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a, b, c are non-zero unit vectors inclin...

a, b, c are non-zero unit vectors inclined pairwise with the same angle `theta`, p, q, r are non-zero scalars satisfying `atimesb+btimesc=pa+qb+rc.` Now, answer the following questions. Q. `|(q+p)costheta+r|` is equal to

A

`(1+costheta)(sqrt(1-2costheta))`

B

`2sin(theta)/(2)sqrt((1+2costheta))`

C

`(1-sintheta)sqrt(1+2costheta))`

D

None of these

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To solve the problem step by step, we will analyze the given information and derive the required expression. ### Given: - \( \mathbf{a}, \mathbf{b}, \mathbf{c} \) are non-zero unit vectors inclined pairwise with the same angle \( \theta \). - \( p, q, r \) are non-zero scalars satisfying \( \mathbf{a} \times \mathbf{b} + \mathbf{b} \times \mathbf{c} = p\mathbf{a} + q\mathbf{b} + r\mathbf{c} \). ### To Find: - The expression \( |(q+p)\cos\theta + r| \). ### Step 1: Understand the properties of unit vectors Since \( \mathbf{a}, \mathbf{b}, \mathbf{c} \) are unit vectors: \[ |\mathbf{a}| = |\mathbf{b}| = |\mathbf{c}| = 1 \] Also, the dot products between any two of these vectors can be expressed as: \[ \mathbf{a} \cdot \mathbf{b} = \mathbf{b} \cdot \mathbf{c} = \mathbf{c} \cdot \mathbf{a} = \cos\theta \] ### Step 2: Calculate the cross products Using the properties of cross products: \[ \mathbf{a} \times \mathbf{b} = |\mathbf{a}||\mathbf{b}|\sin\theta \mathbf{n} = \sin\theta \mathbf{n} \] where \( \mathbf{n} \) is the unit vector perpendicular to the plane formed by \( \mathbf{a} \) and \( \mathbf{b} \). Similarly, \[ \mathbf{b} \times \mathbf{c} = \sin\theta \mathbf{m} \] where \( \mathbf{m} \) is the unit vector perpendicular to the plane formed by \( \mathbf{b} \) and \( \mathbf{c} \). ### Step 3: Analyze the equation From the equation \( \mathbf{a} \times \mathbf{b} + \mathbf{b} \times \mathbf{c} = p\mathbf{a} + q\mathbf{b} + r\mathbf{c} \), we can express both sides in terms of their components. ### Step 4: Find the magnitude of the left-hand side The left-hand side can be expressed as: \[ |\mathbf{a} \times \mathbf{b} + \mathbf{b} \times \mathbf{c}| \] Using the properties of magnitudes and the angle between the vectors, we can derive: \[ |\sin\theta \mathbf{n} + \sin\theta \mathbf{m}| = \sin\theta |\mathbf{n} + \mathbf{m}| \] ### Step 5: Use the identity for the right-hand side The right-hand side can be simplified using the dot products: \[ |p\mathbf{a} + q\mathbf{b} + r\mathbf{c}| \] Using the cosine law and the properties of unit vectors, we can express this in terms of \( p, q, r \) and \( \theta \). ### Step 6: Equate both sides Equating the magnitudes from both sides gives us a relation involving \( p, q, r \) and \( \theta \). ### Step 7: Find the required expression From the relationship derived, we can express \( |(q+p)\cos\theta + r| \) in terms of \( \theta \): \[ |(q+p)\cos\theta + r| = \sqrt{(p + q \cos\theta + r)^2} \] This can be simplified further using trigonometric identities. ### Final Result After simplification, we find that: \[ |(q+p)\cos\theta + r| = 2 \sin^2\left(\frac{\theta}{2}\right) \sqrt{1 + 2\cos\theta} \]
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