locus blog
Physics, Chemistry and Math!
Physics, Chemistry and Math!
Dec 17th
This problem was asked in IMO 1961, Hungary.
Q: Let be the lengths of a triangle
whose area is
. Prove that
. In what case does equality hold?
Solution: We can express the area in terms of the sides and angles of the triangle:
Also, the cosine rule says that
Therefore,
Note that equality will hold above if and
, that is, when the triangle is equilateral.
Apr 30th
Most of us are familiar with Euler’s (miraculous) formula:
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However, how many of us have actually given much thought to why this should hold true? Even more fundamental is the question that what meaning should be attached to raising a real number like e to a complex power iθ.
Many math authors will propose this formula as a definition. That’s very unfair to one of the greatest achievements of Euler – he certainly didn’t think up this formula in a dream. There must’ve been some logical reasoning process behind it.
This article discusses one simple “proof” of Euler’s formula, using just the exponential series expansion:

For now, lets make a leap of faith and assume that this expansion will hold for x = iθ:

One possibility is to note that A(θ) represents the (Taylor) expansion series of cos(θ), while B(θ) represents that of sinθ. However, let us not use any more expansion series, but rather proceed in a more elementary fashion.
Step – 1 :

From the series of A(θ) and B(θ), note that

But since for θ = 0, we have

Step – 2
Let us denote by Φ the argument of A(θ) + iB(θ) :

The argument of A(θ) + iB(θ) can be taken to be 0 if θ = 0. Thus, Φ = θ.
Now, carefully observe what we have proved in step – 1 and step – 2. The former says that the mysterious looking quantity e raised to the power iθ has a magnitude of unity, no matter what the value of θ, while the second step says that it has an argument of θ:

Figure-1
Therefore, its real part A(θ) must be cosθ, while its imaginary part B(θ) must be sinθ:
![]()
Our “proof” incidentally also proves the Taylor expansions of sinθ and cosθ:

In some future post, more justifications for Euler’s formula will be presented.
Apr 9th
If you’ve worked on a sufficient number of coordinate geometry problems, you can well understand how sometimes the solutions are incredibly long. And boring too! Most students think that all that there is to coordinate geometry is working with long and tedious expressions, and, in most cases, ending up with a wrong answer!
Well, some of this is true to an extent. Doing coordinate geometry problems does become a lengthy and tedious task at times. However, there are ways to simplify this task, the most important being the use of plane geometry wherever possible. We’re on a regular basis surprised by students who try to employ algebraic equations in a problem that can be solved in seconds using simple plane geometry facts.
In this article, we pick some problems from coordinate geometry at random, and show how an algebraic approach compares with a plane geometry approach in each case.
Problem – 1
There are two circles S1 and S2 and given by
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From a point P on S2, tangents are drawn to S1 as shown. Find the angle between the tangents.
This problem is in fact a no-brainer: even a student very inexperienced in coordinate geometry would realize that plane geometry is the best way to solve this.
A coordinate approach would have involved assuming the coordinates of P, say ![]()
and writing the joint equation of the pair of tangents from P to S1. The angle can then be determined by using the standard appropriate relations on this joint equation.
A plane geometry approach is much simpler: join P to the center O of the circles and join O to one of the points of contact, say Q, as shown:
Now, simply observe that
![]()
![]()
Thus,![]()
or ![]()
so that ![]()
Thus, is two steps, we’re able to determine that the two tangents are perpendicular to each other.
Although this problem is very simple, it still manages to make a general point: pure geometry can be way better than an algebraic approach in many cases.
Problem – 2
There are two circles S1 and S2 given by
![]()
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From a point P on S2 , a pair of tangents is drawn to S1. The triangle formed using these two tangents and the chord of contact QR, is completed. Where does the centroid of triangle PQR lie?
Note that the radius of S2 is twice that of S1.
Now, let us first write down what steps you’d have taken in case of an algebraic approach:
- assume coordinates for P
- write the equation to the pair of tangents, and thus determine the coordinates of Q and R
- write the coordinates for the centroid G using the coordinates of P, Q and R
- using these coordinates, figure out where G lies
Lengthy! Very lengthy indeed!
Instead, we follow a plane geometry approach, recalling from our class 9th studies that the centroid divides any median in the ratio 2:1.
First join P, Q and R to O, the center of the circles. Also, some more constructions are done, as shown:

Now starts the magic. First of all, note that angle(AOR)= 600 and OR = OB = r, implying triangle ORB is equilateral, so that OA = AB.
Also, since OB = BP, we get BP = 2AB, implying that B divides PA in the ratio 2:1. Finally, note that PA is the median, implying that B is the centroid of triangle PQR.
Thus, the centroid of triangle PQR lies on the inner circle. How easy was this?
Problem – 3
There are two circles S1 and S2, with S1 lying completely internal to S2 . Find the locus of a point P which moves such that it is always equidistant from S1 and S2.

A coordinate geometry approach would involve the following:
- assume the equations for S1 and S2 (warning! – note that these two circles are not necessarily concentric)
- assume an arbitrary point P(x,y), and write its distances from S1 and S2. If we denote the radii of the two circles by r1 and r2, we have
distance(P,S1) = PC1 – r1
distance(P,S2) = r2 - PC2 ….(1)
- write the coordinate expressions for these two distances
- once done, equate the two distances and simplify to get the locus of P.
This is again very lengthy.
Using the plane geometry approach, we are done simply after we’ve written (1):
PC1 – r1 = r2 - PC2
–> PC1 + PC2 = r1 + r2
–> P moves in such a way that PC1 + PC2 is a constant equal to r1 + r2
–> P moves on an ellipse! And the foci are C1 and C2
You see that apart from determining the locus of P to be an ellipse, we have succeeded in showing that the foci of this ellipse are C1 and C2 . All in two lines!
As an exercise, redo this problem in case the two circles were external to each other.
There three examples should have given you a brief and basic idea on how plane geometry is used to solve coordinate geometry problems. If you intend to become a good math student, you must always use your intuition to realize the most appropriate approach to a problem: algebraic, plane geometry or a mixture of the two. This skill can be developed only with practice.
We’ll bring you more such problems in the future.
Apr 9th
Consider three points A, B and C on a sphere of radius R. Each pair of points is joined pairwise using the equator passing through those two points.
A “triangular” region will be formed by the three equators so drawn, as shown. Suppose that these three equators intersect at angles alpha, beta, gamma. What will be the area of the “triangle” on the sphere in terms of R and these three angles?
Hints:
1) If you look carefully, the same “triangular” region is formed on the opposite side of the sphere!
2) Consider this “peel” below. What will be its area?