y=sinx is the y-coordinate of the point at angle x, measured in radians, on the unit circle. As the angle grows the point travels around the circle and its height rises and falls; stretching that motion out along the horizontal axis traces this sine curve1.
Domain and range
The domain is all real numbers. Since the value is the height of a point on the unit circle, −1≤sinx≤1, so the range is the interval [−1,1].
The domain is all real numbers
The range is −1≤y≤1
The maximum is 1 and the minimum is −1
The amplitude is 1 and the period is 2π
Periodicity
Going once around the circle returns the point to where it started, so sin(x+2π)=sinx. The period is 2π, and the same wave repeats endlessly in both directions.
Symmetry
Since sin(−x)=−sinx, it is an odd function whose graph has point symmetry about the origin.
Monotonicity and extrema
The derivative is y′=cosx, so the function increases where cosx>0 and decreases where cosx<0. It attains its maximum 1 at x=2π+2nπ and its minimum −1 at x=23π+2nπ.
The second derivative y′′=−sinx changes sign at every zero x=nπ, so the inflection points sit at x=nπ, where the tangent has slope ±1. Zeros and inflection points coincide because the function satisfies y′′=−y.
Notable values
x
sinx
0
0
6π
21
4π
22
3π
23
2π
1
π
0
The zeros are the solutions of sinx=0, namely x=nπ for integer n, evenly spaced π apart.
Approximation near the origin
The tangent at the origin is the line y=x, of slope 1, which reflects the following limit.
x→0limxsinx=1
This is why sinx≈x for small angles. The Taylor series converges for every real number.
sinx=x−3!x3+5!x5−⋯
That only odd powers appear is how oddness shows up on the side of the series.
The cycle of derivatives
Times differentiated
Derivative
1
cosx
2
−sinx
3
−cosx
4
sinx
Four steps bring it back to the start.
Relationships with other functions
Since cosx=sin(x+2π), the cosine is this wave shifted left by 2π. The identity sin2x+cos2x=1 is just the equation of the unit circle. In Euler's formula eix=cosx+isinx, the sine supplies the imaginary part.
Applications
Simple harmonic motion, such as a spring or a pendulum
Waves of sound, light and radio
Alternating current and voltage
The basic wave of Fourier analysis
Fourier analysis goes further: any periodic wave can be written as a superposition of sine waves2. The sine curve is the basic shape of anything that repeats.