Animated Solution for Mathematics - Inverse Trigonometric Functions: Let (x,y) be such that sin−1(ax)+cos−1(y)+cos−1(bxy)=2π. Match the statements in Column I with statements in Column II and indicate your answer by darkening the appropriate bubbles in the 4×4 matrix given in the ORS.
List-I
(P)
If a=1 and b=0, then (x,y)
(Q)
If a=1 and b=1, then (x,y)
(R)
If a=1 and b=2, then (x,y)
(S)
If a=2 and b=2, then (x,y)
List-II
(1)
lies on the circle x2+y2=1
(2)
lies on (x2−1)(y2−1)=0
(3)
lies on y=x
(4)
lies on (4x2−1)(y2−1)=0
Select Matching Pairs:
* Multiple Allowed
PMatches
QMatches
RMatches
SMatches
Visualized Solution
Analyze the Equation
Given equation: sin−1(ax)+cos−1(y)+cos−1(bxy)=2π
Rearrange to isolate the cosine terms: cos−1(y)+cos−1(bxy)=2π−sin−1(ax)
Apply Complementary Identity
Using identity: sin−1(θ)+cos−1(θ)=2π
Therefore: 2π−sin−1(ax)=cos−1(ax)
Equation becomes: cos−1(y)+cos−1(bxy)=cos−1(ax)
Trigonometric Substitution
Let α=cos−1(y), β=cos−1(bxy), and γ=cos−1(ax)
Then α+β=γ⟹β=γ−α
Taking cosine on both sides: cos(β)=cos(γ−α)
Expand and Substitute Back
Expansion: cos(β)=cos(γ)cos(α)+sin(γ)sin(α)
We know: cos(β)=bxy, cos(γ)=ax, cos(α)=y
And: sin(γ)=1−a2x2, sin(α)=1−y2
Substitute back: bxy=(ax)(y)+1−a2x21−y2
Isolate the Radical and Square
Isolate root: bxy−axy=1−a2x21−y2
Factor left side: (b−a)xy=1−a2x21−y2
Square both sides: (b−a)2x2y2=(1−a2x2)(1−y2)
Case A: a=1,b=0
Substitute a=1,b=0 into the master equation.
(0−1)2x2y2=(1−x2)(1−y2)
x2y2=1−x2−y2+x2y2
Cancel x2y2: x2+y2=1
This represents a circle. (Matches statement p)
Case B: a=1,b=1
Substitute a=1,b=1 into the master equation.
(1−1)2x2y2=(1−x2)(1−y2)
0=(1−x2)(1−y2)
This implies x2=1 or y2=1.
Result: (x2−1)(y2−1)=0 (Matches statement q)
Case C: a=1,b=2
Substitute a=1,b=2 into the master equation.
(2−1)2x2y2=(1−x2)(1−y2)
x2y2=1−x2−y2+x2y2
Cancel x2y2: x2+y2=1
This again represents a circle. (Matches statement p)
Case D: a=2,b=2
Substitute a=2,b=2 into the master equation.
(2−2)2x2y2=(1−4x2)(1−y2)
0=(1−4x2)(1−y2)
This implies 4x2=1 or y2=1.
Result: (4x2−1)(y2−1)=0 (Matches statement s)
Final Summary
Key Takeaways:
Identity sin−1(θ)+cos−1(θ)=2π is powerful for simplification.
Squaring is necessary to remove radicals but can introduce extraneous solutions.
Final Match:
A → p; B → q; C → p; D → s
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The Sigma Insight: Solving Inverse Trigonometric Equations
Solution Diagram
The Art of Inverse Trigonometric Symmetry
Welcome, fellow explorer of the mathematical landscape. Today, we are going to dismantle a problem that, at first glance, looks like a tangled mess of inverse trigonometric functions.
In JEE Advanced, the most complex-looking problems often hide a beautiful, simple symmetry. Let us embark on this journey together.
Phase 1
The Power of the Complementary Identity
We start with the given equation:
sin−1(ax)+cos−1(y)+cos−1(bxy)=2π
When you see 2π on the right-hand side, your mind should immediately race to the complementary angle identity: sin−1(θ)+cos−1(θ)=2π. This is our golden key.
By rearranging our original equation to cos−1(y)+cos−1(bxy)=2π−sin−1(ax), we can instantly transform the right side into cos−1(ax). Now, our equation is uniform:
cos−1(y)+cos−1(bxy)=cos−1(ax)
This uniformity is the first step toward victory.
Phase 2
The Substitution Strategy
Now, we have three inverse cosine terms. Let us simplify our mental load.
Let α=cos−1(y), β=cos−1(bxy), and γ=cos−1(ax). Our equation is now simply α+β=γ.
To get back to the algebraic world, we isolate β and take the cosine of both sides: cos(β)=cos(γ−α).
Using the expansion formula cos(γ−α)=cos(γ)cos(α)+sin(γ)sin(α), we translate our angles back into variables.
We know cos(β)=bxy, cos(γ)=ax, and cos(α)=y.
Recalling that sin(θ)=1−cos2(θ), we find sin(γ)=1−a2x2 and sin(α)=1−y2.
Phase 3
The Radical Dance
Substituting these back, we get:
bxy=(ax)(y)+1−a2x21−y2
This looks intimidating, but do not panic. We isolate the radical term:
(b−a)xy=1−a2x21−y2
Now, we square both sides to eliminate the radicals. This gives us:
(b−a)2x2y2=(1−a2x2)(1−y2)
This is our master equation, the engine that will drive our solutions for all cases.
Phase 4
Unveiling the Geometry
Now, we test our specific cases. When a=1 and b=0, our equation becomes (0−1)2x2y2=(1−x2)(1−y2), which simplifies to x2y2=1−x2−y2+x2y2.
The x2y2 terms cancel out, leaving x2+y2=1, which is the unit circle.
When a=1 and b=1, the left side vanishes, leaving (1−x2)(1−y2)=0, which represents the lines x2=1 or y2=1.
Finally, when a=2 and b=2, we get 0=(1−4x2)(1−y2), leading to 4x2=1 or y2=1.
Each case reveals a distinct geometric shape. You see, the math was not trying to confuse you; it was trying to show you the hidden geometry of the plane. Keep practicing this systematic approach, and you will find that even the most daunting problems are just puzzles waiting to be solved.