Question 13.10.3: The partial pressure of hydrogen in the atmosphere is such t...

The partial pressure of hydrogen in the atmosphere is such that an Fe–C–Ti melt containing 1 wt% C and 3 wt% Ti contains 5 parts per million (by weight) of hydrogen at 1600°C. Calculate the vacuum which is required to decrease the hydrogen content of the melt to 1 ppm, given that e^{Ti}_{H}=-0.08,  that e^{C}_{H}=0.06,  and that hydrogen in pure iron obeys Henry’ s law up to a solubility of 0.0027 wt% under a pressure of 1 atm of hydrogen at 1600°C.

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For the equilibrium between gaseous hydrogen and dissolved H, given as ½H_{2(g)}=[H]_{(1  wt\%  in   Fe)},

K=\frac{f_{H(1  wt\%)}[wt\%H]}{p^{1/2}_{H_2}}

In pure iron, as H obeys Henry’ s law, f_{H(1wt\%)}=1 ,  and thus,

K_{1873  K}=0.0027

Thus,

\log f_{H(1  wt\%)}+\log [wt\%  H]-\frac{1}{2}\log p_{H_2}=\log 0.0027 

But

\log f_{H(1  wt\%)}=e^{H}_{H}[wt\%  H]+e^{Ti}_{H}[wt\%  Ti]+e^{C}_{H}[wt\%  C]

As f_{H(1  wt\%)}=1,  e^{H}_{H}=0 , and hence, at 1600°C,

e^{Ti}_{H}[wt\%  Ti]+e^{C}_{H}[wt\%  C]+\log [wt\%  H]-\frac{1}{2}\log p_{H_2}=\log 0.0027 

When [wt\%  H]=5\times 10^{-4} ,

\log p_{H_2}=2\times [(-0.08\times 3)+(0.06\times 1)+\log (5\times 10^{-4})-\log 0.0027]

=-1.825

which gives p_{H_2}= 0.015  atm. Similarly, when [wt\%  H]=1\times 10^{-4},p_{H_2}=6\times 10^{-4}  atm. Thus,

[wt\%  H]=5  ppm   when  p_{H_2}=0.015  atm      and P_{(total)}=1  atm

And so

[wt\%  H]=1  ppm    when  p_{H_2}=0.0006  atm

and

P_{total}=\frac{0.0006}{0.015}=0.04   atm

Thus, in order to achieve the desired decrease in the content of dissolved H, the total pressure must be decreased from 1 to 0.04 atm.

 

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