Visualizing the Vectors in Space
Imagine you are standing in a three-dimensional coordinate system. Let's look at the two vectors given to us.
Vector A=i^+j^+k^ has components in all three directions: x, y, and z. It points diagonally outwards into space.
On the other hand, vector B=i^+j^ only has components in the x and y directions. This means it lies perfectly flat on the floor, which is the xy-plane.
The Master Equation for Projection
Our goal is to find the vector projection of A onto B. Think of this geometrically: if you were to shine a light straight down from the tip of vector A onto the line created by vector B, the shadow it casts is our projection.
Mathematically, the formula for the vector projection of A on B is given by:
This formula might look intimidating, but it is incredibly logical. The term ∣B∣A⋅B gives us the length of the shadow (the scalar projection). We then divide by another ∣B∣ and multiply by the vector B itself to give that shadow the correct direction.
Executing the Dot Product
Let's carefully substitute our known vectors into this formula. First, we need the dot product of the two vectors.
Remember, the dot product simply multiplies the corresponding components of each vector.
- The i^ components give 1×1=1.
- The j^ components give 1×1=1.
- Vector B has no k^ component (it is 0k^), so that gives 1×0=0.
Adding these up:
Finding the Magnitude Squared
Next, we evaluate the denominator, which is the magnitude squared of vector B. The magnitude squared is simply the sum of the squares of its components.
Since vector B=i^+j^, we square its coefficients:
The Final Calculation
We are at the final step. Let's plug our results back into the master projection formula. We have the dot product (2) divided by the magnitude squared (2).
The fraction simplifies perfectly to 1. This scalar multiplies our vector B.
ProjBA=1×(i^+j^)=i^+j^
This is our final projected vector.
Take a moment to appreciate what just happened. The projection of vector A onto B turned out to be exactly vector B itself! Geometrically, because A is just B plus an extra k^ component, dropping a perpendicular from A straight down to the xy-plane lands perfectly on the tip of B. Beautiful, isn't it?