#### Arbitrary angles and the unit circle

We’ve used the unit circle to define the trigonometric functions for acute angles so far. We’ll need more than acute angles in the next section where we’ll look at oblique triangles. Some oblique triangles are obtuse and we’ll need to know the sine and cosine of obtuse angles. As long as we’re doing that, we should also define the trig functions for angles beyond 180° and for negative angles. First we need to be clear about what such angles are.The ancient Greek geometers only considered angles between 0° and 180°, and they considered neither the straight angle of 180° nor the degenerate angle of 0° to be angles. It’s not only useful to consider those special cases to be angles, but also to include angles between 180° and 360°, too, sometimes called “reflex angles.” With the applications of trigonometry to the subjects of calculus and differential equations, angles beyond 360° and negative angles became accepted, too.

Consider the unit circle. Denote its center (0,0) as *O,* and denote the point (1,0) on it as *A.* As a moving point *B* travels around the unit circle starting at *A* and moving in a counterclockwise direction, the angle *AOB* as a 0° angle and increases. When *B* has made it all the way around the circle and back to *A,* then angle *AOB* is a 360° angle. Of course, this is the same angle as a 0° angle, so we can identify these two angles. As *B* continues the second time around the circle, we get angles ranging from 360° to 720°. They’re the same angles we saw the first time around, but we have different names for them. For instance, a right angle is named as either 90° or 450°. Each time around the circle, we get another name for the angle. So 90°, 450°, 810° and 1170° all name the same angle.

If *B* starts at the same point *A* and travels in the clockwise direction, then we’ll get negative angles, or more precisely, names in negative degrees for the same angles. For instance, if you go a quarter of a circle in the clockwise direction, the angle *AOB* is named as –90°. Of course, it’s the same as a 270° angle.

So, in summary, any angle is named by infinitely many names, but they all differ by multiples of 360° from each other.

#### Sines and cosines of arbitrary angles

Now that we have specified arbitrary angles, we can define their sines and cosines. Let the angle be placed so that its vertex is at the center of the unit circle*O*=(0,0), and let the first side of the angle be placed along the

*x*-axis. Let the second side of the angle intersect the unit circle at

*B.*Then the angle equals the angle

*AOB*where

*A*is (1,0). We use the coordinates of

*B*to define the cosine of the angle and the sine of the angle. Specifically, the

*x*-coordinate of

*B*is the cosine of the angle, and the

*y*-coordinate of

*B*is the sine of the angle.

#### Properties of sines and cosines that follow from this definition

There are several properties that we can easily derive from this definition. Some of them generalize identities that we have seen already for acute angles.- Sine and cosine are periodic functions of period 360°, that is, of period 2
*π*. That’s because sines and cosines are defined in terms of angles, and you can add multiples of 360°, or 2*π*, and it doesn’t change the angle. Thus, for any angle*θ*,sin( *θ*+360°)=sin*θ,*andcos(

*θ*+360°)=cos*θ.*Many of the modern applications of trigonometry follow from the uses of trig to calculus, especially those applications which deal directly with trigonometric functions. So, we should use radian measure when thinking of trig in terms of trig functions. In radian measure that last pair of equations read as

sin( *θ*+2*π*)=sin*θ,*andcos(

*θ*+2*π*)=cos*θ.* - Sine and cosine are complementary:
cos *θ*=sin(*π*/2–*θ*)sin

*θ*=cos(*π*/2–*θ*)We’ve seen this before, but now we have it for any angle

*θ.*It’s true because when you reflect the plane across the diagonal line*y=x,*an angle is exchanged for its complement. - The Pythagorean identity for sines and cosines follows directly from the definition. Since the point
*B*lies on the unit circle, its coordinates*x*and*y*satisfy the equation*x*^{2}+*y*^{2}=1. But the coordinates are the cosine and sine, so we concludesin ^{2}*θ*+ cos^{2}*θ*=1.We’re now ready to look at sine and cosine as functions.

- Sine is an odd function, and cosine is an even function. You may not have come across these adjectives “odd” and “even” when applied to functions, but it’s important to know them. A function
*f*is said to be an*odd*function if for any number*x,**f*(–*x*)=–*f*(*x*). A function*f*is said to be an*even*function if for any number*x,**f*(–*x*)=*f*(*x*). Most functions are neither odd nor even functions, but some of the most important functions are one or the other. Any polynomial with only odd degree terms is an odd function, for example,*f*(*x*)=*x*^{5}+8*x*^{3}–2*x.*(Note that all the powers of*x*are odd numbers.) Similarly, any polynomial with only even degree terms is an even function. For example,*f*(*x*)=*x*^{4}–3*x*^{2}–5. (The constant 5 is 5*x*^{0}, and 0 is an even number.)Sine is an odd function, and cosine is even

sin(– *θ*)=–sin*θ,*andcos(–

*θ*)=cos*θ.*These facts follow from the symmetry of the unit circle across the

*x*-axis. The angle –*t*is the same angle as*t*except it’s on the other side of the*x*-axis. Flipping a point (*x,y*) to the other side of the*x*-axis makes it into (*x,–y*), so the*y*-coordinate is negated, that is, the sine is negated, but the*x*-coordinate remains the same, that is, the cosine is unchanged. - An obvious property of sines and cosines is that their values lie between –1 and 1. Every point on the unit circle is 1 unit from the origin, so the coordinates of any point are within 1 of 0 as well.

#### The graphs of the sine and cosine functions

Let’s use*t*as a variable angle. You can think of

*t*as both an angle as as time. A good way for human beings to understand a function is to look at its graph. Let’s start with the graph of sin

*t.*Take the horizontal axis to be the

*t*-axis (rather than the

*x*-axis as usual), take the vertical axis to be the

*y*-axis, and graph the equation

*y*=sin

*t.*It looks like this.

First, note that it is periodic of period 2*π*. Geometrically, that means that if you take the curve and slide it 2*π* either left or right, then the curve falls back on itself. Second, note that the graph is within one unit of the *t*-axis. Not much else is obvious, except where it increases and decreases. For instance, sin*t* grows from 0 to *π*/2 since the *y*-coordinate of the point *B* increases as the angle *AOB* increases from 0 to *π*/2.

Next, let’s look at the graph of cosine. Again, take the horizontal axis to be the *t*-axis, but now take the vertical axis to be the *x*-axis, and graph the equation *x*=cos*t.*

Note that it looks just like the graph of sin*t* except it’s translated to the left by *π*/2. That’s because of the identity cos*t*=sin(*π*/2+*t*). Although we haven’t come across this identity before, it easily follows from ones that we have seen: cos*t*=cos–*t*=sin(*π*/2–(–*t*))=sin(*π*/2+*t*).

#### The graphs of the tangent and cotangent functions

The graph of the tangent function has a vertical asymptote at x=*π*/2. This is because the tangent approaches infinity as

*t*approaches

*π*/2. (Actually, it approaches minus infinity as

*t*approaches

*π*/2 from the right as you can see on the graph.

You can also see that tangent has period *π*; there are also vertical asymptotes every *π* units to the left and right. Algebraically, this periodicity is expressed by tan(*t*+*π*)=tan*t.*

The graph for cotangent is very similar.

This similarity is simply because the cotangent of *t* is the tangent of the complementary angle *π*–*t.*

#### The graphs of the secant and cosecant functions

The secant is the reciprocal of the cosine, and as the cosine only takes values between –1 and 1, therefore the secant only takes values above 1 or below –1, as shown in the graph. Also secant has a period of 2*π*.

As you would expect by now, the graph of the cosecant looks much like the graph of the secant.