Trigonometric Identities

Every time your phone tidies up a noisy call, a music app strips the hiss from a track, or an engineer tames the current humming through the power grid, trig identities are quietly at work — folding tangled combinations of waves into something simple enough to handle. They all start from one short, surprising fact.

Here is a small miracle. Pick any angle you like — 17^\circ, 90^\circ, 1000^\circ, a random number your calculator spits out. Square its sine, square its cosine, add them. You will always get exactly 1. Not roughly, not usually — always, forever, for every angle that has ever existed.

\sin^2\theta + \cos^2\theta = 1

A statement like this — true for every value of the variable — is called an identity. It's a different beast from an ordinary equation. When you meet 2x = 6 you solve it for the one value that works (x = 3). An identity needs no solving: it is a permanent, always-true fact, and that makes it a tool. Wherever a messy \sin^2\theta + \cos^2\theta appears, you may simply cross it out and write 1. The two workhorses of the whole subject are the one above and its partner,

\tan\theta = \frac{\sin\theta}{\cos\theta}.

Get comfortable with these two and you can bend almost any trig expression into a friendlier shape.

Sine and cosine live on the unit circle

Where does \sin^2\theta + \cos^2\theta = 1 come from? Draw a circle of radius 1 — the unit circle — centred at the origin. A point P on the circle at angle \theta (measured from the positive x-axis) has coordinates

P = (\cos\theta,\ \sin\theta).

That point sits exactly distance 1 from the centre. Drop a vertical line from P to the x-axis and you get a right-angled triangle with horizontal side \cos\theta, vertical side \sin\theta, and hypotenuse 1. Now Pythagoras on that triangle gives

(\cos\theta)^2 + (\sin\theta)^2 = 1^2,

which is our identity, written the way mathematicians prefer: \sin^2\theta + \cos^2\theta = 1. It really is just Pythagoras' theorem wearing a disguise.

See it on the unit circle

Step through the figure: a radius to P, then the right triangle whose sides are \cos\theta and \sin\theta with hypotenuse 1. The Pythagorean identity is the last line to appear — because it is the triangle.

Tangent is just their ratio

Tangent isn't a third mystery to memorise — it's sine divided by cosine:

\tan\theta = \frac{\sin\theta}{\cos\theta}.

And because the Pythagorean identity ties \sin\theta and \cos\theta together, all three ratios belong to one family: give me any one of them (and a quadrant) and I can hand you the other two. That single-family idea is what makes the identities so powerful — they are rearrangements of the same fact. The most useful rearrangements to keep in your pocket:

\sin^2\theta = 1 - \cos^2\theta, \qquad \cos^2\theta = 1 - \sin^2\theta.

Worked example 1 — simplify an expression

Simplify \dfrac{\sin^2\theta}{1 - \cos^2\theta}.

Look at the denominator. By the rearranged identity, 1 - \cos^2\theta = \sin^2\theta. Swap it in:

\frac{\sin^2\theta}{1 - \cos^2\theta} = \frac{\sin^2\theta}{\sin^2\theta} = 1.

A frightening-looking fraction collapses to the number 1 — no calculator, no angle, just the identity. That collapse is exactly what engineers exploit to tame the trig inside wave and circuit equations.

Worked example 2 — prove an identity

Prove that \tan\theta\,\cos\theta = \sin\theta. The golden rule of proving an identity: start with one side and manipulate it until it turns into the other. Never shove terms across the \equiv sign as if you were solving — you'd be assuming the very thing you're trying to prove.

Take the left-hand side and replace \tan\theta with its definition:

\tan\theta\,\cos\theta = \frac{\sin\theta}{\cos\theta}\cdot\cos\theta = \sin\theta.

The \cos\theta cancels, we land on the right-hand side, and the proof is done. One side in, the other side out.

Worked example 3 — find a missing ratio

Given \sin\theta = \tfrac{3}{5} with \theta acute, find \cos\theta and \tan\theta.

Use the Pythagorean identity rearranged for \cos^2\theta:

\cos^2\theta = 1 - \sin^2\theta = 1 - \left(\tfrac{3}{5}\right)^2 = 1 - \tfrac{9}{25} = \tfrac{16}{25}.

So \cos\theta = \tfrac{4}{5} (positive, because \theta is acute — take the + root). Then tangent falls straight out of the ratio:

\tan\theta = \frac{\sin\theta}{\cos\theta} = \frac{3/5}{4/5} = \frac{3}{4}.

The classic 3-4-5 triangle, recovered from a single ratio using nothing but the identities.

Three traps that quietly cost real marks:

Because \sin^2\theta + \cos^2\theta = 1 is a seed. Divide every term by \cos^2\theta and out pops \tan^2\theta + 1 = \sec^2\theta; divide instead by \sin^2\theta and you get 1 + \cot^2\theta = \csc^2\theta. Combine it with the angle-addition formulas and you can unfold double-angle identities, half-angle identities, and the rules that turn a sum of waves into a product.

That last trick matters more than it looks. Engineers who work on alternating current, radio signals, and audio processing live inside sums of sines and cosines. The identities are what let them fold a tangled sum of oscillations into a single clean wave — turning an expression nobody could solve into one that falls open in a couple of lines. A single sentence of Pythagoras, quietly running the modern world.

See it explained