Animated Solution for Mathematics - Vector Algebra: Let a^ and b^ be two unit vectors such that the angle between them is 4π. If θ is the angle between the vectors (a^+b^) and (a^+2b^+2(a^×b^)), then the value of 164cos2θ is equal to :
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Visualized Solution
Defining the Unit Vectors
Given unit vectors: ∣a^∣=1,∣b^∣=1
Angle between them: ϕ=4π
Dot and Cross Products
a^⋅b^=∣a^∣∣b^∣cos(4π)=21
∣a^×b^∣=∣a^∣∣b^∣sin(4π)=21
Defining Vector u and its Magnitude
Let u=a^+b^
∣u∣2=∣a^∣2+∣b^∣2+2(a^⋅b^)
∣u∣2=1+1+2(21)=2+2
Defining Vector v
Let v=a^+2b^+2(a^×b^)
In-plane component: (a^+2b^)
Perpendicular component: 2(a^×b^)
Magnitude Square of v
Since (a^+2b^)⊥(a^×b^):
∣v∣2=∣a^+2b^∣2+∣2(a^×b^)∣2
∣a^+2b^∣2=1+4+4(21)=5+22
∣2(a^×b^)∣2=4(21)=2
∣v∣2=7+22
Dot Product u⋅v
u⋅v=(a^+b^)⋅(a^+2b^+2(a^×b^))
Since u⊥(a^×b^), u⋅(a^×b^)=0
u⋅v=∣a^∣2+3(a^⋅b^)+2∣b^∣2
u⋅v=1+23+2=3+23
Setting up cos2θ
cos2θ=∣u∣2∣v∣2(u⋅v)2
cos2θ=(2+2)(7+22)(3+23)2
Simplifying the Expression
Numerator: (3+23)2=9(1+21)2=29(3+22)
Denominator: (2+2)(7+22)=14+42+72+4=18+112
cos2θ=2(18+112)9(3+22)
Rationalizing the Denominator
Multiply by conjugate: 18−11218−112
Denominator: 2(182−(112)2)=2(324−242)=164
Numerator: 9(3+22)(18−112)=9(54−332+362−44)
Numerator =9(10+32)=90+272
Final Calculation
cos2θ=16490+272
164cos2θ=90+272
Final Answer:90+272
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The Sigma Insight: Vector (Cross) Product
Solution Diagram
Analyzing the Setup
Welcome, future engineer. Today, we are not just solving a vector problem; we are exploring the architecture of space itself.
When you look at the unit vectors a^ and b^, do not just see symbols. See two unit-length arrows originating from the origin, locked in a dance at an angle of 4π.
Our goal is to find the angle θ between two composite vectors, u and v. This is a classic JEE Advanced challenge—it tests your ability to bridge the gap between abstract algebra and geometric intuition.
The Foundation
We begin by defining our vectors. We have u=a^+b^. This vector is the diagonal of the parallelogram formed by a^ and b^, and it lies entirely within the plane defined by these two vectors.
Then we have v=a^+2b^+2(a^×b^). The term 2(a^×b^) is the "outlier." It is the vector that breaks the symmetry of the plane, pointing perpendicularly into the third dimension.
The Power of Orthogonality
To find cosθ, we need the dot product u⋅v and the magnitudes ∣u∣ and ∣v∣. Let us tackle the dot product first:
u⋅v=(a^+b^)⋅(a^+2b^+2(a^×b^))
Because u lies in the plane of a^ and b^, and (a^×b^) is perpendicular to that plane, their dot product is zero. The cross product term vanishes entirely.
We are left with:
u⋅v=(a^+b^)⋅(a^+2b^)=∣a^∣2+3(a^⋅b^)+2∣b^∣2
Substituting ∣a^∣=1, ∣b^∣=1, and a^⋅b^=cos(4π)=21, we find:
u⋅v=1+23+2=3+23
The Magnitude Calculation
For u, the magnitude squared is:
∣u∣2=∣a^∣2+∣b^∣2+2(a^⋅b^)=1+1+2(21)=2+2
For v, we use the Pythagorean theorem because the in-plane component (a^+2b^) and the perpendicular component 2(a^×b^) are orthogonal:
∣v∣2=∣a^+2b^∣2+∣2(a^×b^)∣2
Calculating the components:
∣a^+2b^∣2=∣a^∣2+4∣b^∣2+4(a^⋅b^)=1+4+4(21)=5+22
∣2(a^×b^)∣2=4∣a^∣2∣b^∣2sin2(4π)=4(1)(1)(21)=2
Thus, ∣v∣2=5+22+2=7+22.
The Grand Finale
We use the definition cos2θ=∣u∣2∣v∣2(u⋅v)2. Substituting our values:
cos2θ=(2+2)(7+22)(3+23)2
Expanding the numerator:
(3+23)2=9+29+2(3)(23)=13.5+92=227+182
Expanding the denominator:
(2+2)(7+22)=14+42+72+4=18+112
After algebraic simplification, the expression for 164cos2θ yields the final result: