Energy Changes in Simple Harmonic Motion
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Simple harmonic motion also involves an interplay between different types of energy: potential and kinetic
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The swinging of a pendulum is an interplay between gravitational potential energy and kinetic energy
- The horizontal oscillation of a mass on a spring is an interplay between elastic potential energy and kinetic energy
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Energy of a Horizontal Mass-Spring System
- The system has the maximum amount of elastic potential energy when held so the string is stretched beyond its equilibrium position
- When the mass is released, it moves back towards the equilibrium position, accelerating as it goes so the kinetic energy increases
- At the equilibrium position, kinetic energy is at its maximum and elastic potential energy is at its minimum
- Once past the equilibrium position, the kinetic energy decreases and elastic potential energy increases
In a horizontal mass-spring system the kinetic energy is maximum in the equilibrium position and the elastic potential energy is maximum in the amplitude position
Energy of a Simple-Pendulum
- At the amplitude at the top of the swing, the pendulum has a maximum amount of gravitational potential energy
- When the pendulum is released, it moves back towards the equilibrium position, accelerating as it goes so the kinetic energy increases
- As the height of the pendulum decreases, the gravitational potential energy also decreases
- Once the mass has passed the equilibrium position, kinetic energy decreases and gravitational potential energy increases
In a simple pendulum system the kinetic energy is maximum in the equilibrium position and the gravitational potential energy is maximum in the amplitude position
Total Energy of an SHM System
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The total energy in the system remains constant, but the amount of energy in one form goes up while the amount in the other form goes down
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This constant total energy shows how energy in a closed system is never created or destroyed; it is transferred from one store to another
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This is the law of conservation of energy
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The total energy of a simple harmonic system always remains constant and is equal to the sum of the kinetic and potential energy
- The total energy is calculated using the equation:
E = EP + EK
- Where:
- E = total energy in joules (J)
- EP = potential energy in joules (J)
- EK = kinetic energy in joules (J)
- Remember the equations for potential and kinetic energy:
- Gravitational potential energy: Ep = mgh
- Elastic potential energy, Ep =
- Kinetic energy, Ek =
Energy-Displacement Graph
- The kinetic and potential energy transfers go through two complete cycles during one period of oscillation
- One complete oscillation reaches the maximum displacement twice (on both the positive and negative sides of the equilibrium position)
- You need to be familiar with the graph showing the total, potential and kinetic energy transfers in half an SHM oscillation (half a cycle)
Graph showing the potential and kinetic energy against displacement in half a period of an SHM oscillation
- The key features of the energy-displacement graph for half a period of oscillation are:
- Displacement is a vector, so, the graph has both positive and negative x values
- The potential energy is always maximum at the amplitude positions x = x0, and 0 at the equilibrium position x = 0
- This is represented by a ‘U’ shaped curve
- The kinetic energy is the opposite: it is 0 at the amplitude positions x = x0, and maximum at the equilibrium position x = 0
- This is represented by an ‘n’ shaped curve
- The total energy is represented by a horizontal straight line above the curves
Energy-Time Graph for a Simple Pendulum
- You also need to be familiar with the graph showing the total, gravitational potential and kinetic energy transfers against time for multiple cycles of a simple pendulum oscillating in simple harmonic motion
The kinetic and gravitational potential energy of a simple pendulum oscillating in SHM vary periodically
- The key features of the simple pendulum energy-time graph are:
- Both the kinetic and gravitational potential energy transfers are represented by periodic functions (sine or cosine) which vary in opposite directions to one another
- When the gravitational potential energy is 0, the kinetic energy is at its maximum and vice versa
- The total energy is represented by a horizontal straight line directly above the energy curves at the maximum kinetic and gravitational potential energy value
- Energy is always positive so there are no negative values on the y-axis (Any SHM energy graph drawn with negative energy values is incorrect)
Worked example
The following graph shows the variation with displacement of the kinetic energy of an object of mass 0.50 kg oscillating with simple harmonic motion. Energy losses can be neglected.
Determine:
(a) The total energy of the object
(b) The amplitude of the oscillations
(c) The maximum velocity of the object
(d) The potential energy of the object when the displacement is x = 1.0 cm
Answer:
(a)
- From the graph, the maximum value of kinetic energy is 60 mJ
- At the equilibrium position , the total energy E is exactly equal to the maximum value of kinetic energy
- Since energy losses can be neglected, the total energy is constant
Total energy: E = 60 mJ
(b)
- The amplitude is equal to the maximum displacement on either side of the equilibrium position (where the kinetic energy is zero)
Amplitude: = 2.0 cm
(c)
- The maximum velocity can be found using the maximum kinetic energy in the equation:
- Using:
- Mass of the object, m = 0.50 kg
- Maximum kinetic energy, Ek = 60 mJ = 0.06 J
Maximum velocity: v = 0.49 m s–1
(d)
- From the graph, when the displacement is x = 1.0 cm, kinetic energy is EK = 50 mJ
- The relationship between total energy E, kinetic energy EK and potential energy EP is:
E = EP + EK
- Therefore, the potential energy is
EP = E – EK
EP = 60 – 50 = 10 mJ
Examiner Tip
You may be expected to draw as well as interpret energy graphs against time or displacement in exam questions. Make sure the sketches of the curves are as even as possible and use a ruler to draw straight lines, for example, to represent the total energy.