Animated Solution for Physics - Oscillations: For a simple pendulum, a graph is plotted between its Kinetic Energy (KE) and Potential Energy (PE) against its displacement (d) Which one of the following represents these correctly? (graphs are schematic and not drawn to scale)
Select Answer:
Visualized Solution
Energy in SHM
PE=21kd2
KE=21k(A2−d2)
Potential Energy Curve
PE=21kd2
Equation of an upward-opening parabola.
At d=0, PE=0.
Kinetic Energy Curve
KE=Etotal−PE
KE=21kA2−21kd2
Equation of a downward-opening parabola.
At d=0, KE=Etotal.
Intersection Points
PE=KE⟹21kd2=21k(A2−d2)
2d2=A2⟹d=±2A
Conclusion
Graph (b) correctly shows:
PE as an upward parabola.
KE as a downward parabola.
What if plotted against time?
d=Asin(ωt)
PE=21kA2sin2(ωt)
KE=21kA2cos2(ωt)
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The Sigma Insight: Force and Energy Method in SHM
Solution Diagram
The Energy Dance of a Simple Pendulum
Imagine a simple pendulum swinging back and forth. As it moves, there is a continuous, beautiful exchange between its Kinetic Energy (KE) and Potential Energy (PE). But how exactly do these energies vary with the pendulum's displacement d from its mean position? Let's break down the mathematics behind this energy dance.
Analyzing the Potential Energy
First, let's look at the Potential Energy. For a simple pendulum undergoing Simple Harmonic Motion (SHM), the restoring force is directly proportional to the displacement, given by F=−kd. The potential energy is the work done against this restoring force, which integrates to:
PE=21kd2
Notice the d2 term? This tells us that the relationship is strictly quadratic. If we plot PE against displacement d, we get a perfect parabola opening upwards. At the mean position (d=0), the potential energy is at its absolute minimum, which is zero.
Analyzing the Kinetic Energy
Now, what about the Kinetic Energy? We know from the law of conservation of mechanical energy that the total energy Etotal of the system remains constant (assuming no air resistance). Therefore, the Kinetic Energy is simply the Total Energy minus the Potential Energy:
KE=Etotal−PE
KE=21kA2−21kd2
Here, A is the maximum amplitude. Because of the negative sign in front of the d2 term, the graph of KE against displacement is a parabola opening downwards. At the mean position (d=0), the pendulum is moving at its fastest, so the Kinetic Energy is at its maximum, equal to the total energy Etotal.
The Intersection Points
An interesting feature of these graphs is where they intersect. The intersection occurs when Kinetic Energy equals Potential Energy:
21kd2=21k(A2−d2)
Solving this gives 2d2=A2, or d=±2A. At these exact points, the energy is split perfectly 50-50 between kinetic and potential forms.
Final Conclusion
When we compare our derived parabolic curves with the given options, we can confidently eliminate any graphs showing straight lines or non-parabolic curves. Option (b) perfectly illustrates the upward-opening parabola for Potential Energy and the downward-opening parabola for Kinetic Energy, making it the correct representation of the pendulum's energy dynamics.