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STEP I 1990 question 1 solution

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TSR Wiki > Study Help > Subjects and Revision > Mathematics > STEP > STEP I 1990 question 1 solution


Let \varphi = \angle CDY. Then

\theta + \alpha + \varphi = \pi (1)

Consider the lengths of the altitudes dropped

from Y to CD, from Y to AB and from X to AD.

They are

r\sin\varphi, r\sin\alpha and r\sin\theta respectively.

Thus the areas of the triangles DCY, DYX, DXA are \frac{1}{2}r^2\sin\varphi, \frac{1}{2}r^2\sin\alpha and \frac{1}{2}r^2\sin\theta respectively, and the area of the quadrilateral is

\displaystyle K =  \frac{r^2}{2}\left(\sin \theta + \sin \alpha + \sin \varphi\right) (2)

When \alpha is fixed, and we wish to maximise this area:

\displaystyle K =  \frac{r^2}{2}\left(\sin \theta + \sin \alpha + \sin (\pi - \alpha - \theta)\right)

\displayste \frac{dK}{d\theta} = \frac{r^2}{2}\left(\cos \theta - \cos (\pi - \alpha - \theta)\right)

Setting the derivative to zero, we get

\cos \theta - \cos (\pi - \alpha - \theta) = 0

Now, both \theta and \pi - \alpha - \theta clearly belong in the interval (0, \pi) (the latter because it is the angle marked \varphi), and thus

\theta = \pi - \alpha - \theta

\displaystyle \theta = \frac{1}{2}(\pi - \alpha)

which is the maximum. This can be seen by working out the second derivative,

\displaystyle \frac{d^2K}{d\theta^2} = \frac{r^2}{2}\left(- \sin \theta - \sin (\pi - \alpha - \theta)\right)

which is clearly negative at  \theta = \frac{1}{2}(\pi - \alpha).

Note that in this case, the maximum area is given by

\displaystyle K_{max} = \frac{r^2}{2}\left(2\sin \frac{\pi - \alpha}{2} + \sin \alpha\right) (3)

If we wish to find the maximum when both \alpha and \theta vary, we can proceed by finding the value of \alpha for which the K_{max} is at a maximum. Thus,

\displaystyle \frac{dK_{max}}{d\alpha} = \frac{r^2}{2}\left(-\cos \frac{\pi - \alpha}{2} + \cos \alpha}\right)

Setting the derivative to zero:

\displaystyle -\cos \frac{\pi - \alpha}{2} + \cos \alpha = 0

Now, both \frac{1}{2}(\pi - \alpha) and \alpha are in (0, \pi), and thus we can write

\displaystyle - \frac{\pi - \alpha}{2} + \alpha = 0

from which follows

\displaystyle \alpha = \frac{\pi}{3} (4)

Again, to make that that this is a maximum, let us take the second derivative:

\displaystyle \frac{d^2 K_{max}}{d\alpha^2} = \frac{r^2}{2}\left( -\frac{1}{2} \sin \frac{\pi - \alpha}{2} - \sin \alpha\right)

which again can be seen to be negative, thus ensuring that (4) indeed gives us the maximum K_max.

Now, insertion into (3) gives us the maximum area as

\displaystyle K = 3\frac{r^2}{2}\sin \frac{\pi}{3}, i.e.

\displaystyle K = \frac{3\sqrt{3}r^2}{4}

Just for clarification, note that this happens when

\displaystyle \theta = \alpha = \frac{\pi}{3}.


Alternate Solution

Now you could stop reading here, but for the extra educational benefit or something, I couldn't resist pointing out that this question follows very easily from Jensen's inequality, introduced to us avid STEP-solvers in 2007 II/7:

Let f(x) be a concave function on some interval and let x_1, x_2, \ldots, x_n lie in that interval. Jensen's inequality states that
\displaystyle \frac{1}{n}\sum_{k=1}^n f(x_k) \leq f\left(\frac{1}{n}\sum_{k=1}^n x_k\right)
and that equality holds if and only if x_1 = x_ 2 = \cdots = x_n

Now, in 2007 II/7, it was proven that \sin x was a concave function on (0, \pi).

Setting, in Jensen's inequality, n = 3 , x_1 = \theta , x_2 = \alpha, x_3 = \varphi , and using (2) and (1) we get

\displaystyle K = \frac{3r^2}{2} \cdot \frac{1}{3}\left(\sin \alpha + \sin \theta + \sin \varphi\right) \leq \frac{3r^2}{2}\sin \frac{\pi}{3}

with equality iff \theta = \alpha = \varphi.

This immediately gives us the maximum.

Solution by ukgea.

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