan et al. Jan 2017 B2
9725359 Weber Aug 2017 B2
9761828 Dabich et al. Sep 2017 B2
9776905 Maschmeyer et al. Oct 2017 B2
9783448 Maschmeyer et al. Oct 2017 B2
9802853 Maschmeyer et al. Oct 2017 B2
10150699 Baum, Jr. et al. Dec 2018 B2
10195778 Wolf et al. Feb 2019 B2
20010007723 Tokumoto Jul 2001 A1
20030177790 Langsdorf et al. Sep 2003 A1
20040107733 Yashizawa Jun 2004 A1
20050099618 DiFoggio et al. May 2005 A1
20050138892 Misonou Jun 2005 A1
20050266247 Yoshizawa Dec 2005 A1
20060054774 Yassour et al. Mar 2006 A1
20060121281 Tamai et al. Jun 2006 A1
20060179722 Spindler Aug 2006 A1
20060219605 Devitt Oct 2006 A1
20070122580 Krall et al. May 2007 A1
20070271957 Nakamura et al. Nov 2007 A1
20080314403 Rebours Dec 2008 A1
20090069163 Beall Mar 2009 A1
20090092472 Luo et al. Apr 2009 A1
20090220761 Dejneka et al. Sep 2009 A1
20100035038 Barefoot et al. Feb 2010 A1
20100084016 Aitken et al. Apr 2010 A1
20100130251 Chu May 2010 A1
20100162761 Carney et al. Jul 2010 A1
20100183767 Noordam et al. Jul 2010 A1
20100279068 Cook et al. Nov 2010 A1
20110123832 Matsumoto May 2011 A1
20110123833 Endo et al. May 2011 A1
20110200804 Tomamoto et al. Aug 2011 A1
20110281093 Gulati et al. Nov 2011 A1
20110289971 Brown et al. Dec 2011 A1
20110289972 Brown et al. Dec 2011 A1
20120144867 Busch Jun 2012 A1
20120145991 Nam et al. Jun 2012 A1
20120194974 Weber et al. Aug 2012 A1
20120247063 Grzybowski et al. Oct 2012 A1
20120258250 Rodgers Oct 2012 A1
20120291707 Granneman Nov 2012 A1
20130008500 Lin et al. Jan 2013 A1
20130019639 Saito et al. Jan 2013 A1
20130047673 Lee et al. Feb 2013 A1
20130052347 Kuznetsov et al. Feb 2013 A1
20130071666 Komori et al. Mar 2013 A1
20130122284 Gross May 2013 A1
20130122313 Gross May 2013 A1
20130199448 Granneman et al. Aug 2013 A1
20130255314 Allan et al. Oct 2013 A1
20130323444 Ehemann et al. Dec 2013 A1
20140026622 Wang Jan 2014 A1
20140050912 Isono et al. Feb 2014 A1
20140053605 Mader Feb 2014 A1
20140065401 Donovan et al. Mar 2014 A1
20140113854 Ni et al. Apr 2014 A1
20140120279 Demartino et al. May 2014 A1
20140141217 Gulati et al. May 2014 A1
20140162000 Son et al. Jun 2014 A1
20140218867 Kim et al. Aug 2014 A1
20140242391 Ono et al. Aug 2014 A1
20140290310 Green Oct 2014 A1
20140370303 Jin et al. Dec 2014 A1
20150027169 Fredholm Jan 2015 A1
20150030827 Gomez et al. Jan 2015 A1
20150031752 Keil et al. Jan 2015 A1
20150037552 Mauro Feb 2015 A1
20150052949 Bayne et al. Feb 2015 A1
20150082834 Vehmas et al. Mar 2015 A1
20150083200 Hickman et al. Mar 2015 A1
20150096331 Rantala et al. Apr 2015 A1
20150158757 Amma et al. Jun 2015 A1
20150166401 Yamamoto Jun 2015 A1
20150218045 Balcom et al. Aug 2015 A1
20150240038 Macedo et al. Aug 2015 A1
20150251353 Rodgers et al. Sep 2015 A1
20150274015 Wachinger et al. Oct 2015 A1
20150307385 Klein et al. Oct 2015 A1
20150343704 Stahl et al. Dec 2015 A1
20150368153 Pesansky et al. Dec 2015 A1
20160002103 Wang et al. Jan 2016 A1
20160031742 Maschmeyer et al. Feb 2016 A1
20160031743 Maschmeyer et al. Feb 2016 A1
20160031744 Maschmeyer et al. Feb 2016 A1
20160031752 Maschmeyer et al. Feb 2016 A1
20160168023 Baum, Jr. Jun 2016 A1
20160194233 Van Pelt Jul 2016 A1
20160194239 Seto Jul 2016 A1
20160207819 Cleary et al. Jul 2016 A1
20160281233 Granneman et al. Sep 2016 A1
20160304352 Fernandez et al. Oct 2016 A1
20160326051 Kim Nov 2016 A1
20170072613 Bracha et al. Mar 2017 A2
20170158543 Metz et al. Jun 2017 A1
20170361574 Kiczenski et al. Dec 2017 A1
20180210308 Lam et al. Jul 2018 A1
20180304588 Harris et al. Oct 2018 A1
20190030861 Bellman et al. Jan 2019 A1
20190227357 Williams et al. Jul 2019 A1
20190270284 Couillard et al. Sep 2019 A1
20190391337 Sato Dec 2019 A1
Foreign Referenced Citations (172)
Number Date Country
4265772 Nov 1973 AU
0524573 Sep 1982 AU
0535129 Mar 1984 AU
1148742 Jun 1983 CA
1176468 Oct 1984 CA
2171323 Jan 1996 CA
1208266 Feb 1999 CN
1693247 Nov 2005 CN
1896020 Jan 2007 CN
101312919 Nov 2008 CN
101671112 Mar 2010 CN
101774751 Jul 2010 CN
102149649 Aug 2011 CN
102659305 Sep 2012 CN
102863146 Jan 2013 CN
103253857 Aug 2013 CN
103319082 Sep 2013 CN
103359934 Oct 2013 CN
103534216 Jan 2014 CN
103781733 May 2014 CN
103827051 May 2014 CN
104211288 Dec 2014 CN
104260569 Jan 2015 CN
104310773 Jan 2015 CN
104355530 Feb 2015 CN
104479282 Apr 2015 CN
104583141 Apr 2015 CN
205275454 Jun 2016 CN
106045283 Oct 2016 CN
2233057 Mar 1973 DE
0173418 Mar 1986 EP
0413254 Feb 1991 EP
0882681 Dec 1998 EP
1215039 Jun 2002 EP
1245545 Oct 2002 EP
1380550 Jan 2004 EP
1414762 May 2004 EP
1533282 May 2005 EP
1925952 May 2008 EP
2543644 Jan 2013 EP
2853517 Apr 2015 EP
2326386 Apr 1977 FR
0996423 Jun 1965 GB
1103192 Feb 1968 GB
1112781 May 1968 GB
1160284 Aug 1969 GB
1253681 Nov 1971 GB
1282720 Jul 1972 GB
1289488 Sep 1972 GB
2232978 Jan 1991 GB
202420 May 2005 IN
200803022 Aug 2008 IN
51-103920 Sep 1976 JP
55-104935 Aug 1980 JP
56-155030 Dec 1981 JP
56-155031 Dec 1981 JP
57-067035 Apr 1982 JP
57-067036 Apr 1982 JP
58-088132 May 1983 JP
58-091042 May 1983 JP
59-008626 Jan 1984 JP
59-008627 Jan 1984 JP
59-008628 Jan 1984 JP
59-008629 Jan 1984 JP
59-008630 Jan 1984 JP
59-008631 Jan 1984 JP
59-057923 Apr 1984 JP
60-171245 Sep 1985 JP
61-072637 Apr 1986 JP
61-141756 Jun 1986 JP
62-036030 Feb 1987 JP
63-270330 Nov 1988 JP
02-102436 Apr 1990 JP
02-175624 Jul 1990 JP
03-045526 Feb 1991 JP
03-271127 Dec 1991 JP
06-336533 Dec 1994 JP
07-089739 Apr 1995 JP
07-809739 Apr 1995 JP
07-157322 Jun 1995 JP
07-267664 Oct 1995 JP
11-199257 Jul 1999 JP
2000-072463 Mar 2000 JP
2000-103632 Apr 2000 JP
2000-172202 Jun 2000 JP
2000-327355 Nov 2000 JP
2001-002434 Jan 2001 JP
2001180967 Jul 2001 JP
2001180967 Jul 2001 JP
2001-307662 Nov 2001 JP
2003-040635 Feb 2003 JP
2003-137603 May 2003 JP
2003-261344 Sep 2003 JP
2003-342030 Dec 2003 JP
2004-091311 Mar 2004 JP
2007-191319 Aug 2007 JP
2007-261850 Oct 2007 JP
4397196 Jan 2010 JP
4438126 Mar 2010 JP
4557606 Oct 2010 JP
4642107 Mar 2011 JP
4722371 Jul 2011 JP
4951838 Jun 2012 JP
2012-232882 Nov 2012 JP
5334005 Nov 2013 JP
2015-086080 May 2015 JP
5714701 May 2015 JP
10-0218143 Sep 1999 KR
10-2002-0061567 Jul 2002 KR
10-0690381 Mar 2007 KR
10-0909835 Jul 2009 KR
10-0918577 Sep 2009 KR
10-0937889 Jan 2010 KR
10-1000677 Dec 2010 KR
10-1032825 May 2011 KR
10-2011-0087774 Aug 2011 KR
10-2011-0106629 Sep 2011 KR
10-2011-0112503 Oct 2011 KR
10-1093947 Dec 2011 KR
10-1120262 Mar 2012 KR
10-2012-0051220 May 2012 KR
10-2012-0070450 Jun 2012 KR
10-2013-0024484 Mar 2013 KR
10-1248380 Mar 2013 KR
10-1286131 Jul 2013 KR
10-1413626 Aug 2014 KR
10-2014-0110364 Sep 2014 KR
10-2014-0135846 Nov 2014 KR
2151750 Jun 2000 RU
2199496 Feb 2003 RU
2237621 Oct 2004 RU
2299184 May 2007 RU
2464243 Oct 2012 RU
443845 Sep 1974 SU
537960 Dec 1976 SU
548188 Sep 1982 SU
1098916 Jun 1984 SU
1655920 Jun 1991 SU
9003337 Apr 1990 WO
9944952 Sep 1999 WO
0116040 Mar 2001 WO
200134531 May 2001 WO
WO200134531 May 2001 WO
0216277 Feb 2002 WO
0314035 Feb 2003 WO
2006083902 Aug 2006 WO
2006110145 Oct 2006 WO
2008020509 Feb 2008 WO
2008143999 Nov 2008 WO
2008147558 Dec 2008 WO
2010076903 Jul 2010 WO
2011122678 Oct 2011 WO
2012082709 Jun 2012 WO
2012125857 Sep 2012 WO
2012142629 Oct 2012 WO
2013016157 Jan 2013 WO
2014030682 Feb 2014 WO
2014060108 Apr 2014 WO
2014139147 Sep 2014 WO
2014182776 Nov 2014 WO
2014201315 Dec 2014 WO
2015031148 Mar 2015 WO
2015031594 Mar 2015 WO
2015033562 Mar 2015 WO
2016019171 Feb 2016 WO
2016057590 Apr 2016 WO
2016094262 Jun 2016 WO
2017019837 Feb 2017 WO
2017020041 Feb 2017 WO
2017071911 May 2017 WO
2017139552 Aug 2017 WO
2021025981 Feb 2021 WO
Non-Patent Literature Citations (201)
Entry
JP2001180967 translation (Year: 2001).
WO200134531 translation (Year: 2001).
Chinese Patent Application No. 201880054891.5, Office Action dated Dec. 15, 2021, 13 pages (8 pages of English Translation and 5 pages of Original Document), Chinese Patent Office.
Barsom; “Fracture of Tempered Glass”; J. Am. Ceram. Soc., 51[2] 75-78 (1968).
Gardon; “Thermal Tempering of Glass”; pp. 146-216 in Glass: Science and Technology, vol. 5, Elasticity and Strentth in Glasses, Ed. by D.R. Uhlmann and N.J. Kreidl, Academic Press, New York, 1980.
Gulati, “Frangibility of Tempered Soda-Lime Glass Sheet,” pp. 13-15 in Glass Performance Days, 1997.
International Search Report and Written Opinion of the International Searching Authority; PCT/US2018/047859; dated Feb. 20, 2019; 19 Pages; European Patent Office.
Invitation to Pay Additional Fees of the International Searching Authority; PCT/US2018/047859; dated Dec. 7, 2018; 16 Pages; European Patent Office.
Morey; “The Effect of Boric Oxide on the Devitrification of the Soda-Lime-Silica Glasses. The Quaternary System, Na20—CaO—B2O3—SiO2”; Journal of the Amercian Ceramic Society; vol. 15, Issue 9; pp. 457-475 (1932).
Narayan Aswamy; “Stress and Structural Relaxation in Tempering Glass,” J. Am. Ceram. Soc., 61[3-4] 146-152 (1978).
Ohlberg et al.; “Thermal Stress Calculations Based on a Linear Viscoelastic Deviatoric Response and a Fictive Temperature Component for the Volumetric Response,” Journal of Non-Crystalline Solids, 14 280-286 (1974).
Timoshenko et al; “Theory of Elasticity”; 2nd Ed; p. 146. McGraw-Hill Book Co., New York, 1951.
Chen, et al., “Nanopatterned Graphene on a Polymer Substrate by a Direct Peel-off Technique”, ACS Appl. Mater. Interfaces, vol. 7, Issue 10, 2015, pp. 5938-5943.
Choi et al., “Influence of removing PMMA residues on surface of CVD graphene using a contact-mode atomic force Microscope” RSC Adv., vol. 7, 2017, pp. 6943-6949.
Gammelgaard et al., “Graphene transport properties upon exposure to PMMA processing and heat treatments”, 2D Materials, vol. 1, 2014, 035005, 12 pages.
Lin et al., “Graphene annealing: how clean can it be?”, Nano Lett., vol. 12, Issue 1, 2012, pp. 414-419.
ASTM C1499-09, “Standard Test Method for Monotonic Equibiaxial Flexural Strength of Advanced Ceramics at Ambient Temperature”, 2013, 14 pages.
ASTM C158-02, “Standard Test Methods for Strength of Glass by Flexure” (Determination of Modulus of Rupture), 2012, 9 pages.
Guo, Xiaoju et al. “Unified approach for determining the enthalpic fictive temperature of glasses with arbitrary thermal history” Journal of Non-Crystalline Solids, vol. 357, 2011, pp. 3230-3236.
International Search Report and Written Opinion of the International Searching Authority; PCT/US2020/027913; dated Aug. 3, 2021; 11 pages; European Patent Office.
Luo et al., “Competing Indentation Deformation Mechanisms in Glass Using Different Strengthening Methods”, Frontiers in Materials, vol. 3, No. 52, 2016, 11 pages.
Aben, H. et al., “2.7 Stresses Due to Heterogeneities,” Photoelasticity of Glass, Springer-Verlag, New York, 1993, 260 pages.
Acloque, P., “Influence of Strain-Systems in Glass upon the Course of its Fracture,” Proceedings of the 4th International Glass Congress, vol. 6, 1965, pp. 279-291.
Acloque, Paul, “Comparison Between Heat-Transfer Conditions and Setting Up of Strain in Glass During Heat-Treatment,” Journal of the American Ceramic Society, vol. 44, No. 7, Jul. 1961, pp. 364-373.
Agarwal, Anand et al., “A simple IR spectroscopic method for determining fictive temperature of silica glasses,” Journal of Non-Crystalline Solids, vol. 185, 1995, pp. 191-198.
Agarwal, Anand et al., “Determination of Fictive Temperature of Soda-Lime Silicate Glass,” Journal of the American Ceramic Society, vol. 78, No. 3, Mar. 1995, pp. 827-829.
Akeyoshi, K. et al., “Mechanical Properties of Tempered Glass,” Proceedings of the 7th International Glass Congress, vol. 14, 1965, pp. 80-85.
Alexiades, V. et al., “The New Way/Glaston Problem,” 28th Annual Workshop on Mathematical Problems in Industry, University of Delaware, Jun. 2012, 30 slides.
Argon, A. S., “Chapter 3: Inelastic Deformation and Fracture in Oxide, Metallic, and Polymeric Glasses,” In, “Glass Science and Technology,” vol. 5, Elasticity and Strength in Glass, Academic Press, May 28, 1980, pp. 79-132.
Aronen, Antti et al., “Tempering of Thin Glass,” Glasstec 2012: Engineered Transparency, Oct. 25-26, 2012, pp. 145-153.
Author Unknown, “Application Note AN 527: Depth profiling of complex samples using confocal Raman microscopy,” Bruker Optics Inc., 2012, 3 pages.
Author Unknown, “Architectural ERH2 ,” Architectural Glass Systems, Glasstech, Inc., 2011, 2 pages.
Author Unknown, “Architectural FCH2(Trademark) ,” Architectural Glass Systems, Glasstech, Inc., 2011, 2 pages.
Author Unknown, “Coming(Registered) Gorilla(Trademark) Glass,” Coming Incorporated, 2009, 2 pages.
Author Unknown, “Glass Strengthening Methods,” Abrisa Technologies, Apr. 2015, 2 pages.
Author Unknown, “Heat Treated Glass for Architectural Glazing,” Glass Technical Document: TD-138, PPG Glass Technology, PPG Industries, Inc., Nov. 2011, 8 pages.
Author Unknown, “Introducing-Glasstech CRB-S.TM. 1900 for Solar Parabolic Shapes,” Solar Glass Systems, Glasstech, Inc., Date Unknown, 1 page, Retrieved Jul. 1, 2015.
Author Unknown, “New Way Air Bearings,” 28th Annual Workshop on Mathematical Problems in Industry, University of Delaware, Jun. 2012, 16 slides.
Author Unknown, “Products, Glazing Techniques and Maintenance Section 4: GGF Dalasheet for the Quality of Thermally Toughened Soda Lime Silicate Safety Glass for Building,” Glass and Glazing Federation, Aug. 2009, 12 pages.
Author Unknown, “Schott Technical Glasses—Physical and technical properties,” Schott North America, Inc., Feb. 2010, 44 pages.
Author Unknown, “scratch and dig numbers,” Sizes, Inc., Last Revised: Jun. 24, 2010, 5 pages, http:/fwww.sizes.com/units/scratch_and_dig.him.
Author Unknown, “Solar FCH-S(Trademark),” Solar Glass Systems, Glasstech, Inc., 2011, 2 pages.
Author Unknown, “Standard Specification for Heat-Strengthened and Fully Tempered Flat Glass,” Designation: C 1048-12, ASTM International Standard, 2015, 7 pages.
Author Unknown, “Standard Specification for Heat-Treated Flat Glass-Kind HS, Kind FT Coated and Uncoated Glass,” Designation: C 1048-4, ASTM International Standard, 2009, 7 pages.
Author Unknown, “Subject Index,” Date Unknown, pp. 277-282.
Author Unknown, “Thermal Tempering,” EuropTec GmbH, Nov. 6, 2014, 2 pages.
Author Unknown, “Unsteady Heat Transfer—HT3: Experimental Studies of Thermal Diffusivities and Heat Transfer Coefficients,” Date Unknown, 27 slides.
Ayinder, C.C. et al., “Thermal-Tempering Analysis of Bulk Metallic Glass Plates Using an Instant-Freezing Model,” Metallurgical and Materials Transactions A, vol. 32A, Nov. 2001, pp. 2709-2715.
Baldwin, K. J. et al., “Confocal Raman Microspectroscopy through a Planar Interface,” Applied Spectroscopy, vol. 55, No. 5, 2001, pp. 517-524.
Bandyopadhyay et al; “Application of Fused Deposition in Controlled Microstructure Metal-Ceramic Composites”, Rapid Prototyping Journal, vol. 12 Issue 3, pp. 121 128 (2006).
Barr, J. W., “Glass Tempering by Numbers,” Aug. 2008, 8 pages.
Barr, Jonathan W., “The Tempering Process,” Cardinal Waxachachie Tempering Seminar, Mar. 26, 2008, 36 slides.
Barr, Jonathan, “The Glass Tempering Handbook-Understanding the Glass Tempering Process,” Self Published, 2015, 52 pages, http://www.lambertgtservices.co.uk/book/TheGlassTemperingHandbook.pdf.
Barsom, John M., “Fracture of Tempered Glass,” Journal of the American Ceramic Society, vol. 51, No. 2, Feb. 1968, pp. 75-78.
Bartholomew, Roger F. et al., “Chapter 6: Chemical Strengthening of Glass,” In “Glass: Science and Technology,” vol. 5, Elasticity and Strength in Glass, Academic Press, May 28, 1980, pp. 217-270.
Beauchamp, Edwin K. et al., “Dynamics of Window Glass Fracture in Explosions,” Sandia Report SAND98-0598 UC-700, Sandia National Laboratories, May 1998, 74 pages.
Bird, R. D., W. E. Stewart, and E. N. Lightfoot, Transport Phenomena—Chapter 11: The Equations of Change for Nonisothermal Systems, Wiley, (1960) pp. 349-373.
Bird, R. D., W. E. Stewart, and E. N. Lightfoot, Transport Phenomena—Chapter 3: The Equations of Change for Isothermal Systems, Wiley, (1960) pp. 75-113.
Boaz, Prem, “Tempering Very Thin Glass—What Radio Waves Mean for the Glass Industry,” USGlass Magazine, vol. 45, Issue 3, Mar. 2010, 5 pages.
Boaz, Prem, “Thin glass processing with radio wave assist,” Glass on Web, Last Reviewed: Jan. 2013, 6 pages, http://www.glassonweb.com/articles/article/561/.
Boguslavskll, I. A., “Studying the Nature of the Super-Strength of Glasses Strengthened by the Thermophysical Method,” Glass and Ceramics, vol. 21, No. 10, Oct. 1964, pp. 562-567.
Brown, Angus M., “Nonlinear regression analysis of data using a spreadsheet,” Application Note, ISC, Oct. 2001, pp. 58-59.
CN101671112A English Translation Performed by USPTO Translations Service Center Apr. 2017.
Conradt, Reinhard, “I. Fragility and its Relation to Other Glass Properties,” IMI-NFG's MITT Course on Relaxation Processes in Glass Lecture 21, Apr. 6-8, 2010, 61 slides.
Conradt, Reinhard, “II. Networks,” IIMI-NFG's Min Course on Relaxation Processes in Glass Lecture 22, Apr. 6-8, 2010, 61 slides.
Conway, Jr., Joseph C. et al., “Use of Crack Branching Data for Measuring Near-Surface Residual Stresses in Tempered Glass,” Journal of the American Ceramic Society, vol. 72, No. 9, Sep. 1989, pp. 1584-1587.
Cox, Dr. Chris, “Lecture 3: Complex exponential function, Fourier and Laplace transforms,” IMI-NFG's MITT Course on Relaxation Processes in Glass and Polymers Lecture 3, 2010, 25 slides.
Cox, Dr. Chris, “Lecture 4: Differential Equations,” IMI-NFG's Min Course on Relaxation Processes in Glass and Polymers Lecture 4, 2010, 24 slides.
Danishkin, G. K. et al., “Development of a Continuous Method of Bending and Toughening Glass,” Glass and Ceramics, vol. 34, Issue 8, Aug. 1977, pp. 495-498.
Daudeville, L. et al., “Numerical Simulation of Soda-Lime Silicate Glass Tempering,” Journal de Physique IV, France, vol. 6, No. C1, Jan. 1996, pp. C1-175-C1-185.
Daudeville, Laurent et al., “Thermal Tempering Simulation of Glass Plates: Inner and Edge Residual Stresses,” Journal of Thermal Stresses, vol. 21, 1998, pp. 667-689.
International Search Report and Writien Opinin PCT/US2016/044401 dated Jan. 2, 2017.
International Search Report and Writien Opinion PCT/US2016/044445 dated Oct. 14, 2016.
International Search Report and Written Opinion of the International Searching Authority; PCT/US15/42955; dated Nov. 4, 2015; 10 Pages; European Patent Office.
International Search Report and Written Opinion of the International Searching Authority; PCT/US16/45022; dated Jan. 31, 2017; 20 Pages; European Patent Office.
International Search Report and Written Opinion of the International Searching Authority; PCT/US2016/044406; dated Nov. 25, 2016; 15 Pages; European Patent Office.
International Search Report and Written Opinion of the International Searching Authority; PCT/US2020/062128; dated Mar. 15, 2021; 9 pages; European Patent Office.
International Search Report and Written Opinion of the International Searching Authority; PCT/US2020/062145; dated Mar. 16, 2021, 11 pages; Korean Patent Office.
International Search Report and Written Opinion PCT/US2015/042965 dated Nov. 2, 2015.
Ito, Setsuro, “Brittleness and Nano-Structure of Glass,” 4th International Workshop on Flow and Fracture of Advanced Glasses Presentation, Nov. 5-7, 2007, Shiga, Japan, 37 slides.
Jain, Himanshu, “Electrical Relaxation—Topic 1: Quasi-free ion transport,” IMI-NFG's MITI Course on Relaxation Processes in Glass Lecture 23, Advanced Vitreous State, The Properties of Glass: Dielectric Properties—Lecture 1, 2010, 28 slides.
Jain, Himanshu, “Electrical Relaxation—Topic 3: Nearly constant loss—second universality,” IMI-NFG's Min Course on Relaxation Processes in Glass Lecture 25, Advanced Vitreous State, The Properties of Glass: Dielectric Properties—Lecture 3, 2010, 24 slides.
Jain, Himanshu, “Electrical Relaxation-Topic 2: Universal dielectric response (UDR),” IMI-NFG's MITT Course on Relaxation Processes in Glass Lecture 24, Advanced Vitreous State, The Properties of Glass: Dielectric Properties—Lecture 1, 2010, 22 slides.
Karlsson, Stefan et al., “The technology of chemical glass strengthening—a review,” Glass Technology, European Journal of Glass Science Technology Part A, vol. 51, No. 2, Apr. 2010, pp. 41-54.
Kassir-Bodon, Assia et al., “Raman Mapping of the Indentation-Induced Densification of a Soda-Lime-Silicate Glass,” International Journal of Applied Glass Science, vol. 3, No. 1, 2012, pp. 29-35.
Kiefer, Werner et al., “Method for Thermal Prestressing of Glass,” Strength of Inorganic Glass, Plenum Press, New York, 1985, pp. 501-511.
Kishii, Toru, “Surface Stress Meters Utilising the Optical Waveguide Effect of Chemically Tempered Glasses,” Optics and Lasers in Engineering, vol. 4, 1983, pp. 25-38.
Kistler, S. S., “Stresses in Glass Produced by Nonuniform Exchange of Monovalent Ions,” Journal of the American Ceramic Society, vol. 45, No. 2, Feb. 1962, pp. 59-68.
Klein et al; “Additive Manufacturing of Optically Transparent Glass”; 3D Printing and Additive Manufacturing; vol. 2, No. 3; 2015; pp. 92-105.
Koike, A. et al., “Fictive temperature dependence of subcritical crack growth rate of normal glass and anomalous glass,” Journal of Non-Crystalline Solids, vol. 352, 2006, pp. 5522-5530.
Kong, Jinhak et al., “Residual Stress Analysis with Improved Numerical Methods for Tempered Plate Glasses Based on Structural Relaxation Model,” Metals and Materials International, vol. 13, No. 1, 2007, pp. 67-75.
Lathabai, Srinivasarao et al., “Fracture mechanics model for subthreshold indentation flaws: Part 1—Equilibrium fracture,” Journal of Materials Science, vol. 26, 1991, pp. 2157-2168.
Lee, Hoikwan et al., “Glass Thickness and Fragmentation Behavior in Stressed Glasses,” New Journal of Glass and Ceramics, vol. 2, 2012, pp. 138-143.
Lezzi, P. J. et al., “Confirmation of thin surface residual compressive stress in silica glass fiber by FTIR reflection spectroscopy,” Journal of Non-Crystalline Solids, vol. 390, 2014, pp. 13-18.
Li, Hong et al., “Effect of Fictive Temperature on Dynamic Fatigue Behavior of Silica and Soda-Lime Glasses,” Journal of the American Ceramic Society, vol. 78, No. 5, 1995, pp. 1393-1396.
Loucks, “Lecture 13: The Fictive and Glass Transition Temperatures,” IMI-NFG's Min Course on Relaxation Processes in Glass Lecture 13, Mar. 2, 2010, 25 Slides.
Loucks, “Lecture 15: The Tool-Narayanaswamy-Moynihan Equation Part II and DSC,” IMI-NFG's MITT Course on Relaxation Processes in Glass Lecture 15, Mar. 9, 2010, 33 Slides.
Loucks, Dr. Roger, “Lecture 14: Relaxation and theTool-Narayanaswamy-Moynihan Equation,” IMI-NFG's MITT Course on Relaxation Processes in Glass Lecture 14, Mar. 4, 2010, 27 slides.
Loucks, Dr. Roger, “Lecture 16: The Tool-Narayanaswamy-Moynihan Equation Part II and DSC,” IMI-NFG's MITT Course on Relaxation Processes in Glass Lecture 16, Mar. 11, 2010, 32 slides.
Luo et al; “Additive Manufacturing of Glass for Optical Applications”; Proc. of SPIE, vol. 9738, 2016; pp. 97380Y-1-97380Y-9.
Markovsky, Alex et al., “An Efficient and Stable Algorithm for Calculating Fictive Temperatures,” Communications of the American Ceramic Society, Apr. 1984, 2 pages.
Martin, Dr. Steve, “Lecture 10: Thermodynamic Functions,” IMI-NFG's MITT Course on Relaxation Processes in Glass Lecture 10, 2010, 25 slides.
Martin, Dr. Steve, “Lecture 11: Thermodynamics in the Glass Transition Region,” IMI-NFG's MITT Course on Relaxation Processes in Glass Lecture 11, 2010, 22 slides.
Martin, Dr. Steve, “Lecture 12: The Glass Transition as a Kinetic Transition,” IMI-NFG's Min Course on Relaxation Processes in Glass Lecture 12, 2010, 21 slides.
Martin, Dr. Steve, “Lecture 9: Thermodynamic Concepts and the Law of Thermodynamics,” IMI-NFG's Min Course on Relaxation Processes in Glass Lecture 9, 2010, 32 slides.
Massen, Claire P. et al., “Power-law distributions for the areas of the basins of attraction on a potential energy landscape,” Physical Review E, The American Physical Society, vol. 75, 2007, 4 pages.
Mauricio-Iglesias, M. et al., “Raman depth-profiling characterization of a migrant diffusion in a polymer,” Journal of Membrane Science, vol. 375, 2011, pp. 165-171.
McGlinchy, Timothy B., “Energy Efficient Tripe IG Automation EEE (Triple-E),” DE-EE0000167, GED Integrated Solutions, Feb. 28, 2013, 45 pages.
McMaster, Ronald A et al., “Annealed and Tempered Glass,” Engineered Materials Handbook, vol. 4, Ceramics and Glasses, 1991, 9 pages.
McMaster, Ronald A., “Flat Glass Tempering—How II Works,” Glass Industry, Jun. 1989, pp. 10-15.
McMaster, Ronald A., “Fundamentals of Tempered Glass,” Proceedings of the 49th Conference on Glass Problems Ceramic Engineering and Science Proceedings, vol. 10, Issue 3/4, 1989, pp. 193-206.
Mikowski, A. et al., “Statistical analysis of threshold load for radial crack nucleation by Vickers indentation in commercial soda-lime silica glass,” Journal of Non-Crystalline Solids, vol. 352, 2006, pp. 3544-3549.
Mognato, Ennio et al., “Thermally toughened safety glass,” Glass on Web, Last Reviewed: Jul. 2011, 9 pages, http://www.glassonweb.com/articles/article/727/.
Moynihan, C. T. et al., “Structural Relaxation in Vitreous Materials,” Annals of the New York Academic of Sciences, vol. 279, Oct. 1976, pp. 15-35.
Narayanaswamy, 0. S et al., “Calculation of Residual Stresses in Glass,” Journal of the American Ceramic Society, vol. 52, No. 10, Oct. 1969, pp. 554-558.
Narayanaswamy, O. S., “Stress and Structural Relaxation in Tempering Glass,” Journal of the American Ceramic Society, vol. 61, No. 3-4, Mar.-Apr. 1978, pp. 146-152.
Oakley, David R., “Crack branching in float glass subjected to biaxial loading,” Journal of Non-Crystalline Solids, vol. 196, 1996, pp. 139-143.
Ohlberg, S.M. et al., “Thermal Stress Calculations Based on a Linear Viscoelastic Deviatoric Response and a Fictive Temperature Component for the Volumetric Response,” Journal of Non-Crystalline Solids, vol. 14, 1974, pp. 280-286.
Paschel, Richard, “History of the Safety Glazing Certification Council,” Safety Glazing Certification Council, Date Unknown, 11 pages.
Ray, N. H. et al., “Increasing the strength of glass by treatment in molten salts,” Physics and Chemistry of Glasses, vol. 8, No. 1, Feb. 1967, pp. 30-34.
Rekhson, S. M., “Chapter 1: Viscoelasticity of Glass,” In “Glass: Science and Technology,” vol. 3, 1986, 117 pages.
Rekson, S. M., “Structural Relaxation and Shear Stresses in the Glass-Transition Region,” Soviet Journal of Glass Physics and Chemistry, 1975, pp. 417-421.
Sastry, Srikanth, “The relationship between fragility, configurational entropy and the potential energy landscape of glass-forming liquids,” Nature, vol. 409, Jan. 11, 2001, pp. 164-167.
Scherer, George W., “Use of the Adam-Gibbs Equation in the Analysis of Structural Relaxation,” Journal of the American Ceramic Society, vol. 67, No. 7, Jul. 1984, pp. 504-511.
Sciortino, Francesco, “Potential energy landscape description of supercooled liquids and glasses,” Journal of Statistical Mechanics: Theory and Experiment, May 31, 2005, 35 pages.
Sehgal, Jeetendra et al., “A New Low-Brittleness Glass in the Soda-Lime-Silica Glass Family,” Journal of the American Ceramic Society, vol. 81, No. 9, Sep. 1998, pp. 2485-2488.
Setsuro, Ito et al., “Processing Technical Books to the Glass High-Functions,” Chapter 3: Sections 2.5, 3, 3.1, 3.2 & 3.3, Science & Technology Co., Ltd., Sep. 27, 2012, pp. 58-65.
Sglavo, V., A. Prezzi, M. Alessandrini, “Processing of Glasses with Engineered Stress Profiles,” Journal of Non-Crystalline Solids, 344 (2004), 73-78.
Shelby “Introduction to Glass Science and Technology”; The Royal Chemical Society, 2nd Edition, 2005; p. 193.
Shimodaira, N. et al., “Raman spectra of fluorine-doped silica glasses with various fictive temperatures,” Journal of Applied Physics, vol. 91, No. 6, Mar. 15, 2002, pp. 3522-3525.
Shinkai, Norihiko et al., “Indentation Fracture of Tempered Glasses,” Reports of the Research Laboratory, Asahi Glass Co., Ltd., vol. 23, No. 2, 1973, pp. 83-99.
Shouyuan, Zhai et al., “Influence of Temperature and Time on Glass Strength During Chemical Tempering,” [8J Journal of Shangdong Institute of Light Industry (Natural Science Edition), Feb. 1996, 3 pages.
Shutov, A. I. et al., “Prediction of the Character of Tempered Glass Fracture,” Glass and Ceramics, vol. 55, Nos. 1-2, 1998, pp. 8-10.
Soules, Thomas F. et al., “Finite-Element Calculation of Stresses in Glass Parts Undergoing Viscous Relaxation,” Journal of the American Ceramic Society, vol. 70, No. 2, Feb. 1987, pp. 90-95.
Southard, J. C., “The Thermal Properties of Crystalline and Glassy Boron Trioxide,” Journal of the American Chemical Society, vol. 63, No. 11, Nov. 1941, pp. 3147-3150.
Spaght, Monroe E. et al., “Studies on Glass. VIII. The Coefficient of Thermal Expansion of Boron Trioxide,” Journal of Physical Chemistry, vol. 38, No. 1, 1934, pp. 103-110.
Specialty Glass Products, “Soda Lime/AR/Flint Glass”; http://www.sgpinc.com/sodalime.htm accessed Aug. 11, 2016.
Stillinger, Frank H. et al., “Packing Structures and Transitions in Liquids and Solids,” Science, New Series, vol. 225, No. 4666, Sep. 7, 1984, pp. 983-989.
Stillinger, Frank H., “A Topographic View of Supercooled Liquids and Glass Formation,” Science, New Series, vol. 267, No. 5206, Mar. 31, 1995, pp. 1935-1939.
Tallant, D. R. et al., “The Effects of Tensile Stress on the Raman Spectrum of the Silica Glass,” Journal of Non-Crystalline Solids, vol. 106, 1988, pp. 380-383.
Tandon, Rajan et al., “Controlling the Fragmentation Behavior of Stressed Glass,” Fracture Mechanics of Ceramics, vol. 14, 2005, pp. 77.
Tomlinson, R., G. Calvert, and A. Conway, “A Photoelastic Investigation Into Spontaneous Glass Fracture”, Proceedings of the XIth International Congress and Exposition, (Jun. 2008) 8 pgs.
Varughese, Binoy et al., “Effect of fictive temperature on mechanical strength of soda-lime glasses,” Journal of Non-Crystalline Solids, vol. 241, 1998, pp. 134-139.
Walrafen, G. E. et al., “Raman investigation of optical fibers under high tensile stress,” Journal of Applied Physics, vol. 52, No. 4, Apr. 1981, pp. 2832-2836.
Wang et al.; “Glass and Hot Extrusion by me Module for 3D Additive Manufacturing”; IEEE, 2016; pp. 1167-1171.
Wang, Fei et al., “Pressure Raman effects and internal stress in network glasses,” Physical Review B, vol. 71, 2005, 32 pages.
Weissmann, Rand D. Durkop, “A Novel Method for Measuring Stresses in Flat Glass”, XV International Congress on Glass Leningrad 1898, Proceeding 3b, O. V. Mazurin, ed., pp. 217-220.
Yamane, Masayuki, “Chapter 3: Thermal Processing,” Glass Engineering Handbook, Asakura Publishing Co. Ltd., Jul. 1999, pp. 410-417.
Yue, Y.Z. et al., “Determination of the fictive temperature for a hyperquenched glass,” Chemical Physics Letters, vol. 357, Issues 1-2, May 3, 2002, pp. 20-24.
Zaccaria et al; “Thermal Healing of Realistic Flaws in Glass”; J. Mater. Civ. Eng 2016, 28(2) pp. 04015127-1-04015127-9.
Zaman, F. D. et al., “Cooling of a Plate with General Boundary Conditions,” International Journal of Mathematics and Mathematical Sciences, vol. 23, No. 7, 2000, pp. 477-485.
De Grauw, C. J. et al., “Axial resolution of confocal Raman microscopes: Gaussian beam theory and practice,” Journal of Microscopy, vol. 188, PI. 3, Dec. 1997, pp. 273-279.
Deschamps, T. et al., “Soda-lime silicate glass under hydrostatic pressure and indentation: a micro-Raman study,” Abstract, 2011, 1 page.
Deschamps, T. et al., “Soda-lime silicate glass under hydrostatic pressure and indentation: a micro-Raman study,” Journal of Physics: Condensed Matter, vol. 23, 2011, 7 pages.
Donald, I. W , “Review: Methods for improving the mechanical properties of oxide glasses,” Journal of Materials Science, vol. 24,1989, pp. 4177-4208.
Electronic Cooling Editors, “The Thermal Conductivity of Gases”, Design, Materials, Adhesives, Substrates, No. 3, Technical Data, Test & Measurement, vol. 4, Gases, Thermal Conductivity, Sep. 1, 1998, 2 pages.
English Translation of CN104211288A, Performed by Phoenix Translations Jun. 2016.
Ernsberger, F. M., “Chapter 1: Elastic Properties of Glasses,” In “Glass: Science and Technology,” vol. 5, Elasticity and Strength in Glasses, Academic Press, Inc., May 28, 1980, pp. 1-19.
Ernsberger, F. M., “Chapter 4: Techniques of Strengthening Glasses,” In “Glass: Science and Technology,” vol. 5, Elasticity and Strength in Glasses, Academic Press, Inc., May 28, 1980, pp. 133-144.
European Patent Application No. 15757030 Office Action dated Jun. 23, 2021; 5 Pages; European Patent Office.
European Patent Application No. 15757030.0 Office Action dated Mar. 2, 2018; 5 Pages; European Patent Office.
European Patent Application No. 16750337.4 Office Action dated Jan. 24, 2020; 4 Pages; European Patent Office.
EUROPTEC; “Themal Tempering”; EUROPTEC GMBH, DIC, Jun. 11, 2014; www.europtec.de.
Everall, Neil et al., “Optimizing Depth Resolution in Confocal Raman Microscopy: A Comparison of Metallurgical, Dry Corrected, and Oil Immersion Objectives,” Applied Sprectroscopy, vol. 61, No. 3, 2007, pp. 251-259.
Everall, Neil J., “Confocal Raman Microscopy: Why the Depth Resolution and Spatial Accuracy Can Be Much Worse then You Think,” Applied Spectroscopy, vol. 54, No. 10, 2000, pp. 1515-1520.
Fajans, Kasimir et al., “Properties and Structures of Vitreous and Crystalline Boron Oxide,” Journal of the American Chemical Society, vol. 74, No. 11, Jun. 5, 1952, pp. 2761-2768.
Fotheringham, Dr. Ulrich, “Lecture 1: Internet teaching set-up,” IMI-NFG's MITT Course on Relaxation Processes in Glass and Polymers Lecture 1, 2010, 6 slides.
Fotheringham, Dr. Ulrich, “Lecture 2: Phenomenology of viscoelasticity & glass transition,” IMI-NFG's MITT Course on Relaxation Processes in Glass and Polymers Lecture 2, 2010, 17 slides.
Fotheringham, Dr. Ulrich, “Lecture 5: Viscoelasticity I—Shear,” IMI-NFG's MITT Course on Relaxation Processes in Glass and Polymers Lecture 5, 2010, 19 slides.
Fotheringham, Dr. Ulrich, “Lecture 6: Viscoelasticity II—Bulk Viscoelasticity,” IMI-NFG's MITT Course on Relaxation Processes in Glass and Polymers Lecture 6, 2010, 16 slides.
Fotheringham, Dr. Ulrich, “Lecture 7: Viscoelasticity III—Dynamic Testing,” IMI-NFG's MITT Course on Relaxation Processes in Glass and Polymers Lecture 7, 2010, 19 slides.
Fotheringham, Dr. Ulrich, “Lecture 8: Viscoelasticity IV—Important Application of Pre-Stressing,” IMI-NFG's MITT Course on Relaxation Processes in Glass and Polymers Lecture 8, 2010, 12 slides.
Freiman, S. W., “Chapter 2: Fracture Mechanics of Glass,” In “Glass: Science and Technology,” vol. 5, Elasticity and Strength in Glasses, Academic Press, Inc., May 28, 1980, pp. 21-78.
Frick, B. et al., “The Microscopic Basis of the Glass Transition in Polymers from Neutron Scattering Studies,” Science, vol. 267, Mar. 31, 1995, pp. 1939-1945.
Galeener, Frank L., “Raman and ESR Studies of the Thermal History of Amorphous SiO.sub.2,” Journal of Non-Crystalline Solids, vol. 71, 1985, pp. 373-386.
Gang, Zhang Ming, “Manufacturing and Properties of Glass Used in Construction,” Guangdong Golden Glass Technologies Ltd, Dec. 27, 2002, 11 pages.
Gardon, Robert, “Calculation of Temperature Distributions in Glass Plates Undergoing Heat-Treatment,” Journal of the American Ceramic Society, vol. 41, No. 6, Jun. 1958, pp. 200-209.
Gardon, Robert, “Chapter 5: Thermal Tempering of Glass,” In “Glass: Science and Technology,” vol. 5, Elasticity and Strength in Glasses, Academic Press, Inc., May 28, 1980, pp. 145-216.
Gardon, Robert, “Tempering Glass with Modulated Cooling Schedules,” Journal of the American Ceramic Society, vol. 71, No. 10, Oct. 1988, pp. 876-878.
Gardon, Robert, “Variation of Densities and Refractive Indices in Tempered Glass,” Journal of the American Ceramic Society, vol. 61, No. 3-4, Mar.-Apr. 1978, pp. 143-146.
Glass, Jill et al., “Processing and Properties of Ion Exchanged Glasses,” Glass and Optical Materials Division Fall Meeting, Nov. 6-12, 2004, Cape Canaveral, FL, 33 slides.
Glass, S. J. et al., “Stressed Glass Technology for Actuators and Removable Barrier Applications,” Sandia Report SAND2007-4106, Sandia National Laboratories, Jul. 2007, 18 pages.
Gomez, Sinue et al., “69.2: Designing Strong Glass for Mobile Devices,” SID Symposium Digest of Technical Papers, vol. 40, No. 1, Jan. 2009, pp. 1045-1048.
Gross, T.M., “Deformation and cracking behavior of glasses indented with diamond tips of various sharpness,” Journal of Non-Crystalline Solids, vol. 358, Issue 24, Dec. 12, 2012, pp. 3445-3452.
Guillemet, C., “Annealing and Tempering of Glass,” Journal of Non-Crystalline Solids, vol. 123, 1990, pp. 415-426.
Gulati, Suresh T., “Frangibility of Tempered Soda-Lime Glass Sheet,” Glass Processing Days, 13-15, Sep. 1997, pp. 72-76.
Gupta, Prabhat K. et al., “The laboratory glass transition,” The Journal of Chemical Physics, vol. 126, 2007, 9 pages.
Gupta, Prabhat, “Landscape Approach to Glass Transition and Relaxation: Basic Concepts (contd.),” IMI-NFG's MITT Course on Relaxation Processes in Glass Lecture 18, Mar. 25, 2010, 23 slides.
Gupta, Prabhat, “Landscape Approach to Glass Transition and Relaxation: Four lectures on ‘The Landscape Approach,’” IMI-NFG's MITT Course on Relaxation Processes in Glass Lecture 17, Mar. 23, 2010, 28 slides.
Gupta, Prabhat, “Landscape Approach to Glass Transition and Relaxation: Liquid to Glass Transition,” IMI-NFG's MITT Course on Relaxation Processes in Glass Lecture 19, Mar. 30, 2010, 25 slides.
Gupta, Prabhat, “Landscape Approach to Glass Transition and Relaxation: Relaxation in the glassy state,” IMI-NFG's Min Course on Relaxation Processes in Glass Lecture 20, Apr. 1, 2010, 20 slides.
Gy, Rene, “Ion exchange for glass strengthening,” Materials Science and Engineering B, vol. 149, 2008, pp. 159-165.
Hara, Morihisa et al., “Vickers Hardness of Toughened Sheet Glass,” Reports of the Research Laboratory, Asahi Glass Co., Ltd., vol. 12, No. 2, 1962, pp. 99-104.
Hibino, Yoshinori et al., “Raman study on silica optical fibers subjected to high tensile stress,” Applied Physics Letters, vol. 47, No. 8, Oct. 15, 1985, pp. 812-814.
Hodge, Ian M., “Physical Aging in Polymer Glasses,” Science, vol. 267, , No. 5206, Mar. 31, 1995, pp. 1945-1947.
Hrma et al.; “Thermal Healing of Cracks in Glass”; Journal of Non-Crystalline Solids; vol. 102, (1988); pp. 88-94.
Huang, Liping et al., “Polyamorphic transitions in vitreous B2O3 under pressure,” Journal of Physics: Condensed Matter, vol. 20, 2008, 8 pages.
Hubert, Mathieu, “Lecture 9: Annealing and tempering,” IMI-NFG Course on Processing in Glass—Lecture 9, Feb. 19, 2015, 72 slides.
Hutchins, J. and R. Harrington, “Glass”, Kirk-Othmer Encyclopedia of Chemical Technology, 2nd Edition, 10 pp. 533-604.
International Preliminary Report on Patentability of the International Searching Authority; PCT/US15/42955; dated Feb. 9, 2017; 9 Pages; European Patent Office.
International Preliminary Report on Patentability of the International Searching Authority; PCT/US16/45022; dated Feb. 8, 2018; 15 Pages; European Patent Office.
Related Publications (1)
Number Date Country
20210122665 A1 Apr 2021 US
Provisional Applications (1)
Number Date Country
62549507 Aug 2017 US