Animated Solution for Mathematics - Vector Algebra: For any two vectors u and v, prove that (a) (u⋅v)2+∣u×v∣2=∣u∣2∣v∣2 and (b) (1+∣u∣2)(1+∣v∣2)=(1−u⋅v)2+∣u+v+(u×v)∣2.
Visualized Solution
Visualizing the Vectors
Consider two vectors u and v in a plane.
Let θ be the angle between them, where 0≤θ≤π.
The Cross Product Vector
The cross product u×v is a vector perpendicular to the plane containing u and v.
Defining the Dot Product
The dot product is defined as:
u⋅v=∣u∣∣v∣cosθ
Defining the Cross Product Magnitude
The magnitude of the cross product is:
∣u×v∣=∣u∣∣v∣sinθ
Squaring and Adding Terms
LHS of part (a): (u⋅v)2+∣u×v∣2
Substitute the definitions:
(∣u∣∣v∣cosθ)2+(∣u∣∣v∣sinθ)2
Factoring and Trigonometric Identity
Factor out the common terms:
∣u∣2∣v∣2(cos2θ+sin2θ)
Using the identity sin2θ+cos2θ=1:
∣u∣2∣v∣2(1)=∣u∣2∣v∣2
Conclusion of Part (a)
Thus, we have proven Lagrange's Identity:
(u⋅v)2+∣u×v∣2=∣u∣2∣v∣2
Starting Part (b) - Expanding RHS
RHS of part (b): (1−u⋅v)2+∣u+v+(u×v)∣2
Let's expand the second term using ∣A+B∣2=∣A∣2+∣B∣2+2A⋅B
Let A=u+v and B=u×v
Applying Vector Magnitude Property
Expanding the second term:
∣u+v∣2+∣u×v∣2+2(u+v)⋅(u×v)
The Perpendicularity Trick
Recall that u×v is perpendicular to both u and v.
Therefore, it is perpendicular to their sum: (u+v)⋅(u×v)=0
Next Challenge: Explore the Vector Triple Product a×(b×c) and its related identities.
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The Sigma Insight: Vector (Cross) Product
Solution Diagram
Analyzing the Geometric Harmony
Imagine you are standing in a 3D space with two vectors, u and v, originating from the same point. Let θ be the angle between them.
We know the dot product, u⋅v=∣u∣∣v∣cosθ, measures how much these vectors 'agree' with each other. Conversely, the cross product magnitude, ∣u×v∣=∣u∣∣v∣sinθ, measures the area of the parallelogram they span.
Now, consider the expression (u⋅v)2+∣u×v∣2. If we substitute our definitions, we obtain:
(∣u∣∣v∣cosθ)2+(∣u∣∣v∣sinθ)2
The common factor ∣u∣2∣v∣2 is waiting to be pulled out. Once we factor it, we are left with (cos2θ+sin2θ).
Since this is the fundamental identity of trigonometry, which equals 1, we arrive at the elegant Lagrange's Identity:
(u⋅v)2+∣u×v∣2=∣u∣2∣v∣2
This is the Pythagorean theorem manifesting in vector space. It confirms that the square of the projection and the square of the perpendicular area always sum to the square of the product of the magnitudes.
The Grand Expansion
Now, let us tackle the second expression: (1−u⋅v)2+∣u+v+(u×v)∣2. In JEE Advanced, complexity is often just a mask for simplicity.
Let us focus on the second term. We treat A=(u+v) and B=(u×v) as two distinct entities. Using the expansion ∣A+B∣2=∣A∣2+∣B∣2+2A⋅B, we get:
∣u+v∣2+∣u×v∣2+2(u+v)⋅(u×v)
Here is the 'Aha!' moment. The vector (u×v) is, by definition, perpendicular to the plane containing u and v.
Therefore, it is perpendicular to their sum (u+v). The dot product 2(u+v)⋅(u×v) vanishes into thin air, leaving us with:
∣u+v∣2+∣u×v∣2
The Final Convergence
Now, we expand the remaining pieces. Expanding (1−u⋅v)2 gives us 1−2u⋅v+(u⋅v)2.
Expanding ∣u+v∣2 gives us ∣u∣2+∣v∣2+2u⋅v. When we combine everything, the −2u⋅v and +2u⋅v terms cancel out perfectly.
We are left with:
1+∣u∣2+∣v∣2+(u⋅v)2+∣u×v∣2
Look closely at the last two terms. They are exactly what we solved in Part (a). Replacing them with ∣u∣2∣v∣2, we get:
1+∣u∣2+∣v∣2+∣u∣2∣v∣2
With one final act of factoring by grouping, we pull out (1+∣u∣2) to reach the final result:
(1+∣u∣2)(1+∣v∣2)
You have just proven that these vectors, no matter how they are oriented, obey a beautiful, rigid logic. Keep that curiosity alive, and you will conquer any problem the exam throws at you.