From a Periodic Pattern to a Rate Model
A periodic quantity repeats its pattern after a fixed amount of time. Examples include the height of a point on a rotating wheel, a tide level, or a temperature that rises and falls in a regular cycle. A sinusoidal function is a useful model when the quantity oscillates smoothly around a typical level.
Building the model requires more than recognizing a wave shape. The baseline tells us the central level, the amplitude tells us the size of the oscillation, the period tells us how long one cycle takes, and the phase tells us where in the cycle the pattern begins. Once these features are specified, differentiation gives the instantaneous rate of change and indicates whether the quantity is rising or falling.
The amplitude is a distance from the midline, so it is positive. If the largest and smallest modeled values are \(y_{\max}\) and \(y_{\min}\), then $$ C=\frac{y_{\max}+y_{\min}}{2}, \qquad A=\frac{y_{\max}-y_{\min}}{2}. $$ These formulas apply when the maximum and minimum describe the same repeating cycle and the model oscillates symmetrically about its midline.
Choosing the Phase and Frequency
The factor \(2\pi/T\) is the angular frequency, commonly written \(\omega\). A full cycle corresponds to an increase of \(2\pi\) in the sine’s angle. Since the cycle takes time \(T\), the angle must increase at a rate of \(2\pi/T\) radians per unit time: $$ \omega=\frac{2\pi}{T}. $$ Thus the model can also be written \(y(t)=C+A\sin(\omega(t-h))\).
In this sine form, \(t=h\) is a rising crossing of the midline: the angle is zero, the sine is zero, and immediately after \(h\) the sine increases. A cosine form is often more convenient when a maximum or minimum time is known. Since cosine equals \(1\) at angle zero, a maximum at time \(t_{\max}\) can be represented by $$ y(t)=C+A\cos\left(\frac{2\pi}{T}(t-t_{\max})\right). $$ Both forms describe the same type of periodic pattern; the choice is made to match the phase information clearly.
Why Differentiation Gives the Rate
The derivative \(y'(t)\) is the instantaneous rate of change of \(y\) with respect to \(t\). Applying the chain rule to the sine model differentiates both the sine and its time-dependent angle. The derivative of \(\sin(u)\) is \(\cos(u)u'\), and here \(u=\frac{2\pi}{T}(t-h)\) has derivative \(2\pi/T\).
The constant baseline contributes no rate because its derivative is zero. The amplitude scales the rate, and the factor \(2\pi/T\) comes from the changing angle. Since cosine ranges from \(-1\) to \(1\), the rate lies between \(-2\pi A/T\) and \(2\pi A/T\). It is zero at a maximum or minimum of the modeled quantity, and its magnitude is largest at a midline crossing.
Use the maximum and minimum, if known, to calculate \(C\) and \(A\).
For period \(T\), set \(\omega=2\pi/T\), keeping the time unit consistent.
Use a rising midline crossing for the sine form or a maximum time for the cosine form.
Include the chain-rule factor, evaluate at the requested time, and report the rate with its sign and units.
Worked Models and Rates
Worked Example: A Rising Midline Crossing Is Known
A point moves vertically between \(4\) cm and \(16\) cm in a repeating motion with period \(8\) seconds. It crosses its midline while rising at \(t=2\) seconds. Build a model and find its rate at \(t=2\), \(t=4\), and \(t=6\).
First calculate the baseline and amplitude: $$ C=\frac{16+4}{2}=10\text{ cm}, \qquad A=\frac{16-4}{2}=6\text{ cm}. $$ The angular frequency is $$ \omega=\frac{2\pi}{8}=\frac{\pi}{4}\text{ radians per second}. $$ The rising midline crossing sets \(h=2\), so the model is $$ y(t)=10+6\sin\left(\frac{\pi}{4}(t-2)\right)\text{ cm}. $$
Differentiate, retaining the factor \(\pi/4\) from the angle: $$ y'(t)=6\left(\frac{\pi}{4}\right)\cos\left(\frac{\pi}{4}(t-2)\right) =\frac{3\pi}{2}\cos\left(\frac{\pi}{4}(t-2)\right)\text{ cm/s}. $$ At \(t=2\), the angle is \(\frac{\pi}{4}(2-2)=0\), so \(y'(2)=\frac{3\pi}{2}\cos(0)=\frac{3\pi}{2}\text{ cm/s}\). The positive sign means the point is rising. At \(t=4\), the angle is \(\frac{\pi}{4}(4-2)=\frac{\pi}{2}\), so \(y'(4)=\frac{3\pi}{2}\cos(\pi/2)=0\text{ cm/s}\). At \(t=6\), the angle is \(\frac{\pi}{4}(6-2)=\pi\), so \(y'(6)=\frac{3\pi}{2}\cos(\pi)=-\frac{3\pi}{2}\text{ cm/s}\); the point is falling.
Check the model’s values at those times. The angles are \(0,\pi/2,\pi\), giving \(y(2)=10\) cm, \(y(4)=16\) cm, and \(y(6)=10\) cm. Thus \(t=4\) is a maximum, where the rate is zero, and the motion has changed from rising to falling, consistent with the calculated rates.
Worked Example: A Maximum Time Determines the Phase
A water level varies between \(14\) m and \(26\) m, has a period of \(12\) hours, and reaches a maximum at \(t=1\) hour. Construct a cosine model and find the rate at \(t=4\) hours.
The baseline and amplitude are $$ C=\frac{26+14}{2}=20\text{ m}, \qquad A=\frac{26-14}{2}=6\text{ m}. $$ The angular frequency is $$ \omega=\frac{2\pi}{12}=\frac{\pi}{6}\text{ radians per hour}. $$ Because the maximum occurs at \(t=1\), use that time as the cosine phase shift: $$ y(t)=20+6\cos\left(\frac{\pi}{6}(t-1)\right)\text{ m}. $$
Differentiating gives $$ y'(t)=-6\left(\frac{\pi}{6}\right)\sin\left(\frac{\pi}{6}(t-1)\right) =-\pi\sin\left(\frac{\pi}{6}(t-1)\right)\text{ m/h}. $$ At \(t=4\), the angle is \(\frac{\pi}{6}(4-1)=\pi/2\). Therefore, $$ y'(4)=-\pi\sin(\pi/2)=-\pi\text{ m/h}. $$ The negative sign indicates that the level is falling. As a check, the level at \(t=4\) is \(y(4)=20+6\cos(\pi/2)=20\) m, the midline. Three hours after the maximum is one quarter of the 12-hour period, so a descending midline crossing and a negative rate are consistent. Also, differentiating the displayed model gives \(-\pi\sin\left(\frac{\pi}{6}(t-1)\right)\), as used in the calculation.
Worked Example: A Falling Midline Crossing Determines the Phase
A signal has baseline \(30\) units, amplitude \(8\) units, and period \(20\) minutes. It crosses the midline while falling at \(t=5\) minutes. Find a sine model and the rate at that crossing.
The angular frequency is $$ \omega=\frac{2\pi}{20}=\frac{\pi}{10}\text{ radians per minute}. $$ For a sine model, a falling midline crossing occurs when the angle is \(-\pi\) (equivalently, \(\pi\)). Set the angle at \(t=5\) to \(-\pi\): $$ \frac{\pi}{10}(5-h)=-\pi. $$ Dividing by \(\pi/10\) gives \(5-h=-10\), so \(h=15\). The model is therefore $$ y(t)=30+8\sin\left(\frac{\pi}{10}(t-15)\right). $$
Differentiate: $$ y'(t)=8\left(\frac{\pi}{10}\right)\cos\left(\frac{\pi}{10}(t-15)\right) =\frac{4\pi}{5}\cos\left(\frac{\pi}{10}(t-15)\right)\text{ units/min}. $$ At \(t=5\), the angle is \(\frac{\pi}{10}(5-15)=-\pi\), so $$ y'(5)=\frac{4\pi}{5}\cos(-\pi)=-\frac{4\pi}{5}\text{ units/min}. $$ The model value at the crossing is \(y(5)=30+8\sin(-\pi)=30\), exactly the baseline. The negative rate confirms that it is a falling crossing. Differentiating the model gives the rate formula above, and substituting the crossing time produces the stated result.
A Common Frequency and Phase Mistake
A period \(T\) is measured in units of time; it is not the angular frequency. The correct conversion is \(\omega=2\pi/T\). For example, if \(T=8\) seconds, then \(\omega=2\pi/8=\pi/4\) radians per second. Using \(2\pi T=16\pi\) as the frequency reverses the role of period and frequency and gives an angle that changes far too quickly.
In the first example, that incorrect choice would produce the model \(10+6\sin(16\pi(t-2))\). Its proposed rate at \(t=2\) would be \(96\pi\text{ cm/s}\), because differentiating multiplies by \(6(16\pi)\). The correct model gives \(3\pi/2\text{ cm/s}\). The correction is to divide \(2\pi\) by the period, not multiply by it.
Phase also needs attention. A rising midline crossing and a falling midline crossing are different events. In the sine form, \(h\) marks the rising crossing specifically; it should not be set equal to the time of a falling crossing. Instead, choose the angle for the observed event, such as \(-\pi\) for a falling crossing, and solve for the phase shift.
Interpreting the Rate in Context
A derivative is not just another number from the formula. Its sign describes direction: positive means the modeled quantity is increasing, and negative means it is decreasing. A zero rate at a maximum or minimum indicates an instantaneous turning point in the sinusoidal model. At a midline crossing, the rate has its greatest magnitude, \(2\pi A/T\), because the cosine factor is \(1\) or \(-1\).
Units provide an additional check. If \(y\) is measured in metres and \(t\) in hours, then \(y'(t)\) is measured in metres per hour. The angular frequency has units of radians per hour, with radians treated as a dimensionless angle in the derivative formula. Always attach the rate units and state what the sign means in the situation.
Check Your Understanding
Use the model and rate ideas to answer each question. Keep track of phase and units.
- A periodic quantity ranges from \(3\) to \(11\) units. What are its baseline and amplitude?
- A model has period \(10\) seconds. What is its angular frequency?
- For \(y(t)=5+3\sin\left(\frac{\pi}{4}(t-1)\right)\), find \(y'(t)\), including the units if \(y\) is in metres and \(t\) in seconds.
- In the sine convention used here, what kind of crossing does \(h\) represent?
- Why should the rate at a smooth maximum of a sinusoidal model be zero?