Explore This 2 Summary
In the Explore This activity, you may have noticed that when the physical features of Windmill B changed compared to Windmill A, the properties of the function measuring the height of a blade’s tip over time changed as well.
For example, if you made Windmill B’s tower taller, then the amplitude, period, and phase shift all remained the same, but the function’s axis translated vertically upward.
The table below summarizes the results of changing Windmill B’s tower height, blade length, location of a point on the path of rotation, and the speed of rotation, as compared with Windmill A.
Physical Feature of Windmill B
as Compared With Windmill A |
|
Function
Property
|
Increase
Tower Height
|
Increase
Blade Length
|
Move Point on
Path of Rotation
|
Increase
Speed of Rotation
|
 |
 |
 |
 |
 |
|
Amplitude
|
same |
larger |
same |
same |
|
Period
|
same |
same |
same |
shorter time |
|
Phase Shift
|
max at
\(t = 0\)
|
max at
\(t = 0\)
|
max at
\(t \ne 0\)
|
max at
\(t = 0\)
|
|
Axis
|
higher
|
same
|
same
|
same
|
Example 3
- Windmill A spins at \(5\) seconds per revolution, has a tower height of \(100\) m, and \(40\) m long blades. Determine an equation to model the height of a blade tip starting at the maximum height.
- Windmill B spins at \(3\) seconds per revolution, but its other features are identical to Windmill A. Determine an equation to model the height of a blade tip starting at the maximum height.
Solution — Part A
Since the equation will model the height starting at the maximum, using a cosine function will not require a phase shift or any reflections. We will use the physical features of the windmill to determine the value of the parameters of
\[h\left(t\right)=a\cos\left(bt\right)+k\]
where the independent variable \(t\) represents the time in seconds after the initial maximum and the dependent variable \(h\left(t\right)\) represents the height of the blade tip in metres.
The windmill spins \(5\) seconds per revolution so \(b=\dfrac{360}{5}=72\).
Since the tower height is \(100\) m, then \(k=100\).
The blades are \(40\) m long, so \(a=40\).
Therefore, the height of a blade tip starting at the maximum can be modelled by \(h\left(t\right)=40\cos\left(72t\right)+100,t\ge0\).
Solution — Part B
The speed of rotation for Windmill B is \(3\) seconds per revolution, so \(b=\dfrac{360}{3}=120\).
Since Windmill A and B are identical otherwise, the other parameters will be the same, \(a=40\), \(h=0\), and \(k=100\).
The height of a blade tip of Windmill B starting at the maximum can be modelled by \(h\left(t\right)=40\cos\left(120t\right)+100,t\ge0\).
Example 4
The depth of the water in a harbour is \(11.3\) metres at high tide and \(2.7\) metres at low tide. The time between consecutive high tides is \(12\) hours. Write an equation to model the depth of the water in metres as a function of time in hours after high tide.
Solution
Let \(t\) represent the time in hours after high tide and \(d\left(t\right)\) represent the depth of the water in metres.
We could use a sine or a cosine function for the base function. We are modelling the depth of the water after high tide, which is a maximum, so using a cosine function would not require a phase shift, \(h=0\), or any reflections, \(a,b\gt0\).
The amplitude of the function is \(a=\dfrac{11.3-2.7}{2}=4.3\).
The period is \(12\) hours, so \(b=\dfrac{360}{12}=30\).
The average depth of the water is \(\dfrac{11.3+2.7}{2}=7\), so \(k=7\).
The depth of the water in the harbour can be estimated by the function \(d\left(t\right)=4.3\cos\left(30t\right)+7\).
Example 5
A mass attached to a spring oscillates up and down \(5\) times in \(24\) s. When the mass is at its lowest position, the spring is \(6.8\) cm long; when the mass is at its highest position, the spring is \(4.0\) cm long.
- Write an equation to model the length of the spring, in cm, as a function of time, in s, after the mass reaches its lowest position.
- Sketch at least two cycles of this function.

Svjo. (2013, April 22). Animation of a mass and spring, an example of an undamped harmonic oscillator. Retrieved from https://commons.wikimedia.org/wiki/File:Animated-mass-spring.gif and licensed under CC BY-SA 3.0
Solution — Part A
Let \(t\) represent the time in seconds after the mass reaches its lowest position and \(L\left(t\right)\) represent the length of the spring in cm.
We are modelling the length of the spring after the lowest mass position, which is a minimum, so using a cosine function with a reflection in the \(x\)-axis, \(a\lt0\), would not require a phase shift, \(h=0\).
The spring oscillates up and down \(5\) times in \(24\) s so the period is \(24\div5=4.8\) s. Therefore,
\(b=\dfrac{360}{4.8}=75\)
The maximum length of the spring is \(6.8\) cm and the minimum length is \(4.0\) cm. The amplitude is \(\dfrac{6.8-4.0}{2}=1.4\), and, since \(a\lt0\), \(a=-1.4\). We can also calculate the average spring length,
\(k=\dfrac{6.8+4.0}{2}=5.4\)
A model equation for the length of the spring is \(L\left(t\right)=-1.4\cos\left(75t\right)+5.4,~t\ge0\).
Solution — Part B
The graph of the spring's length over time is as follows:

Math in Action
A mass suspended by a spring exhibits simple harmonic motion. The period of oscillation \(T\) depends on the suspended mass \(m\) and the stiffness of the spring, identified by a spring constant \(k\). This relation is described by the equation
\[T=2\pi\sqrt{\dfrac mk}\]