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JEE Main 2026 (21 January Shift 2)
LEVELJEE Main

Animated Solution for Mathematics - Conic Sections: Let be the parabola with its vertex at . Let be a point on the parabola and be a point on the -axis such that . Then the locus of the centroid of such triangles is :

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Visualized Solution

Visualizing the Parabola

  • Given Parabola:
  • Comparing with
  • Vertex

Parametric Coordinates of

  • Let the parametric coordinates of be
  • Substituting :

Defining Point and Triangle

  • Point lies on the x-axis, so
  • We form the triangle

The Orthogonality Condition

  • Given condition:
  • This means vectors and are perpendicular.

Setting up the Dot Product

  • Dot Product:

Solving for

  • Divide by (assuming ):
  • So,

Finding the Centroid

  • Centroid
  • We need to find the locus of this centroid.

Substituting Coordinates into Centroid

Simplifying the Centroid Coordinates

Eliminating the Parameter

  • To find the locus, we must eliminate .
  • From
  • Substitute in :

The Final Locus Equation

  • Rearranging:
  • Replacing with :
  • Final Equation:

The Sigma Insight: Standard Equations of Parabola, Ellipse, and Hyperbola

Solution Diagram

Analyzing the Setup

Welcome, fellow traveler of the coordinate plane. Today, we are not just solving an equation; we are witnessing a dance.
We have a parabola, , and a point moving along it. As moves, it drags a triangle with it, forcing point to shift along the x-axis to keep the angle at perfectly square.
Our mission is to find the path—the locus—traced by the centroid of this triangle. Let us begin.

The Power of Parametrization

First, let us ground ourselves. We are given . By comparing this to the standard form , we immediately identify , which gives us .
The vertex is at . Now, instead of wrestling with and as independent variables, let us use the elegance of parametric coordinates.
Any point on this parabola can be represented as . Substituting our value of , we get .
By reducing the position of to a single parameter, , we have turned a two-dimensional problem into a one-dimensional journey. This is the secret to simplifying complex geometry.

The Orthogonality Condition

The problem imposes a strict condition: . This is the heartbeat of the problem.
Geometrically, this means the vector and the vector are perpendicular. In the language of vectors, this is a gift; it means their dot product must be zero: .
Let us calculate these vectors. Since , the vector is simply the negative of the coordinates of : .
For point , which lies on the x-axis, we define it as . Thus, . Now, we perform the dot product:
Expanding this, we get . Assuming $t eq 0$, we divide by to find , which simplifies beautifully to .
We have found the x-coordinate of in terms of our parameter .

The Centroid and the Locus

We are now ready to find the centroid . The centroid of a triangle with vertices , , and is the average of its coordinates.
For our triangle , the vertices are , , and . Calculating the coordinates of :
We have expressed the centroid's position entirely in terms of . To find the locus, we must eliminate . From the equation for , we have .
Substituting this into the equation for :

The Final Reveal

Let us simplify this expression. We have , which simplifies to .
Multiplying by , we get . Rearranging, we arrive at the final equation of the locus:
Replacing and with the standard variables and , we get .
Look at that! The centroid itself traces out a parabola. It is a perfect, elegant conclusion to our journey.

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