Trigonometry and phase: turning rotation into a wave
Connect the unit circle to sine, cosine, frequency, and relative timing.
On this page
The question for today
What you’ll understand
- Interpret sine and cosine as coordinates on a unit circle.
- Convert between period, frequency, and angular frequency.
- Explain how amplitude and phase change a sinusoidal signal.
Imagine a dot moving around a circle at a steady angular rate. Its horizontal shadow moves back and forth, slowing near each extreme and moving fastest through the center. That shadow is a cosine wave. This geometric connection gives meaning to a formula that otherwise looks like a collection of constants. It prepares you to read sound waves, electrical signals, Fourier components, and the phases of quantum amplitudes without treating them as unrelated tricks.
Angles measure a fraction of a turn
An angle in radians is arc length divided by circle radius. The ratio is dimensionless, and a complete turn corresponds to radians. Measuring angles this way is natural for calculus because the arc length on a unit circle equals the angle numerically. Degrees remain useful for communication, but formulas involving derivatives of sine and cosine assume radians unless an explicit conversion factor is included.
On a circle of radius one, cosine is the horizontal coordinate and sine the vertical coordinate. Negative values represent points on the opposite side of an axis; they are not negative distances from the origin. The circle equation constrains the coordinates. Knowing one coordinate does not always determine the angle, because points in different quadrants can share a sine or cosine value.
Amplitude, period, and phase answer different questions
Amplitude sets the size of an excursion away from the central value. A period is the time needed for a complete repeat, and frequency counts repeats per unit time. Angular frequency counts radians of rotation per unit time. Keeping these concepts separate prevents a common factor-of- error. High amplitude does not imply high frequency, and neither alone specifies a wave's initial position in its cycle.
Phase specifies that position within a cycle. A phase offset shifts the pattern relative to the chosen time origin. Only relative phase matters when comparing two oscillations measured with the same clock. Adding to a phase gives the same sine or cosine, so different numerical angles can describe the same cycle position. For positive angular frequency, a positive offset in cosine moves a given peak earlier in time.
Adding waves depends on relative timing
Two equal signals in phase add to twice the amplitude at every instant. If their phases differ by , one is the negative of the other and their sum is zero. Cancellation describes the sum at the same location and time under a linear addition rule. It does not mean either source disappears or that energy accounting can be ignored in a physical interference experiment.
A sinusoid is an ideal building block. Real signals can contain many frequencies, changing amplitudes, noise, or abrupt transitions. A single frequency model is still useful when an experiment is close to periodic or when a complicated signal is decomposed into components. Before interpreting a wave picture, ask which axis is time and whether the animation represents a point's oscillation or a pattern traveling through space.
Work it through
Read a complete oscillation model
A displacement is millimeters with t in seconds. Find its amplitude, period, and displacement at the starting time.
Read the coefficient outside cosine: maximum displacement magnitude is 3 mm. The negative minimum is −3 mm; amplitude itself is nonnegative.
Angular frequency is radians per second. Divide by to obtain a period of 0.5 s, giving frequency 2 Hz.
At t = 0 the angle is , whose cosine is zero. Zero starting displacement is consistent with nonzero amplitude because phase chooses where motion begins.
Amplitude is 3 mm, period 0.5 s, frequency 2 Hz, and initial displacement 0 mm.
The living notebook
Explore the model
Interactive lab · waves
Compare two phases
The lab adds to . The controls set relative amplitude a and phase difference in degrees; playback advances the common time. Choose equal amplitudes, then compare zero and 180° phase difference. This dimensionless model illustrates linear interference without simulating a particular material.
- Sum at x = 0
- 0.866
- Resultant amplitude
- 1.732
- Phase difference
- 60°
Two waves share the same frequency and wave number. Playback advances t in sin(2x − t) + a sin(2x − t + phase). Parameter changes pause playback and recompute the model at the current elapsed time. Reset restores both parameters and returns time to zero. Playback starts paused. Adjust either parameter, then choose Play or Step.
Look forRelative phase determines reinforcement or cancellation; amplitude ratio determines whether cancellation can be complete.
Pause & reason
Check your understanding
Your turn
Try it yourself
Write a cosine signal with amplitude 2, period 4 s, and a maximum at t = 0. Find its value at t = 1 s.
Take a moment to make a prediction or work it out on paper. Open a hint when you need one.
Give me a hint
Set phase to zero and use .
Compare with the solution
Angular frequency is radians per second, so one model is . At one second its angle is , giving zero. One second is a quarter of the period, consistent with moving from a cosine maximum to its next zero crossing.
Keep the idea
Take it with you
- Sine and cosine are coordinates of rotation.
- Angular frequency is 2π times frequency in cycles per unit time.
- Relative phase determines whether equal-frequency components reinforce or cancel.
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