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Note: 1–2 lectures, §10.3 in [EP], not in [BD]

#### 5.3.1Forced vibrating string.

Suppose that we have a guitar string of length . We have studied the wave equation problem in this case, where was the position on the string, was time and was the displacement of the string. See Figure 5.3.

The problem is governed by the equations

 (5.6)

We saw previously that the solution is of the form

where and were determined by the initial conditions. The natural frequencies of the system are the (circular) frequencies for integers .

But these are free vibrations. What if there is an external force acting on the string. Let us assume say air vibrations (noise), for example a second string. Or perhaps a jet engine. For simplicity, assume nice pure sound and assume the force is uniform at every position on the string. Let us say as force per unit mass. Then our wave equation becomes (remember force is mass times acceleration)

 (5.7)

with the same boundary conditions of course.

We want to ﬁnd the solution here that satisﬁes the above equation and

 (5.8)

That is, the string is initially at rest. First we ﬁnd a particular solution of (5.7) that satisﬁes . We deﬁne the functions and as

We then ﬁnd solution of (5.6). If we add the two solutions, we ﬁnd that solves (5.7) with the initial conditions.

Exercise 5.3.1: Check that solves (5.7) and the side conditions (5.8).

So the big issue here is to ﬁnd the particular solution . We look at the equation and we make an educated guess

We plug in to get

or after canceling the cosine. We know how to ﬁnd a general solution to this equation (it is a nonhomogeneous constant coeﬃcient equation). The general solution is

The endpoint conditions imply . So

or , and also

Assuming that is not zero we can solve for to get

 (5.9)

Therefore,

The particular solution we are looking for is

Exercise 5.3.2: Check that works.

Now we get to the point that we skipped. Suppose that . What this means is that is equal to one of the natural frequencies of the system, i.e. a multiple of . We notice that if is not equal to a multiple of the base frequency, but is very close, then the coeﬃcient in (5.9) seems to become very large. But let us not jump to conclusions just yet. When for even, then and hence we really get that . So resonance occurs only when both and . That is when for odd .

We could again solve for the resonance solution if we wanted to, but it is, in the right sense, the limit of the solutions as gets close to a resonance frequency. In real life, pure resonance never occurs anyway.

The above calculation explains why a string will begin to vibrate if the identical string is plucked close by. In the absence of friction this vibration would get louder and louder as time goes on. On the other hand, you are unlikely to get large vibration if the forcing frequency is not close to a resonance frequency even if you have a jet engine running close to the string. That is, the amplitude will not keep increasing unless you tune to just the right frequency.

Similar resonance phenomena occur when you break a wine glass using human voice (yes this is possible, but not easy2) if you happen to hit just the right frequency. Remember a glass has much purer sound, i.e. it is more like a vibraphone, so there are far fewer resonance frequencies to hit.

When the forcing function is more complicated, you decompose it in terms of the Fourier series and apply the above result. You may also need to solve the above problem if the forcing function is a sine rather than a cosine, but if you think about it, the solution is almost the same.

Example 5.3.1: Let us do the computation for speciﬁc values. Suppose and and and . Then

Write for simplicity.

Then plug in to get

and after diﬀerentiating in we see that .

Hence to ﬁnd we need to solve the problem

Note that the formula that we use to deﬁne is not odd, hence it is not a simple matter of plugging in to apply the D’Alembert formula directly! You must deﬁne to be the odd, 2-periodic extension of . Then our solution would look like
 (5.10)

It is not hard to compute speciﬁc values for an odd extension of a function and hence (5.10) is a wonderful solution to the problem. For example it is very easy to have a computer do it, unlike a series solution. A plot is given in Figure 5.4.

#### 5.3.2Underground temperature oscillations

Let be the temperature at a certain location at depth underground at time . See Figure 5.5.

Figure 5.5: Underground temperature.

The temperature satisﬁes the heat equation , where is the diﬀusivity of the soil. We know the temperature at the surface from weather records. Let us assume for simplicity that

where is the yearly mean temperature, and is midsummer (you can put negative sign above to make it midwinter if you wish). gives the typical variation for the year. That is, the hottest temperature is and the coldest is . For simplicity, we will assume that . The frequency is picked depending on the units of , such that when , then . For example if is in years, then .

It seems reasonable that the temperature at depth will also oscillate with the same frequency. This, in fact, will be the steady periodic solution, independent of the initial conditions. So we are looking for a solution of the form

for the problem

 (5.11)

We will employ the complex exponential here to make calculations simpler. Suppose we have a complex valued function

We will look for an such that . To ﬁnd an , whose real part satisﬁes (5.11), we look for an such that

 (5.12)

Exercise 5.3.3: Suppose satisﬁes (5.12). Use Euler’s formula for the complex exponential to check that satisﬁes (5.11).

Substitute into (5.12).

Hence,

or

where . Note that so you could simplify to . Hence the general solution is

We assume that an that solves the problem must be bounded as since should be bounded (we are not worrying about the earth core!). If you use Euler’s formula to expand the complex exponentials, you will note that the second term will be unbounded (if ), while the ﬁrst term is always bounded. Hence .

Exercise 5.3.4: Use Euler’s formula to show that is unbounded as , while is bounded as .

Furthermore, since . Thus . This means that

We will need to get the real part of , so we apply Euler’s formula to get

Then ﬁnally

Yay!

Notice the phase is diﬀerent at diﬀerent depths. At depth the phase is delayed by . For example in cgs units (centimeters-grams-seconds) we have (typical value for soil), . Then if we compute where the phase shift we ﬁnd the depth in centimeters where the seasons are reversed. That is, we get the depth at which summer is the coldest and winter is the warmest. We get approximately 700 centimeters, which is approximately 23 feet below ground.

Be careful not to jump to conclusions. The temperature swings decay rapidly as you dig deeper. The amplitude of the temperature swings is . This function decays very quickly as (the depth) grows. Let us again take typical parameters as above. We will also assume that our surface temperature swing is Celsius, that is, . Then the maximum temperature variation at 700 centimeters is only Celsius.

You need not dig very deep to get an eﬀective “refrigerator,” with nearly constant temperature. That is why wines are kept in a cellar; you need consistent temperature. The temperature diﬀerential could also be used for energy. A home could be heated or cooled by taking advantage of the above fact. Even without the earth core you could heat a home in the winter and cool it in the summer. The earth core makes the temperature higher the deeper you dig, although you need to dig somewhat deep to feel a diﬀerence. We did not take that into account above.

#### 5.3.3Exercises

Exercise 5.3.5: Suppose that the forcing function for the vibrating string is . Derive the particular solution .

Exercise 5.3.6: Take the forced vibrating string. Suppose that , . Suppose that the forcing function is the square wave that is 1 on the interval and on the interval . Find the particular solution. Hint: You may want to use result of Exercise 5.3.5.

Exercise 5.3.7: The units are cgs (centimeters-grams-seconds). For , , . Find the depth at which the temperature variation is half ( degrees) of what it is on the surface.

Exercise 5.3.8: Derive the solution for underground temperature oscillation without assuming that .

Exercise 5.3.101: Take the forced vibrating string. Suppose that , . Suppose that the forcing function is a sawtooth, that is on extended periodically. Find the particular solution.

Exercise 5.3.102: The units are cgs (centimeters-grams-seconds). For , , . Find the depth at which the summer is again the hottest point.

2Mythbusters, episode 31, Discovery Channel, originally aired may 18th 2005.