Glass, Volume 26Minoru Tomozawa, R. H. Doremus Academic Press, 1977 - Glass |
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Page 207
... given in micrometers [ 1 μm = 1000 nanometers ( nm ) = 10,000 angstroms ( Å ) ] . An alternative unit often used in the infrared region is the reciprocal of wavelength , i.e. , the frequency or wave number v , given in reciprocal ...
... given in micrometers [ 1 μm = 1000 nanometers ( nm ) = 10,000 angstroms ( Å ) ] . An alternative unit often used in the infrared region is the reciprocal of wavelength , i.e. , the frequency or wave number v , given in reciprocal ...
Page 308
... given knowledge of σ1 , when L1 / L2 = 10 , it would predict a high tensile stress at L1 / L2 < 2 ; given the result that σ1 0 when L1 / L2 = 3 , the elastic solution would predict zero stress for any no . In contrast , Eq . ( 168 ) ...
... given knowledge of σ1 , when L1 / L2 = 10 , it would predict a high tensile stress at L1 / L2 < 2 ; given the result that σ1 0 when L1 / L2 = 3 , the elastic solution would predict zero stress for any no . In contrast , Eq . ( 168 ) ...
Page 311
... given the following constants : bo = a2212223 1+ a2 ( 175 ) 2 α2 ( λ1λ1⁄2 + λ2λ3 + λ3λ1 ) + αo b1 ( 176 ) = 1 1+ a2 b2 = ( 177 ) 1+ a2 ( 178 ) ( 179 ) a2 ( λ1 + λ2 + λ3 ) + a1 a 。= w1λ2λ3 + w2λ1λ3 + w3λ112 , a1 = w1 ( λ2 + λ3 ) + w2 ...
... given the following constants : bo = a2212223 1+ a2 ( 175 ) 2 α2 ( λ1λ1⁄2 + λ2λ3 + λ3λ1 ) + αo b1 ( 176 ) = 1 1+ a2 b2 = ( 177 ) 1+ a2 ( 178 ) ( 179 ) a2 ( λ1 + λ2 + λ3 ) + a1 a 。= w1λ2λ3 + w2λ1λ3 + w3λ112 , a1 = w1 ( λ2 + λ3 ) + w2 ...
Contents
vii | 57 |
RONALD E LOEHMAN 119 Sandia National Laboratories Albuquerque | 119 |
HeavyMetal Fluoride Glasses | 151 |
Copyright | |
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absorption coefficient AlF3 analysis Basis for Nuclear bead seal behavior Bendow borosilicate glass bulk glasses bulk modulus CCl4 Ceram chemical composite sphere constant cooling corrosion crystalline crystallization curve dB/km devices dielectric Drexhage effects elastic electrical electron energy fibers fluorohafnate fluorozirconate glasses fused silica glass formation glass transition glass transition temperature glass-clad glass-forming region heavy-metal fluoride glasses increase interface traps ions layers leachability leaching Loehman Lucas materials measured melt metal Mitachi modulus MOSFET Moynihan nitride nitrogen Non-Cryst Nuclear Waste Nuclear Waste Management observed optical optical fibers oxide glasses oxynitride glasses Phys Poulain properties Radioactive Waste radionuclides refractive index Rekhson result sample sandwich seal Scherer seal Eq setting temperature shown in Fig silicon SiO2 SiO2 films Solids solution split ring stiffness ratio stress relaxation structural relaxation studies Subsection substrate surface Table techniques thermal thickness viscoelastic viscosity vitreous vitrification Waste Management waste-glass forms wavelength ZBLA ZBLAN ZrF4