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714 A p p e n d i x A : U s e f u l M a t h<br />

+15<br />

x (feet)<br />

0<br />

5 10 15 20<br />

time<br />

(seconds)<br />

–15<br />

Figure A.3.3 Horizontal position of Ferris wheel chair versus elapsed time.<br />

smoothly drawn curve, suddenly you’ll have a duplicate of Fig. A.3.1—a sine wave, in<br />

other words!<br />

How can this be? You know, from having watched your friends take many rides,<br />

that once the ride has started, the Ferris wheel rotates at a constant rate. Yet your shadow<br />

has obviously moved along the ground beneath the Ferris wheel at a varying rate.<br />

What’s going on here?<br />

The answer is this: The shadow on the ground was an exact replica of how the<br />

horizontal position of your chair varied with time. You, of course, were moving vertically<br />

as well as horizontally, so what you saw when your eyes followed the car your<br />

friends were in was a result of their total motion, but what your friend saw when he<br />

watched the shadow of your car intently was just the horizontal component of your<br />

total motion.<br />

Now, it turns out that if you had ridden the Ferris wheel at night and we had shone<br />

a very bright light at the Ferris wheel from the side and marked a utility pole or other<br />

post on the opposite side of the wheel with the same white stripes as before, with y = 0<br />

marked at the midheight of your travel, your friend could collect the same kind of data<br />

about your vertical motion. If we use the same time intervals and the same exact starting<br />

time as before, that curve will look like Figure A.3.4. Note that while it, too, is a sine<br />

wave, it “starts” at a different time than the first one. Specifically, when your horizontal<br />

position was halfway between the left and right extremes of travel (the first or leftmost<br />

data point in Fig. A.3.3), your vertical position was at the very bottom or the very top of<br />

its range.<br />

For reasons we don’t need to discuss right now, we call the curve of Fig. A.3.1 or Fig.<br />

A.3.3 a sine curve or a sine function, and we call the curve of Fig. A.3.4 a cosine curve or a<br />

cosine function. (This particular cosine function is negative—that is, since we assumed<br />

the Ferris wheel rotation started when your chair went past the loading gate, the cosine<br />

function is starting at y = -15.) But both are sine waves or sinusoidal functions. When we<br />

travel a complete circle, or one complete rotation, we say we have gone through 360<br />

degrees (often written 360°), just as there are 360 degrees on a compass. Thus, each of<br />

our sine waves repeats every 360 degrees, and the sinusoidal wave of your vertical position<br />

lags the sinusoidal wave of your horizontal position by a quarter rotation, or 90<br />

degrees. We say these two waves are in quadrature with respect to each other.

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