Here’s a simple proof: Let 𝛼 be a unit vector denoting the direction of our chord, and 𝑃 be our position. Then, the desired lengths are the signed values of 𝑡 such that 𝑃+𝑡𝛼=𝑟. Expanding, we get that

𝑃2+2𝑡(𝑃𝛼)+𝑡2=𝑟2

By Vieta’s, the products of the roots of this equation are just 𝑃2𝑟2, which, importantly, is independent of 𝛼. This quite elegantly proves Power of a Point without needing to resort to casework.