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Question: For some non-zero vector \[\overrightarrow V \], if the sum of \[\overrightarrow V \] and the vector...

For some non-zero vector V\overrightarrow V , if the sum of V\overrightarrow V and the vector obtained from V\overrightarrow V by rotating it by an angle 2α2\alpha equals to the vector obtained from V\overrightarrow V by rotating it by a then the value of α\alpha , is where nn is a integer.
A.2nπ=π32n\pi = \dfrac{\pi }{3}
B.nπ=π3n\pi = \dfrac{\pi }{3}
C.2nπ=2π32n\pi = \dfrac{{2\pi }}{3}
D.nπ=2π3n\pi = \dfrac{{2\pi }}{3}

Explanation

Solution

Hint : In this problem, A nonzero vector is a vector with magnitude not equal to zero. The vector obtained by rotating the vector V\overrightarrow V by an angle α\alpha in the anticlockwise direction is defined by trigonometric formula. A vector is an object that has both a magnitude and a direction.

Complete step-by-step answer :

First, we have to sketch a diagram for some non-zero vector V\overrightarrow V , if the sum of V\overrightarrow V and the vector obtained from V\overrightarrow V by rotating it by an angle 2α2\alpha equals to the vector obtained from V\overrightarrow V by rotating it by a then the value of α\alpha , is where nn is a integer.
According to the condition in this problem, the vector obtained by rotating the vector V\overrightarrow V by an angleα\alpha in the anticlockwise direction, then
vivcos(π2α)i^+vsin(π2α)j^=vcosαi^+vsinαj^vi - v\cos (\pi - 2\alpha )\hat i + v\sin (\pi - 2\alpha )\hat j = v\cos \alpha \hat i + v\sin \alpha \hat j
We use the trigonometric identity cos(πθ)=cosθ\cos (\pi - \theta ) = - \cos \theta and sin(πθ)=sinθ\sin (\pi - \theta ) = \sin \theta , we can get
Since, cos(π2α)=cos2α\cos (\pi - 2\alpha ) = - \cos 2\alpha and sin(π2α)=sin2α\sin (\pi - 2\alpha ) = \sin 2\alpha
vi^v(cos2αi^)+vsin2αj^=vcosαi^+vsinαj^v\hat i - v( - cos2\alpha \hat i) + v\sin 2\alpha \hat j = v\cos \alpha \hat i + v\sin \alpha \hat j,
vi^+vcos2αi^+vsin2αj^=vcosαi^+vsinαj^v\hat i + vcos2\alpha \hat i + v\sin 2\alpha \hat j = v\cos \alpha \hat i + v\sin \alpha \hat j
Put common factor ‘v’ from bracket, we have
v(1+cos2α)i^+vsin2αj^=vcosαi^+vsinαj^v(1 + cos2\alpha )\hat i + v\sin 2\alpha \hat j = v\cos \alpha \hat i + v\sin \alpha \hat j
On separating i and j part on both sides of the equation, then
v(1+cos2α)=vcosαv(1 + \cos 2\alpha ) = v\cos \alpha and vsin2α=vsinαv\sin 2\alpha = v\sin \alpha
By dividing on both sides by ‘v’, we get
(1+cos2α)=cosα(1 + \cos 2\alpha ) = \cos \alpha and sin2α=sinα\sin 2\alpha = \sin \alpha
Here, by using this trigonometric identity , cos2α=2cos2α1\cos 2\alpha = 2{\cos ^2}\alpha - 1 and 2sinαcosα=sinα2\sin \alpha \cos \alpha = \sin \alpha
1+2cos2α1=cosα1 + 2{\cos ^2}\alpha - 1 = \cos \alpha and 2sinαcosα=sinα2\sin \alpha \cos \alpha = \sin \alpha
On further simplification, we get
2cos2α=cosα2{\cos ^2}\alpha = \cos \alpha and 2cosα=12\cos \alpha = 1
2cos2αcosα=02{\cos ^2}\alpha - \cos \alpha = 0 and cosα=12\cos \alpha = \dfrac{1}{2}
Take out cosα\cos \alpha commonly on the first function, then
cosα(2cosα1)=0\cos \alpha (2\cos \alpha - 1) = 0 and cosα=12\cos \alpha = \dfrac{1}{2}
Separate the factors to find the value of , then
cosα=0\cos \alpha = 0, (2cosα1)=0(2\cos \alpha - 1) = 0 and cosα=12\cos \alpha = \dfrac{1}{2}
Expanding the equation from LHS to RHS, then
cosα=0\cos \alpha = 0, 2cosα=1cosα=122\cos \alpha = 1 \Rightarrow \cos \alpha = \dfrac{1}{2} and cosα=12\cos \alpha = \dfrac{1}{2}
cosα=0\cos \alpha = 0,cosα=12\cos \alpha = \dfrac{1}{2} and cosα=12\cos \alpha = \dfrac{1}{2}
We know that, the formula cosπ2=0α=2nπ±π2\cos \dfrac{\pi }{2} = 0 \Rightarrow \alpha = 2n\pi \pm \dfrac{\pi }{2} and cosπ3=12α=2nπ±π3\cos \dfrac{\pi }{3} = \dfrac{1}{2} \Rightarrow \alpha = 2n\pi \pm \dfrac{\pi }{3},
α=2nπ±π2\alpha = 2n\pi \pm \dfrac{\pi }{2}, α=2nπ±π3\alpha = 2n\pi \pm \dfrac{\pi }{3} and α=2nπ±π3\alpha = 2n\pi \pm \dfrac{\pi }{3}
Therefore, α=2nπ±π3\alpha = 2n\pi \pm \dfrac{\pi }{3} satisfies both equations.
Hence, The final answer is option(A) 2nπ=π32n\pi = \dfrac{\pi }{3}
So, the correct answer is “Option A”.

Note : Geometrically, we can define a vector as a directed line segment, whose length is the magnitude of the vector and with an arrow indicating the direction. The direction of the vector is from its tail to its head.