Title: Problem 31: SteadyState Diffusion
1Problem 31Steady-State Diffusion
- Presented by Eric Burkhart
- 14 Feb. 2007
2Problem Statement
3What Type of Diffusion
- Hydrogen moving between neighboring interstitial
sites in steel - Interstitial diffusion is often much faster than
vacancy diffusion
4Where to Start
- Trying to find kg/h of hydrogen diffusing out of
steel vessel
Where A is the area over which diffusion is
occurring and J is the diffusion flux.
- We can first find A, the surface area of a cube
from the volume of the cube (1m3)
6 Cube Faces 1m2 per Face 6m2 Surface Area
5How to Find J
Where D is the diffusion coefficient and dC/dx is
the slope of the concentration profile
- Diffusivity is given in the problem statement
WARNING Diffusivity varies with temperature, use
eqn. 6.8 to find D given a specific temperature.
- Okay, but what is a concentration profile?
6Concentration Profiles
- In this case, the denominator is simply the
thickness of a wall (2mm). - CA is the concentration of Hydrogen on the
inside steel wall, and CB is the concentration
of Hydrogen on the outside steel wall, given by
the problem statement as zero.
7Concentration and Solubility
- Concentration is in terms of atoms or mass per
length3. - Solubility is in mass of Hydrogen per overall
mass. In this case kg H/ kg Steel assuming
negligible mass addition from Hydrogen. - Problem statement says
Solubility
And gives the initial condition that at 300C and
1 atm, solubility is 1 ppm by weight, allowing us
to solve for a.
8Calculating Concentration
- Given pressure of 12.86 atm (189psia), solubility
on inside wall is
3.586e-6 kg Hydrogen/ kg Steel
- To get concentration, multiply solubility by
density of steel.
CA 3.586e-6 kg H/kg Steel 7500 kg steel/m3
Steel 0.02690 kg H/m3 Steel
9Back to the Beginning
A6m2
D5e-10 m2/s CA 0.02690 kg H/m3 Steel
CB0 xA-xB2mm
1.453x10-4 kg Hydrogen/hour
10Relevance
Pressure Vessel Design -
- Gas loss (particularly Hydrogen and other small
gasses) not always insignificant. - High temperature, high pressure and thin walls
all increase the rate of loss.
Why is solubility proportional to square root of
pressure?
- Sieverts' Law H2 dissociates into
monatomic Hydrogen and then passes
through steel, becoming diatomic again on the
other side.