Scientists want to place a {msat} kg satellite in orbit around Mars. They plan to have the satellite orbit at a speed of {vsat} m/s in a perfectly circular orbit. Here is some information that may help solve this problem:
mass of mars: $M$ = 6.4191 × 1023 kg
radius of orbit: $R$= 3.397 × 106 m
$G$ = 6.67428 × 10-11 N-m2/kg2
This is the part that causes the greatest headache. You can save a lot of trouble by using ratios. We want a ratio involving $v$ and $T$ equal to a constant with no other variable. The problem is that $v$, $R$ an $T$ are all related. $$ \frac{GMm}{R^2} = \frac{mv^2}{R}$$ Get rid of the $v$ and introduce the $T$ (the period) by using the old standby $$ v =\frac{2\pi R}{T}$$ sub into the previous eqn and get rid of the $m$'s $$ \frac{GM}{R^2} = \frac{(\frac{2\pi R}{T})^2}{R}$$ We get our ratio as follows: $$\frac{R^3}{T^2} = \frac{GM}{4\pi^2}$$ (This is Kepler's 3rd law.) Darn. We've got $R$ in the ratio not $v$. (This is actually what we need for the previous problem.
Anyhow, Substitute $R = Tv/2\pi$ $$\frac{(Tv/2\pi)^3}{T^2} = \frac{GM}{4\pi^2}$$ $$v^3 T = {\rm constant}$$ The important point is that this ratio is equal to a constant and we really don't care what that constant is. If we're given that $T_2/T_1 = 8$ we can easily get $v_2/v_1$. $$\left(\frac{v_2}{v_1} \right)^3 = \frac{T_1}{T_2} $$ $$\frac{v_2}{v_1} = \sqrt[3]{ \frac{T_1}{T_2} } = \left( \frac{T_1}{T_2}\right)^{1/3}$$ Thus $$\frac{v_2}{v_1} = \frac{1}{2}$$