Glasses

Information

  • Patent Grant
  • 10683231
  • Patent Number
    10,683,231
  • Date Filed
    Wednesday, March 23, 2016
    9 years ago
  • Date Issued
    Tuesday, June 16, 2020
    4 years ago
Abstract
Glasses are disclosed having a composition comprising the following oxides (in weight %): SiO2 61 to 70%, Al2O3 0 to 9%, Na2O 10 to 13%, K2O 0 to 1%, MgO 2 to 6%, CaO 6 to 16%, SrO 0 to 1%, ZrO2 0 to 1%, TiO2 2 to 15%, the glasses having a strain point greater than 570° C. The glasses have good dimensional stability at high temperatures, making them suitable for fire protection glazings and substrates which are processed at elevated temperatures, e.g. substrates for display panels, information storage discs and semiconductor devices, including photovoltaic cells. Physical properties of the glasses, such as thermal expansion coefficient, density and refractive index, are disclosed, as are the melting and liquidus temperatures. The glasses are suitable for manufacture by the float process, yielding flat glass in the form of sheets.
Description
BACKGROUND OF THE INVENTION

The present invention relates to glass, more specifically to novel glasses, novel glass compositions and to substrates composed of the novel glass compositions. The novel glass compositions are soda lime silica glasses, but possess relatively high strain points compared with known soda lime silica glasses, in particular those soda lime silica glasses which are in common use to produce flat glass by the float process. Consequently, the novel glasses of the invention are suited to applications requiring good dimensional stability at high temperatures, such as fire protection glazings and substrates for processing at high temperature. The substrates are suitable for the deposition of coatings and the manufacture of display panels, discs, e.g. magnetic recording discs, semiconductor devices, including photovoltaic cells, especially solar cells, amongst other applications.


While normal soda lime silica glass (i.e. soda lime silica glass compositions in common use for windows and other glazings for buildings and vehicles) has suitable properties at room temperature for many of the above applications, the applications may require processing of the glass at high temperatures, i.e. at temperatures which are above the strain point, or the annealing point, or even the softening point of the glass. Processing the glass at such elevated temperatures would result in the creation of permanent internal stresses in the glass, possibly leading to distortion or fracture of the glass. The glass may even become distorted or deformed during processing. Attempts have therefore been made to provide glasses which are more suited to high temperature processing, i.e. which possess improved high temperature stability by virtue of having relatively high strain points.


The strain point (which is defined as the temperature at which the viscosity of the glass is 1014.5 poise, denoted T log 14.5 poise) of soda lime float glass in common use is in the region of about 510° C. to 540° C., depending on the precise composition. However, many glasses with higher strain points are known. One group of glasses with high strain points is the so-called alkali-free glasses. Unfortunately, these glasses are difficult and expensive to produce, owing to the lack of alkali which acts as a flux. Many of these glasses are also unsuitable for forming by the float process. The use of alternative forming processes generally adds further to the cost, and may result in inferior flatness or smoothness of the surface. A further problem with alkali-free glasses is that they tend to have very low coefficients of thermal expansion, which renders them unsuitable for some applications.


Another group of glasses with relatively high strain points contains increased potash and reduced soda, compared with common or “normal” soda lime silica float glass.


TiO2


Unfortunately, high potash glasses are themselves difficult to produce in the open regenerative furnaces generally employed in float plants, because high potash glasses may be difficult to refine in such furnaces.


A number of attempts have been made to provide a soda lime silica glass composition having a higher strain point than common float glass. U.S. Pat. No. 5,599,754 discloses a glass composition for a substrate, which is useful for flat display panels, particularly for plasma display panels. The claimed compositions contain from 6 to 9% SrO, which is expensive, and adds significantly to the cost of raw materials when used at these relatively high levels.


U.S. Pat. No. 6,905,991 is an example of a soda lime silica glass composition containing relatively low levels of soda (from 2 to 8% Na2O) and relatively high levels of potash (from 0-8%, but all of the Examples contain at least 3.5% K2O). The resulting glasses may be used for producing fireproof glazing panels or for substrates for display panels.


WO 98/49111 discloses a glass composition for a plasma display panel, the glass having a lower density than previous glasses for plasma display panels. The total amount of BaO and SrO included in the total alkaline earth metal oxides in the glass lies in the range of 1 to 8%. Again, these oxides are expensive.


U.S. Pat. No. 6,087,284 relates to an aluminosilicate glass which is suitable for use in display technology. This patent seeks to find a glass which has a high transition temperature, low density and is solarisation-stable. Preferably the glass contains MgO in trace levels at most, or not at all. It therefore represents a substantial departure from the composition of normal or common float glass.


U.S. Pat. No. 7,273,668 relates to a glass composition having high heat resistance which is suitable for chemical strengthening. The composition may be used to produce glass substrates for magnetic recording media, e.g. hard disk drives. Unfortunately this glass is prone to devitrification, which can make manufacturing difficult, and reduce yields.


KR 2009 0111680 A discloses a glass composition for display panels, which seeks to improve reactivity and failure rate of electrode patterns.


JP 2010 143790 A discloses a method for producing a glass substrate for a solar cell in which waste glass can be efficiently recycled. The waste glass is used as part of the glass raw material, which is then melted in a glass melting furnace and formed into the glass substrate.


U.S. Pat. No. 8,828,897 relates to aluminosilicate glasses having high thermal stability and low processing temperatures. The glasses may be used as substrate glass, superstrate glass and/or cover glass for photovoltaic applications and other solar technology applications.


U.S. Pat. No. 8,895,463 relates to a glass substrate for a solar cell such as a Cu—In—Ga—Se (“CIGS) solar cell. The glass compositions of the invention deviate significantly from common soda lime silica glass, being low in soda and high in potash.


US 2013/0306145 A1 also relates to a glass substrate for a CIGS solar cell, and again, the glass compositions are low in soda and high in potash.


US 2013/0313671 A1 relates to glass substrates for solar cells, such as CdTe or CIGS cells. It is stated that the content of SrO, BaO, B2O3 and/or ZrO2 is advantageously zero in order not to penalize the cost of the glass sheet. However, judging by the Examples provided, this approach yields only modest increases in strain point compared with common soda lime silica glass.


SUMMARY OF THE INVENTION

It would be desirable to provide novel glasses which achieve a substantial increase in strain point without a substantial increase in the cost of the glass. The cost of glass comprises the cost of the raw materials together with the cost of converting them into finished glass sheets, which itself comprises elements such as the cost of fuel, labour, the plant employed, its level of efficiency, the yields obtained, etc. It would therefore further be desirable to provide novel glass compositions which achieve a substantial increase in strain point and are also able to be readily manufactured by the float process, since this process is a very efficient way of making flat glass. The desired novel glass compositions are therefore ones which lend themselves to economic manufacture.


It has surprisingly been found that the addition of TiO2 to a normal float glass composition yields a substantial increase in the strain point of the glass.


According to the present invention there is provided a glass having a composition comprising the following oxides (in weight %):

















SiO2
61 to 70%



Al2O3
0 to 9%



Na2O
10 to 13%



K2O
0 to 1%



MgO
2 to 6%



CaO
 6 to 16%



SrO
0 to 1%



ZrO2
0 to 1%



TiO2
 2 to 15%










the glass having a strain point greater than 570° C.







DETAILED DESCRIPTION OF THE INVENTION

It has also been found that increasing the amount of Al2O3 in the glass composition, in addition to increasing the amount of TiO2, further increases the strain point of the glass.


Glasses according to the invention are suitable for processing at higher temperatures than normal float glass. The inventive glasses are less susceptible to deformation or distortion at elevated temperatures, and so have higher dimensional stability and improved heat resistance.


Preferably, the glass comprises certain oxides in the following ranges (in weight %):

















SiO2
61 to 69%



Al2O3
0 to 8%



CaO
 7 to 13%



TiO2

2 to 13%.










Advantageously, the glass comprises from 3 to 12% TiO2, preferably from 3 to 11% TiO2, more preferably from 4 to 10% TiO2, still more preferably from 4 to 9% TiO2, yet more preferably from 4 to 8% TiO2, most preferably from 4 to 7% TiO2. Particularly suitable glass compositions may contain from 4 to 6% TiO2. Optionally, such glass compositions may also contain from 3 to 8% Al2O3, preferably from 4 to 7% Al2O3, more preferably from 5 to 6% Al2O3. Since titania (TiO2) is more expensive than other raw materials employed in the manufacture of float glass, this allows glasses according to the invention to be tailored to achieve the desired balance between performance and cost.


Optionally, the glass is free of any one, or any number, of the following oxides: As2O3, BaO, B2O3, BeO, CeO2, Er2O3, GeO2, Li2O, P2O5, PbO, Sb2O3, SnO2, SrO, V2O5, ZnO, ZrO2. These oxides may be objectionable for reasons of toxicity, cost or their adverse effect on the furnace structure. However, traces of these oxides may be present as a result of impurities in the raw materials. In particular, the glass composition may contain from 0 to 1% BaO or B2O3. In many of the applications contemplated, it is not necessary or not desirable to tint the glass, so in such cases the glass is free of colourants, e.g. CdO, CeO2, CoO, Co3O4, Cr2O3, CuO, Er2O3, MnO2, Nd2O3, NiO, Se, V2O5.


Preferably, a glass according to the invention has a strain point greater than 580° C., preferably greater than 585° C., more preferably greater than 590° C. As mentioned above, it is desirable to provide glasses which are readily manufactured by the float process. Therefore, while increasing the strain point of a glass, it is also important to take account of other properties of the glass, such as melting temperature, liquidus temperature and working range, which determine how readily the glass may be melted and formed. Surprisingly, the inventors were able to tailor all these properties simultaneously, to provide glasses with high strain points and favourable manufacturing properties.


Preferably, a glass according to the invention has a melting temperature (defined as the temperature at which the viscosity is 100 poise, i.e. log 2 poise, denoted T log 2 poise) less than 1500° C., preferably less than 1480° C., more preferably less than 1460° C. This allows the raw materials to be melted and turned into glass without excessive fuel usage and without causing undue wear to the structure of the furnace in which the glass is melted.


Advantageously, a glass according to the invention has a liquidus temperature less than 1200° C., preferably less than 1180° C., more preferably less than 1160° C., yet more preferably less than 1140° C., still more preferably less than 1120° C., most preferably less than 1100° C. A lower liquidus temperature reduces the risk of devitrification in molten glass in the cooler regions of the furnace. The term “devitrification” refers to the formation of crystals such as wollastonite (abbreviated to “Woll.” in Table I below) or diopside in the glass, which is undesirable because such crystals may end up in the final product, causing it to be rejected.


Desirably, a glass according to the invention has a working range (defined as the forming temperature, i.e. T log 4 poise, minus the liquidus temperature) greater than −100° C., preferably greater than −80° C., more preferably greater than −60° C., yet more preferably greater than −40° C., still more preferably greater than −20° C., most preferably greater than 0° C., i.e. preferably the working range is positive. Some glass forming processes are more tolerant of a negative working range than others, and the float glass process is able to operate with a negative working range. A less negative, or more positive, working range facilitates forming of the molten glass into a product (e.g. a ribbon of flat glass) without devitrification occurring.


It is advantageous for the physical properties of the final product (e.g. sheet of glass, glass substrate, display panel, disc, etc) to be suited to the particular application for which the glass is intended. For some of these applications, normal soda lime silica glass possesses suitable physical properties at room temperature, but, as mentioned previously, it cannot be processed at sufficiently high temperatures without negative effects. According to an additional aspect of the invention, glasses are provided which not only have increased strain points, and lend themselves to economic manufacture, but also retain suitable physical properties at room temperature.


For instance, according to this aspect of the invention, a glass is provided having a coefficient of thermal expansion from 70 to 90×10−7° C.−1 (50-350° C.), preferably from 72 to 88×10−7° C.−1 (50-350° C.), more preferably from 74 to 86×10−7° C.−1 (50-350° C.), and most preferably from 76 to 84×10−7° C.−1 (50-350° C.).


Moreover, properties such as density and refractive index are also important when the glass produced by a furnace is changed over from one composition to another. A changeover of particular significance is the changeover from normal float glass to a glass according to the invention. Such changeovers are carried out “on the run”, i.e. the mixture of raw materials fed to the furnace is changed to the mixture which is appropriate for the new composition without draining the furnace or stopping melting. The time taken for the changeover can be reduced if both glass compositions have similar density and refractive index, since mixing of the two compositions then occurs more readily.


It is therefore also desirable to provide a glass having a density from 2.50 to 2.70 g cm−3 at 25° C., preferably from 2.51 to 2.69 g cm−3 at 25° C., more preferably from 2.52 to 2.68 g cm−3 at 25° C., further preferably from 2.53 to 2.67 g cm−3 at 25° C., yet more preferably from 2.54 to 2.66 g cm−3 at 25° C., most preferably from 2.55 to 2.66 g cm−3 at 25° C.


Similarly, it is desirable if a glass according to the invention has a refractive index from 1.50 to 1.62, preferably from 1.51 to 1.60, more preferably from 1.52 to 1.59, more preferably from 1.53 to 1.58.


The invention also encompasses glass articles having a glass composition according to the appended claims, and in particular a sheet of glass formed from glass having a glass composition as claimed herein. Additionally, the invention includes a fire resistant glazing made with one or more sheets of such glass. Furthermore, the invention also includes a glass substrate comprising glass as claimed herein, and any of the products manufactured using such a glass substrate, including but not limited to a display panel, a disc, a semiconductor device and a photovoltaic cell, especially a solar cell. Glass substrates according to the invention may be used for CdTe and CIGS (Cu—In—Ga—Se) solar cells amongst others.


The invention will now be further described with reference to the following non-limiting Examples set out in Table 1. In the table, Examples 3 to 7 are according to the invention, and Examples 1, 2 and 8 to 20 are comparative examples. In particular, Example 1 is representative of normal float glass, and has a strain point of 536° C. In contrast, Examples 2 to 20 have strain points ranging from 574° C. to 595° C., and the Examples according to the invention span the same range of strain points.


It may be seen that Example 7 has the highest strain point, namely 595° C. This Example also has a very low melting temperature, namely 1290° C. In fact, this Example generally has relatively low viscosity at high temperature, including a forming temperature of only 972° C. Since the liquidus temperature of this glass is relatively high at 1171° C., this leads to a large negative working range of −199° C. Examples 5 and 6 concede only one or two degrees in terms of their strain points, and have working ranges of −91° C. and −108° C. respectively, which makes them better propositions from the manufacturing aspect.


Glasses having a glass composition according to the invention therefore offer a considerably increased strain point while retaining suitable manufacturing and room temperature properties, rendering it suitable for high temperature processing and other applications requiring increased dimensional stability at elevated temperatures.
















TABLE 1







Example Number
1
2
3
4
5
6
7





Composition (wt %)









SiO2
72.8
69.7
64.2
61.5
66.6
65.4
62


Na2O
13.4
10
11.8
11.7
10.1
10.1
10.1


CaO
8.71
15.3
12.06
12.0
9.2
10.2
12.1


MgO
4.26
4.24
4.29
4.15
4.13
4.22
4.35


Al2O3
0.4
0.4
0.11
7.06
5.03
4.12
0.08


ZrO2









TiO2


7.2
3.1
4.6
5.5
10.8


SrO









BaO









SO3
0.31
0.34
0.31
0.34
0.24
0.28
0.34


Fe2O3 (Trace components)
0.015
0.015
0.013
0.107
0.102
0.105
0.103


K2O
0.01
0.01
0.01
0.01
0.01
0.01
0.01


Forming Characteristics









Liquidus Temperature (° C.)
1066
1201
1116
1157
1158
1154
1171


Working Range (liquidus minus T log 4)
−39
−179
−143
−135
−91
−108
−199


Primary Devitrification Phase
Woll.
Woll.
Woll.
Woll.
Woll.
Woll.
Woll.


Physical Properties









Coeff. of Thermal Expansion
87.1
84.9
89.0
86.4
76.2
77.9
83.1


(50°-350° C.)









Young's modulus E (GNm-2)
74.8
79.9
84.1
80.8
79.2
80.8
84.5


Shear Modulus G (GNm-2)
30.5
32.5
33.8
32.9
32.5
33.3
34.3


Poisson's Ratio σ
0.23
0.23
0.25
0.23
0.22
0.21
0.23


Density (g/cm3 @ 25° C.)
2.495
2.563
2.619
2.594
2.551
2.572
2.661


Refractive Index (Nad)
1.5182
1.5388
1.5688
1.5492
1.5441
1.5517
1.589


Viscosity Profile (° C.)









T log 2 poise (Melting Temperature)
1448
1389
1309
1389
1476
1431
1290


T log 2.5 poise
1304
1265
1195
1264
1336
1300
1182


T log 3 poise
1191
1167
1105
1165
1227
1197
1097


T log 4 poise (Forming Temperature)
1027
1021
973
1021
1067
1046
972


T log 5 poise
912
919
881
921
957
941
885


T log 7.6 poise (Softening Point)
732
755
734
762
782
775
747


T log 13 poise (Annealing Point)
563
600
596
613
619
619
616


T log 13.4 poise
555
592
589
606
611
612
610


T log 14.5 poise (Strain Point)
536
575
574
589
593
594
595





Example Number
8
9
10
11
12
13
14





Composition (wt %)









SiO2
68.0
68.7
69.1
66.2
64.8
67.7
67.0


Na2O
11.7
12
12.3
10.9
11.8
11.9
11.5


CaO
9.86
8.52
7.24
6.23
11.9
6.51
11.5


MgO
4.43
4.52
4.62
4.21
4.24
4.42
4.40


Al2O3
3.47
1.88
0.28
0.08
0.03
0.08
5.20


ZrO2
2.14
4.06
6.1
6.8
6.8
8.8



TiO2









SrO



5.0





BaO









SO3
0.22
0.21
0.185
0.29
0.31
0.24
0.26


Fe2O3 (Trace components)
0.075
0.075
0.077
0.058
0.015
0.104
0.075


K2O
0.01
0.01
0.01
0.02
0.01
0.02
0.02


Forming Characteristics









Liquidus Temperature (° C.)
1148
1129
1079
1030
1149
1075
1164


Working Range (liquidus minus T log 4)
−84
−46
14
57
−105
44
−110


Primary Devitrification Phase

Diopside
Diopside
Woll.
Woll.
Woll.



Physical Properties









Coeff. of Thermal Expansion (50°-350° C.)
81.8
80.9
79.9
78.7
84.2
76.8
84.7


Young's modulus E (GNm-2)
78.3
79.3
78.1
80.4
82.8
80
78


Shear Modulus G (GNm-2)
32.1
32.4
32.2
33.3
33.6
33.7
32.1


Poisson's Ratio σ
0.22
0.22
0.21
0.21
0.23
0.19
0.22


Density (g/cm3 @ 25° C.)
2.554
2.568
2.581
2.668
2.664
2.620
2.541


Refractive Index (Nad)
1.5322
1.5347
1.5361
1.5452
1.5544
1.5436
1.5298


Viscosity Profile (° C.)









T log 2 poise (Melting Temperature)
1456
1472
1478
1453
1380
1482
1452


T log 2.5 poise
1324
1343
1352
1334
1269
1365
1317


T log 3 poise
1219
1239
1249
1237
1180
1268
1211


T log 4 poise (Forming Temperature)
1064
1082
1093
1087
1043
1118
1054


T log 5 poise
953
970
980
977
944
1007
944


T log 7.6 poise (Softening Point)
775
786
793
794
781
818
769


T log 13 poise (Annealing Point)
605
607
608
609
619
626
602


T log 13.4 poise
597
598
599
600
611
617
594


T log 14.5 poise (Strain Point)
577
577
577
579
592
594
575
















Example Number
15
16
17
18
19
20





Composition (wt %)








SiO2
65.8
67.7
63.9
64.0
64.8
63.3


Na2O
11.6
11.6
11.3
11.3
10.8
11.5


CaO
11.61
11.88
12.1
10.9
12.6
7.5


MgO
4.21
2.05
4.14
5.27
4.3
4.86


Al2O3
6.35
6.41
8.03
8.00
7.06
8.0


ZrO2








TiO2








SrO





4.3


BaO








SO3
0.27
0.22
0.33
0.33
0.28
0.27


Fe2O3 (Trace components)
0.014
0.012
0.105
0.105
0.107
0.107


K2O
0.06
0.06
0.01
0.01
0.01
0.02


Forming Characteristics








Liquidus Temperature (° C.)
1168
1174
1178
1209
1173
1140


Working Range (liquidus minus T log 4)
−118
−107
−116
−140
−109
−69


Primary Devitrification Phase
Woll.
Woll.
Diopside
Diopside
Diopside



Physical Properties








Coeff. of Thermal Expansion (50°-350° C.)
85.2
84.8
84.1
83.4
82.9
83.9


Young's modulus E (GNm-2)
79.8
77.2
78.9
79.1
79.7
78.7


Shear Modulus G (GNm-2)
32.8
31.5
32.8
32.4
32.6
32


Poisson's Ratio σ
0.22
0.22
0.20
0.22
0.23
0.23


Density (g/cm3 @ 25° C.)
2.5478
2.5225
2.556
2.550
2.556
2.582


Refractive Index (Nad)
1.5311
1.5268
1.5321
1.5317
1.5325
1.5294


Viscosity Profile (° C.)








T log 2 poise (Melting Temperature)
1444
1495
1451
1462
1452
1472


T log 2.5 poise
1310
1347
1320
1329
1321
1337


T log 3 poise
1204
1233
1216
1224
1217
1230


T log 4 poise (Forming Temperature)
1049
1066
1062
1068
1064
1071


T log 5 poise
940
952
953
959
955
958


T log 7.6 poise (Softening Point)
768
772
780
783
782
776


T log 13 poise (Annealing Point)
604
605
615
616
617
602


T log 13.4 poise
597
598
607
608
609
594


T log 14.5 poise (Strain Point)
578
579
588
589
590
574








Claims
  • 1. A soda lime silica glass having a strain point greater than 570° C., comprising the following oxides (in weight %):
  • 2. The glass as claimed in claim 1, comprising from 3 to 11% TiO2.
  • 3. The glass as claimed in claim 1, comprising from 4 to 10% TiO2.
  • 4. The glass as claimed in claim 1, comprising from 4 to 6% TiO2.
  • 5. The glass as claimed in claim 1 having a strain point greater than 580° C.
  • 6. The glass as claimed in claim 1 having a melting temperature (at which viscosity=log 2 poise) less than 1500° C.
  • 7. The glass as claimed in claim 1 having a liquidus temperature less than 1200° C.
  • 8. The glass as claimed in claim 1 having a working range (defined as T log 4 poise minus the liquidus temperature) greater than −100° C.
  • 9. The glass as claimed in claim 1 having a coefficient of thermal expansion from 70 to 90×10−7° C.−1 (50-350° C.).
  • 10. The glass as claimed in claim 1 having a density from 2.50 to 2.70 g cm−3 at 25° C.
  • 11. The glass as claimed in claim 1 having a refractive index from 1.50 to 1.62.
  • 12. A sheet of glass formed from glass as claimed in claim 1.
  • 13. A glass substrate comprising glass as claimed in claim 1.
  • 14. A photovoltaic cell comprising the glass substrate of claim 13.
  • 15. A flat glass produced by an on-line float glass process, having a strain point greater than 570° C., comprising the following oxides (in weight %):
  • 16. A glass substrate for a photovoltaic cell comprising the flat glass as claimed in claim 15.
  • 17. A flat glass substrate having a strain point greater than 570° C., comprising the following oxides (in weight %):
  • 18. A photovoltaic cell comprising the flat glass substrate of claim 17.
Priority Claims (1)
Number Date Country Kind
1505091.7 Mar 2015 GB national
PCT Information
Filing Document Filing Date Country Kind
PCT/GB2016/050812 3/23/2016 WO 00
Publishing Document Publishing Date Country Kind
WO2016/151322 9/29/2016 WO A
US Referenced Citations (85)
Number Name Date Kind
3753674 Ohlberg Aug 1973 A
4792536 Pecoraro Dec 1988 A
5071796 Jones Dec 1991 A
5489558 Moffatt Feb 1996 A
5599754 Maeda Feb 1997 A
5776844 Koch Jul 1998 A
5780371 Rifqi Jul 1998 A
5830814 Combes Nov 1998 A
5925583 Yoshii Jul 1999 A
5958812 Koch Sep 1999 A
5990023 Siedel Nov 1999 A
6087284 Brix Jul 2000 A
6150028 Mazon Nov 2000 A
6162750 Miwa Dec 2000 A
6313052 Nakashima Nov 2001 B1
6335300 Bordeaux Jan 2002 B1
6797658 Pecoraro Sep 2004 B2
6878652 Pecoraro Apr 2005 B2
6905991 El Khiati Jun 2005 B1
7153798 Bordeaux Dec 2006 B2
7273668 Kurachi Sep 2007 B2
7557053 Thomsen Jul 2009 B2
7772144 Landa Aug 2010 B2
7893350 Thomsen Feb 2011 B2
8377834 Nagai Feb 2013 B2
8455375 Nishizawa et al. Jun 2013 B2
8828897 Fechner Sep 2014 B2
8895463 Kuroiwa Nov 2014 B2
8921245 Nishizawa Dec 2014 B2
20020042068 Mizuno Apr 2002 A1
20020065187 Bordeaux May 2002 A1
20020074930 Futagami Jun 2002 A1
20020147102 Yamazaki Oct 2002 A1
20020169062 Pecoraro Nov 2002 A1
20020193232 Itoh Dec 2002 A1
20030054938 Pecoraro Mar 2003 A1
20030220183 Kurachi Nov 2003 A1
20030230112 Ikeda Dec 2003 A1
20040142811 Torr Jul 2004 A1
20050003136 Kurachi Jan 2005 A1
20050028559 Hiromatsu Feb 2005 A1
20050037912 Ek Khiati Feb 2005 A1
20060068209 Hirose Mar 2006 A1
20060073081 Nomoto Apr 2006 A1
20060169316 Thomsen Aug 2006 A1
20060182980 Barton Aug 2006 A1
20060194687 Seto Aug 2006 A1
20060216552 Ikenishi Sep 2006 A1
20060217257 Nagashima Sep 2006 A1
20070015653 Lautenschlaeger Jan 2007 A1
20070032368 Landa Feb 2007 A1
20070037686 Goulas Feb 2007 A1
20070209698 Thomsen Sep 2007 A1
20070215205 Thomsen Sep 2007 A1
20080053152 Kurachi Mar 2008 A1
20080096754 Thomsen Apr 2008 A1
20080113857 Lee May 2008 A1
20090103040 Shimizu Apr 2009 A1
20090217978 Thomsen Sep 2009 A1
20090253567 Nagai Oct 2009 A1
20090297806 Dawson-Elis Dec 2009 A1
20100040812 Buckett Feb 2010 A1
20100089606 Kwon Apr 2010 A1
20100300535 Aitken Dec 2010 A1
20100304949 Sachot Dec 2010 A1
20110135938 Kim Jun 2011 A1
20120052275 Hashimoto Mar 2012 A1
20120053044 Lee Mar 2012 A1
20120132269 Hickman May 2012 A1
20120141804 Miyabe Jun 2012 A1
20120199203 Nishizawa Aug 2012 A1
20120207995 Shelestak Aug 2012 A1
20130160845 Kuroiwa Jun 2013 A1
20130164521 Myoung Jun 2013 A1
20130178355 Nagai Jul 2013 A1
20130233386 Hanawa Sep 2013 A1
20130306145 Hanawa Nov 2013 A1
20130313671 Cintora Nov 2013 A1
20140087935 Muguruma Mar 2014 A1
20140209169 Hanawa Jul 2014 A1
20140235425 Nishizawa Aug 2014 A1
20140323286 Gardiner Oct 2014 A1
20180099895 Horsley Apr 2018 A1
20180099896 Horsley Apr 2018 A1
20180099897 Horsley Apr 2018 A1
Foreign Referenced Citations (59)
Number Date Country
1712375 Dec 2005 CN
1792919 Jun 2006 CN
100366560 Jun 2006 CN
101239779 Aug 2008 CN
101462825 Jun 2009 CN
102718404 Oct 2012 CN
102 718 404 Dec 2014 CN
734356 Oct 1996 EP
769481 Apr 1997 EP
2371775 May 2011 EP
2492247 Aug 2012 EP
2774895 Sep 2014 EP
61136936 Jun 1986 JP
S61 136936 Jun 1986 JP
63147843 Jun 1988 JP
S63 147843 Jun 1988 JP
H05221683 May 1993 JP
H08133771 May 1996 JP
3040933 Jun 1997 JP
10025129 Jan 1998 JP
10025130 Jan 1998 JP
H10025128 Jan 1998 JP
H11111342 Jan 1999 JP
11322358 Nov 1999 JP
2000143280 May 2000 JP
2000169177 Jun 2000 JP
2000169179 Jun 2000 JP
2000169180 Jun 2000 JP
2001026437 Jan 2001 JP
2002053340 Feb 2002 JP
2005330181 Feb 2005 JP
4158249 Jul 2008 JP
2008280189 Nov 2008 JP
2010-143790 Jul 2010 JP
20100143790 Jul 2010 JP
153457 Jul 1998 KR
2009111680 Oct 2009 KR
20090111680 Oct 2009 KR
2010080436 Jul 2010 KR
96-11888 Apr 1996 WO
9801400 Jan 1998 WO
9849111 Nov 1998 WO
WO-9849111 Nov 1998 WO
9901391 Jan 1999 WO
9926269 May 1999 WO
0216277 Feb 2002 WO
2008096876 Aug 2008 WO
2010023419 Mar 2010 WO
2011035889 Mar 2011 WO
2011069338 Jun 2011 WO
2013111749 Jan 2013 WO
2014024850 May 2013 WO
2013099970 Jul 2013 WO
2013108790 Jul 2013 WO
2014038409 Jul 2013 WO
2013118897 Aug 2013 WO
2013133273 Dec 2013 WO
2014203481 Dec 2014 WO
9805760 Jul 1998 ZA
Non-Patent Literature Citations (1)
Entry
Definition of Flake, American Heritage® Dictionary of the English Language, Fifth Edition. Copyright © 2016 by Houghton Mifflin Harcourt Publishing Company. Published by Houghton Mifflin Harcourt Publishing Company. (Year: 2016).
Related Publications (1)
Number Date Country
20180118607 A1 May 2018 US