Animated Solution for Mathematics - Vector Algebra: Let a=2i^+5j^−k^, b=2i^−2j^+2k^ and c be three vectors such that (c+i^)×(a+b+i^)=a×(c+i^). If a⋅c=−29, then c⋅(−2i^+j^+k^) is equal to:
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Visualized Solution
Define Substitution p
Let p=c+i^
The given equation is: (c+i^)×(a+b+i^)=a×(c+i^)
By substituting p, we get: p×(a+b+i^)=a×p
Simplify Cross Product
Using a×p=−(p×a)
Equation becomes: p×(a+b+i^)=−(p×a)
Rearranging: p×(a+b+i^)+(p×a)=0
Combining terms: p×(a+b+i^+a)=0
The Parallel Condition
Simplified Equation: p×(2a+b+i^)=0
This implies p is parallel to (2a+b+i^)
So, p=λ(2a+b+i^) for some scalar λ
Calculate Sum Vector
Calculate 2a+b+i^:
2(2i^+5j^−k^)+(2i^−2j^+2k^)+i^
=(4i^+10j^−2k^)+(2i^−2j^+2k^)+i^
=(4+2+1)i^+(10−2)j^+(−2+2)k^
=7i^+8j^
Express c in terms of λ
Since p=λ(7i^+8j^), we have:
c+i^=λ(7i^+8j^)
c=(7λ−1)i^+8λj^
Apply Dot Product Condition
Given a⋅c=−29
(2i^+5j^−k^)⋅((7λ−1)i^+8λj^)=−29
2(7λ−1)+5(8λ)+(−1)(0)=−29
Solve for λ
14λ−2+40λ=−29
54λ=−27
λ=−5427=−21
Determine Vector c
Substitute λ=−21 into c:
c=(7(−21)−1)i^+8(−21)j^
c=(−27−1)i^−4j^
c=−29i^−4j^
Final Calculation
Calculate c⋅(−2i^+j^+k^):
(−29i^−4j^+0k^)⋅(−2i^+j^+k^)
=(−29)(−2)+(−4)(1)+(0)(1)
=9−4+0=5
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The Sigma Insight: Vector (Cross) Product
Solution Diagram
The Vector Landscape
A Journey of Simplification
Welcome, fellow explorer of the mathematical universe. Today, we are going to dismantle a vector problem that, at first glance, looks like a tangled mess of cross products and unknown variables.
But as we peel back the layers, you will see that it is actually a beautifully orchestrated dance of geometry and algebra. Let us begin by looking at the equation:
(c+i^)×(a+b+i^)=a×(c+i^)
Phase 1
The Power of Substitution
Whenever you see a repeating term in a complex equation, your intuition should scream 'substitution!' Notice how (c+i^) appears on both sides?
Let us define a new vector p=c+i^. Suddenly, the equation transforms into:
p×(a+b+i^)=a×p
This is much cleaner, isn't it? We have effectively reduced the noise, allowing us to focus on the core relationship between these vectors.
Phase 2
The Cross Product Dance
Now, we need to bring all our terms to one side to set the equation to zero. Remember the anti-commutative property of the cross product: a×p=−(p×a).
By applying this, our equation becomes:
p×(a+b+i^)+(p×a)=0
Because the cross product is distributive, we can combine these terms:
p×(a+b+i^+a)=0
This simplifies to:
p×(2a+b+i^)=0
Phase 3
The Geometric Insight
Here is the moment of truth. If the cross product of two vectors is the zero vector, they must be parallel. This means p is a scalar multiple of the vector (2a+b+i^).
Let us call this scalar λ. So, p=λ(2a+b+i^).
Now, let us calculate that resultant vector. Given a=2i^+5j^−k^ and b=2i^−2j^+2k^, we compute:
2a+b+i^=2(2i^+5j^−k^)+(2i^−2j^+2k^)+i^
Summing the components, we get:
(4+2+1)i^+(10−2)j^+(−2+2)k^=7i^+8j^
Phase 4
Solving for the Unknown
We now have c+i^=λ(7i^+8j^), which means c=(7λ−1)i^+8λj^. We are given a⋅c=−29.
Substituting our expressions, we get:
(2i^+5j^−k^)⋅((7λ−1)i^+8λj^)=−29
This simplifies to 2(7λ−1)+5(8λ)=−29. Solving this linear equation:
14λ−2+40λ=−29⇒54λ=−27⇒λ=−21
The Final Victory
With λ=−21, we find:
c=(7(−21)−1)i^+8(−21)j^=−29i^−4j^
Finally, we calculate the dot product c⋅(−2i^+j^+k^):
(−29)(−2)+(−4)(1)+(0)(1)=9−4=5
We have arrived at our answer: 5. You have successfully navigated the vector landscape!