Animated Solution for Mathematics - Straight Lines: Consider three points P=(−sin(β−α),−cosβ), Q=(cos(β−α),sinβ) and R=(cos(β−α+θ),sin(β−θ)), where 0<α,β,θ<4π. Then,
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Visualized Solution
Introduction to Points P,Q,R
Given points:
P=(−sin(β−α),−cosβ)
Q=(cos(β−α),sinβ)
R=(cos(β−α+θ),sin(β−θ))
Constraints: 0<α,β,θ<4π
Determinant Condition for Collinearity
For points to be collinear, the area of the triangle must be zero.
Δ=21xPxQxRyPyQyR111=0
Expanding xR
xR=cos(β−α+θ)
Using cos(A+B)=cosAcosB−sinAsinB:
xR=cos(β−α)cosθ−sin(β−α)sinθ
Notice that xQ=cos(β−α) and xP=−sin(β−α)
∴xR=xQcosθ+xPsinθ
Expanding yR
yR=sin(β−θ)
Using sin(A−B)=sinAcosB−cosAsinB:
yR=sinβcosθ−cosβsinθ
Notice that yQ=sinβ and yP=−cosβ
∴yR=yQcosθ+yPsinθ
The Hidden Vector Relationship
From the expansions, we found:
xR=xQcosθ+xPsinθ
yR=yQcosθ+yPsinθ
In vector form: R=(sinθ)P+(cosθ)Q
This linear dependency will help simplify the determinant.
Applying Row Operations
Δ=xPxQxRyPyQyR111
Apply operation: R3→R3−(sinθ)R1−(cosθ)R2
Δ=xPxQ0yPyQ0111−sinθ−cosθ
Simplifying the Determinant
Expanding along the third row (R3):
Δ=(1−sinθ−cosθ)xPxQyPyQ
Δ=(1−sinθ−cosθ)(xPyQ−xQyP)
Evaluating the 2×2 Minor
Substitute the coordinates of P and Q:
xPyQ−xQyP=(−sin(β−α))(sinβ)−(cos(β−α))(−cosβ)
=cos(β−α)cosβ−sin(β−α)sinβ
Simplifying with Trigonometric Identities
Using the identity cosAcosB−sinAsinB=cos(A+B):
Here, A=β−α and B=β
xPyQ−xQyP=cos((β−α)+β)=cos(2β−α)
∴Δ=(1−sinθ−cosθ)cos(2β−α)
Analyzing the First Factor
Factor 1: 1−(sinθ+cosθ)
Given constraint: 0<θ<4π
In this interval, 1<sinθ+cosθ≤2
∴1−(sinθ+cosθ)=0
Analyzing the Second Factor
Factor 2: cos(2β−α)
Given constraints: 0<α,β<4π
Bounds for the angle: −4π<2β−α<2π
In this interval, the cosine function is strictly positive.
∴cos(2β−α)=0
Final Conclusion
Since both factors are non-zero, Δ=0
The area of the triangle is not zero.
Therefore, the points P,Q,R are non-collinear.
Correct Option: (d)
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The Sigma Insight: Area of Triangle
Solution Diagram
The Geometry of Hidden Patterns
My dear student, welcome to a problem that, at first glance, looks like a chaotic mess of trigonometric functions. We have points P,Q, and R defined by angles α,β, and θ.
If you try to calculate the slopes directly, you will likely find yourself drowning in a sea of identities. But here is the secret: JEE Advanced problems are rarely about brute force. They are about finding the hidden, elegant structure beneath the surface.
Phase 1
Deconstructing the Coordinates
Let us look at our points:
P=(−sin(β−α),−cosβ)Q=(cos(β−α),sinβ)R=(cos(β−α+θ),sin(β−θ))
Do not be intimidated by the complexity. Let us focus on R. The x-coordinate is cos(β−α+θ).
Using the compound angle formula cos(A+B)=cosAcosB−sinAsinB, we can expand this as:
xR=cos(β−α)cosθ−sin(β−α)sinθ
Look closely at the terms. cos(β−α) is exactly xQ, and −sin(β−α) is exactly xP. Thus, we have discovered that xR=xQcosθ+xPsinθ. This is not a coincidence; it is the heartbeat of the problem.
Phase 2
The Hidden Vector Relationship
If we apply the same logic to the y-coordinate of R, using sin(A−B)=sinAcosB−cosAsinB, we get:
yR=sinβcosθ−cosβsinθ
Again, sinβ is yQ, and −cosβ is yP. So, yR=yQcosθ+yPsinθ.
We have just uncovered a beautiful vector relationship: R=(sinθ)P+(cosθ)Q. This tells us that R is a linear combination of P and Q. In the world of geometry, this is a massive shortcut.
Phase 3
The Determinant Masterclass
To check for collinearity, we use the determinant Δ of the matrix formed by the coordinates. If Δ=0, the points are collinear. We set it up as:
Δ=xPxQxRyPyQyR111
Instead of expanding this directly, we use the linear relationship we found. We apply the row operation R3→R3−(sinθ)R1−(cosθ)R2.
Because of our discovery in Phase 2, the first two elements of the third row vanish! We are left with:
Δ=xPxQ0yPyQ0111−sinθ−cosθ
Expanding along the third row, we get Δ=(1−sinθ−cosθ)det(P,Q).
Phase 4
The Final Verdict
Now, we evaluate the 2×2 minor, det(P,Q)=xPyQ−xQyP. Substituting the coordinates, we get:
(−sin(β−α))(sinβ)−(cos(β−α))(−cosβ)
=cos(β−α)cosβ−sin(β−α)sinβ
This is the classic expansion for cos(A+B), where A=β−α and B=β. So, the minor simplifies to cos(2β−α).
Finally, we check our factors. Given 0<θ<4π, the sum sinθ+cosθ is always greater than 1, so $1 - \sin\theta - \cos\theta
eq 0$.
Similarly, for 0<α,β<4π, the angle 2β−α stays within a range where the cosine is strictly positive. Since neither factor is zero, the determinant is non-zero. The points are non-collinear. We have conquered the problem with logic, not just calculation!