$$\newcommand{\mtn}{\mathbb{N}}\newcommand{\mtns}{\mathbb{N}^*}\newcommand{\mtz}{\mathbb{Z}}\newcommand{\mtr}{\mathbb{R}}\newcommand{\mtk}{\mathbb{K}}\newcommand{\mtq}{\mathbb{Q}}\newcommand{\mtc}{\mathbb{C}}\newcommand{\mch}{\mathcal{H}}\newcommand{\mcp}{\mathcal{P}}\newcommand{\mcb}{\mathcal{B}}\newcommand{\mcl}{\mathcal{L}} \newcommand{\mcm}{\mathcal{M}}\newcommand{\mcc}{\mathcal{C}} \newcommand{\mcmn}{\mathcal{M}}\newcommand{\mcmnr}{\mathcal{M}_n(\mtr)} \newcommand{\mcmnk}{\mathcal{M}_n(\mtk)}\newcommand{\mcsn}{\mathcal{S}_n} \newcommand{\mcs}{\mathcal{S}}\newcommand{\mcd}{\mathcal{D}} \newcommand{\mcsns}{\mathcal{S}_n^{++}}\newcommand{\glnk}{GL_n(\mtk)} \newcommand{\mnr}{\mathcal{M}_n(\mtr)}\DeclareMathOperator{\ch}{ch} \DeclareMathOperator{\sh}{sh}\DeclareMathOperator{\th}{th} \DeclareMathOperator{\vect}{vect}\DeclareMathOperator{\card}{card} \DeclareMathOperator{\comat}{comat}\DeclareMathOperator{\imv}{Im} \DeclareMathOperator{\rang}{rg}\DeclareMathOperator{\Fr}{Fr} \DeclareMathOperator{\diam}{diam}\DeclareMathOperator{\supp}{supp} \newcommand{\veps}{\varepsilon}\newcommand{\mcu}{\mathcal{U}} \newcommand{\mcun}{\mcu_n}\newcommand{\dis}{\displaystyle} \newcommand{\croouv}{[\![}\newcommand{\crofer}{]\!]} \newcommand{\rab}{\mathcal{R}(a,b)}\newcommand{\pss}[2]{\langle #1,#2\rangle} $$
Bibm@th
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Formulaire - Linéarisation des fonctions trigonométriques

\begin{align*} \cos a \cos b &= \frac{1}{2} \left( \cos(a + b) + \cos(a - b) \right) \\ \sin a \sin b &= \frac{1}{2} \left( \cos(a - b) - \cos(a + b) \right) \\ \sin a \cos b &= \frac{1}{2} \left( \sin(a + b) + \sin(a - b) \right) \\ \frac{\tan b}{\tan a} &= \frac{\sin(a + b) - \sin(a - b)}{\sin(a - b) + \sin(a + b)} \\ \tan a \tan b &= \frac{\cos(a - b) - \cos(a + b)}{\cos(a - b) + \cos(a + b)} \\ \cos^2 a &= \frac{1 + \cos 2a}{2} \\ \sin^2 a &= \frac{1 - \cos 2a}{2} \\ \tan^2 a &= \frac{1 - \cos 2a}{1 + \cos 2a} \end{align*}

Pour linéariser des puissances supérieures de sin et cos, on utilise en règle générale les nombres complexes et la formule d'Euler.