# Trigonometric Functions

*The integrals which we have obtained are not only general expressions which satisfy the differential equation, they represent in the most distinct manner the natural effect which is the object of the phenomenon…when this condition is fulfilled, the integral is, properly speaking, the equation of the phenomenon; it expresses clearly the character and progress of it, in the same manner as the finite equation of a line or curved surface makes known all the properties of those forms.*(Fourier)*God does not care about our mathematical difficulties. He integrates empirically.*(Einstein)

# Defining Differential Equation

The *trigonometric functions* and are elementary functions defined by the solution of the IVP of a *harmonic oscillator:*

- ,

as and . These functions can be extended to as solutions to the same differential equations for .

The trigonometric functions and .

# Properties of Trigonometric Functions

By definition, we have

- .

Further, we have with and ,

- ,

showing that is constant in time, and since , we have for all

- . (1)

# Geometric Interpretation

We shall now give an interpretation of and in the plane with the usual Cartesian coordinate system .

If we write and , then the defining differential equation is written

- ,

from which follows with that

- ,

which means that the *velocity vector* is perpendicular to the vector connecting the origin with the point $x$.

Recalling from (1) that

- (2)

it follows that as varies, the point moves along a unit circle centered at the origin with unit speed, as illustrated in the following picture:

We can thus choose time to be a measure of the angle, from the horisontal.

# Pythagoras Theorem

Note that we can interpret (1) and (2) as Pythagoras Theorem. We have thus given a proof of Pythagoras theorem which is different from that suggested in Fig. \ref{figpytahagorasthm} based on similarity.

# Measuring Angles in Radians

We have seen that are the coordinates of a point moving counterclockwise on the unit circle with unit velocity starting at for . Let us denote by the smallest $t$ for which and .

By periodicity it follows that for the point will be back to and thus the length of the circumference of a unit circle is equal to . If we agree to measure the angle formed by the line from the origin to the point by , which represents the length of the circle arc from to , then we measure the angle in the unit of *radians*. One revolution will then correspond to radians. In other words radians, or

- .

We shall see below that the choice of in fact covers the general case (since a general vetoer of length 1 can be rotated to by an orthogonal transformation which does not change the scalar product).

# Angle vs Scalar Product

Let and be two points in the plane with corresponding vectors (or arrows) from the origin also denoted by and . Since

- ,

where is the angle in radians between and . This formula extends to any two vectors $x$ and $y$:

- ,

where is the angle between the vectors.

# Table of Values

# Read More

- \hyperref[pythagoras]{Pythagoras.}
- \hyperref[trig]{Trigonometric functions.}
- \hyperref[geomR2]{Geometry in $\bbR^2$.}
- \hyperref[chaptercomplexnumbers]{Complex numbers.}

# To Think About

- How are trigonomteric functions defined in standard Calculus texts?

Archimedes computed the value of by inscribing and circumscribing polygons (octagons) toa circle. What value did he obtain?

# Complex Numbers

We define with the imaginary unit satisfying . We compute

- ,

and thus find that is the solution to the IVP

- for all real with .

We have thus defined the exponential function for all imaginary numbers . The rules for the usual exponential extend to :

- ,

for real numbers a,b and c.

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