# 6. Composite Trigonometric Curves

by M. Bourne

## a. Adding trigonometric and other functions

When adding 2 or more trigonometric graphs, we **add ordinates** (*y*-values) to find the
resultant curve.

### Later, on this page...

See the interactive spring activity below for an example of composite trigonometric curves.### Example 1: Electronics

One of the simplest examples of composite trigonometric curves is from electronics. An AC (alternating current) signal (*v* = 3 cos 8*t*) is added to a `10` volt DC (direct current) voltage source. The resulting signal looks like the following.

Graph of `v=10+3cos 8t`, the sum of a DC and an AC voltage.

The combined graph that you see has equation: *v* = 10 + 3 cos 8*t*.

We are simply adding `10` to all the *v*-values of the cosine curve.

### Example 2

Water waves

When two water waves meet on a pond, they combine such that when 2 crests meet, they are added to give a larger crest, and when 2 troughs meet, they add to give a deeper trough. A crest and a trough tend to cancel each other out when they meet.

In this example, let's assume the following 2 waves meet.

`a(x) = 5 sin x`

`b(x) = 4 cos(2x + π/3) `

### Need Graph Paper?

Sketch the graph of the combined wave:

`y=5 sin(x)+4 cos(2x+pi/3)`

Continues below ⇩

### Example 3: Double springs interactive graph

We have two springs with different thicknesses (and spring constants) with two different sized masses connected and hanging vertically. While holding the top mass still, we pull down the bottom mass. Then we let go of both masses and allow the system to move freely.

We can also grab the mass in the middle to compress or stretch the top spring.

In a real experiment, we'd have a motion sensor connected to a computer and we would be able to see the resulting movement of the masses as time progresses, just as you can in this simulation.

(You need to "reset" the whole thing to drag the maases again.)

Copyright © www.intmath.com Frame rate: 0

Stretch (or compress) either of the springs by dragging either of the masses, then let go to see the resulting waveforms. Such waveforms are the result of adding different trigonometric curves.

**Notes: **

- Our springs are constrained to move in one dimension only.
- The springs slow down as time goes on, due to friction.
- You can see other spring examples in Graphs of y = a sin bx and y = a cos bx, and in the section on Work by a Variable Force, which is an application of Calculus.

Depending on the masses, the lengths of the springs and the spring constants, we could get a curve similar to the following (for one or the other mass positions), which is the **sum** of two cosine
curves:

x= 0.0572 cos(4.667t) + 0.0218 cos(12.22t)

Graph of `x=0.0572 cos(4.667t) + 0.0218 cos(12.22t)`, a composite trigonometric model of a double spring system.

[The function *x*(*t*) given above is obtained
using differential equations, an interesting
topic which we meet later in the calculus section**.**]

**Reference:** Morland, T "Modeling a Simple
Mechanical System", Teaching Mathematics and Its Applications,
Vol 18 No 2 1999.

### Exercises

1. Graph the composite trigonometric curve `y = x^2/10 − sin\ πx`

2. Graph the curve *y *= 2 cos 2*x *+ 3 sin *x*

### Example 4: Real-world Case

Atmospheric carbon dioxide levels have been rapidly increasing since the beginning of the industrial revolution.

This chart using data from the National Oceanographic and Atmospheric Administration shows the increase in CO2 since records began in 1958, on Mauna Loa in Hawaii. The dark green line is yearly averages, while the magenta (pink) line gives weekly readings (the data start in 1974), that go up and down with the seasons.

### Atmospheric CO_{2} at Mauna Loa Observatory

CO_{2} concentrations - weekly data with yearly averages.

[Latest data: 04 Feb 2018]

We can closely model the (pink) weekly curve as the sum of a cosine and cubic curve as follows:

y= 3.07 cos(2πx− 1.2) + 0.00002052590807(x− 1958)^{3}+ 0.01105601542(x− 1958)^{2}+ 0.8044611048(x− 1958) + 314.634017

(For more background and information on where this model came from, see Earth killer - composite trigonometry CO2 graph.)

Here is the graph of the model. It is similar to what we had in Exercise 1 above.

### Example 5: Standing wave

We have two sine curves with the same period and amplitude, moving left to right (they gray curve) and right to left (the magenta curve). The **sum** of those two curves is a **standing wave**, one that doesn't move left-right, but is stationary, and at its full extent, has twice the amplitude of the gray and magenta sine curves.

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The **dots** along the *x*-axis are called **nodes**, where there is no movement of the particles making up the waves.

## b. Composite Trigonometric Graphs - Product of Functions

The following examples show composite trigonometric graphs where we are taking the **product** of two functions.

### Example 6: Graph the function *y* = *x* sin *x*

In this example, we are multiplying the sine of each *x*-value by the *x*-value.

So for example, if `x = 2`, the *y*-value will be `y = 2 sin 2 = 1.819`.

### Example 7: RCL Circuit - Constant Forced Response

In electronics, an RCL circuit has a resistor, a capacitor and an inductor connected in series. If we apply a constant voltage to the circuit, there is an initial pulse in the current. The resulting function is a product of an exponential decay function and a sin function.

i=e^{-0.3t}sint

The graph of the current at time *t* has the following appearance. The current reduces quickly after the initial pulse.

Graph of `i=e^(-0.3t)sin(t)`, a composite trigonometric curve of an RLC circuit response.

We learn how to solve these problems later in Applications of Second Order Differential Equations.

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