Given that a ⃗ \vec{a} a and b ⃗ \vec{b} b are two unit vectors such that a ⃗ ⋅ b ⃗ = 0 \vec{a} \cdot \vec{b} = 0 a ⋅ b = 0 , we have:
∣ a ⃗ ∣ = 1 , ∣ b ⃗ ∣ = 1 , and a ⃗ ⋅ b ⃗ = 0 |\vec{a}| = 1, \quad |\vec{b}| = 1, \quad \text{and} \quad \vec{a} \cdot \vec{b} = 0 ∣ a ∣ = 1 , ∣ b ∣ = 1 , and a ⋅ b = 0
The magnitude of the cross product a ⃗ × b ⃗ \vec{a} \times \vec{b} a × b is given by:
∣ a ⃗ × b ⃗ ∣ = ∣ a ⃗ ∣ ∣ b ⃗ ∣ sin ( π 2 ) = 1 |\vec{a} \times \vec{b}| = |\vec{a}||\vec{b}|\sin\left(\frac{\pi}{2}\right) = 1 ∣ a × b ∣ = ∣ a ∣∣ b ∣ sin ( 2 π ) = 1
Furthermore, the vectors a ⃗ \vec{a} a , b ⃗ \vec{b} b , and a ⃗ × b ⃗ \vec{a} \times \vec{b} a × b are mutually orthogonal unit vectors, forming an orthonormal basis.
We are given the vector c ⃗ \vec{c} c :
c ⃗ = x a ⃗ + y b ⃗ + ( a ⃗ × b ⃗ ) \vec{c} = x\vec{a} + y\vec{b} + (\vec{a} \times \vec{b}) c = x a + y b + ( a × b )
Taking the magnitude squared on both sides:
∣ c ⃗ ∣ 2 = x 2 ∣ a ⃗ ∣ 2 + y 2 ∣ b ⃗ ∣ 2 + ∣ a ⃗ × b ⃗ ∣ 2 |\vec{c}|^2 = x^2 |\vec{a}|^2 + y^2 |\vec{b}|^2 + |\vec{a} \times \vec{b}|^2 ∣ c ∣ 2 = x 2 ∣ a ∣ 2 + y 2 ∣ b ∣ 2 + ∣ a × b ∣ 2
Given that ∣ c ⃗ ∣ = 2 |\vec{c}| = 2 ∣ c ∣ = 2 , we substitute the magnitudes:
2 2 = x 2 ( 1 ) + y 2 ( 1 ) + 1 2 2^2 = x^2(1) + y^2(1) + 1^2 2 2 = x 2 ( 1 ) + y 2 ( 1 ) + 1 2
4 = x 2 + y 2 + 1 ⟹ x 2 + y 2 = 3 — (1) 4 = x^2 + y^2 + 1 \implies x^2 + y^2 = 3 \quad \text{--- (1)} 4 = x 2 + y 2 + 1 ⟹ x 2 + y 2 = 3 — (1)
Next, taking the dot product of c ⃗ \vec{c} c with a ⃗ \vec{a} a :
c ⃗ ⋅ a ⃗ = ( x a ⃗ + y b ⃗ + a ⃗ × b ⃗ ) ⋅ a ⃗ = x ( a ⃗ ⋅ a ⃗ ) + y ( b ⃗ ⋅ a ⃗ ) + ( a ⃗ × b ⃗ ) ⋅ a ⃗ = x \vec{c} \cdot \vec{a} = (x\vec{a} + y\vec{b} + \vec{a} \times \vec{b}) \cdot \vec{a} = x(\vec{a} \cdot \vec{a}) + y(\vec{b} \cdot \vec{a}) + (\vec{a} \times \vec{b}) \cdot \vec{a} = x c ⋅ a = ( x a + y b + a × b ) ⋅ a = x ( a ⋅ a ) + y ( b ⋅ a ) + ( a × b ) ⋅ a = x
Since the vector c ⃗ \vec{c} c makes an angle α \alpha α with a ⃗ \vec{a} a :
c ⃗ ⋅ a ⃗ = ∣ c ⃗ ∣ ∣ a ⃗ ∣ cos α = 2 ⋅ 1 ⋅ cos α = 2 cos α \vec{c} \cdot \vec{a} = |\vec{c}||\vec{a}|\cos \alpha = 2 \cdot 1 \cdot \cos \alpha = 2 \cos \alpha c ⋅ a = ∣ c ∣∣ a ∣ cos α = 2 ⋅ 1 ⋅ cos α = 2 cos α
Equating the two expressions for c ⃗ ⋅ a ⃗ \vec{c} \cdot \vec{a} c ⋅ a :
x = 2 cos α x = 2 \cos \alpha x = 2 cos α
Similarly, taking the dot product of c ⃗ \vec{c} c with b ⃗ \vec{b} b :
c ⃗ ⋅ b ⃗ = ( x a ⃗ + y b ⃗ + a ⃗ × b ⃗ ) ⋅ b ⃗ = y \vec{c} \cdot \vec{b} = (x\vec{a} + y\vec{b} + \vec{a} \times \vec{b}) \cdot \vec{b} = y c ⋅ b = ( x a + y b + a × b ) ⋅ b = y
Since c ⃗ \vec{c} c also makes an angle α \alpha α with b ⃗ \vec{b} b :
c ⃗ ⋅ b ⃗ = ∣ c ⃗ ∣ ∣ b ⃗ ∣ cos α = 2 cos α \vec{c} \cdot \vec{b} = |\vec{c}||\vec{b}|\cos \alpha = 2 \cos \alpha c ⋅ b = ∣ c ∣∣ b ∣ cos α = 2 cos α
Thus, we have:
y = 2 cos α y = 2 \cos \alpha y = 2 cos α
Now, substituting x = 2 cos α x = 2 \cos \alpha x = 2 cos α and y = 2 cos α y = 2 \cos \alpha y = 2 cos α into equation (1):
( 2 cos α ) 2 + ( 2 cos α ) 2 = 3 (2\cos \alpha)^2 + (2\cos \alpha)^2 = 3 ( 2 cos α ) 2 + ( 2 cos α ) 2 = 3
4 cos 2 α + 4 cos 2 α = 3 4\cos^2 \alpha + 4\cos^2 \alpha = 3 4 cos 2 α + 4 cos 2 α = 3
8 cos 2 α = 3 8\cos^2 \alpha = 3 8 cos 2 α = 3