Step 1: Recall Gauss's law: the flux through a closed surface depends only on the enclosed charge:
\[\Phi = \frac{q}{\epsilon_0}\]
Step 2 (part a): If the radius of the spherical Gaussian surface is doubled, the same point charge is still the only charge enclosed. Since the flux does not depend on the radius, it stays the same:
\[\Phi' = \Phi = -1.0\times10^{3}\,\text{N m}^2\,\text{C}^{-1}\]
Step 3 (part b): Find the charge from \(\Phi = q/\epsilon_0\), so \(q = \epsilon_0\,\Phi\). Substitute the values:
\[q = (8.85\times10^{-12})\times(-1.0\times10^{3})\]
Step 4: Do the arithmetic:
\[q = -8.85\times10^{-9}\,\text{C} = -8.85\,\text{nC}\]
The negative sign shows the charge is negative (consistent with inward flux).
\[\boxed{\Phi' = -1.0\times10^{3}\,\text{N m}^2\,\text{C}^{-1},\quad q = -8.85\,\text{nC}}\]