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Processing and Properties of Ion Exchanged Glasses
Jill Glass and Raj TandonSandia National Labs, Albuquerque, NM
Prof. Arun Varshneya and Ian SpinelliSaxon Glass Technology, Inc.
Glass and Optical Materials Division Fall MeetingCape Canaveral, FL
Nov. 6-12, 2004
Sandia is a multiprogram laboratory operated by Sandia Corporation, a Lockheed Martin Company, for the United States Department of Energy’s National Security Administration under Contract DE-ACO4-94AL85000.
041106 Stressed glass-Cocoa.ppt -2
Recent Severe Hailstorm in New Mexico
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Truck Bomb Attacks on Federal Buildings Have Focused Attention on Glass Behavior
Embassy in NairobiAugust 7, 1998 Truck Bomb
Embassy in Dar Es SalaamAugust 7, 1998 Truck Bomb
1995- Murrah Building, Oklahoma City, OK
1996- Khobar Towers, Saudi Arabia
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Glass Fragment Character and Size, and Glass Strength Depend on Processing
Plate Glass- 5 kg Indent Plate Glass - As-Rec’d Ion Exchanged
041106 Stressed glass-Cocoa.ppt -10
Video
To view the video showing the breaking glass sheet for
standard glass compared to ion exchanged glass
use the link on the IMI-NFG website orhttp://rm1.cc.lehigh.edu:8080/dept/IMI/EdVideo/RealTime&SloMoGlassBreakage.mpg
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Exchange of a Na-containingglass in a bath of molten KNO3 salt
Ion Exchange Process Replaces Small Ions in Glass Surface with Large Ions
K
Na
041106 Stressed glass-Cocoa.ppt -12
Ion Exchange Stress Profile Increases Glass Strength and Fragmentation
12 hr exchangeStrength = 759 MPa
48 hr exchangeStrength = 706 MPa
Tension
Compression
Glass Thickness
Magnitude of surface compressive stress determinesstrength
Magnitude of central tension determines fragmentation
Disk diameter=1 inchStress profile = - - - - - -
The more a crack branches as it propagatesthe greater the degree of fragmentation.
041106 Stressed glass-Cocoa.ppt -13
Fragment Size Largely Determined by Central Tension, σt and Crack Branching Behavior
( )( )δ
νσ −
+=ttKx
t
c
5.012
21Fragment size,
KIC=toughness, t=thickness, δ=ion exchange depth
tδx2
δ
041106 Stressed glass-Cocoa.ppt -14
Schott Robax and Corning 0317 Glass Exchanged at 450 & 500C for Different Times
Wt% ofoxides
Corning0317
SchottRobax
SiO2 62.3 67.2Na2O 12.8 0.4K2O 3.5 0.23CaO 0.3 0.05MgO 3.3 1.1Al2O3 16.4 20.1Fe2O3 0.24
TiO2 0.75 2.7SnO2 0.04Li2O 3.2BaO 0.9
As2O3 0.9ZrO2 1.7ZnO 1.7
Total 99.53 99.92 As Rec’d Schott Robax
As Rec’d Corning 0317
HV=5.95±0.19 GPaKIC=0.82±0.03 MPa√m
HV=6.44±0.19 GPaKIC=1.09±0.03 MPa√m
041106 Stressed glass-Cocoa.ppt -15
Comparison of Amount of Ion Being Exchanged
Robax
Constituents Wt% Mol%
SiO2 67.20 72.92Na2O 0.35 0.37
K2O 0.23 0.16CaO 0.05 0.06MgO 1.06 1.71Al2O3 20.10 12.85TiO2 2.65 2.16Li2O 3.15 6.87BaO 0.88 0.37
As2O3 0.87 0.29ZrO2 1.73 0.92ZnO 1.65 1.32
Total 99.9 100.0
Corning Constituents Wt% Mol%
SiO2 61.96 65.33Na2O 11.88 12.14K2O 3.41 2.29CaO 0.41 0.46MgO 3.34 5.24Al2O3 16.50 10.25Fe2O3 0.08 0.03TiO2 0.67 0.53Li2O 1.75 3.71Total 100.00 100.00
041106 Stressed glass-Cocoa.ppt -16
Indentation Behavior of Exchanged Schott Glass Show Improved Damage Tolerance
Exchanged at 500C, 6 hr, 2000 g
R-11-19-11
As received, 2000 g indent
R-11-19-22
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Indentation Behavior of Exchanged Corning 0317 Glass Shows Improved Damage Tolerance
Exchanged at 450°C/3 hr As-Rec’d
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0
20
40
60
80
100
120
140
160
0 50 100 150 200
Exchange time (hr)
Centr
al Tensi
on (
MP
a)
Central Tension as a Function of Ion Exchange Temperature and Glass Thickness
Arrow joins same ion exchange conditions (t & T) and glass thickness. 110 MPa vs. 42 MPa.
0
20
40
60
80
100
120
140
160
0 20 40 60 80 100
021010 0317Cent T, strength&BD 12:20:45 PM 10/10/02
t=2.2 mm, 450Ct=2.2 mm, 500C
Mea
sure
d C
entr
al T
ensi
on
(M
Pa)
Ion Exchange Time (hr)
Corning 0317 Schott Robax
041106 Stressed glass-Cocoa.ppt -19
K Ion Exchange Depth for Schott Robax- 6 hr @500C
K penetration depth ~ 20 microns.
0
14
28
42
56
70
0 20 40 60 80 100
Na2OAl2O3SiO2K2OTiO2As2O3ZrO2BaOLi2O
Con
cent
ratio
n (w
t. %
)
Distance (µm)
Trace From100µm Inside Glass to Edge on 500° C, 6 HourSample (R-11-19-18) of Schott Robax in KNO3
041106 Stressed glass-Cocoa.ppt -20
K Ion Exchange Depth for Corning 0317- 6 hr @500C
K penetration depth ~ 90 microns.
0
14
28
42
56
70
0 20 40 60 80 100
Na2OMgOAl2O3SiO2K2OCaOTiO2Li2OC
once
ntra
tion
(wt.
%)
Distance (µm)
Trace From100µm Inside Corning Glass 0317 to Edge on 500° C, 6 Hour Sample, Trace 1
041106 Stressed glass-Cocoa.ppt -21
0
50
100
150
200
250
0 2 4 6 8 10Square Root of Exchange Time (hr0.5)
T=450CT=500C
Schott Robax Has a Much Smaller Ion Exchange Depth than Corning 0317 for the Same T and t
0
50
100
150
200
250
0 2 4 6 8 10
Square root of ion exchange time (hr0.5)
K i
on
exch
an
ge d
ep
th (
µm
)
T=450C
T=500 C
Corning 0317 Schott Robax
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Comparison of Critical Central Tensionsfor Crack Branching in 1” Diameter Disk
Measured Values for Critical Central Tensions (MPa) for Branching in 1” Disks
42
t=1.0
~ < 47
t=1.2
40
t=1.8
~ <47
34
t=2.2
1.09Schott Robax
0.82Corning 0317
Thick.Glass
KIC (MPa√m)(Indentation)
041106 Stressed glass-Cocoa.ppt -23
Fragment Size Comparisons for Two Glasses with Equivalent t’s and σt’s
C-6-21-21t=0.085”=2.2 mm500C/6 hrσt=38.7 MPa
R-11-20-6t=0.085”=2.2 mm500C/96 hrσt=41 MPa
Corning 0317 Schott Robax
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Fragment Size Comparisons for Two Glasses with Equivalent t’s and σt’s
C-6-21-21t=0.085”=2.2 mm500C/6 hrσt=38.7 MPa
R-11-20-6t=0.085”=2.2 mm500C/96 hrσt=41 MPa
R-11-20-36t=0.085”=2.2 mm500C/192 hrσt=47 MPa
Corning 0317 Schott Robax Schott Robax
041106 Stressed glass-Cocoa.ppt -25
Fragment Size Comparisons for Two Glasses with Equivalent t’s and σt’s
( )( )δ
νσ −
+=ttKx
t
c
5.012
21
C-6-21-21t=0.085”=2.2 mm500C/6 hrσt=38.7 MPa
R-11-20-6t=0.085”=2.2 mm500C/96 hrσt=41 MPa
R-11-20-36t=0.085”=2.2 mm500C/192 hrσt=47 MPa
Corning 0317 Schott Robax Schott Robax
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Fragment Size Comparisons for Two Glasses with Equivalent t’s and σt’s
( )( )δ
νσ −
+=ttKx
t
c
5.012
21
C-6-21-21t=0.085”=2.2 mm500C/6 hrσt=38.7 MPa
R-11-20-6t=0.085”=2.2 mm500C/96 hrσt=41 MPa
R-11-20-36t=0.085”=2.2 mm500C/192 hrσt=47 MPa
Corning 0317 Schott Robax Schott Robax
Critical σt is ~ 34 MPa for Corning and 47 MPafor Robax (ratio=0.72)
Toughness ratio=0.75 (0.82 vs. 1.09 MPa.m0.5)
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For a Given Ion Exchange Depth There is More Central Tension in the Corning Glass
500C Exchanget=2.2 mm
0102030405060708090
0 100 200 300
Ion Exchange Depth (microns)
Centr
al Tensi
on (
MPa)
Corning 0317
Schott Robax
041106 Stressed glass-Cocoa.ppt -28
For a Given Ion Exchange Depth There is More Central Tension in the Corning Glass
500C Exchanget=2.2 mm
0102030405060708090
0 100 200 300
Ion Exchange Depth (microns)
Centr
al Tensi
on (
MPa)
Corning 0317
Schott Robax
Corning: 12.14 mol% Na2O (+3.71 mol% Li2O) being replaced by K2ORobax: 6.87 mol% Li2O + 0.37 mol% Na2O being replaced by K2O
Pauling’s ionic radii: Li+=1.2Å, Na+=1.90Å, K+=2.66Å
041106 Stressed glass-Cocoa.ppt -29
Surface Residual Stress Profile and Case Depth Measurements for Schott Robax
Com
pres
sive
Sur
face
Str
ess
(MP
a)
R2 = 0.9916R2 = 0.9919
R2 = 0.9951R2 = 0.9834 R2 = 0.9918
-1000
-900
-800
-700
-600
-500
-400
-300
-200
-100
00 10 20 30 40 50 60 70 80 90
Case Depth (µm)
Unb
roke
n St
ress
(MPa
)
6 hr
24 hr
48 hr
72 hr
192hr
Measurements by I. Spinelli, Saxon Glass Technology, Inc.
T=500CT=2.2 mm
041106 Stressed glass-Cocoa.ppt -30
Schott Robax Biaxial Flexure Strength vs. Ion Exchange Time
0
100
200
300
400
500
600
700
800
900
1000
0 25 50 75 100 125 150 175 200Ion Exchange Time (hr)
Bia
xia
l Fle
xure
Str
ength
(M
Pa)
450C,t=1.2 mm
500C, t=1.2 mm
450C, t=2.2 mm
500C, t=2.2 mm
550C, t=2.2 mm
450C, t=5.0 mm
500C, t=5.0 mm
041106 Stressed glass-Cocoa.ppt -31
Summary and Conclusions
• Ion exchange provides remarkable damage tolerance and strengthening of glass
• Indentation induced fragment size determined by branching distance (central tension, t, δ) and number of branches
• Corning 0317 has greater ion exchange depth and central tension than Schott Robax for a given exchange time and T
• For similar values of central tension Corning has greater degreeof fragmentation than Robax because of lower toughness (0.82 vs. 1.09 MPa.m0.5, ratio=0.75)
• Critical σt for fragmentation is ~ 34 MPa for 2.2 mm Corning and just below 47 MPa for Robax (ratio=0.72)
• Glasses with higher KIC require higher central tensions to achieve fragmentation and have larger fragments for a given σt
• High values of surface compression and strengths can be achieved for Schott Robax - K+ for Li+ exchange
• High strengths, even for long exchanges, suggest that fracture controlled by compressive maximum
041106 Stressed glass-Cocoa.ppt -32
Acknowledgments
• Clay Newton and Ed Beauchamp, Sandia National Labs
• Students: Jason Kooi, Erica Hoover, Jen Rygel, Roman Wolf-Cecil, Karl Nieman, Luke Degruyter
• D. Gerling, Sierracin/Sylmar Corp., Sylmar, CA
Sandia is a multiprogram laboratory operated by Sandia Corporation, a Lockheed Martin Company, for the United States Department of Energy’s National Security Administration under Contract DE-ACO4-94AL85000.
End