Periodicity of Trigonometric Functions

All trigonometric functions are defined in terms of the cosine and sine functions. The cosine and sine functions are characterized as the x and y coordinates of the intersection point P of the terminal side of the angle θ and the unit circle (Figure 1).

Figure 1

Because one revolution corresponds to 2π radians or 360 degrees, the same point P is obtained for θ+2πk where k is an integer. Thus the values of the trigonometric functions repeat when θ increases by 2π. The sine and cosine functions are periodic with period 2π
sin(θ+2π)=sinθ,cos(θ+2π)=cosθ but the tangent and cotangent functions have a smaller period π, because (see Equation 18(c) in Trignometric Identities)
tan(θ+π)=tanθ,cot(θ+π)=cotθ.

We may use the periodicity of trigonometric functions to sketch their graphs. So we can just sketch the graphs of sine and cosine functions for θ between 0 and 2π (or for θ between π and π or in general for θ between a and a+2π for any real number a) and then obtain the graph for all real values of θ by infinitely many repetitions of this cycle, to the right and to the left.

Graph of y = sin 𝜽

To sketch the graph of sinθ, we just need to look at Figure 2 and follow how the y coordinate of the point P varies as θ increases from 0 to 2π and P completes one counterclockwise revolution. We know sin0=0. As θ goes from 0 to π/2, sinθ increases until it reaches +1 at θ=π/2. As θ goes from π/2 to π, sinθ decreases until reaches 0 at θ=π. When θ is between π to 3π/2, sinθ is negative and keep decreasing until it reaches 1 at θ=3π/2. Finally as θ goes from 3π/2 to 2π, sinθ increases from 1 to 0 and will be ready to start all over again.

Figure 2: Graph of y=sinθ in one period

The complete graph y=sinθ consists of infinitely many repetitions of one cycle just shown (Figure 3).

Figure 3: Graph of y=sinθ. Domain=(,), range =[1,1], period=2π

  •  Note that y=sinθ is an odd function (that is, sin(θ)=sinθ),and thus its graph is symmetric about the origin.

Graph of y = cos 𝜽

We can graph y=cosθ essentially the same way. The main difference is cos0=1 and cosθ decreases until it becomes cosπ2=0 and finally it reaches 1 at θ=π. At this point, cosθ starts to increase until it becomes cos3π2=0 and then cos2π=1 (Figure 4(a)), and it will start all over again (Figure 4(b)).

(a) (b)Domain =(,), range=[1,1],
period=2π

Figure 4: Graph of y=cosθ (a) in one cycle (b) in several cycles

Another way of drawing the graph of y=cosθ is by shifting the graph of y=sinθ to the left π/2 units (Figure 5) because cosθ=sin(θ+π2) (see Equation 17(a) in Trigonometric Identites). As we can see in Figure 5:

  • The sine and cosine functions are defined for all values of θ and their range is {y|1y1}=[1,1].
  • The sine function takes on 0 at x=0,±π,±2π,±3π,.
  • The cosine function takes on 0 at x=±π2,±3π2,±5π2,±7π2,
Figure 5: Graph of y=cosθ is obtained by shifting the graph of y=sinθ to the left π/2 units.

Note that y=cosθ is an even function (that is, cos(θ)=cosθ), and thus its graph is symmetric about the y-axis.

Graph of y = tan 𝜽

Now let’s sketch the graph of y=tanθ. We discussed that the period of this function is π, so we can plot it in one period and find the complete graph by repeating what we obtain in one interval. For example, we can take the interval
π2<θ<π2. Note that tanθ=sinθ/cosθ is not defined for θ=±π/2 because because cos(±π/2)=0 and division by zero is not defined. We know tan0=0. When π2<θ<0 (that is when θ is in the fourth quadrant), tanθ<0 and when 0<θ<π2, tanθ>0. As θ increases toward π/2, tanθ is positive and becomes indefinitely great, while as θ decreases toward π2, tanθ is negative and becomes indefinitely great. You can also see this in Figure 6(a).

  •  The domain of y=tanθ is the set of all θ-values such that
    θ(2k+1)π2,k is an integer.
  • As we can see in Figure 6, the range of y=tanθ is the entire set of real numbers R or (,).
  • To graph trigonometric functions in the coordinate plane, as usual, we often denote the independent variable by x. So we often talk about the graphs of y=sinx,y=cosx, y=tanx, etc.
(a) (b) Domain ={θ| θ(2k+1)π2, kZ}

Figure 6: (a) Graph of y=tanθ in one period π2<θ<π2. (b) The complete graph of y=tanθ.


Examples

Example 1
Given the graph of y=tanx, use transformations to graph y=cotx, and then determine its domain and its range.
Solution
We know
tan(π2x)=cotx. So we start with the graph of y=tanx (Figure 7(a)). Then we can plot the graph of y=f(x), where
f(x)=tan(x), by reflecting the graph of y=tanx in the y-axis (Figure 7(b)). Now we can get the graph of y=f(x+π/2)=tan(x+π/2)=cotx by shifting the graph of f to the left π/2 units (Figure 7(c)). As we can see cotx is defined for all x-values such that
x0,±π,±2π,±3π, or
Dom(cotx)={x| xkπ,kZ} and its range is
{y| <y<} or the entire set of real numbers R.
(a) Graph of y=tanx (b) Graph of y=f(x)=tan(x) (c) Graph of y=f(x+π/2)=cotx

Figure 7: Sketching graph of y=cotx by transforming the graph of y=tanx.

Example 2
Use the graph of y=sinx to plot y=3sin2x.
Solution
Recall that to obtain the graph of y=f(cx) for c>1, we horizontally compress the graph of y=f(x) by a fractor of 1/c. Thus here we horizontally compress the graph of y=sinx by a factor of 1/2 to obtain the graph of y=sin2x (Figure 8(a)). Then we vertically scale it by a fractor of 3, to get the graph of y=3sin2x (Figure 8(b)). We see that when x is a multiple of π/2, y=0 and when x is an odd multiple of π/4, y=3 or y=3. For all other values of x, 3<y<3.

(a) (b)

Figure 8