Animated Solution for Mathematics - Vector Algebra: Let a, b and c be distinct positive numbers. If the vectors ai^+aj^+ck^,i^+k^ and ci^+cj^+bk^ are co-planar, then c is equal to:
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Visualized Solution
Defining the Vectors
Let the given vectors be:
u=ai^+aj^+ck^
v=1i^+0j^+1k^
w=ci^+cj^+bk^
Condition for Coplanarity
For three vectors to lie in the same plane, their Scalar Triple Product must be zero.
[uvw]=0
The Determinant Form
The scalar triple product is calculated using the determinant of their components.
a1ca0cc1b=0
Expanding Along Row 1
Let's expand the determinant along the first row.
First term: a(0⋅b−1⋅c)=a(0−c)
Expanding Along Row 1
Second term (remember the negative sign):
−a(1⋅b−1⋅c)=−a(b−c)
Expanding Along Row 1
Third term:
+c(1⋅c−0⋅c)=+c(c−0)
Assembling the Equation
Combining all the expanded terms:
a(−c)−a(b−c)+c(c)=0
Algebraic Expansion
Multiply the terms inside the brackets:
−ac−ab+ac+c2=0
Simplifying the Equation
Notice that −ac and +ac cancel each other out perfectly.
−ab+c2=0
Isolating c
Rearranging the equation to solve for c:
c2=ab
c=ab
Geometric Mean
The value of c is the Geometric Mean of a and b.
Final Answer:c=ab (Option 4)
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The Sigma Insight: Scalar Triple Product
Solution Diagram
The Geometry of Flatness
Understanding Coplanarity
Imagine you are standing in a vast, three-dimensional space. You have three vectors, u, v, and w, all originating from the same point.
Usually, these three vectors would reach out into space and define a volume—a parallelepiped. But today, the problem gives us a special condition: these vectors are coplanar.
They are trapped, forced to lie flat on a single two-dimensional plane. This is a powerful geometric constraint, meaning the volume of the parallelepiped they would otherwise form is exactly zero. This is the key to unlocking the problem.
The Mathematical Gatekeeper
The Scalar Triple Product
How do we translate this 'flatness' into algebra? We use the Scalar Triple Product, denoted as [uvw].
This product is the mathematical equivalent of calculating the volume of the parallelepiped formed by the vectors. If the volume is zero, the vectors are coplanar.
We define our vectors as u=ai^+aj^+ck^, v=1i^+0j^+1k^, and w=ci^+cj^+bk^. To find the scalar triple product, we arrange their components into a determinant:
a1ca0cc1b=0
This determinant is our master equation. It encapsulates the entire geometric reality of the problem.
The Expansion
Unveiling the Algebra
Now, let's expand this determinant along the first row. We must be meticulous with our signs.
We take the first element, a, and multiply it by the determinant of the remaining 2×2 matrix: 0c1b. This gives us a(0⋅b−1⋅c)=a(0−c)=−ac.
Next, we move to the second element, a, remembering the alternating sign convention (plus, minus, plus). So, we subtract a multiplied by the minor 1c1b, which is −a(1⋅b−1⋅c)=−a(b−c).
Finally, we add the third element, c, multiplied by its minor 1c0c, resulting in +c(1⋅c−0⋅c)=+c(c)=c2. Combining these, we get the equation:
−ac−a(b−c)+c2=0
The Elegance of Cancellation
Let's distribute the terms and watch the magic happen. Expanding −a(b−c) gives us −ab+ac.
Now, our full equation looks like this: −ac−ab+ac+c2=0. Look closely at the terms −ac and +ac; they are exact opposites and cancel each other out perfectly.
This leaves us with a beautifully simple expression:
−ab+c2=0
This is the moment where the complexity of the 3D geometry collapses into a simple algebraic relationship. We rearrange this to find c2=ab, which leads us directly to c=ab.
Conclusion
The Geometric Mean
We have arrived at our destination. The value of c is the square root of the product of a and b.
In the language of sequences and series, we recognize this as the Geometric Mean of a and b. This result is not just a number; it is the condition required for these three vectors to exist in perfect, flat harmony on a single plane.