What if there is no angle?
The tide at a harbour does not turn through an angle. Neither do the hours of daylight or the number of snowshoe hares in a forest. Yet all of them rise and fall in smooth cycles. Can sine and cosine still describe them? Yes. The trick is to let the input be time, and to use k to turn time into degrees.
Time in, degrees inside
In a model such as h = a cos(k(t − d)) + c, the variable t is a time (seconds, hours, days, years). The calculator still needs degrees inside the cosine. That is the job of k:
k = 360 ÷ period
When t increases by one full period, k(t − d) increases by exactly 360°, so the cosine completes exactly one cycle. For example, tides with a period of 12.4 h use k = 360 ÷ 12.4 ≈ 29.0: the inside of the function grows by about 29° for every hour.
For a Ferris wheel, k(t − d) really is the angle the wheel has turned. For tides or daylight it is not a real angle at all; it is just a clock that runs from 0° to 360° once per cycle. That is why sinusoidal functions can model so many things that do not involve angles.
Tides
At many Canadian harbours there are two high tides and two low tides a day, and the time from one high tide to the next is about 12.4 hours (12 h 25 min). The Bay of Fundy, between New Brunswick and Nova Scotia, is famous for having some of the largest tides on Earth.
Hands-on activityPredict your paper-plate Ferris wheel
You need: the paper-plate Ferris wheel from the first lesson of this unit (or make a new one: a paper plate pinned through its centre to cardboard taped upright), a ruler and a calculator.
- Measure the plate's radius r and the height H of the pin above the counter.
- Let n be the number of eighth-turns from the bottom. One full turn is 8 eighth-turns, so k = 360 ÷ 8 = 45. Write the model h = −r cos(45n) + H.
- Predict the height of the dot after n = 3 and after n = 5 eighth-turns.
- Turn the plate and measure those heights. How close were your predictions?
- Rewrite the model for a rider who boards at the top instead.
What to look for: with r = 11 cm and H = 15 cm, h = −11 cos(45n) + 15 predicts 15 + 11(0.707) ≈ 22.8 cm for both n = 3 and n = 5 (they are mirror positions). Measurements within a few millimetres mean the model works. A rider who boards at the top has h = r cos(45n) + H.