The problem of finding the angle between two vectors given a relationship between their sum and difference is a classic in kinematics and vector algebra. It tests your geometric intuition and your algebraic discipline. Let's dive into the fascinating physics and math behind this problem!
Visualizing the Vectors
Imagine you are standing at the origin of a coordinate system. You draw two vectors, x and y, starting from where you stand.
The problem states that these two vectors have the exact same magnitude. If you were to complete the parallelogram formed by these two vectors, you wouldn't just get any parallelogram—you would get a rhombus.
In this rhombus, the diagonal starting from the origin represents the vector sum, x+y. The other diagonal, connecting the tips of the two vectors, represents the vector difference, x−y.
The Master Equation
We are given a very specific constraint: the magnitude of the difference is n times the magnitude of the sum.
Mathematically, this is written as:
∣x−y∣=n∣x+y∣
Dealing with magnitudes directly often involves square roots, which can be messy. To make our lives easier, we square both sides of the equation:
∣x−y∣2=n2∣x+y∣2
The Power of the Parallelogram Law
Now, we bring in the heavy artillery: the Parallelogram Law of Vector Addition.
The squared magnitude of the sum of two vectors is given by:
∣x+y∣2=x2+y2+2xycosθ
Similarly, the squared magnitude of their difference is:
∣x−y∣2=x2+y2−2xycosθ
Substituting these into our squared constraint equation, we get:
x2+y2−2xycosθ=n2(x2+y2+2xycosθ)
Algebraic Simplification
This equation looks a bit intimidating, but remember our initial condition: the vectors have equal magnitudes! This means we can substitute y=x everywhere in the equation.
Let's see the magic happen:
x2+x2−2x2cosθ=n2(x2+x2+2x2cosθ)
Combining the like terms, we get:
2x2−2x2cosθ=n2(2x2+2x2cosθ)
Notice how every single term has a 2x2 in it? Assuming our vectors are non-zero (which is a safe assumption in such problems), we can divide the entire equation by 2x2.
This beautifully simplifies our equation to:
1−cosθ=n2(1+cosθ)
The Final Angle
We are now in the home stretch. Our goal is to isolate
cosθ. Let's expand the right side:
1−cosθ=n2+n2cosθ
Next, we group all the terms containing
cosθ on one side, and the constant terms on the other:
1−n2=cosθ+n2cosθ
Factoring out
cosθ on the right side gives:
1−n2=cosθ(1+n2)
Finally, we divide by
(1+n2) to completely isolate
cosθ:
cosθ=1+n21−n2
To find the angle
θ, we simply take the inverse cosine:
θ=cos−1(1+n21−n2)
And there we have it! A beautiful geometric relationship distilled into a clean algebraic result.