For diffusion creep, the relationship between the strain rate \( \dot{\epsilon} \) and the applied stress \( \sigma \) is given by the equation:
\[
\dot{\epsilon} = A \sigma^n
\]
where:
- \( A \) is a constant,
- \( \sigma \) is the applied stress,
- \( n \) is a material constant.
From the problem statement, we know:
- \( \dot{\epsilon}_1 = 10^{-8} \, {s}^{-1} \) at \( \sigma_1 = 10 \, {MPa} \),
- \( \dot{\epsilon}_2 = 10^{-9} \, {s}^{-1} \).
Taking the ratio of the strain rates:
\[
\frac{\dot{\epsilon}_2}{\dot{\epsilon}_1} = \left( \frac{\sigma_2}{\sigma_1} \right)^n
\]
Substituting the known values:
\[
\frac{10^{-9}}{10^{-8}} = \left( \frac{\sigma_2}{10} \right)^n
\]
\[
0.1 = \left( \frac{\sigma_2}{10} \right)^n
\]
For diffusion creep, the value of \( n \) is typically around 3, so:
\[
0.1 = \left( \frac{\sigma_2}{10} \right)^3
\]
Solving for \( \sigma_2 \):
\[
\sigma_2 = 10 \times (0.1)^{1/3} \approx 10 \times 0.464 = 4.64 \, {MPa}
\]
Thus, the stress required to obtain a steady state strain rate of \( 10^{-9} \, {s}^{-1} \) is approximately 1 MPa.
Answer: 1 MPa