We develop a topological framework for understanding where zero-mean functions vanish or change sign. A key observation is that function families from Fourier analysis can sometimes be described in a unified geometric way. For example, a (real) trigonometric polynomial of degree \(d\) can be written as
\[ f(t)=\sum_{k=1}^d \big(a_k \cos(2\pi k t)+ b_k \sin(2\pi k t)\big), \]where $a_k,b_k\in \mathbb R$ for all $k$. Rather than viewing \(f\) in isolation, we package the sine and cosine terms into a single map
\[ \gamma(t)=(\cos(2\pi t),\sin(2\pi t),\dots,\cos(2\pi d t),\sin(2\pi d t))\in\mathbb{R}^{2d}. \]This map is equivariant with respect to the natural rotational symmetry of the circle. Every trigonometric polynomial of degree at most \(d\) can then be written as the composition of \(\gamma\) with a linear functional on \(\mathbb{R}^{2d}\), namely
\[ f(t)=\langle a,\gamma(t)\rangle \]for a suitable coefficient vector \(a\).
This perspective allows us to apply tools from equivariant topology and configuration-space methods inspired by Borsuk--Ulam-type theorems. Using these ideas, we obtain sharp bounds on the size of intervals or regions on which all functions in the family must vanish or change sign. Our results recover and strengthen several classical theorems on one- and multi-dimensional periodic functions, and extend to compositions of linear functionals with arbitrary equivariant maps. We also show how our framework yields existence results for efficient numerical integration formulas.