Understanding a Symmetry Argument

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A rectangle has dimensions $a$ units by $b$ units with $a > b$. A diagonal divides the rectangle into two triangles. A square, with sides parallel to those of the rectangle, is inscribed in each triangle. Find the distance between the vertices (of the squares) that lie in the interior of the rectangle.

In the solution, we find that one square has an 'interior' vertex $(\frac{ab}{a+b},\frac{ab}{a+b})$, because the vertex must lie on both $y=x$ and $y = -\frac{b}{a}x + b$. Then the author asserts that symmetry permits us to conclude that the coordinates of the other vertex of the other inscribed square are $(\frac{a^2}{a+b}.\frac{b^2}{a+b})$. I have drawn several pictures trying to see the symmetry, but I can't seem to discern it, so I left no other option but a (relatively) brute-force method. Perhaps someone with a more geometric eye could kindly point out the symmetry being appealed to.

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You've set $(0,0)$ as the bottom left vertex and the diagonally opposite vertex as $(a,b)$. In addition, the diagonal drawn has negative gradient.

I believe 'by symmetry' just simply means that if $(p,q)$ is the interior vertex of one square, since the diagram has a rotational symmetry of $180°$ about the centre of the rectangle, then the interior vertex of the other square will be $(a-p, b-q)$.

Here, $(p,q)=(\frac{ab}{a+b},\frac{ab}{a+b})$, so

$$(a-p, b-q)=\left(a-\frac{ab}{a+b},b-\frac{ab}{a+b}\right)=\left(\frac{a^2+ab-ab}{a+b},\frac{b^2+ab-ab}{a+b}\right)=\left(\frac{a^2}{a+b},\frac{b^2}{a+b}\right)$$

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If we let rectangle have vertices $(0,0), (a,0), (0,b), (a,b)$, then we have central symmetry with respect to $(\frac a2,\frac b2)$ (this is the intersection of diagonals). This central symmetry is given by formula $(x,y)\mapsto (a-x, b -y)$, and thus $(\frac{ab}{a+b},\frac{ab}{a+b})\mapsto (\frac{a^2}{a+b},\frac{b^2}{a+b}).$

To find formula for central symmetry with respect to $(x_0,y_0)$, remember that central symmetry is affine transformation, and thus of the form $f(v) = Av + b$, where $A$ is linear map. To find central symmetry, first observe that $f(0,0) = 2(x_0,y_0)$, while $Av = -v$ (because that is central symmetry with respect to origin). Thus, central symmetry is given by $f(x,y) = (2x_0-x,2y_0-y)$.

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We can draw a picture of this situation as follows:

Image

We need to find $c,d,e,f$ to know the interior vertices of the squares.

Can you see that this is rotationally symmetric, if we spin it around by $180^\circ$, it will be exactly the same problem?

This means that the distance between $(0,b)$ and $(c,f)$ is equal to the distance between $(e,d)$ and $(a,0)$. Equally, the distance from $(c,f)$ to $(a,0)$ is equal to the distance from $(e,d)$ to $(0,b)$.

We can see that $$(c,f)=\left(\frac{ab}{a+b}, \frac{ab}{a+b}\right)$$ by the definition of a square, and then we can find the distance from here to $(a,0)$:

\begin{align}D_1&=\sqrt{\left(a-\frac{ab}{a+b}\right)^2+\left(0-\frac{ab}{a+b}\right)^2}\\ &=\sqrt{\left(\frac{a^2}{a+b}\right)^2+\left(-\frac{ab}{a+b}\right)^2}\\ &=\sqrt{\frac{a^4}{(a+b)^2}+\frac{a^2b^2}{(a+b)^2}}\\ &=\frac{a\sqrt{a^2+b^2}}{a+b}\end{align}

Now we know that the distance from $(e,d)$ to $(0,b)$ is equal to this:

\begin{align}\sqrt{e^2+(d-b)^2}&=\frac{a\sqrt{a^2+b^2}}{a+b}\end{align}

We can repeat this with the other distances to get \begin{align}D_2&=\sqrt{\left(\frac {ab}{a+b}-0\right)^2+\left(\frac{ab}{a+b}-b\right)^2}\\ &=\frac{b\sqrt{a^2+b^2}}{a+b}\end{align}

and therefore \begin{align}\sqrt{(e-a)^2+d^2}&=\frac{b\sqrt{a^2+b^2}}{a+b}\end{align}

Now we have two simultaneous equations in $e,d$ to solve:

\begin{align}\sqrt{e^2+(d-b)^2}&=\frac{a\sqrt{a^2+b^2}}{a+b}\\ \sqrt{(e-a)^2+d^2}&=\frac{b\sqrt{a^2+b^2}}{a+b}\end{align}

If we solve these while remembering that $0<e<a$ and $0<d<b$ then we find that \begin{align}e&=\frac{a^2}{a+b}\\ d&=\frac{b^2}{a+b}\end{align}

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The figure should be drawn in the following way:-

enter image description here

The result of $P = (\dfrac {ab}{a + b}, \dfrac {ab}{a + b})$ can be found by solving the two mentioned equations.

We use the vertical line through Q as the line of symmetry (for P and R). Its equation is $x = \dfrac {a}{2}$. The symmetrical distance between P (and also R) from that line is $\dfrac {a}{2} - \dfrac {ab}{a + b}$.

Then the x- coordinate of the other vertex (T) = that of R is given by:- $\dfrac {ab}{a + b} + 2 \times [\dfrac {a}{2} - \dfrac {ab}{a + b}] = … =\dfrac {a^2}{a + b}$.

The y-coordinate of T can be found in a similar fashion.