Decoding the Graph
When you first look at the problem, you are presented with a graph plotting the square of velocity (v2) against displacement (x). The most crucial observation here is the shape of the graph—it is a perfectly straight line. In physics, whenever you see a straight line graph, your immediate instinct should be to relate it to the standard equation of a straight line: y=mx+c.
Here, our y-axis represents v2 and our x-axis represents x. So, the equation governing this motion takes the form v2=mx+c. But what do the slope (m) and the y-intercept (c) represent physically? To answer that, we need to dive into our kinematics toolkit.
The Kinematic Connection
We need an equation that connects velocity, displacement, and constant acceleration without involving time. The third equation of motion is the perfect fit:
Let's rearrange this slightly to match our straight-line format:
By comparing this with y=mx+c, a beautiful relationship emerges. The slope of our graph, m, is exactly equal to twice the acceleration (2a). Furthermore, the y-intercept, c, corresponds to the square of the initial velocity (u2). This means that just by finding the slope of this line, we can unlock the value of the acceleration.
Calculating the Slope
Now, let's extract the slope from the given graph. The slope m is defined as the "rise over run", or the change in the y-variable divided by the change in the x-variable:
We can pick any two clear points on the line to calculate this. Let's use the starting point (0,20) and the final point (30,80).
The Final Acceleration
We have established that the slope of the graph is 2, and from our kinematic comparison, we know that the slope is equal to 2a. Setting these equal to each other gives us a simple algebraic equation:
Solving for a, we get:
And there we have it! By simply understanding the geometric properties of the graph and linking them to fundamental kinematic equations, we effortlessly arrived at the constant acceleration of the particle.