The Anatomy of a Highway Emergency
Imagine you are cruising down a straight highway at a brisk 108 km/h. Suddenly, the brake lights of the car ahead flare up. You slam on your brakes, but there is an inevitable human delay—a reaction time.
This problem is a classic exploration of relative motion and kinematics. It forces us to analyze not just how cars stop, but how they stop relative to each other.
Setting the Stage
Deceleration
First, we must standardize our units. A speed of 108 km/h converts cleanly to 30 m/s.
Next, we evaluate the braking power of both vehicles. Car A can halt in 7.0 s, giving it a deceleration of aA=730 m/s2. Car B takes 10 s to stop, meaning its deceleration is aB=3 m/s2.
The critical insight: Car A has significantly stronger brakes than Car B. This asymmetry completely changes the dynamics depending on who is in front!
Case (a)
The Intuitive Scenario
If Car A is leading, we have a highly dangerous situation. The car in front can stop much faster than the car behind it.
When A brakes, B continues at 30 m/s for a full 1.0 s due to reaction time. Even after B starts braking, it cannot decelerate as quickly as A. Therefore, the gap between them will continuously shrink until both vehicles come to a complete halt.
To avoid a collision, the initial separation must be greater than the difference in their total stopping distances. Car A's stopping distance is sA=21(30)(7)=105 m. Car B travels 30 m during the reaction time, plus 21(30)(10)=150 m while braking, totaling 180 m.
The minimum safe distance is simply 180 m−105 m=75 m.
Case (b)
The Counter-Intuitive Trap
Now, let's flip the order. Car B is in front. B slams the brakes, and A reacts 1.0 s later.
Initially, this looks terrifying. A is hurtling forward at 30 m/s while B is already slowing down. The gap is closing rapidly! However, once A finally hits the brakes, its superior stopping power kicks in.
The turning point: The cars will be closest to each other at the exact instant their speeds become equal. If they don't crash before this moment, A will begin to pull away, and they are safe.
The Geometric Masterstroke
We could use heavy algebra to find the minimum separation, but there is a far more elegant way: the velocity-time graph.
If we plot v versus t for both cars, the extra distance Car A travels relative to Car B is simply the area between their curves up to the moment their speeds match.
Setting their velocity equations equal, 30−730(t−1)=30−3t, we find they reach the same speed at t=310 s. At this instant, both are moving at 20 m/s.
Looking at the graph, the area between the curves forms a perfect triangle! The base of this triangle is the 1.0 s reaction time (where A's speed is constant). The height is the drop in speed from 30 m/s to 20 m/s, which is 10 m/s.
The area is 21×base×height=21(1)(10)=5.0 m.
This means Car A covers exactly 5.0 m more than Car B during the critical approach phase. Thus, a mere 5.0 m of initial separation is enough to prevent a crash!
This is the power of graphical analysis in physics—transforming pages of algebra into a single, beautiful geometric shape.