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Double Angle Trigonometric Identities


sin() = 2sin θ · cos θ
θ35°
Bisected apex sceneOABMa = 1b = 1C = θθcos θsin θsin θ
Step 0 of 6

sin(2θ)

0.940

2 sin θ cos θ

0.940

Derivation
Press Play to step through the proof.
Function
Identity
Value
Source







Switching Between Functions

A row of six tabs at the top lets you select which double-angle identity to study: sin(2θ)\sin(2\theta), cos(2θ)\cos(2\theta), tan(2θ)\tan(2\theta), csc(2θ)\csc(2\theta), sec(2θ)\sec(2\theta), cot(2θ)\cot(2\theta).

How selection changes the view:
sin\sin and cos\cos open the geometric proof scene with a step-by-step animation.
tan\tan, csc\csc, sec\sec, and cot\cot open the derived identity card with the algebraic chain.
• The active tab is highlighted in deep blue.
• The URL updates with ?fn=...?fn=..., so links you copy preserve the selected function.

You can also click any row of the formula table at the bottom to jump directly to that function.

Adjusting the Angle θ

Each view exposes a slider for the base angle θ\theta in degrees, between 10°10° and 80°80°.

What changes as you slide:
• On geometric scenes, the SVG triangle resizes and reshapes in real time.
• The number readout next to the slider shows the exact degree value.
• The verification cards at the bottom recompute both sides of the identity using the new θ\theta.

Slow sweeps near 45°45° are useful for seeing how the relationships behave in the most symmetric case, while values near the extremes (10°10° or 80°80°) show how the same identities still hold for narrow and wide triangles.

Playing Through a Geometric Proof

When sin\sin or cos\cos is active, an animated proof unfolds in six steps. A toolbar gives you control:

Reset — return to step 0 with a blank scene.
Prev / Next — step through one stage at a time.
Play / Pause — advance automatically.
Speed selector0.5×0.5\times, 1×1\times, 1.5×1.5\times, or 2×2\times.

Each step adds one geometric element (radii, triangle fill, bisector, half-angles, leg labels, final metrics). The right-hand panel logs each step's name and rationale, so you can stop and re-read at any point.

Reading the Geometric Scene

The SVG shows the unit circle with two radii OAOA and OBOB of length 11 meeting at the center OO with angle 2θ2\theta between them.

Elements that appear across the steps:
Red arc at OO — the apex angle, labeled C=2θC = 2\theta.
Indigo chord ABAB — the base of the isosceles triangle.
Blue segment OMOM — the perpendicular bisector, equal to cosθ\cos\theta.
Half-angles at OO — each labeled θ\theta once the bisector is drawn.
Half-chord labels — each labeled sinθ\sin\theta on segments MAMA and MBMB.

A small right-angle mark appears at MM when the perpendicular bisector becomes visible.

Working with Derived Identities

Selecting tan(2θ)\tan(2\theta), csc(2θ)\csc(2\theta), sec(2θ)\sec(2\theta), or cot(2θ)\cot(2\theta) opens a different card layout. Instead of a triangle, the page shows the algebraic derivation as a chain of equations.

Layout of the derived card:
• A short intro explains which earlier identity the current one rests on.
Jump buttons link directly to the geometric proofs of the source identities.
• A multi-line derivation block shows each manipulation with a brief side note.
• Verification cards confirm both sides match numerically.

This split keeps the geometric ideas isolated to two functions and treats the other four as quick algebraic consequences.

Reading the Formula Table

A reference table beneath every scene lists all six identities at once:

Function column — the name of the trig function with 2θ2\theta argument.
Identity column — the right-hand side of the formula.
Value column — the numeric value computed at the current θ\theta.
Source column — labels each identity as geometric (sin\sin, cos\cos) or via X for derived ones.

Click any row to make that function active. The current selection gets a deep-blue left border and a tinted background, making it easy to track context.

Verifying Identities Numerically

Every scene includes two metric cards near the bottom that compute both sides of the active identity at the current θ\theta.

Example for sin(2θ)\sin(2\theta):
• Left card shows sin(2θ)\sin(2\theta).
• Right card shows 2sinθcosθ2\sin\theta\cos\theta.

The two numbers always match (within rounding to three decimals). Sweeping the slider while watching the cards is a fast empirical check that the identity holds for every angle, not just the one in the picture. The formula table mirrors this behavior across all six functions simultaneously.

Geometric Proofs: sin(2θ) and cos(2θ)

The two foundational identities are proved by drawing an isosceles triangle with two unit radii.

sin(2θ) = 2 sin θ cos θ — area is computed two ways:
area=12sin(2θ)=sinθcosθ\text{area} = \tfrac{1}{2}\sin(2\theta) = \sin\theta\cos\theta

Multiplying by 22 gives the identity.

cos(2θ) = 1 - 2 sin²θ — the law of cosines gives AB2=22cos(2θ)|AB|^2 = 2 - 2\cos(2\theta), while the half-chord computation gives AB2=4sin2θ|AB|^2 = 4\sin^2\theta. Equating the two yields the result.

For full coverage of these proofs and equivalent forms, see the double angle identities theory page.

Derived Identities: tan(2θ), csc(2θ), sec(2θ), cot(2θ)

The four remaining identities follow directly from the first two:

tan(2θ) — from tan=sin/cos\tan = \sin / \cos:
tan(2θ)=2tanθ1tan2θ\tan(2\theta) = \frac{2\tan\theta}{1 - \tan^2\theta}


csc(2θ) — reciprocal of sin(2θ)\sin(2\theta):
csc(2θ)=12sinθcosθ\csc(2\theta) = \frac{1}{2\sin\theta\cos\theta}


sec(2θ) — reciprocal of cos(2θ)\cos(2\theta):
sec(2θ)=112sin2θ\sec(2\theta) = \frac{1}{1 - 2\sin^2\theta}


cot(2θ) — reciprocal of tan(2θ)\tan(2\theta):
cot(2θ)=1tan2θ2tanθ\cot(2\theta) = \frac{1 - \tan^2\theta}{2\tan\theta}


For step-by-step derivations of each, see the trigonometric identities page and the reciprocal identities page.

Why Double-Angle Identities Matter

Double-angle identities show up across mathematics and physics:

Integrationsin2θ\sin^2\theta and cos2θ\cos^2\theta become integrable after substituting cos(2θ)=12sin2θ\cos(2\theta) = 1 - 2\sin^2\theta or 2cos2θ12\cos^2\theta - 1.
Equation solving — equations mixing sinθ\sin\theta with sin(2θ)\sin(2\theta) collapse to single-angle equations after substitution.
Wave physics and signal processing — sums of sinusoids reduce via these formulas, separating frequency components.
Geometry and circular motion — relating arc, chord, and apothem in regular polygons uses sin(2θ)\sin(2\theta) and cos(2θ)\cos(2\theta) directly.

For applications and worked examples, see the trigonometric identities applications page.

The Sine Double-Angle Identity

The identity sin(2θ)=2sinθcosθ\sin(2\theta) = 2\sin\theta\cos\theta is proved geometrically in the explorer by computing the area of one isosceles triangle two different ways.
OAB11Mθθsin θsin θcos θsin 2θ = 2 sin θ cos θ
The complete sine proof, frozen

The area of one isosceles triangle computed two ways: ½ sin 2θ must equal sin θ cos θ.

The proof runs through six stages: setup, area the first way, bisect, read off the legs, area the second way, and equate.

This identity is the source of two others in the tool: cosecant's formula is its reciprocal, and tangent's numerator comes from it.

The Cosine Double-Angle Identity

The identity cos(2θ)=12sin2θ\cos(2\theta) = 1 - 2\sin^2\theta falls out of measuring the chord ABAB two ways — once by the law of cosines, once through the half-chords.
OAB11Mθθsin θsin θcos θcos 2θ = 1 − 2 sin²θ
The complete cosine proof, frozen

The chord AB measured twice — law of cosines against half-chords — forcing cos 2θ = 1 − 2 sin²θ.

The proof's six stages: setup, law of cosines, bisect, read off the half-chord, square the chord, and equate.

Substituting sin2θ=1cos2θ\sin^2\theta = 1 - \cos^2\theta gives the equivalent forms 2cos2θ12\cos^2\theta - 1 and cos2θsin2θ\cos^2\theta - \sin^2\theta. In the tool, secant's identity is this one inverted, and tangent's denominator comes from it.

The Tangent Double-Angle Identity

Tangent needs no new geometry: it is sine over cosine, so its double-angle formula follows algebraically from the two proved identities.
tan(2θ) = 2 tan θ / (1 − tan²θ)tan(2θ) =sin(2θ) / cos(2θ)definition=(2 sin θ · cos θ) / (cos²θ − sin²θ)substitute the two identities=2 tan θ / (1 − tan²θ)divide top and bottom by cos²θ
tan(2θ), derived

Three algebraic lines: sine over cosine, substitute both proved identities, divide through by cos²θ.

tan(2θ)=sin(2θ)cos(2θ)=2sinθcosθcos2θsin2θ=2tanθ1tan2θ\tan(2\theta) = \frac{\sin(2\theta)}{\cos(2\theta)} = \frac{2\sin\theta\cos\theta}{\cos^2\theta - \sin^2\theta} = \frac{2\tan\theta}{1 - \tan^2\theta}


The last step divides numerator and denominator by cos2θ\cos^2\theta — the move that turns a sine-and-cosine expression into a pure tangent one. The formula fails where tanθ=±1\tan\theta = \pm 1 (θ=45°\theta = 45°), exactly where 2θ=90°2\theta = 90° makes tan(2θ)\tan(2\theta) undefined. Its own reciprocal gives cotangent's formula; its ingredients come from sine and cosine.

The Cosecant Double-Angle Identity

Cosecant is the reciprocal of sine, so its double-angle formula is one substitution away from the geometric result.
csc(2θ) = 1 / (2 sin θ · cos θ)csc(2θ) =1 / sin(2θ)definition=1 / (2 sin θ · cos θ)substitute sin(2θ)
csc(2θ), derived

One substitution into the reciprocal: 1 over the sine identity.

csc(2θ)=1sin(2θ)=12sinθcosθ\csc(2\theta) = \frac{1}{\sin(2\theta)} = \frac{1}{2\sin\theta\cos\theta}


The formula is undefined wherever sin(2θ)=0\sin(2\theta) = 0 — within the tool's 10°10°80°80° slider range that never happens, so the verification cards always agree. The source identity is sine's, reachable from the card's jump button.

The Secant Double-Angle Identity

Secant inverts cosine, so the double-angle version inverts the cosine identity.
sec(2θ) = 1 / (1 − 2 sin²θ)sec(2θ) =1 / cos(2θ)definition=1 / (1 − 2 sin²θ)substitute cos(2θ)
sec(2θ), derived

The cosine identity inverted — with poles wherever cos 2θ = 0.

sec(2θ)=1cos(2θ)=112sin2θ\sec(2\theta) = \frac{1}{\cos(2\theta)} = \frac{1}{1 - 2\sin^2\theta}


It diverges where cos(2θ)=0\cos(2\theta) = 0, i.e. at θ=45°\theta = 45° — sweep the slider there and watch both verification cards blow up together, which is itself a check that the two sides agree. The source identity is cosine's.

The Cotangent Double-Angle Identity

Cotangent is the reciprocal of tangent, so its formula is the tangent identity flipped upside down.
cot(2θ) = (1 − tan²θ) / (2 tan θ)cot(2θ) =1 / tan(2θ)definition=(1 − tan²θ) / (2 tan θ)substitute tan(2θ)
cot(2θ), derived

The tangent formula flipped upside down: zeros and poles exchange places.

cot(2θ)=1tan(2θ)=1tan2θ2tanθ\cot(2\theta) = \frac{1}{\tan(2\theta)} = \frac{1 - \tan^2\theta}{2\tan\theta}


Flipping exchanges the roles of the zeros and the poles: cotangent diverges where tangent is zero and vanishes where tangent diverges. Because tangent itself was derived, cotangent sits two steps from the geometry — resting ultimately on sine and cosine.

Sine Proof, Step 1: Setup

The sine proof opens with two radii OAOA and OBOB of length 11 meeting at the center OO with angle 2θ2\theta between them. Together with the chord ABAB they form an isosceles triangle.
OAB11
Step 1: the isosceles setup

Two unit radii meeting at 2θ, joined by the chord AB.

Everything the proof needs is already in this picture: a triangle whose apex angle is the double angle we want, built from sides whose length we know exactly.

Sine Proof, Step 2: Area, First Way

The triangle's area comes from the standard formula: half the product of two sides times the sine of the included angle. With OA=OB=1OA = OB = 1 meeting at 2θ2\theta:
OAB11area = ½ · 1 · 1 · sin 2θ = ½ sin 2θ
Step 2: area, first way

Half the product of the unit sides times sin 2θ shades the whole triangle.

area=1211sin(2θ)=12sin(2θ)\text{area} = \tfrac{1}{2} \cdot 1 \cdot 1 \cdot \sin(2\theta) = \tfrac{1}{2}\sin(2\theta)


This is the left-hand side of the identity in disguise — one honest measurement of the shaded region.

Sine Proof, Step 3: Bisect

Drop OMOM perpendicular to the chord ABAB. Because the triangle is isosceles, OMOM bisects the apex: two half-angles of θ\theta at OO, and two congruent right triangles.
OAB11Mθθ
Step 3: the bisector

OM splits the apex into two θ halves and makes two congruent right triangles.

The small square at MM marks the right angle — the key that unlocks the next step, since right triangles are where sinθ\sin\theta and cosθ\cos\theta live as plain side lengths.

Sine Proof, Step 4: Read Off the Legs

In right triangle OMAOMA the hypotenuse is OA=1OA = 1 and the angle at OO is θ\theta. Its legs are therefore exactly the basic ratios:
OAB11Mθθsin θsin θcos θ
Step 4: legs as ratios

A unit hypotenuse means the legs are literally sin θ and cos θ.

MA=sinθOM=cosθMA = \sin\theta \qquad OM = \cos\theta


No approximation, no extra construction — with a unit hypotenuse, opposite and adjacent legs ARE sine and cosine.

Sine Proof, Step 5: Area, Second Way

Each right triangle has legs sinθ\sin\theta and cosθ\cos\theta, so each has area 12sinθcosθ\tfrac{1}{2}\sin\theta\cos\theta. The two congruent halves together give:
OAB11Mθθsin θsin θcos θeach half: ½ sin θ cos θ — together: sin θ cos θ
Step 5: area, second way

Two congruent halves, each ½ sin θ cos θ — together sin θ cos θ.

area=212sinθcosθ=sinθcosθ\text{area} = 2 \cdot \tfrac{1}{2}\sin\theta\cos\theta = \sin\theta\cos\theta


The same shaded region as step 2, measured a second, independent way.

Sine Proof, Step 6: Equate

Two measurements of one area must agree:
OAB11Mθθsin θsin θcos θsin 2θ = 2 sin θ cos θ
Step 6: equate

The two area measurements meet: sin 2θ = 2 sin θ cos θ.

12sin(2θ)=sinθcosθ        sin(2θ)=2sinθcosθ\tfrac{1}{2}\sin(2\theta) = \sin\theta\cos\theta \;\;\Longrightarrow\;\; \sin(2\theta) = 2\sin\theta\cos\theta


The verification cards below the scene confirm it numerically at every slider position — both sides always match to three decimals.

Cosine Proof, Step 1: Setup

The cosine proof starts from the same figure as sine's: radii OAOA and OBOB of length 11 with apex angle 2θ2\theta at the center.
OAB11
Step 1: same setup, new target

The same unit triangle — but now the chord AB is the thing to measure.

This time the target of the measurement will not be the triangle's area but the length of the chord ABAB.

Cosine Proof, Step 2: Law of Cosines on Triangle OAB

Apply the law of cosines to the triangle, with the apex angle 2θ2\theta between the two unit sides:
OAB11|AB|² = 1 + 1 − 2cos 2θ = 2 − 2cos 2θ
Step 2: law of cosines

|AB|² = 2 − 2 cos 2θ, straight from the apex angle.

AB2=12+12211cos(2θ)=22cos(2θ)|AB|^2 = 1^2 + 1^2 - 2 \cdot 1 \cdot 1 \cdot \cos(2\theta) = 2 - 2\cos(2\theta)


The chord's squared length now contains cos(2θ)\cos(2\theta) — the quantity the proof is hunting.

Cosine Proof, Step 3: Bisect

Drop the perpendicular bisector OMOM: it lands on the midpoint MM of the chord and splits the apex into two half-angles of θ\theta.
OAB11Mθθ
Step 3: the bisector

OM lands on the midpoint M, halving the apex into two θ angles.

Same construction as in the sine proof, used here for a different purpose — to measure the chord instead of the area.

Cosine Proof, Step 4: Read Off the Half-Chord

Right triangle OMAOMA has hypotenuse 11 and angle θ\theta at OO, so the half-chord is MA=sinθMA = \sin\theta — and the full chord is twice that:
OAB11Mθθsin θsin θcos θAB = 2 sin θ
Step 4: the half-chord

MA = sin θ, so the whole chord is 2 sin θ.

AB=2sinθAB = 2\sin\theta


A second, completely independent expression for the same chord the law of cosines measured.

Cosine Proof, Step 5: Square the Chord

Square the half-chord result to match the form of step 2:
OAB11Mθθsin θsin θcos θ|AB|² = (2 sin θ)² = 4 sin²θ
Step 5: square it

(2 sin θ)² = 4 sin²θ — the second expression for |AB|².

AB2=(2sinθ)2=4sin2θ|AB|^2 = (2\sin\theta)^2 = 4\sin^2\theta


Both routes now express AB2|AB|^2 — one through cos(2θ)\cos(2\theta), one through sin2θ\sin^2\theta.

Cosine Proof, Step 6: Equate

Set the two expressions for AB2|AB|^2 equal and solve:
OAB11Mθθsin θsin θcos θcos 2θ = 1 − 2 sin²θ
Step 6: equate

The two chord measurements force cos 2θ = 1 − 2 sin²θ.

22cos(2θ)=4sin2θ        cos(2θ)=12sin2θ2 - 2\cos(2\theta) = 4\sin^2\theta \;\;\Longrightarrow\;\; \cos(2\theta) = 1 - 2\sin^2\theta


As with sine, the verification cards keep both sides in numerical agreement across the whole slider range.