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.
- \sin^2\theta + \cos^2\theta = 1 — the Pythagorean identity;
- \tan\theta = \dfrac{\sin\theta}{\cos\theta};
- rearranged: \sin^2\theta = 1 - \cos^2\theta and
\cos^2\theta = 1 - \sin^2\theta;
- so given any one ratio you can find the others.
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:
-
\sin^2\theta means (\sin\theta)^2
— the sine, then squared. It is not \sin(\theta^2) (the sine of
the angle squared). The little index sits up by the "sin" purely to avoid the ugly brackets of
(\sin\theta)^2. Read it as "sine-squared", and never feed
\theta^2 into your calculator.
-
An identity is not an equation. An identity (write it with
\equiv) is true for all \theta and
needs no solving. An equation like \sin\theta = 0.5 is true only for
special values, which you go and find — that's the whole job of
solving trig equations.
-
When proving, work one side only. Massage the left-hand side (or the right) until
it becomes the other. Don't "add \cos^2\theta to both sides" or move
terms across — that treats an unproven claim as if it were already true.
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