In short

Inverse trigonometric functions satisfy a web of identities that mirror — and sometimes invert — the identities you already know for sine, cosine, and tangent. The most powerful ones are the sum formulas: \tan^{-1} a + \tan^{-1} b = \tan^{-1}\!\frac{a+b}{1-ab} (with a sign correction when ab > 1), and similar formulas for \sin^{-1} and \cos^{-1}. Mastering these turns messy inverse-trig expressions into clean single values.

Take a moment with this expression:

\tan^{-1} 1 + \tan^{-1} 2 + \tan^{-1} 3

Three inverse tangents of three simple integers. What does the sum equal? It is not obvious — \tan^{-1} is not linear, so you cannot just add the arguments. But there is a formula that collapses pairs of \tan^{-1} terms into a single \tan^{-1}, and if you apply it twice, the entire expression simplifies to \pi. Three numbers in, one clean answer out. The formula that does this is the subject of this article.

Before the formulas, though, there is a layer of properties that sits underneath them — relations between the six inverse trig functions themselves. These are simpler, but they are the foundation on which the addition formulas rest.

Relations between inverse functions

Complementary relations

You already know from basic trigonometry that \sin\!\left(\frac{\pi}{2} - \theta\right) = \cos\theta. This means sine and cosine are complementary: one at angle \theta equals the other at \frac{\pi}{2} - \theta.

The same relationship holds for their inverses.

Complementary-pair identities

For all x in [-1, 1]:

\sin^{-1} x + \cos^{-1} x = \frac{\pi}{2}

For all x in \mathbb{R}:

\tan^{-1} x + \cot^{-1} x = \frac{\pi}{2}

For all |x| \geq 1:

\sec^{-1} x + \csc^{-1} x = \frac{\pi}{2}

Proof of the first identity. Let \sin^{-1} x = \alpha. Then \sin\alpha = x, with \alpha \in [-\pi/2, \pi/2]. Since \cos(\pi/2 - \alpha) = \sin\alpha = x, you need to check that \pi/2 - \alpha falls in the principal range of \cos^{-1}, which is [0, \pi]. Since \alpha \in [-\pi/2, \pi/2], the value \pi/2 - \alpha ranges over [0, \pi]. So \cos^{-1} x = \pi/2 - \alpha, giving \sin^{-1} x + \cos^{-1} x = \alpha + (\pi/2 - \alpha) = \pi/2.

The proofs for the other two pairs follow the same pattern — the co-function identity from trigonometry translates directly into a complementary-sum identity for the inverses, as long as the principal-value ranges line up.

Complementary pair: arcsin and arccos always sum to pi over 2A horizontal bar diagram showing that for any x between negative 1 and 1, the angle arcsin x and the angle arccos x together fill a total of pi over 2 radians. The bar is split into two coloured segments whose lengths change with x but always sum to the same total. sin⁻¹ x cos⁻¹ x always = π/2 example: x = 1/2 π/6 π/3 sum = π/2 ✓
No matter what value $x$ takes in $[-1,1]$, the two angles $\sin^{-1} x$ and $\cos^{-1} x$ always add up to exactly $\pi/2$. The split changes, but the total is fixed. For $x = 1/2$: $\pi/6 + \pi/3 = \pi/2$.

Negative-argument identities

What happens when you feed a negative number into an inverse trig function? The answer depends on which function you are using, and it depends on the symmetry (odd or even) of the original function.

\sin^{-1}(-x) = -\sin^{-1} x \qquad \text{(odd function)}
\cos^{-1}(-x) = \pi - \cos^{-1} x
\tan^{-1}(-x) = -\tan^{-1} x \qquad \text{(odd function)}

Why the difference? Sine is an odd function (\sin(-\theta) = -\sin\theta), so its inverse inherits oddness. Cosine is an even function (\cos(-\theta) = \cos\theta), but \cos^{-1} is not even — it compensates through the shift \pi - \cos^{-1} x instead. The geometric reason: the principal branch of \cos^{-1} lives in [0, \pi], which is not symmetric about the origin. When you negate the input, the output reflects about \pi/2, the midpoint of that interval.

Reciprocal-argument identities

For positive x:

\tan^{-1} x + \tan^{-1}\!\frac{1}{x} = \frac{\pi}{2}

Proof. Let \tan^{-1} x = \alpha, so \tan\alpha = x with \alpha \in (0, \pi/2) since x > 0. Then \tan(\pi/2 - \alpha) = \cot\alpha = 1/x. Since \pi/2 - \alpha \in (0, \pi/2), this is the principal value. So \tan^{-1}(1/x) = \pi/2 - \alpha, and the sum is \pi/2.

For negative x, the sum is -\pi/2 instead. Combining both cases:

\tan^{-1} x + \tan^{-1}\!\frac{1}{x} = \begin{cases} \frac{\pi}{2} & \text{if } x > 0 \\ -\frac{\pi}{2} & \text{if } x < 0 \end{cases}

Similarly, \sin^{-1}(1/x) = \csc^{-1} x and \cos^{-1}(1/x) = \sec^{-1} x for |x| \geq 1.

Sum and difference formulas

These are the workhorses. They let you combine two inverse trig values into one.

The \tan^{-1} addition formula

Sum formula for arctan

\tan^{-1} a + \tan^{-1} b = \begin{cases} \tan^{-1}\!\dfrac{a+b}{1-ab} & \text{if } ab < 1 \\[8pt] \pi + \tan^{-1}\!\dfrac{a+b}{1-ab} & \text{if } ab > 1,\; a > 0 \\[8pt] -\pi + \tan^{-1}\!\dfrac{a+b}{1-ab} & \text{if } ab > 1,\; a < 0 \end{cases}

Full derivation. Let \tan^{-1} a = \alpha and \tan^{-1} b = \beta. Then \tan\alpha = a and \tan\beta = b. Apply the tangent addition formula from compound angles:

\tan(\alpha + \beta) = \frac{\tan\alpha + \tan\beta}{1 - \tan\alpha\tan\beta} = \frac{a + b}{1 - ab}

So far, so clean. The temptation is to write \alpha + \beta = \tan^{-1}\!\frac{a+b}{1-ab} and call it done. But there is a subtlety: \tan^{-1} returns values in (-\pi/2, \pi/2), and the sum \alpha + \beta might fall outside that interval.

Since \alpha \in (-\pi/2, \pi/2) and \beta \in (-\pi/2, \pi/2), the sum \alpha + \beta lies in (-\pi, \pi). Three cases arise:

The case ab = 1 makes the denominator zero: \frac{a+b}{1-ab} is undefined, and the sum equals \pm\pi/2 directly.

Three cases of the arctan addition formula shown on a number lineA diagram showing the principal value interval of arctan as a horizontal segment from negative pi over 2 to positive pi over 2. Three arrows show the three cases: when the sum falls inside the interval (no correction), when it overshoots above (add pi), and when it undershoots below (subtract pi). −π/2 0 π/2 principal range of tan⁻¹ Case 1: ab < 1 α + β lands inside — no correction Case 2: ab > 1, a > 0 α + β overshoots π/2 — add π to the raw tan⁻¹ Case 3: ab > 1, a < 0 α + β undershoots −π/2 — subtract π
The three cases of the $\tan^{-1}$ addition formula arise from whether $\alpha + \beta$ falls inside or outside the principal range $(-\pi/2, \pi/2)$. When $ab < 1$, the sum stays inside. When $ab > 1$, the tangent function's periodicity causes the raw $\tan^{-1}$ to land in the wrong period, and a correction of $\pm\pi$ is needed.

The difference formula follows immediately by replacing b with -b:

\tan^{-1} a - \tan^{-1} b = \tan^{-1}\!\frac{a - b}{1 + ab} \qquad \text{(when } ab > -1\text{)}

The \sin^{-1} addition formula

\sin^{-1} a + \sin^{-1} b = \sin^{-1}\!\left(a\sqrt{1 - b^2} + b\sqrt{1 - a^2}\right)

valid when a^2 + b^2 \leq 1 (or when a, b \geq 0 and a^2 + b^2 \leq 1). Outside this range, a correction of \pi or -\pi applies, similar to the \tan^{-1} case.

Derivation. Let \sin^{-1} a = \alpha and \sin^{-1} b = \beta. Then \sin\alpha = a, \cos\alpha = \sqrt{1 - a^2} (non-negative because \alpha \in [-\pi/2, \pi/2]), and similarly \cos\beta = \sqrt{1 - b^2}. Now use the sine addition formula:

\sin(\alpha + \beta) = \sin\alpha\cos\beta + \cos\alpha\sin\beta = a\sqrt{1 - b^2} + b\sqrt{1 - a^2}

When \alpha + \beta stays in [-\pi/2, \pi/2], you can apply \sin^{-1} to both sides directly.

The \cos^{-1} addition formula

\cos^{-1} a + \cos^{-1} b = \cos^{-1}\!\left(ab - \sqrt{1 - a^2}\sqrt{1 - b^2}\right) \qquad \text{when } a + b \geq 0

Derivation. Let \cos^{-1} a = \alpha, \cos^{-1} b = \beta. Then \cos\alpha = a, \sin\alpha = \sqrt{1 - a^2} (non-negative because \alpha \in [0, \pi]). Apply the cosine addition formula:

\cos(\alpha + \beta) = \cos\alpha\cos\beta - \sin\alpha\sin\beta = ab - \sqrt{1 - a^2}\sqrt{1 - b^2}

When \alpha + \beta \in [0, \pi], apply \cos^{-1} to both sides. The condition a + b \geq 0 ensures this. When a + b < 0, the sum exceeds \pi, and you write \cos^{-1} a + \cos^{-1} b = 2\pi - \cos^{-1}(ab - \sqrt{1-a^2}\sqrt{1-b^2}).

Multiple angle formulas

These express 2\tan^{-1} x, 3\tan^{-1} x, and similar multiples as a single inverse trig value.

Double-angle formula for \tan^{-1}

Setting a = b = x in the addition formula:

2\tan^{-1} x = \tan^{-1}\!\frac{2x}{1 - x^2} \qquad \text{for } |x| < 1

This is the inverse-trig version of \tan 2\theta = \frac{2\tan\theta}{1 - \tan^2\theta}.

There are two alternative forms using \sin^{-1} and \cos^{-1}:

2\tan^{-1} x = \sin^{-1}\!\frac{2x}{1 + x^2} \qquad \text{for } |x| \leq 1
2\tan^{-1} x = \cos^{-1}\!\frac{1 - x^2}{1 + x^2} \qquad \text{for } x \geq 0

Proof of the \sin^{-1} form. Let \tan^{-1} x = \theta, so \tan\theta = x. Then:

\sin 2\theta = \frac{2\tan\theta}{1 + \tan^2\theta} = \frac{2x}{1 + x^2}

Since |x| \leq 1 implies |\theta| \leq \pi/4, the angle 2\theta lies in [-\pi/2, \pi/2], the principal range of \sin^{-1}. So 2\theta = \sin^{-1}\!\frac{2x}{1+x^2}.

Proof of the \cos^{-1} form. Similarly:

\cos 2\theta = \frac{1 - \tan^2\theta}{1 + \tan^2\theta} = \frac{1 - x^2}{1 + x^2}

For x \geq 0, we have \theta \in [0, \pi/2), so 2\theta \in [0, \pi), which sits inside the principal range of \cos^{-1}. Hence 2\theta = \cos^{-1}\!\frac{1 - x^2}{1 + x^2}.

Three equivalent forms of 2 arctan xA diagram showing three boxes connected by equal signs, representing the three equivalent forms of the double-angle formula: 2 arctan x equals arctan of 2x over 1 minus x squared, equals arcsin of 2x over 1 plus x squared, equals arccos of 1 minus x squared over 1 plus x squared. 2 tan⁻¹ x = tan⁻¹ [2x/(1−x²)] |x| < 1 sin⁻¹ [2x/(1+x²)] |x| ≤ 1 cos⁻¹ [(1−x²)/(1+x²)] x ≥ 0
The three faces of $2\tan^{-1} x$. Each form is useful in different simplification contexts. The $\tan^{-1}$ form comes from the double-angle formula for tangent; the $\sin^{-1}$ and $\cos^{-1}$ forms come from the Weierstrass substitution identities for $\sin 2\theta$ and $\cos 2\theta$ in terms of $\tan\theta$.

Triple-angle formula

Applying the addition formula twice:

3\tan^{-1} x = \tan^{-1}\!\frac{3x - x^3}{1 - 3x^2} \qquad \text{for } |x| < \frac{1}{\sqrt{3}}

This mirrors the identity \tan 3\theta = \frac{3\tan\theta - \tan^3\theta}{1 - 3\tan^2\theta}.

Simplification techniques

The real test of these formulas is using them to simplify complicated expressions. There are a few recurring patterns.

Pattern 1: Recognise a substitution

When you see \tan^{-1}\!\frac{2x}{1 - x^2}, recognise it as 2\tan^{-1} x (for |x| < 1).

When you see \sin^{-1}(2x\sqrt{1 - x^2}), try x = \sin\theta. Then 2x\sqrt{1-x^2} = 2\sin\theta\cos\theta = \sin 2\theta, so the expression becomes \sin^{-1}(\sin 2\theta) = 2\theta = 2\sin^{-1} x (when |x| \leq 1/\sqrt{2}).

Pattern 2: Convert everything to \tan^{-1}

Many problems become easier if you convert \sin^{-1} and \cos^{-1} into \tan^{-1} using right-triangle reasoning.

If \sin^{-1} x = \theta, then \sin\theta = x and \cos\theta = \sqrt{1-x^2}, so \tan\theta = \frac{x}{\sqrt{1-x^2}}, giving:

\sin^{-1} x = \tan^{-1}\!\frac{x}{\sqrt{1 - x^2}}

Similarly:

\cos^{-1} x = \tan^{-1}\!\frac{\sqrt{1 - x^2}}{x} \qquad \text{for } x > 0
Right triangle connecting arcsin x to arctanA right triangle with hypotenuse 1, opposite side x, and adjacent side square root of 1 minus x squared. The angle theta equals arcsin x, and the same angle also equals arctan of x over the square root of 1 minus x squared. √(1 − x²) x 1 θ θ = sin⁻¹ x = tan⁻¹[x / √(1−x²)]
The right triangle that connects $\sin^{-1} x$ to $\tan^{-1}$. If the hypotenuse is $1$ and the opposite side is $x$, then the adjacent side is $\sqrt{1-x^2}$. The angle $\theta$ can be read off as either $\sin^{-1} x$ or $\tan^{-1}\!\frac{x}{\sqrt{1-x^2}}$. This triangle is the universal conversion tool between inverse trig functions.

Pattern 3: Telescoping sums

A powerful technique for sums like \sum_{r=1}^{n} \tan^{-1}\!\frac{1}{1 + r + r^2}.

The key observation: \frac{1}{1 + r + r^2} = \frac{(r+1) - r}{1 + r(r+1)}. This has the form \frac{a - b}{1 + ab} with a = r+1 and b = r. By the difference formula:

\tan^{-1}\!\frac{(r+1) - r}{1 + r(r+1)} = \tan^{-1}(r+1) - \tan^{-1} r

So each term is a difference of two consecutive \tan^{-1} values. The sum telescopes:

\sum_{r=1}^{n} \tan^{-1}\!\frac{1}{1 + r + r^2} = \tan^{-1}(n+1) - \tan^{-1} 1 = \tan^{-1}(n+1) - \frac{\pi}{4}

Worked examples

Example 1: Simplify $\tan^{-1} 1 + \tan^{-1} 2 + \tan^{-1} 3$

Step 1. Start with the first two terms. Apply the addition formula to \tan^{-1} 1 + \tan^{-1} 2. Here a = 1, b = 2, so ab = 2 > 1 with both positive. Use the corrected formula:

\tan^{-1} 1 + \tan^{-1} 2 = \pi + \tan^{-1}\!\frac{1 + 2}{1 - 1 \cdot 2} = \pi + \tan^{-1}\!\frac{3}{-1} = \pi + \tan^{-1}(-3)

Why: since ab = 2 > 1 and both a, b > 0, the sum overshoots \pi/2, so you must add \pi to the raw \tan^{-1}.

Step 2. Use the odd-function property: \tan^{-1}(-3) = -\tan^{-1} 3. So:

\tan^{-1} 1 + \tan^{-1} 2 = \pi - \tan^{-1} 3

Why: \tan^{-1} is an odd function, so negative arguments flip the sign.

Step 3. Add the third term:

\pi - \tan^{-1} 3 + \tan^{-1} 3 = \pi

Why: the \tan^{-1} 3 terms cancel perfectly.

Step 4. Verify numerically. \tan^{-1} 1 \approx 0.7854, \tan^{-1} 2 \approx 1.1071, \tan^{-1} 3 \approx 1.2490. Sum \approx 3.1416 = \pi. It checks out.

Result: \tan^{-1} 1 + \tan^{-1} 2 + \tan^{-1} 3 = \pi.

The graph of $y = \tan^{-1} x$. The three red points mark the values at $x = 1, 2, 3$. Their $y$-coordinates sum to exactly $\pi$ — a fact that is not visible from the graph alone, but the formula proves it. The dashed line at $y = \pi/2$ is the asymptote that $\tan^{-1} x$ approaches but never reaches.

The result \tan^{-1} 1 + \tan^{-1} 2 + \tan^{-1} 3 = \pi is one of those identities that looks like a coincidence but is actually forced by the addition formula and the odd-function property. Each piece slots into place with no room for any other answer.

Example 2: Prove that $\cos^{-1}\!\frac{4}{5} + \cos^{-1}\!\frac{12}{13} = \cos^{-1}\!\frac{33}{65}$ (a geometric identity)

Step 1. Let \alpha = \cos^{-1}\!\frac{4}{5}. Then \cos\alpha = \frac{4}{5}, and since \alpha \in [0, \pi], \sin\alpha = \frac{3}{5}.

Why: use \sin^2\alpha + \cos^2\alpha = 1. Since \alpha is in the first quadrant (cosine is positive), sine is also positive. \sqrt{1 - 16/25} = \sqrt{9/25} = 3/5.

Step 2. Let \beta = \cos^{-1}\!\frac{12}{13}. Then \cos\beta = \frac{12}{13}, \sin\beta = \frac{5}{13}.

Why: \sqrt{1 - 144/169} = \sqrt{25/169} = 5/13.

Step 3. Compute \cos(\alpha + \beta) using the cosine addition formula:

\cos(\alpha + \beta) = \cos\alpha\cos\beta - \sin\alpha\sin\beta = \frac{4}{5} \cdot \frac{12}{13} - \frac{3}{5} \cdot \frac{5}{13} = \frac{48}{65} - \frac{15}{65} = \frac{33}{65}

Why: the cosine addition formula lets you compute \cos(\alpha + \beta) from the individual sines and cosines without ever finding \alpha or \beta as decimal angles.

Step 4. Since both \alpha and \beta are in (0, \pi/2) and their sum is less than \pi, the principal value applies directly:

\alpha + \beta = \cos^{-1}\!\frac{33}{65}

Result: \cos^{-1}\!\frac{4}{5} + \cos^{-1}\!\frac{12}{13} = \cos^{-1}\!\frac{33}{65}.

Two right triangles showing the Pythagorean triples behind the identityTwo right triangles side by side. The first has sides 3, 4, 5 with angle alpha at the base. The second has sides 5, 12, 13 with angle beta at the base. Together these angles produce the combined cosine 33 over 65. 4 3 5 α 12 5 13 β cos(α + β) = (4·12 − 3·5) / (5·13) = 33/65
The two Pythagorean triples $(3, 4, 5)$ and $(5, 12, 13)$ hiding behind the identity. Angle $\alpha$ has cosine $4/5$; angle $\beta$ has cosine $12/13$. The cosine addition formula combines them into $33/65$ — itself part of the triple $(33, 56, 65)$, since $33^2 + 56^2 = 1089 + 3136 = 4225 = 65^2$. Pythagorean triples generate inverse-cosine identities.

The numbers \frac{4}{5}, \frac{12}{13}, and \frac{33}{65} are all cosines of angles in Pythagorean right triangles. The identity is really saying: if you place two such triangles next to each other, the combined angle has a cosine that comes from a third Pythagorean triple. This is the geometry hiding inside the algebra.

Common confusions

Going deeper

If you came here to learn the main identities and how to use them, you have them — you can stop here. The rest of this section is for readers who want to see some deeper connections.

Why the correction term exists: a topological view

The tangent function has period \pi. So \tan^{-1}, which inverts it, can only return values in a single period — the interval (-\pi/2, \pi/2). When the true sum \alpha + \beta leaves that interval, the raw \tan^{-1} wraps it back in, landing in the wrong period. The correction \pm\pi is a "winding number" — it counts how many times you have gone around the period.

This is the same phenomenon that makes complex logarithms multi-valued, and it is the same \pm\pi that appears in the argument of a complex number. When you study complex numbers and the polar form, the correction term will reappear as the branch-cut adjustment for \arg(z_1 z_2).

Madhava's arctangent series and a formula for \pi

The infinite series

\tan^{-1} x = x - \frac{x^3}{3} + \frac{x^5}{5} - \frac{x^7}{7} + \cdots \qquad \text{for } |x| \leq 1

was discovered by Madhava of Sangamagrama in the 14th century, centuries before it appeared in European mathematics. Setting x = 1:

\frac{\pi}{4} = 1 - \frac{1}{3} + \frac{1}{5} - \frac{1}{7} + \cdots

This series converges very slowly. But using the addition formula, you can accelerate it. Observe that \frac{\pi}{4} = \tan^{-1}\!\frac{1}{2} + \tan^{-1}\!\frac{1}{3}, and both \tan^{-1} series converge much faster for arguments less than 1. A further refinement is the identity \frac{\pi}{4} = 4\tan^{-1}\!\frac{1}{5} - \tan^{-1}\!\frac{1}{239}, which converges rapidly because 1/5 and 1/239 are small. The addition formulas you learned above are the engine behind every fast \pi computation that uses arctangent series.

Interplay with trigonometric equations

These identities are the bridge between trigonometric identities (which manipulate angles) and trigonometric equations (which solve for angles). An equation like \tan^{-1}(x+1) + \tan^{-1}(x-1) = \tan^{-1}\!\frac{8}{31} becomes solvable by applying the addition formula to the left side and comparing.

Where this leads next