Making Connections: Damped Oscillator

Example 16.8 Damping an Oscillatory Motion: Friction on an Object Connected to a Spring

Damping oscillatory motion is important in many systems, and the ability to control the damping is even more so. This is generally attained using non-conservative forces such as the friction between surfaces, and viscosity for objects moving through fluids. The following example considers friction. Suppose a 0.200-kg object is connected to a spring as shown in Figure 16.24, but there is simple friction between the object and the surface, and the coefficient of friction ${\mu }_k$ is equal to 0.0800. (a) What is the frictional force between the surfaces? (b) What total distance does the object travel if it is released 0.100 m from equilibrium, starting at $v=0$? The force constant of the spring is $k\text{ = 50 N/m}\text{.}$

Figure 16.24 The transformation of energy in simple harmonic motion is illustrated for an object attached to a spring on a frictionless surface.

Strategy

This problem requires you to integrate your knowledge of various concepts regarding waves, oscillations, and damping. To solve an integrated concept problem, you must first identify the physical principles involved. Part (a) is about the frictional force. This is a topic involving the application of Newton’s Laws. Part (b) requires an understanding of work and conservation of energy, as well as some understanding of horizontal oscillatory systems.

Now that we have identified the principles we must apply in order to solve the problems, we need to identify the knowns and unknowns for each part of the question, as well as the quantity that is constant in Part (a) and Part (b) of the question.

Solution a

1. Choose the proper equation: Friction is $f={\mu }_{\mathrm{k}}\text{mg}$.
2. Identify the known values.
3. Enter the known values into the equation
   16.58 $$f=\text{(0.0800)}\mathrm{(0}\text{.200 kg)}\mathrm{(9}\text{.80 m}/{\text{s}}^{\text{2}}\text{)}.$$
4. Calculate and convert units: $f=\text{0.157 N}.$

Discussion a

The force here is small because the system and the coefficients are small.

Solution b

Identify the known:

• The system involves elastic potential energy as the spring compresses and expands, friction that is related to the work done, and the kinetic energy as the body speeds up and slows down.
• Energy is not conserved as the mass oscillates because friction is a non-conservative force.
• The motion is horizontal, so gravitational potential energy does not need to be considered.
• Because the motion starts from rest, the energy in the system is initially ${\text{PE}}_{\mathrm{el,i}}=(1/2){\text{kX}}^2$. This energy is removed by work done by friction $W_{\text{nc}}=–\text{fd}$, where $d$ is the total distance traveled and $f={\mu }_{\text{k}}\text{mg}$ is the force of friction. When the system stops moving, the friction force will balance the force exerted by the spring, so ${\text{PE}}_{\text{e1,f}}=(1/2){\text{kx}}^2$ where $x$ is the final position and is given by
  16.59 $$\begin{array}{lll}{F}_{\text{el}}& =& f\\ \text{kx}& =& {\mu }_{\text{k}}\text{mg}\\ x& =& \frac{{\mu }_{\text{k}}\text{mg}}{k}\text{.}\end{array}$$

1. By equating the work done to the energy removed, solve for the distance $d$ .
2. The work done by the non-conservative forces equals the initial, stored elastic potential energy. Identify the correct equation to use.
   16.60 $${\text{W}}_{\text{nc}}=\Delta \left(\text{KE}+\text{PE}\right)={\text{PE}}_{\text{el,f}}-{\text{PE}}_{\text{el,i}}=\frac{1}{2}k\left({\left(\frac{{\mu }_{\mathrm{k}}\mathit{\text{mg}}}{k}\right)}^2-X^2\right).$$
3. Recall that $W_{\text{nc}}=–\text{fd}$.
4. Enter the friction as $f={\mu }_{\text{k}}\text{mg}$ into $W_{\text{nc}}=–\text{fd}$, thus
   16.61 $$W_{\text{nc}}={–\mu }_{\text{k}}\text{mgd}.$$
5. Combine these two equations to find
   16.62 $$\frac{1}{2}k\left({\left(\frac{{\mu }_k\text{mg}}{k}\right)}^2-X^2\right)=-{\mu }_{\text{k}}\text{mgd}.$$
6. Solve the equation for $\mathrm{d.}$
   16.63 $$d=\frac{\text{k}}{{\text{2}\mu }_{\text{k}}\text{mg}}(X^2–{\left(\frac{{\mu }_{\text{k}}\text{mg}}{k}\right)}^2).$$
7. Enter the known values into the resulting equation
   16.64 $$d=\frac{\text{50}\text{.}\mathrm{0\; N/m}}{2\left(0\text{.}\text{0800}\right)\left(0\text{.}\text{200}\text{kg}\right)\left(9\text{.}\text{80}{\text{m/s}}^2\right)}\left({\left(0\text{.}\text{100}\text{m}\right)}^2-{\left(\frac{\left(0\text{.}\text{0800}\right)\left(0\text{.}\text{200}\text{kg}\right)\left(9\text{.}\text{80}{\text{m/s}}^2\right)}{\text{50}\text{.}0\text{N/m}}\right)}^2\right).$$
8. Calculate $d$ and convert units.
   16.65 $$d=1\text{.}\text{59}\text{m}.$$

Discussion b

This is the total distance traveled back and forth across $x=0$, which is the undamped equilibrium position. The number of oscillations about the equilibrium position will be more than $d/X=(1\text{.}\text{59}\text{m})/(0\text{.}\text{100}\text{m})=\text{15}\text{.}9$ because the amplitude of the oscillations is decreasing with time. At the end of the motion, this system will not return to $x=0$ for this type of damping force, because static friction will exceed the restoring force. This system is underdamped. In contrast, an overdamped system with a simple constant damping force would not cross the equilibrium position $x=0$ a single time. For example, if this system had a damping force 20 times greater, it would only move 0.0484 m toward the equilibrium position from its original 0.100-m position.

This worked example illustrates how to apply problem-solving strategies to situations that integrate the different concepts you have learned. The first step is to identify the physical principles involved in the problem. The second step is to solve for the unknowns using familiar problem-solving strategies. These are found throughout the text, and many worked examples show how to use them for single topics. In this integrated concepts example, you can see how to apply them across several topics. You will find these techniques useful in applications of physics outside a physics course, such as in your profession, in other science disciplines, and in everyday life.