Answer:
25.2 s
Explanation:
In an uniformly accelerated motion starting from rest, the time taken for the motion is given by the equation
[tex]d=\frac{1}{2}at^2 \rightarrow t=\sqrt{\frac{2d}{a}}[/tex]
where t is the time, d is the distance covered, a is the acceleration.
We also know that the acceleration can be found by using Newton's second law:
[tex]\sum F = ma \rightarrow a=\frac{\sum F}{m}[/tex]
where [tex]\sum F[/tex] is the net force on the object and m its mass. Substituting into the previous equation,
[tex]t=\sqrt{\frac{2md}{\sum F}}[/tex] (1)
So we see that the time taken for the motion is inversely proportional to the square root of the net force.
Let's consider now the space probe in the problem. Let's call F the magnitude of the force generated by each engine.
When the two forces are applied in the same direction, the net force on the space probe is
[tex]\sum F = F+F = 2F[/tex]
But when the two forces are applied perpendicularly, the net force is
[tex]\sum F' = \sqrt{F^2+F^2}=\sqrt{2} F[/tex]
Using eq.(1) we can write:
[tex]\frac{t}{t'}=\sqrt{\frac{\sum F'}{\sum F}}[/tex]
where t' is the new duration of the motion. Solving for t',
[tex]t'=\sqrt{\frac{\sum F}{\sum F'}}t=\sqrt{\frac{2F}{\sqrt{2}F}}(21.2 s)=25.2 s[/tex]