Solutions on an interval and classical equations
So far we have solved the equations in $\mathbb{R}$, obtaining infinite families of solutions. Often, however, only solutions in a range are of interest — for example, the angles of a triangle, which are between $0$ and $\pi$. And certain equations appear so much that they have their own methods: they are classical equations.
The story The equation $a\operatorname{sen} x + b\cos x = c$ is the equation of the sum of two oscillations of the same period: it appears in astronomy (the combination of two circular movements), in wave physics and in electricity (out-of-phase alternating currents). The trick of rewriting $a\operatorname{sen} x + b\cos x$ as a single displaced sinusoid — the auxiliary angle $\theta$ — was already used by 18th century astronomers. It gained industrial importance at the end of the 19th century, when the engineer Charles Steinmetz showed, in 1893, that alternating currents could be added as complex numbers: each sinusoid becomes an arrow with length (the amplitude) and slope (the phase), and adding oscillations becomes adding arrows. This is exactly what we do when writing $a\operatorname{sen} x + b\cos x = \sqrt{a^2 + b^2}\,\operatorname{sen}(x + \theta)$.