Lesson 1 - Energy Conservation: Weighted Spring

Energy Conservation: Weighted Spring simulates the simple harmonic motion of a weighted spring in order to graphically explore changes in the weighted spring's potential and kinetic energy, velocity, and position over time. The spring constant, mass, and amplitude can be varied.


Prerequisites

Students should be familiar with the general properties of simple harmonic motion (SHM). Students should also be familiar with the concepts of kinetic and potential energy and energy conservation.

Learning Outcomes

Students will learn how to use energy conservation to obtain information about the potential energy of a weighted spring. They will be able to describe the time dependence of the potential energy when the spring is oscillating. They will learn that the energy of the weighted spring is proportional to the square of the amplitude of oscillation of the spring.

Instructions

Students should understand the applet functions that are described in Help and ShowMe. The applet should be open. The step-by-step instructions on this page are to be done in the applet. You may need to toggle back and forth between instructions and applet if your screen space is limited.


Contents

  1. Kinetic Energy as a Function of Time
  2. Potential Energy as a Function of Time

1. Kinetic Energy as a Function of Time

The kinetic energy KE of weighted spring varies in time when the weight is oscillating up and down.

exercise 1

Does the kinetic energy of a weighted spring depend on time t? If so, how? Use the applet to find out. On the applet,

image

Figure 1

  • click "Reset" (Reset)
  • set the spring constant to k = 80 N /m
  • keep the mass and the amplitude at their default values of m = 1.25 kg and A = 0.20 m
  • start the motion from its default position, which has the weight in its top position
  • display the position vs. time and velocity vs. time graphs by selecting them from the graph menu (image):

image

 

Sketch the position (y) vs. time (t) and velocity (vy) vs. time (t) graphs below. On the graphs, mark the points where the spring passes its top (T), bottom (B), and equilibrium positions (E).

Position vs. Time

image

Velocity vs. Time

image

 

exercise 2

Based on the velocity vs. time graph, is the kinetic energy of the weighted spring changing with time? Explain.




exercise 3

Sketch the kinetic energy KE of the oscillating spring vs. time by selecting it from the graph menu (image) image

Kinetic Energy vs. Time

image

Does your kinetic energy graph support your answer from Exercise 2?

The Kinetic Energy of a spring is related to its mass (m) amplitude (A), angular frequency (w) and time (t).
Expressed as an equation,

image (1)

Quantity

Symbol

SI Unit

kinetic energy KE J
mass m kg
amplitude A m
angular frequency ω rad/s
time t s

exercise 4

Rewind the applet, and step through the motion until the weight is as close to its equilibrium point as possible (the energy column would be entirely red at the equilibrium point). Record the value of the kinetic energy at this point from the Data box.

KE = _____________ J

Demonstrate how this value is calculated using equation (1).




2. Potential Energy as a Function of Time

The potential energy of the simple pendulum is strictly speaking the gravitational potential energy of the pendulum-earth system. We will refer to it as the "potential energy of the pendulum" for short.

The mechanical energy E, energy for short, of the simple pendulum stays constant during the pendulum's motion (if the motion is undamped, as it is in the applet). One says the energy is conserved. The mechanical energy is the sum of kinetic and potential energy,

E = KE + PE (2)

exercise 5

On the applet, play the motion and observe how there is an ongoing conversion of potential into kinetic energy or vice versa during the motion even though the sum of the two energies remains constant. This is observed by selecting the potential energy, kinetic energy, and mechanical energy from the graph menu. Sketch all three energy lines on single graph.

Energy vs. Time

image


Now we will use equation (2) together with equation (1) to obtain information about the time dependence of the potential energy.

exercise 6

Reset (Reset) the applet.

  • set the spring constant to k = 80 N /m
  • keep the mass and the amplitude at their default values of m = 1.25 kg and A = 0.20 m
  • play the motion
  • select the potential energy graph from the graph menu

Sketch a graph of the potential energy as function of time. Mark the points where the weight passes the top (T), bottom (B), and equilibrium positions (E).

Potential Energy vs. Time

image

 

The potential energy at the bob's far right and far left positions and the value of the mechanical energy are calculated as follows.

The potential energy of the spring is 0 when the weight is at its equilibrium position. Therefore, at this point, the mechanical energy E is equal to the kinetic energy KE (all the energy at the equilibrium position is in the form of kinetic).

When the weight is either at the top or bottom positions, it is momentarily at rest and therefore its kinetic energy equals zero. At these two positions, all the energy is in the form of potential.

Since E is constant during the motion, the potential energy at the top or bottom is equal to the kinetic energy when the weight is passing its equilibrium position,

PEtop,bottom = E = KEmax (3)

Equation (3) combined with equation (1) for the kinetic energy, is used to derive a general expression for the potential energy at the top or bottom of the motion and for the energy E.

Potential Energy The potential energy of a weighted spring is related to its mass (m) amplitude (A), angular frequency (w).
Expressed as an equation,

image (4)

Quantity

Symbol

SI Unit

potential energy PE J
mass m kg
amplitude A m
angular frequency ω rad/s

exercise 7

Use equation (4) to calculate the values of PEtop,bottom and E for the applet settings in Exercise 6. Verify your answer with the values in the Data box and also with the value of the kinetic energy near the equilibrium point determined in Exercise 4 of the previous section. Note: the latter may not be quite equal to KEmax if you did not stop the motion at the exact equilibrium point.




There is one other useful equation for determining the potential energy at the maximum amplitude. The angular frequency w is related to the spring constant (k) and the mass of the weight (m).

image (5)

Substituting this expression for ω2 into equation (4) gives an expression for the energy in terms of k and A.

image (6)

exercise 8

Substitute the applet settings into equation (6) and check if the resulting value of PEtop,bottom agrees with that obtained in Exercise 7.






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Last Updated: June 16, 2004