# 6.3.1 Damped harmonic oscillator

Starting once again with Newton's second law but including the additional damping force in the equation gives:

## SAQ 10

Where did the term *ω*_{0}^{2} in Equation (5.9) come from?

### Answer

The term *ω*_{0}^{2} comes from rearranging Equation (5.5). This is due to the solution that I identified for the simple (undamped) harmonic oscillator, *x* = *A* cos*ω*_{0}*t*. Remember that *ω*_{0} is the natural angular frequency of the system.

Transposing and writing this expression in differential form I have:

Remember that d*x*/d*t* = *v*, the velocity.

As with the simple harmonic oscillator, we can solve this equation for *x* as a function of *t*. This time there are three solutions and they depend on the values of the constants.

Before you look at these solutions answer the following question.

## SAQ 11

The effect of damping is bound to make the oscillations die away. Imagine holding one end of the spring of a mass-spring system and setting it into oscillation:

(a) What would you expect the influence of a large damping coefficient to be on the rate of decay?

(b) What would you expect the influence of a large mass to be on the rate of decay?

### Answer

(a) A large damping coefficient would imply that the losses are high, so I would expect the oscillations to decay quickly.

(b) A large mass will resist the damping more readily (think of a heavy mass on a spring; it will be less affected by the surrounding air) and so it will tend to reduce the rate of decay.

It is the value of *b/m* that is significant in identifying how the system will behave. In the extreme, where this value is very small (large mass or small damping coefficient) the system will behave like the undamped system described earlier and oscillate indefinitely.

You can see that, in this case, the velocity-dependent term in Equation (5.10) will disappear as *b/m* tends to zero and the equation will be identical to Equation (5.7). On the other hand, if *b/m* is very large then this term will dominate and, as you will see, the system will not oscillate at all.

And now to the three solutions.

**1. The underdamped case**

The underdamped case occurs when *ω*_{0} > *b*/2*m*. As in the previous case, the system oscillates but now, as expected, the amplitude decays. The solution takes the form:

Again, I have ignored the phase term. The more general solution is but an appropriate choice of start time enables me to set *φ* to zero.

The amplitude term *Ae*^{−(b/2m)t} will decay with time; the minus sign in the exponent combined with large values for *t* (as time goes on) ensures this. The rate of decay will depend on the value of *b/m*. If this value is large, then the decay will be rapid. This corresponds to a large damping force or a small mass. See Figure 25(a).

**2. The overdamped case**

The overdamped case occurs when *ω*_{0} < *b*/2*m*. Now the system doesn't oscillate at all; the motion simply dies away. This is characterised by a solution which decays exponentially:

The important thing to notice here is that there are no oscillations; you can see this because there is no cosine term. See Figure 25(b).

**3. The critically damped case**

The critically damped case occurs when *ω*_{0} = *b/*2*m*. The solution has the form:

This is a special case where the displacement goes to zero at the fastest possible rate. Clearly, again, there are no oscillations. You can think of this as the smallest value of *b/m* before the onset of oscillatory behaviour. See Figure 26(c).

As with the solution for the simple harmonic oscillator (SHO), you can check these results by differentiating the solutions above and inserting them into the appropriate places in Equation (5.10).

## SAQ 12

If I want to engineer a damped mass-spring system to have a high natural frequency and a rapid decay rate, what physical properties should I prescribe?

### Answer

There are three physical parameters for which I can choose the properties: the spring constant, the mass and the damping coefficient. The natural period is proportional to so I should choose either a large value for the spring constant or a small mass. On the other hand, the decay rate is inversely proportional to *b*/*m*. So I need either a small damping coefficient or a large mass. In practice, choosing which of the above to alter will depend on the options that I have available.