## Treatise on materials science and technology, Volume 1 |

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Page 139

In these directions pl and p2 waves become true longitudinal and

and the wave polarized perpendicular to the xy plane will be referred to as the ...

In these directions pl and p2 waves become true longitudinal and

**transverse****waves**, respectively. The p2 wave will be referred to as the /^-**transverse wave**and the wave polarized perpendicular to the xy plane will be referred to as the ...

Page 146

We notice that due to a relatively large value of c33, the propagation of waves in

the yz plane in the present model is almost ... The wave given by Eq. (82) will be

labeled as the ^-

We notice that due to a relatively large value of c33, the propagation of waves in

the yz plane in the present model is almost ... The wave given by Eq. (82) will be

labeled as the ^-

**transverse wave**and is always a true**transverse wave**.Page 164

(3) z-

120) 2Ds1nk,rn , , , Cgx = — - — -[2cosfc1+cosA:2] (121) 20sin*2cosfc, C„ = 1 (

122) "'I ^ = 0 We notice from Eq. (118) that the angle of polarization is

independent ...

(3) z-

**transverse wave**m2 = 2i)(l-cos2A:1) + 40(1 -cosfc1 cosfc2) (119) ^ = [0,0,1] (120) 2Ds1nk,rn , , , Cgx = — - — -[2cosfc1+cosA:2] (121) 20sin*2cosfc, C„ = 1 (

122) "'I ^ = 0 We notice from Eq. (118) that the angle of polarization is

independent ...

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activation energy alloys angle annealing Argon Arsenault axis binding energy bond calculated carbon chemical vapor deposition crystal curvature curve CVD tungsten Debye decrease deposition determined dipole displacement distribution effect elastic constants elastic waves electron equation equilibrium experimental Fe-Mn-N Fe-N fibers force constants fracture free energy function geometric given grain boundaries group velocities growth path envelope Hasson hoop stress impingement increase interface internal friction interstitial ions kcal/mole kinetics laminate lattice layer manganese measured mechanism metal microstructural change molecules neighbors niobium nitrogen nitrogen atoms nucleation obtained oxygen parameters particles peak broadening peak height phase potential propagation reinforcing elements relaxation processes rhenium s-i interaction s-i pair scavenging Section shear shown in Fig Snoek peak solid specimen structure substitutional addition substitutional solute substrate surface tensile ternary alloys tetragonal titanium transverse wave triple line tungsten values vanadium volume fraction xy plane yield stress zirconium