Use the identity: sin(2x)sin(29x)=1+2cos(x)+2cos(2x)+2cos(3x)+2cos(4x).
Part (D): Evaluating the Integral
Integrating term by term: ∫−ππ1dx=2π.
For all n≥1, ∫−ππcos(nx)dx=0.
So, I=2π. Required value: π2I=4.
Final Matching Summary
(A) → 6
(B) → -4, 4
(C) → 0, 5
(D) → 4
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The Sigma Insight: Fundamental Theorem & Properties of Definite Integrals
Solution Diagram
The JEE Marathon
A Journey Through Four Dimensions
Welcome, future engineers! Today, we are not just solving a problem; we are embarking on a grand tour of the JEE Advanced syllabus.
We have a multi-concept challenge that spans the vast landscapes of 3D Geometry, Inverse Trigonometry, Vector Algebra, and Calculus. Take a deep breath, as this is about seeing the connections between these domains.
Phase 1
The Geometry of Laser Beams
Imagine two laser beams crossing through space, defined by lines L1 and L2. We need to find a line from the origin that intersects both.
We define a point P on the first line using parameter λ as (2+λ,1−2λ,−1+λ). Similarly, we define point Q on the second line using μ as:
Q=(38+2μ,−3−μ,1+μ)
The origin O, P, and Q are collinear, meaning the direction ratios of OP and OQ must be proportional:
38+2μ2+λ=−3−μ1−2λ=1+μ−1+λ
Solving this system yields λ=3 and μ=31. Substituting these back gives the fixed points P(5,−5,2) and Q(310,−310,34). The distance squared, d2, between these two points is 6.
Phase 2
The Triangle of Truth
We face the inverse trigonometry equation: tan−1(x+3)−tan−1(x−3)=sin−1(53).
Visualize a right-angled triangle where the opposite side is 3 and the hypotenuse is 5. By the Pythagorean theorem, the adjacent side is 4, so sin−1(53)=tan−1(43).
Using the identity tan−1A−tan−1B=tan−1(1+ABA−B), we simplify the left side:
tan−1(1+(x+3)(x−3)(x+3)−(x−3))=tan−1(x2−86)
Equating the arguments, we get x2−86=43, which simplifies to x2=16. Thus, the solutions are x=±4.
Phase 3
The Vector Waltz
Given a=μb+4c and the condition a⋅b=0, we substitute a into the dot product:
(μb+4c)⋅b=0⇒b⋅c=−4μ∣b∣2
We then use the second condition, 2∣b+c∣=∣b−a∣. Squaring both sides and expanding, we substitute our dot product relationship.
The vector terms vanish, leaving us with the quadratic equation μ2−5μ=0. This yields the final values μ=0 or μ=5.
Phase 4
The Calculus Symphony
Finally, we tackle the integral I=π2∫−ππsin(2x)sin(29x)dx. This expression is a hidden trigonometric series: