The work-energy theorem states that the work done by the retarding force is equal to the change in the kinetic energy of the car.
\[
W = \Delta KE = \frac{1}{2} m v^2
\]
where \( m \) is the mass of the car and \( v \) is the initial velocity. The work done by the force \( F \) over a distance \( d \) is:
\[
W = F \times d
\]
Thus, we have the equation:
\[
F \times d = \frac{1}{2} m v^2
\]
For the car moving with a speed \( 3v \), its initial kinetic energy will be:
\[
KE_{{new}} = \frac{1}{2} m (3v)^2 = \frac{1}{2} m \times 9v^2 = 9 \times \left( \frac{1}{2} m v^2 \right)
\]
Since the car is to stop within the same distance \( d \), the work done by the retarding force should equal this new kinetic energy:
\[
F_{{new}} \times d = 9 \times \left( F \times d \right)
\]
Thus, the new force required to stop the car moving with speed \( 3v \) is:
\[
F_{{new}} = 9F
\]
Hence, the force needed to stop the car moving with speed \( 3v \) within the same distance is \( 9F \).
\[
\boxed{9F}
\]