It depends on how you define the trigonometric functions. If you use the definition over their series
\cos x=\sum_{k=0}^{\infty} \frac{(-1)^k}{(2k)!} x^{2k}, \quad \sin x=\sum_{k=0}^{\infty} \frac{(-1)^k}{(2k+1)!} x^{2k+1},
which defines these functions for all \mathbb{R}, you can easily prove that
\cos' x=-\sin x, \quad \sin' x=\cos x
and from this
\frac{\mathrm{d}}{\mathrm{d} x}[\cos^2 x+\sin^2 x]=0 \; \Rightarrow \cos^2 x+\sin^2 x=\text{const},
and from that, because of \cos 0=1, \quad \sin 0=0 you get \cos^2 x + \sin^2 x=1.
Then you can define the number \pi/2 as the smallest positive solution of \cos(\pi/2)=0.
In this way you can derive step by step all the properties of sin and cos without using any geometric definitions. Then you can prove the geometrical properties of these functions from the unit circle's standard parametrization
x=\cos \varphi, \quad y=\sin \varphi, \quad \varphi \in [0,2 \pi).
This is, however, obviously not precalculus anymore.