The Geometry of the Tilted Square
Welcome, future engineer. Today, we are not just solving a coordinate geometry problem; we are embarking on a journey of visualization.
Imagine you are standing at the origin of a Cartesian plane. In front of you lies a square, OABC, with side length a. But this isn't a boring, axis-aligned square; it is tilted, resting on a slope of angle α.
If you can master the geometry of this rotation, you can master any problem in JEE Advanced.
Phase 1
The Art of Coordinates
Let us begin by pinning down our vertices. We know vertex O is at (0,0).
The side OA makes an angle α with the positive x-axis. This is a classic application of polar coordinates. If the length of the side is a, then the coordinates of A are simply (acosα,asinα).
Now, consider vertex C. In a square, the sides meeting at the origin are perpendicular. This means the side OC is at an angle of 90∘+α from the positive x-axis.
Using our trigonometric definitions, the coordinates of C become (acos(90∘+α),asin(90∘+α)). Applying the reduction formulas, we find C is at (−asinα,acosα).
Do you see the beauty here? The negative sign in the x-coordinate is not an error; it is the physical manifestation of the square rotating into the second quadrant. Always trust the math over your intuition when the geometry gets complex.
Phase 2
The Slope of the Diagonal
We need the equation of the diagonal AC. To find the equation of any line, we need two things: a point and a slope.
We have the points A(acosα,asinα) and C(−asinα,acosα). Let us calculate the slope m using the standard formula m=x2−x1y2−y1.
Substituting our coordinates, we get:
m=−asinα−acosαacosα−asinα
It looks messy, doesn't it? But look closer. We can factor out the a from the numerator and denominator and cancel it.
Then, pull out a negative sign from the denominator. We are left with:
This is the slope of our diagonal. It captures the essence of the tilt α.
Phase 3
The Algebraic Dance
Now, we use the point-slope form: y−y1=m(x−x1). Let us use point A as our anchor.
The equation becomes:
y−asinα=−(sinα+cosα)cosα−sinα(x−acosα)
This is where most students panic. The expression looks daunting, but take a deep breath. We are going to cross-multiply.
Multiply both sides by −(sinα+cosα):
−(y−asinα)(sinα+cosα)=(x−acosα)(cosα−sinα)
Now, expand both sides carefully. On the left, we get −y(sinα+cosα)+asin2α+asinαcosα. On the right, we get x(cosα−sinα)−acos2α+asinαcosα.
Do you see it? The term asinαcosα appears on both sides. It is a gift! It cancels out perfectly. This is the elegance of mathematics—the complexity vanishes when you follow the logic.
Phase 4
The Grand Finale
After the cancellation, we group the variables on one side and the constants on the other:
y(cosα+sinα)+x(cosα−sinα)=asin2α+acos2α
Finally, factor out the a on the right side. We are left with a(sin2α+cos2α).
We know the fundamental identity sin2α+cos2α=1. The entire right side collapses into just a.
Our final equation is:
y(cosα+sinα)+x(cosα−sinα)=a
You have successfully navigated the rotation, the coordinate geometry, the slope calculation, and the algebraic simplification. This is how you conquer JEE Advanced problems—one logical step at a time. Keep this confidence, and you will be unstoppable.