The Dance of Geometry
Finding the Foot of the Perpendicular
Imagine you are standing in a vast, three-dimensional space. You have a line L stretching out into infinity, and two planes, π1 and π2, slicing through the void.
This is not just an algebra problem; it is a story of intersection and alignment. We are tasked with finding a specific point Q, the foot of a perpendicular dropped from a point P on line L to plane π1.
But there is a twist: Q is not just any point; it is a prisoner of two worlds, lying on both π1 and π2. Let us embark on this journey to uncover its coordinates.
Phase 1
The Parametric Leap
Our first challenge is to tame the line L. The equation is given as 2x−1=−1y+1=1z.
In the world of JEE Advanced, we never treat a line as a static object. We treat it as a path. By setting this entire expression equal to a scalar parameter λ, we unlock the ability to describe any point P on this line.
This is our 'moving point.' As λ changes, P glides along the line. Our mission is to find the specific value of λ that forces the perpendicular from P to land exactly on the intersection of our two planes.
Phase 2
The Intersection Insight
Before we touch the perpendicular formula, let us look at the planes: π1:x+y+z=3 and π2:x−y+z=3. If point Q lies on both, it must satisfy both equations simultaneously.
This is where the magic happens. Instead of solving for x,y, and z individually, let us look at the system as a whole. Subtracting the second equation from the first:
This is a massive breakthrough! We have just discovered that the y-coordinate of our target point Q is zero. We have reduced the dimensionality of our problem with a single stroke of subtraction.
Phase 3
The Bridge of the Perpendicular
Now, we need to connect P to Q. We use the standard formula for the foot of the perpendicular from a point (x1,y1,z1) to a plane ax+by+cz+d=0:
ax−x1=by−y1=cz−z1=−a2+b2+c2ax1+by1+cz1+d
For our plane π1 (x+y+z−3=0), the coefficients are a=1,b=1,c=1, and d=−3. The denominator becomes 12+12+12=3.
We know yQ=0. Let us focus solely on the y-component of the formula:
Phase 4
The Final Calculation
Substitute our parametric coordinates of P into the equation. We know yQ=0 and yP=−λ−1.
0−(−λ−1)=−3(2λ+1)+(−λ−1)+λ−3
Simplifying the left side gives λ+1. Simplifying the numerator on the right: (2λ−λ+λ)+(1−1−3)=2λ−3.
Multiply both sides by 3:
The math has collapsed beautifully into λ=0. This means our point P is located at (1,−1,0).
Conclusion
The Coordinates of Q
With λ=0, we can find the coordinates of Q. The common ratio in our formula was −32(0)−3=1. Using xQ−xP=1(a), yQ−yP=1(b), and zQ−zP=1(c):
The coordinates of Q are (2,0,1). We have traversed the geometry, used the parametric form, exploited the intersection, and arrived at the solution. Remember, in JEE Advanced, the most complex problems often yield to the simplest geometric insights.