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Question: If a be a constant vector and b be a vector of constant magnitude such that \(∣\vec {b}∣\)=\(\dfrac{...

If a be a constant vector and b be a vector of constant magnitude such that b∣\vec {b}∣=a2\dfrac{a}{2}​ and a0∣\vec {a}∣ \neq 0. then maximum value of angle between a\vec a and a+b\vec a + \vec b is:
A) 5π6\dfrac{{5\pi }}{6}
B) 5π3\dfrac{{5\pi }}{3}
C) 2π3\dfrac{{2\pi }}{3}
D) π6\dfrac{\pi }{6}

Explanation

Solution

A vector is represented by a line with an arrowhead. The point where the arrow starts is called the origin of the vector and the point where the arrow ends is called the tip. A vector remains unchanged when it is displaced parallel to itself.

Complete step by step solution:
Consider the vector b makes an angle θ\theta with the negative side of vector a. Then the resultant component in the x-direction is given by
(a+b)x(a + b)_x =abcosθ= a - b\cos \theta
\Rightarrow (a+b)x(a + b)_x =aa2cosθ= a - \dfrac{a}{2}\cos \theta (b=a2)\left( {\because b = \dfrac{a}{2}} \right)
\Rightarrow (a+b)x(a + b)_x = a2(2cosθ)\dfrac{a}{2}(2 - \cos \theta )
Similarly, the resultant vector of the y component is given by
(a+b)y(a + b)_y = bsinθb\sin \theta
\Rightarrow (a+b)y(a + b)_y = \dfrac{a}{2}\sin \theta $$$$$$\left( {\because b = \dfrac{a}{2}} \right)
We know that according to the parallelogram law of vector addition, the angle between the resultant with the first vector is given by,
tanα=(a2sinθa2(2+cosθ))=sinθ(2+cosθ)\tan \alpha = \left( {\dfrac{{\dfrac{a}{2}\sin \theta }}{{\dfrac{a}{2}\left( {2 + \cos \theta } \right)}}} \right) = \dfrac{{\sin \theta }}{{(2 + \cos \theta )}}
If α has to be maximum, then dαdθ\dfrac{{d\alpha }}{{d\theta }} must be equal to zero, thus we have ddθ(tanα)=ddθ(sinθ2+cosθ)\dfrac{d}{{d\theta }}\left( {\tan \alpha } \right) = \dfrac{d}{{d\theta }}\left( {\dfrac{{\sin \theta }}{{2 + \cos \theta }}} \right)
sec2α(dαdθ)=sinθ(sinθ)(2+cosθ)(cosθ)(2+cosθ)2\Rightarrow se{c^2}\alpha \left( {\dfrac{{d\alpha }}{{d\theta }}} \right) = \dfrac{{\sin \theta \left( { - \sin \theta } \right) - \left( {2 + \cos \theta } \right)\left( {\cos \theta } \right)}}{{{{(2 + cos\theta )}^2}}}
sin2θ2cosθcos2θ=0 2cosθ=1 θ=2π3  \Rightarrow - si{n^2}\theta - 2\cos \theta - co{s^2}\theta = 0 \\\ \Rightarrow 2\cos \theta = - 1 \\\ \Rightarrow \theta = \dfrac{{2\pi }}{3} \\\
Thus for the above value θ\theta , the angle between the resultant and vector a is maximum.
\therefore The maximum value of the angle α\alpha is,
tanα=sinθ(2+cosθ)\tan \alpha = \dfrac{{\sin \theta }}{{(2 + \cos \theta )}}
Substituting the value of θ\theta , we get
tanα=sin(2π3)(2+cos(2π3))\Rightarrow \tan \alpha = \dfrac{{\sin \left( {\dfrac{{2\pi }}{3}} \right)}}{{(2 + \cos \left( {\dfrac{{2\pi }}{3}} \right))}} (θ=2π3)(\because \theta = \dfrac{{2\pi }}{3})
tanα=  32  (212)\Rightarrow \tan \alpha = \dfrac{{\;\sqrt {\dfrac{3}{2}} \;}}{{(2 - \dfrac{1}{2})}}
tanα=13\Rightarrow \tan \alpha = \dfrac{1}{{\sqrt 3 }}
α=tan1(13)\Rightarrow \alpha = ta{n^{ - 1}}\left( {\dfrac{1}{{\sqrt 3 }}} \right)
α=π6\Rightarrow \alpha = \dfrac{\pi }{6}
\therefore The maximum value of the angle, \alpha = \dfrac{\pi }{6}$$$$\;\;

Hence the correct option is D.

Note: 1) When a vector is multiplied by a scalar quantity then we get a new vector in the same direction but having a new magnitude. The vector product is distributive and the addition is commutative. The vector has a definite direction. Vectors obey the law of parallelograms of addition.
2) Zero vector is the one that has zero magnitudes and also no specific direction.
3) If two vectors have equal magnitude and are in the same direction, then they are called equal vectors.