The Journey of the Car
Imagine you are driving a car on a long, straight highway. You press the gas pedal, and the car accelerates at a constant rate α. You reach a top speed, and then immediately hit the brakes, decelerating at a constant rate β until you come to a complete stop. The entire journey takes exactly t seconds. Our goal is to find the total distance you travelled during this time.
While we could use the standard equations of motion (v=u+at and s=ut+21at2) to solve this, there is a much more elegant and powerful method: Graphical Analysis.
Visualizing with a Velocity-Time Graph
Let's plot the car's velocity against time.
Since the car starts from rest, the graph begins at the origin (0,0). It accelerates uniformly, meaning the velocity increases linearly, forming a straight line with a positive slope α. Let's say it reaches a maximum velocity v0 at time t1.
Then, the car decelerates uniformly to rest. The graph goes down as a straight line with a negative slope −β, hitting the time axis at the total time t. Let the duration of this deceleration phase be t2.
The Math of Slopes
The slope of a velocity-time graph represents acceleration.
For the acceleration phase, the slope is
α:
α=t1v0⟹t1=αv0
For the deceleration phase, the magnitude of the slope is
β:
β=t2v0⟹t2=βv0
The Time Constraint
We know the total time of the journey is
t. Therefore, the sum of the acceleration time and deceleration time must equal
t:
t1+t2=t
Substituting our expressions for
t1 and
t2:
αv0+βv0=t
Now, let's factor out the maximum velocity
v0:
v0(α1+β1)=t
Finding a common denominator gives us:
v0(αβα+β)=t
Rearranging this to solve for
v0, we get a beautiful standard result for the peak velocity:
v0=α+βαβt
The Area is the Key
To find the total distance travelled, we need to find the area under the velocity-time graph. Because the car never reverses direction, the displacement and distance are identical.
Our graph forms a simple triangle with a base of
t and a height of
v0. The area of a triangle is:
s=21×base×height
s=21×t×v0
Finally, we substitute the expression for
v0 that we just derived:
s=21×t×(α+βαβt)
Multiplying the terms together, we arrive at our final answer:
s=2(α+β)αβt2
This is a classic and highly useful formula in kinematics. Memorizing it can save you valuable time in competitive exams!