Problem 2

Triangle Points

Answer Format: Equation

Let AA and BB be points in space. For any line segment AB\overline{AB}, there exists at least one point CC such that ACB\angle ACB is a right angle. Find an equation which represents the set of all possible points of CC in Rn\mathbb{R}^n space.

(xAB2)AB=xAB212AB=0\begin{aligned} (\vec{x}-\frac{\overrightarrow{AB}}{2}) \cdot \overrightarrow{AB} = \| \vec{x}-\frac{\overrightarrow{AB}}{2} \| -\frac{1}{2} \| \overrightarrow{AB} \| = 0 \end{aligned}

Explanation


Each point CC can be described as a vector from the midpoint of AB\overrightarrow{AB} to the point CC. Let's call this vector C\vec{C}. C\vec{C} has 2 important properties; it is orthogonal to AB\overrightarrow{AB} and it's magnitude is constant for all terminal points CC. It shouldn't be that hard to convince yourself of this, try solving the problem in R2\mathbb{R}^2 and it should become apparent fairly quickly.


Here's the intuition that I used. Given AB\overrightarrow{AB} in Rn\mathbb{R}^n space, we can draw an infinite amount of planes that contain AB\overrightarrow{AB} (assuming n>2n>2). For example, in R3\mathbb{R}^3 space, imagine rotating a plane about an axis along AB\overrightarrow{AB}. That's the set of all planes that contain AB\overrightarrow{AB}.


On each of these planes, we can draw the problem in 2 dimensions. You have probably noticed that there are always 2 solutions in R2\mathbb{R}^2. Simply draw a square with the diagonal being AB\overrightarrow{AB} and calculate where the last 2 corners are. In fact, because the solutions in R2\mathbb{R}^2 are the secondary diagonal points of a square, this tells us that the magnitude of C\vec{C} is half that of the diagonal (C=12AB\|\vec{C}\|=\frac{1}{2}\|\overrightarrow{AB}\|).


Similarly, we can determine that C\vec{C} must be orthogonal to AB\overrightarrow{AB} using the idea of square diagonals. The diagonals of a square are by definition orthogonal to each other. This means that CAB=0\vec{C} \cdot \overrightarrow{AB} = 0.


To combine these conditions, we can write the first condition as C12AB=0\|\vec{C}\|-\frac{1}{2}\|\overrightarrow{AB}\|=0. Then we equate this to the second condition. Of course, we still need to specify that both of these expressions are equal to zero.