Maximized Parallelepiped

Algebra Level 3

Let u ^ \hat{u} and v ^ \hat{v} be unit vectors and w \vec{w} be a vector such that w + ( w × u ^ ) \vec{w}+(\vec{w}\ \times \hat{u}) = = v ^ \hat{v} .

The angle in degrees between u ^ \hat{u} and v ^ \hat{v} such that ( u ^ × v ^ ) w |(\hat{u} \times \hat{v}) \cdot \vec{w}| is maximized is θ \theta and the maximum value of ( u ^ × v ^ ) w |(\hat{u} \times \hat{v}) \cdot \vec{w}| is M M . Find the value of θ + M \theta + M .

I m a g e Image C r e d i t : Credit : W i k i p e d i a Wikipedia


The answer is 90.5.

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2 solutions

Led Tasso
Aug 20, 2014

1 ) 1) w \vec{w} + + ( w × u ^ ) (\vec{w}\ \times \hat{u}) = = v ^ \hat{v}

Taking dot product on both sides by v ^ \hat{v} ,

2 ) 2) v ^ w \hat{v} \cdot \vec{w} + + v ^ ( w × u ^ ) \hat{v} \cdot (\vec{w} \times \hat{u}) = 1 = 1

Taking dot product of equation 1 ) 1) with u ^ \hat{u} ,

3 ) 3) u ^ w \hat{u} \cdot \vec{w} = = u ^ v ^ \hat{u} \cdot \hat{v}

Taking cross product of equation 1 ) 1) with u ^ \hat{u} ,

u ^ × w \hat{u} \times \vec{w} + + u ^ × ( w × u ^ ) \hat{u} \times (\vec{w} \times \hat{u}) = = u ^ × w \hat{u} \times \vec{w} + + w \vec{w} - ( u ^ w ) (\hat{u} \cdot \vec{w}) u ^ \hat{u} = = u ^ × v ^ \hat{u} \times \hat{v} . The last step comes from opening the vector triple product u ^ × ( w × u ^ ) \hat{u} \times (\vec{w} \times \hat{u})

Using equation 3 ) 3) , we get

u ^ × w \hat{u} \times \vec{w} + + w \vec{w} - ( u ^ v ^ ) (\hat{u} \cdot \hat{v}) u ^ \hat{u} = u ^ × v ^ \hat{u} \times \hat{v}

Taking dot proguct with v ^ \hat{v} ,

v ^ ( u ^ × w ) \hat{v} \cdot (\hat{u} \times \vec{w}) + + v ^ w \hat{v} \cdot \vec{w} - ( v ^ u ^ ) 2 ({\hat{v} \cdot \hat{u}})^2 = 0 = 0

Using equation 2 ) 2) ,

v ^ ( u ^ × w ) \hat{v} \cdot (\hat{u} \times \vec{w}) + 1 + 1 - v ^ ( w × u ^ ) \hat{v} \cdot (\vec{w} \times \hat{u}) - ( u ^ v ^ ) 2 ({\hat{u} \cdot \hat{v}})^2 = = 0 0

\Rightarrow 2 ( u ^ × v ^ ) w (\hat{u} \times \hat{v}) \cdot \vec{w} = = 1 1 - ( u ^ v ^ ) 2 ({\hat{u} \cdot \hat{v}})^2

Now it is easy to note that ( u ^ × v ^ ) w |(\hat{u} \times \hat{v}) \cdot \vec{w}| is maximized when u ^ v ^ \hat{u} \cdot \hat{v} is zero or θ = 9 0 \theta = 90^\circ and its maximum value is M = 0.5 M = 0.5 . Hence θ + M = 90.5 \theta + M = \boxed{90.5} .

If you have any queries, please ask in the comment box.

Beautiful solution. I just wanted to ask how did you think of the third and fourth step. I could only work out till second step and afterwards I couldn't think of anything further and saw the solution. Thanks.

Pranav Rao - 5 years, 4 months ago

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That time I was in 12th grade with the vectors chapter going on in my coaching. :P

And so it came out quite naturally.:D

Led Tasso - 5 years, 4 months ago

excellent brother

Md. Ibrahim Khandakar - 1 year, 3 months ago
Aditya Raut
Aug 22, 2014

( u ^ × v ^ ) w = u v sin θ w = w sin θ \left| (\hat{u} \times \hat{v} ) \cdot \vec{w} \right| = \left| uv \sin\theta w \right| = \left| w \sin \theta \right| .... where w w is magnitude of w \vec{w} .

This is maximum when sin θ \sin \theta is maximum, and it is at θ = 9 0 \theta = 90^\circ .

In the given first equation, think of the magnitudes on L H S LHS and R H S RHS .

( w × u ^ ) u = w sin θ 1 \left| (\vec{w} \times \hat{u}) \right| u = w \sin \theta_1 , let direction vector be x ^ \hat{x} , θ 1 \theta_1 is angle between vectors w and u.

v ^ = 1 | \hat{v} |= 1

Thus we have in LHS, magnitude of vector in LHS is given by

w 2 + w 2 sin 2 θ 1 + 2 w 2 sin θ 1 cos θ 2 \sqrt {w^2 + w^2 \sin^2 \theta_1 + 2w^2 \sin\theta_1 \cos\theta_2}

and see that it is maximum at sin θ 1 = cos θ 2 = 1 \sin \theta_1 = \cos \theta_2 =1 , for which we get w = 1 2 | w| = \frac{1}{2}

Thus in asked values, maximum M M is 0.5 0.5 and angle in degrees is 9 0 90^\circ . Answer being 90.5 \boxed{90.5}

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