Imagine you are pushing a heavy block across a floor. The harder you push, and the farther you push it, the more energy you transfer to the block. This fundamental idea is beautifully captured by the Work-Energy Theorem, which is the star of this problem.
Analyzing the Setup
We are given a particle that starts from rest, meaning its initial velocity u=0. Consequently, its initial kinetic energy Ki is exactly 0 J. The particle is subjected to a variable force, and we are provided with a Force-Displacement (F−x) graph. Our goal is to find the kinetic energy of the particle after it has travelled a distance of 3 m.
The Master Equation
The Work-Energy Theorem states that the net work done on an object equals its change in kinetic energy:
Since Ki=0, the final kinetic energy Kf is simply equal to the total work done W. But how do we find the work done from a graph? Mathematically, work is the integral of force with respect to displacement (W=∫Fdx). Geometrically, this integral is exactly the area under the Force-Displacement curve.
Breaking Down the Area
To find the total area under the curve from x=0 to x=3, we can break the complex shape into three simple, manageable geometric figures:
1. The First Rectangle (A1):
From
x=0 to
x=2, the force is constant at
2 N. This forms a rectangle with a width of
2 m and a height of
2 N.
A1=width×height=2×2=4 J
2. The Second Rectangle (A2):
From
x=2 to
x=3, we can draw a smaller rectangle at the base. Its width is
1 m (from
2 to
3) and its height is
2 N.
A2=width×height=1×2=2 J
3. The Triangle (A3):
Sitting right on top of the second rectangle (from
x=2 to
x=3) is a triangle. Its base is
1 m, and its height goes from
2 N to
3 N, which is a height of
1 N.
A3=21×base×height=21×1×1=0.5 J
Final Calculation
Now, we simply sum up these individual areas to find the total work done:
W=A1+A2+A3
W=4+2+0.5=6.5 J
Since the final kinetic energy equals the total work done, we have:
The Way Forward
This problem was straightforward because the force was always positive, meaning it was constantly adding kinetic energy to the particle. However, always be cautious! If the force graph dips below the x-axis, the area becomes negative. Negative work means the force is opposing the motion, which would decrease the particle's kinetic energy. Always respect the sign conventions in graphical physics problems!