Animated Solution for Mathematics - Vector Algebra: Let u=i^+j^,v=i^−j^ and w=i^+2j^+3k^. If n^ is a unit vector such that u⋅n^=0 and v⋅n^=0, then ∣w⋅n^∣ is equal to
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Visualized Solution
Given Vectors u and v
u=i^+j^
v=i^−j^
The Orthogonality Condition
u⋅n^=0
v⋅n^=0
This implies n^⊥u and n^⊥v
Direction of n^
A vector perpendicular to both u and v is given by their cross product.
n^=±∣u×v∣u×v
Setting up u×v
u×v=i^11j^1−1k^00
Evaluating the Cross Product
Expanding along the third column (k^):
u×v=k^[(1)(−1)−(1)(1)]
u×v=−2k^
Finding the Unit Vector n^
Magnitude: ∣u×v∣=02+02+(−2)2=2
n^=±2−2k^=±k^
Introducing Vector w
w=i^+2j^+3k^
We need to find ∣w⋅n^∣
Setting up the Dot Product
w⋅n^=(i^+2j^+3k^)⋅(±k^)
Computing w⋅n^
i^⋅k^=0, j^⋅k^=0, k^⋅k^=1
w⋅n^=(1)(0)+(2)(0)+(3)(±1)
w⋅n^=±3
The Final Answer
We need the absolute value: ∣w⋅n^∣
∣±3∣=3
Final Answer: 3
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The Sigma Insight: Vector (Cross) Product
Solution Diagram
The Geometry of Orthogonality
A Journey into 3D Space
Welcome, future engineer. Today, we are not just solving a vector problem; we are learning to navigate the architecture of 3D space.
When you look at vectors u=i^+j^ and v=i^−j^, I want you to see them as two lines drawn on a flat sheet of paper—the xy-plane. They are trapped in that two-dimensional world.
But the problem introduces a third vector, w=i^+2j^+3k^, which breaks free into the z-dimension. Our goal is to find the relationship between this 3D vector w and a mysterious unit vector n^ that is perpendicular to our original 2D plane.
Phase 1
The Search for the Normal
We are told that u⋅n^=0 and v⋅n^=0. In the language of physics and geometry, a dot product of zero is a signal. It screams orthogonality.
It tells us that n^ is standing perfectly upright, perpendicular to the plane formed by u and v.
How do we find a vector that is perpendicular to two others? We reach for the most powerful tool in our vector arsenal: the cross product.
The cross product u×v is specifically designed to generate a vector that is orthogonal to the plane containing u and v.
Phase 2
The Determinant Dance
Let us compute this cross product. We set up our determinant, the standard machinery for this operation:
u×v=i^11j^1−1k^00
I know determinants can look intimidating, but look at the structure. The third column is all zeros, except for the k^ component. This is a gift!
We expand along the third column:
u×v=k^[(1)(−1)−(1)(1)]=k^[−1−1]=−2k^
Just like that, the complexity collapses. We have found that the vector perpendicular to our plane is −2k^.
Phase 3
Normalizing the Vector
We are almost there. The problem asks for a unit vectorn^. A vector is only a unit vector if its magnitude is 1.
Our current vector, −2k^, has a magnitude of 2. To fix this, we divide by the magnitude:
n^=±2−2k^=±k^
Why the ±? Because a line perpendicular to a plane can point in two directions—up or down. Both are valid normals. This is the beauty of the math; it accounts for all possibilities.
Phase 4
The Final Projection
Now, we bring in our third vector, w=i^+2j^+3k^. We need to find the absolute value of the dot product ∣w⋅n^∣.
This is essentially asking: "How much of w lies along the direction of the normal vector n^?"
Substituting our values:
w⋅n^=(i^+2j^+3k^)⋅(±k^)
Using the properties of dot products, we know that i^⋅k^=0 and j^⋅k^=0. Only the k^ component survives the interaction:
w⋅n^=(3)(±1)=±3
Finally, we take the absolute value as requested:
∣±3∣=3
And there it is. The answer is 3. You have successfully navigated the 3D space, used the cross product to find a normal, and projected a vector onto that normal.