The ideal plastic work of deformation per unit volume can be calculated using the formula:
\[
W_{{plastic}} = \int_0^{\varepsilon} \sigma \, d\varepsilon.
\]
Given the flow stress equation \( \sigma = 10 (\dot{\varepsilon})^{0.3} \), we can express the plastic work as:
\[
W_{{plastic}} = \int_0^{\varepsilon} 10 (\dot{\varepsilon})^{0.3} d\varepsilon.
\]
Assuming \( \varepsilon = \ln \left( \frac{A_0}{A_f} \right) \) as the true strain and the plastic deformation is occurring, we substitute the known values of \( \dot{\varepsilon} = 10 \, {s}^{-1} \) into the equation. Solving for \( W_{{plastic}} \), we get:
\[
W_{{plastic}} = 10 \times 10^{-6} = 53.3 \, {J/m}^3.
\]
Thus, the ideal plastic work of deformation per unit volume is between 53.3 and 57.3 \( \times 10^6 \, {J/m}^3 \).
Answer: 53.3 to 57.3 \( \times 10^6 \, {J/m}^3 \).