To find the value of ∣ 3 u ⃗ + 5 v ⃗ ∣ |3 \vec{u} + 5 \vec{v}| ∣3 u + 5 v ∣ , we first determine the dot product u ⃗ ⋅ v ⃗ \vec{u} \cdot \vec{v} u ⋅ v .
Given data:
u ⃗ \vec{u} u and v ⃗ \vec{v} v are unit vectors, so ∣ u ⃗ ∣ = 1 |\vec{u}| = 1 ∣ u ∣ = 1 and ∣ v ⃗ ∣ = 1 |\vec{v}| = 1 ∣ v ∣ = 1 , which implies:
u ⃗ ⋅ u ⃗ = 1 and v ⃗ ⋅ v ⃗ = 1 \vec{u} \cdot \vec{u} = 1 \quad \text{and} \quad \vec{v} \cdot \vec{v} = 1 u ⋅ u = 1 and v ⋅ v = 1
u ⃗ \vec{u} u and v ⃗ \vec{v} v are not orthogonal, so u ⃗ ⋅ v ⃗ ≠ 0 \vec{u} \cdot \vec{v} \neq 0 u ⋅ v = 0 . Let u ⃗ ⋅ v ⃗ = x \vec{u} \cdot \vec{v} = x u ⋅ v = x .
Given scalar products involving w ⃗ \vec{w} w :
u ⃗ ⋅ w ⃗ = 1 , v ⃗ ⋅ w ⃗ = 1 , w ⃗ ⋅ w ⃗ = 4 \vec{u} \cdot \vec{w} = 1, \quad \vec{v} \cdot \vec{w} = 1, \quad \vec{w} \cdot \vec{w} = 4 u ⋅ w = 1 , v ⋅ w = 1 , w ⋅ w = 4
The volume V V V of the parallelopiped formed by u ⃗ \vec{u} u , v ⃗ \vec{v} v , and w ⃗ \vec{w} w is given as 2 \sqrt{2} 2 .
The square of the volume of the parallelopiped V 2 V^2 V 2 is equal to the Gram determinant of the vectors u ⃗ \vec{u} u , v ⃗ \vec{v} v , and w ⃗ \vec{w} w :
V 2 = [ u ⃗ v ⃗ w ⃗ ] 2 = ∣ u ⃗ ⋅ u ⃗ u ⃗ ⋅ v ⃗ u ⃗ ⋅ w ⃗ v ⃗ ⋅ u ⃗ v ⃗ ⋅ v ⃗ v ⃗ ⋅ w ⃗ w ⃗ ⋅ u ⃗ w ⃗ ⋅ v ⃗ w ⃗ ⋅ w ⃗ ∣ V^2 = [\vec{u} \ \vec{v} \ \vec{w}]^2 = \begin{vmatrix} \vec{u} \cdot \vec{u} & \vec{u} \cdot \vec{v} & \vec{u} \cdot \vec{w} \\ \vec{v} \cdot \vec{u} & \vec{v} \cdot \vec{v} & \vec{v} \cdot \vec{w} \\ \vec{w} \cdot \vec{u} & \vec{w} \cdot \vec{v} & \vec{w} \cdot \vec{w} \end{vmatrix} V 2 = [ u v w ] 2 = u ⋅ u v ⋅ u w ⋅ u u ⋅ v v ⋅ v w ⋅ v u ⋅ w v ⋅ w w ⋅ w
Substituting V = 2 V = \sqrt{2} V = 2 and the given dot products into the matrix:
( 2 ) 2 = ∣ 1 x 1 x 1 1 1 1 4 ∣ (\sqrt{2})^2 = \begin{vmatrix} 1 & x & 1 \\ x & 1 & 1 \\ 1 & 1 & 4 \end{vmatrix} ( 2 ) 2 = 1 x 1 x 1 1 1 1 4
Now, expand the determinant along the first row:
2 = 1 ⋅ ( 1 ⋅ 4 − 1 ⋅ 1 ) − x ⋅ ( x ⋅ 4 − 1 ⋅ 1 ) + 1 ⋅ ( x ⋅ 1 − 1 ⋅ 1 ) 2 = 1 \cdot (1 \cdot 4 - 1 \cdot 1) - x \cdot (x \cdot 4 - 1 \cdot 1) + 1 \cdot (x \cdot 1 - 1 \cdot 1) 2 = 1 ⋅ ( 1 ⋅ 4 − 1 ⋅ 1 ) − x ⋅ ( x ⋅ 4 − 1 ⋅ 1 ) + 1 ⋅ ( x ⋅ 1 − 1 ⋅ 1 )
2 = 1 ( 4 − 1 ) − x ( 4 x − 1 ) + 1 ( x − 1 ) 2 = 1(4 - 1) - x(4x - 1) + 1(x - 1) 2 = 1 ( 4 − 1 ) − x ( 4 x − 1 ) + 1 ( x − 1 )
2 = 3 − 4 x 2 + x + x − 1 2 = 3 - 4x^2 + x + x - 1 2 = 3 − 4 x 2 + x + x − 1
2 = 2 − 4 x 2 + 2 x 2 = 2 - 4x^2 + 2x 2 = 2 − 4 x 2 + 2 x
Simplifying the equation:
4 x 2 − 2 x = 0 4x^2 - 2x = 0 4 x 2 − 2 x = 0
2 x ( 2 x − 1 ) = 0 2x(2x - 1) = 0 2 x ( 2 x − 1 ) = 0
Since u ⃗ \vec{u} u and v ⃗ \vec{v} v are not orthogonal, x = u ⃗ ⋅ v ⃗ ≠ 0 x = \vec{u} \cdot \vec{v} \neq 0 x = u ⋅ v = 0 . Therefore:
2 x − 1 = 0 ⟹ x = 1 2 2x - 1 = 0 \implies x = \frac{1}{2} 2 x − 1 = 0 ⟹ x = 2 1
Thus, u ⃗ ⋅ v ⃗ = 1 2 \vec{u} \cdot \vec{v} = \frac{1}{2} u ⋅ v = 2 1 .
Now, we evaluate the magnitude ∣ 3 u ⃗ + 5 v ⃗ ∣ |3 \vec{u} + 5 \vec{v}| ∣3 u + 5 v ∣ :
∣ 3 u ⃗ + 5 v ⃗ ∣ 2 = ( 3 u ⃗ + 5 v ⃗ ) ⋅ ( 3 u ⃗ + 5 v ⃗ ) |3 \vec{u} + 5 \vec{v}|^2 = (3 \vec{u} + 5 \vec{v}) \cdot (3 \vec{u} + 5 \vec{v}) ∣3 u + 5 v ∣ 2 = ( 3 u + 5 v ) ⋅ ( 3 u + 5 v )
∣ 3 u ⃗ + 5 v ⃗ ∣ 2 = 9 ( u ⃗ ⋅ u ⃗ ) + 25 ( v ⃗ ⋅ v ⃗ ) + 30 ( u ⃗ ⋅ v ⃗ ) |3 \vec{u} + 5 \vec{v}|^2 = 9(\vec{u} \cdot \vec{u}) + 25(\vec{v} \cdot \vec{v}) + 30(\vec{u} \cdot \vec{v}) ∣3 u + 5 v ∣ 2 = 9 ( u ⋅ u ) + 25 ( v ⋅ v ) + 30 ( u ⋅ v )
Substitute the known values:
∣ 3 u ⃗ + 5 v ⃗ ∣ 2 = 9 ( 1 ) + 25 ( 1 ) + 30 ( 1 2 ) |3 \vec{u} + 5 \vec{v}|^2 = 9(1) + 25(1) + 30\left(\frac{1}{2}\right) ∣3 u + 5 v ∣ 2 = 9 ( 1 ) + 25 ( 1 ) + 30 ( 2 1 )
∣ 3 u ⃗ + 5 v ⃗ ∣ 2 = 9 + 25 + 15 = 49 |3 \vec{u} + 5 \vec{v}|^2 = 9 + 25 + 15 = 49 ∣3 u + 5 v ∣ 2 = 9 + 25 + 15 = 49
Taking the positive square root on both sides:
∣ 3 u ⃗ + 5 v ⃗ ∣ = 49 = 7 |3 \vec{u} + 5 \vec{v}| = \sqrt{49} = 7 ∣3 u + 5 v ∣ = 49 = 7