Step 1: Recall the orbit time formula.
For a circular orbit, balancing gravity and the centripetal need gives \[ T=2\pi\sqrt{\frac{r^3}{GM}}. \] Notice $M$ here is the Earth's mass, not the satellite's.
Step 2: Mass of the satellite drops out.
The satellite mass never appears, so the fact that $B$ is heavier ($2m$) makes no difference to its period.
Step 3: Keep the dependence on radius.
Everything except $r$ is constant, so \[ T\propto r^{3/2}. \]
Step 4: Write the ratio.
With $r_A=r$ and $r_B=2r$, \[ \frac{T_A}{T_B}=\left(\frac{r}{2r}\right)^{3/2}=\left(\frac{1}{2}\right)^{3/2}. \]
Step 5: Simplify the power.
\[ \left(\frac12\right)^{3/2}=\frac{1}{2\sqrt2}. \]
Step 6: Express as a ratio.
\[ T_A:T_B=1:2\sqrt2. \]
\[ \boxed{T_A:T_B=1:2\sqrt2} \]