# Trigonometry, obtuse angles and a negative length?

I've been looking for an answer as to why when $\cos x<0$ and $\tan x<0$ the angle is obtuse.

I found a few identical explanations online where, a right-angle triangle is formed in the second quadrant from the corner (of the obtuse angle triangle) where the hypotenuse and opposite side meet.

Here they show that the length of the adjacent side of the newly formed right angled triangle is negative, which as a result causes $\cos x<0$ and $\tan x<0$ since $\cos x=\frac{-a}{h}$ and $\tan x=\frac{o}{-a}$.

But how can a length be negative? Is the explanation wrong? Or am I missing something?

• It is not a "length" that is negative. It is a "coordinate" that is negative. – GEdgar May 6 '16 at 20:30

Stage 1: This uses actual triangles. Then all the lengths are positive, and the ratios are of positive numbers, but angles only make sense in the interval $[0,\pi/2]$ radians. In this setting, we can place a right triangle so that one vertex is at the origin of our coordinate system, the leg it is on runs along the $x$-axis to the right angle, then the other leg runs parallel to the $y$-axis to the other vertex, and the hypotenuse is a line segment from the origin to this last vertex, lying entirely in the first quadrant. (Or, in the degenerate case where the second leg is zero, on the $x$-axis, which is not part of the first quadrant.) In this stage, we say things like "the sine of an angle is the ratio of the opposite to the hypotenuse".
Stage 2: We allow the hypotenuse to lie in any quadrant. Then we still construct right triangles ("reference triangles") in "standard position" as: put one of the vertices not at the right angle at the origin, put one leg along the $x$-axis, turn at right angles from the $x$-axis and run parallel to the $y$-axis for the other leg. This allows positive and negative values for the $x$- and $y$-coordinates of the hypotenuse and hence for the signed lengths of the first and second legs. Then we say things like "the sine of the angle is the ratio of the $y$-coordinate to the hypotenuse". (The length of the hypotenuse is always positive because it is always a length, not a coordinate.)
Stage 3: We generalize to angles less than $0$ and greater than $2\pi$ radians. This is where we get "coterminal angles". Everything still happens with right triangles, signed leg lengths, and on one copy of the coordinate plane, but we imagine that we have spun our angle around the origin many, many times in either direction. (This more accurately models real rotating systems -- a wheel doesn't rotate exactly once and then stop...)