The migration of H in high-purity material was studied by using the Gorsky-effect anelastic technique. The observed H diffusivities depended upon the concentrations of trapping sites such as dislocations and O atoms. At low interstitial solute levels and low dislocation densities (104/cm2), the activation energy was 0.080eV. As the number of O trapping sites increased, the activation energy increased to a value of 0.096eV at 0.23at%O (table 85). The introduction of dislocation trapping sites by cold-rolling (10% reduction of area) increased the activation energy to 0.093eV. High activation energies were also observed in specimens which contained high H concentrations after extensive hydride precipitation had occurred. This was consistent with the large amount of plastic deformation that occurred when such hydrides were precipitating.

G.Matusiewicz, R.Booker, J.Keiser, H.K.Birnbaum: Scripta Metallurgica, 1974, 8[12], 1419-25

 

Table 84

Parameters for H Diffusion in NbHx

 

x

Do (cm2/s)

E (eV)

0.10

3.2 x 10-4

0.115

0.33

4.9 x 10-4

0.142

0.55

1.0 x 10-3

0.168

0.70

7.2 x 10-4

0.174

0.89

5.6 x 10-4

0.164

 

 

Figure 16

Diffusivity of H in Nb

 

 

Table 85

Parameters for H Diffusion in Nb at Temperatures above 165K

 

O (at%)

N (at%)

C (at%)

H (at%)

Method

Do (cm2/s)

E (eV)

0.14

0.06

<0.01

2.2

dynamic

2.8 x 10-4

0.089

0.08

0.02

<0.01

1.6

dynamic

2.8 x 10-4

0.089

0.23

0.005

0.006

0.28

static

2.4 x 10-4

0.096

0.043

0.006

0.005

0.095

static

1.7 x 10-4

0.081

0.029

0.009

0.005

0.11

static

1.6 x 10-4

0.080