Setup. We choose the axis oriented along the direction of motion, with the origin of positions at the point where the cat is at the initial instant (sA=0). The motion has two phases and three events (A, B, C). Let’s summarise the known data in the event table:
| Event | t (s) | s (m) | v (m/s) | a (m/s²) |
|---|
| A | 5 | 0 | 7 | |
| B | 8 | 10 | vB | |
| C | tC | sC | 0 | −1 |
Leg A→B. In this leg the average velocity coincides with the arithmetic mean of the velocities (uniformly accelerated motion). From tB−tAsB−sA=2vA+vB:
310=27+vB⇒vB=320−7=−31m/s
The negative result shows that the cat was in fact slowing down: the velocity at B is directed opposite to the initial motion. The acceleration in this leg is:
aAB=tB−tAvB−vA=3−31−7=−922≈−2.44m/s2
Leg B→C. In the final phase the cat decelerates with ∣a∣=1m/s2 until it stops (vC=0). The time needed to zero the velocity is Δt=∣vB∣/∣a∣=31s, so:
tC=tB+avC−vB=8+−10+31=325≈8.33s
sC=sB+2avC2−vB2=10+−20−91=10+181=18181≈10.06m
vB=−31m/s,tC=325s,sC=18181m