Animated Solution for Mathematics - Vector Algebra: Let a=i^+2j^+k^,b=3i^−j^+3k^,c=2i^−j^+2k^ and d be a vector such that b×d=c×d and a⋅d=4. Then ∣(a×d)∣2 is equal to ______ .
Enter Numerical Value:
Visualized Solution
The Vector Space
Let's visualize the coordinate system and the given vectors.
Analyze the Cross Product Equation
Given: b×d=c×d
Rearranging: b×d−c×d=0
Distributive property: (b−c)×d=0
Interpret the Parallel Condition
If u×v=0, then u∥v.
Therefore, d∥(b−c).
We can write: d=λ(b−c).
Calculate the Difference Vector b−c
b−c=(3−2)i^+(−1−1)j^+(3−2)k^
b−c=i^−2j^+k^
Express d in Terms of λ
Since d=λ(b−c)
d=λ(i^−2j^+k^)
Apply the Dot Product Condition
We are given another condition: a⋅d=4
Vector a=i^+2j^+k^
Substitute Vectors into Dot Product
(i^+2j^+k^)⋅λ(i^−2j^+k^)=4
Evaluate the Dot Product
λ[(1)(1)+(2)(−2)+(1)(1)]=4
λ[1−4+1]=4
Solve for λ
λ(−2)=4
λ=−2
Find the Exact Vector d
d=−2(i^−2j^+k^)
d=−2i^+4j^−2k^
Introduce Lagrange's Identity
We need to find ∣a×d∣2.
Using Lagrange's Identity:
∣a×d∣2=∣a∣2∣d∣2−(a⋅d)2
Calculate Squared Magnitudes
∣a∣2=(1)2+(2)2+(1)2=1+4+1=6
∣d∣2=(−2)2+(4)2+(−2)2=4+16+4=24
Substitute into Lagrange's Identity
∣a×d∣2=(6)(24)−(4)2
Final Computation
∣a×d∣2=144−16
∣a×d∣2=128
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The Sigma Insight: Vector (Cross) Product
Solution Diagram
Analyzing the Setup
Welcome, fellow traveler on the path to JEE mastery! Today, we are going to unravel a beautiful puzzle involving vectors. Imagine you are standing in a three-dimensional coordinate system with three known vectors, a, b, and c, and one mysterious vector, d.
We are given two clues about d: a cross product relationship and a dot product constraint. Our mission is to find the squared magnitude of the cross product of a and d.
Let us begin by examining the first clue: b×d=c×d. If we bring everything to one side, we get b×d−c×d=0.
By the distributive property of the cross product, this simplifies to (b−c)×d=0. This is a profound geometric statement! When the cross product of two vectors is the zero vector, it implies that the vectors are parallel.
Thus, our mysterious vector d must be parallel to the vector (b−c). We can express this as d=λ(b−c), where λ is a scalar constant.
Calculating the Direction
First, let us find the vector (b−c). Following the logic provided in the problem steps, we utilize the vector difference:
(b−c)=i^−2j^+k^
Consequently, we define our vector d in terms of the scalar λ:
d=λ(i^−2j^+k^)
The Dot Product Constraint
Now, we use the second clue: a⋅d=4. With a=i^+2j^+k^, we substitute our expression for d:
(i^+2j^+k^)⋅λ(i^−2j^+k^)=4
This expands to the following scalar equation:
λ[(1)(1)+(2)(−2)+(1)(1)]=4
Simplifying the terms inside the bracket, we get:
λ[1−4+1]=4⇒−2λ=4
Thus, we find the value of the scalar constant:
λ=−2
Substituting this back, our vector d is:
d=−2(i^−2j^+k^)=−2i^+4j^−2k^
The Elegant Shortcut
We need to calculate ∣a×d∣2. Instead of computing the cross product directly, we use Lagrange's Identity:
∣a×d∣2=∣a∣2∣d∣2−(a⋅d)2
First, we calculate the squared magnitudes:
∣a∣2=12+22+12=6
∣d∣2=(−2)2+42+(−2)2=4+16+4=24
Finally, substituting these values into the identity:
∣a×d∣2=(6)(24)−(4)2
∣a×d∣2=144−16=128
And there we have it! The final result is 128. Keep practicing, and remember that every vector problem is just a story waiting to be told.