Analyzing the Setup
The problem presents a block of mass m=2 kg initially at rest. A time-varying force F(t) acts on it, and we are given its graph. Our ultimate goal is to find the kinetic energy of the block at t=4.5 s.
To bridge the gap between a force-time graph and kinetic energy, we must rely on the Impulse-Momentum Theorem.
The Master Equation
According to Newton's Second Law, force is the rate of change of momentum:
F=dtdp
By integrating both sides with respect to time, we get the impulse, which equals the change in momentum:
Δp=∫Fdt
Graphically, the integral ∫Fdt is exactly the area under the F−t graph. Since the block starts from rest, its initial momentum is zero, meaning the final momentum p is simply equal to this area.
Decoding the Graph
The graph consists of two triangular regions: a positive area A1 above the time axis (from t=0 to t=3 s) and a negative area A2 below the time axis (from t=3 s to t=4.5 s).
Before calculating
A2, we need the height of the second triangle, which corresponds to the force at
t=4.5 s. The graph is a straight line, so its slope is constant:
m=3−00−4=−34 N/s
Using the point-slope form, the force at
t=4.5 s is:
F(4.5)=−34(4.5−3)+0=−34(1.5)=−2 N
Calculating the Impulse
Now we can compute the areas of the two triangles.
The positive area
A1 is:
A1=21×3×4=6 Ns
The negative area
A2 is:
A2=21×1.5×(−2)=−1.5 Ns
The net area, and thus the final momentum
p, is the sum of these areas:
p=A1+A2=6−1.5=4.5 kg m/s
Final Calculation
With the momentum in hand, we can find the kinetic energy using the classic relation:
K=2mp2
Substituting the values
p=4.5 kg m/s and
m=2 kg:
K=2×2(4.5)2=420.25=5.0625 J
Rounding to two decimal places, the kinetic energy is 5.06 J, which perfectly matches option (c).