\(\mathbf{v}\) and \(\mathbf{n}\) are unit vectors in \(3\)-dimensional space, with \(\mathbf{v} \cdot \mathbf{n} \neq 0\).
Let \(P\) be a plane with unit normal \(\mathbf{n}\). The reflection of \(\mathbf{v}\) in plane \(P\), \(\mathbf{w}\), is given by the formula\[\mathbf{w} = \mathbf{v} - 2(\mathbf{v} \cdot \mathbf{n})\mathbf{n} . \quad (*)\]
When the unit vectors \(\mathbf{v}\) and \(\mathbf{n}\) vary, the formula \((*)\) will always result in a unit vector for \(\mathbf{w}\).
Before photovoltaic technology allowed for cost-effective direct conversion of sunlight to electrical energy in solar panels, solar power plants relied on arrays of mirrors to concentrate a large area of sunlight into a receiver. In one such plant (see diagram), the receiver is modelled as a single point \(C\) with coordinates \((0, 0, 10)\), with mirrors surrounding it. One particular mirror has centre \(M\) with coordinates \((-10, -5, 0)\), and its surface is modelled as part of a plane \(P\) passing through \(M\) with unit normal \(\mathbf{n}\).

At midday, incoming beams of sunlight can be modelled as travelling along the direction \(\mathbf{v} = \begin{pmatrix} 0 \\ 0 \\ -1 \end{pmatrix}\). The mirror is angled so that a beam of sunlight shining on \(M\) is reflected to pass through the receiver \(C\).
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