Animated Solution for Mathematics - Vector Algebra: If u,v,w are non-coplanar vectors and p,q are real numbers, then the equality [3upvpw]−[pvwqu]−[2wqvqu]=0 holds for :
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Visualized Solution
Visualizing Non-Coplanar Vectors
Given vectors u,v,w are non-coplanar.
This implies they form a parallelepiped with non-zero volume.
Mathematically: [uvw]=0.
Properties of Scalar Triple Product
Linearity:[kalbmc]=klm[abc] where k,l,m are scalars.
Cyclic Symmetry:[uvw]=[vwu]=[wuv].
Anti-Symmetry:[wvu]=−[uvw] (due to one swap).
Expanding the First Term
First term: [3upvpw]
Pull out scalars: (3)⋅(p)⋅(p)[uvw]
Simplified: 3p2[uvw]
Expanding the Second Term
Second term: [pvwqu]
Pull out scalars: (p)⋅(1)⋅(q)[vwu]
Using cyclic property: [vwu]=[uvw]
Simplified: pq[uvw]
Expanding the Third Term
Third term: [2wqvqu]
Pull out scalars: (2)⋅(q)⋅(q)[wvu]
Using anti-cyclic property: [wvu]=−[uvw]
Simplified: −2q2[uvw]
Combining the Terms
Substitute terms into the equation:
3p2[uvw]−pq[uvw]−(−2q2[uvw])=0
Factor out [uvw]:
(3p2−pq+2q2)[uvw]=0
The Non-Coplanar Condition
We have (3p2−pq+2q2)[uvw]=0.
Since u,v,w are non-coplanar, [uvw]=0.
Therefore, the scalar coefficient must be zero:
3p2−pq+2q2=0
Analyzing the Quadratic Equation
To solve 3p2−pq+2q2=0, complete the square:
2p2+(p2−pq+4q2)+47q2=0
2p2+(p−2q)2+47q2=0
Since p,q are real, each squared term is ≥0.
Final Conclusion
For the sum to be zero, each term must be zero:
1) 2p2=0⇒p=0
2) 47q2=0⇒q=0
3) (p−2q)2=(0−0)2=0 (Consistent)
The only solution is (p,q)=(0,0).
Correct Option: exactly one value of (p,q)
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The Sigma Insight: Scalar Triple Product
Solution Diagram
Analyzing the Setup
Imagine you are standing in a three-dimensional room. You have three vectors, u, v, and w, originating from the corner of the floor.
If they were coplanar, they would lie flat on the floor, and the volume they enclose would be zero. However, the problem specifies that they are non-coplanar.
This means they reach out into the third dimension, forming a parallelepiped with a definite, non-zero volume. In the language of JEE Advanced, this is our anchor: the scalar triple product $[\vec{u} \ \vec{v} \ \vec{w}]
eq 0$. This is the key that will unlock the entire problem.
The Algebra of Symmetry
Before we touch the equation, let us sharpen our tools. The scalar triple product is not just a random collection of symbols; it is a highly structured operator.
We have three main properties:
1. Linearity, which allows us to pull scalar coefficients out of the box.
2. Cyclic Symmetry, which allows us to rotate the vectors without changing the value.
3. Anti-Symmetry, which forces a sign change if we swap two vectors.
Think of these as the laws of physics for our vector space.
Expanding the Terms
Let us break down the equation term by term. The first term is [3upvpw].
Using linearity, we extract the scalars 3, p, and p. This gives us:
3p2[uvw]
Now, consider the second term: [pvwqu]. We pull out p and q to obtain pq[vwu].
By applying cyclic symmetry, we know this is identical to [uvw]. So, we get:
pq[uvw]
Finally, the third term is [2wqvqu]. We extract 2, q, and q, leaving us with 2q2[wvu].
Here is the trap: the order is w,v,u. This is one swap away from u,v,w, so we must introduce a negative sign:
−2q2[uvw]
The Quadratic Revelation
Now, we combine these into our master equation:
3p2[uvw]−pq[uvw]−2q2[uvw]=0
Factoring out the common box product, we arrive at:
(3p2−pq−2q2)[uvw]=0
Since we established that the box product is non-zero, we are left with the scalar equation:
3p2−pq−2q2=0
Final Calculation
We can factor the quadratic expression 3p2−pq−2q2=0 as follows:
(3p+2q)(p−q)=0
This implies that either p=q or 3p=−2q.
If the problem implies that p and q are real constants, there are infinitely many pairs (p,q) satisfying this relationship. However, if the context requires a specific constraint or unique solution, one must verify the coefficients provided in the original prompt.
Based on the derived quadratic, the relationship between the variables is defined by the set of points lying on the lines p=q and 3p=−2q.