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Question: The resultant of two forces \(3P\) and \(2P\) is \(R\) if the first force is doubled then the result...

The resultant of two forces 3P3P and 2P2P is RR if the first force is doubled then the resultant is also doubled. The angle between the two forces is
(A) 60{60^ \circ }
(B) 120{120^ \circ }
(C) 70{70^ \circ }
(D) 180{180^ \circ }

Explanation

Solution

Use the given two forces and form the two equations with the resultant forces. Arrange the two equations in such a way that they can be solved by each other. By solving the equations, get the value of the cosine angle between the forces and from that take inverse to find the answer.

Complete step by step answer:
Given: The first force is 3P3P
The second force is 2P2P
The resultant force is RR
If the first force doubles then the resultant force also doubles.
The first equation is R2=9P2+4P2+12P2cosθ{R^2} = 9{P^2} + 4{P^2} + 12{P^2}\cos \theta
By simplifying the above equation , we get
R2=13P2+12P2cosθ{R^2} = 13{P^2} + 12{P^2}\cos \theta ------------(1)
By getting the second equation of the resultant forces,
(2R)2=(2×3P)2+4P2+24P2cosθ{\left( {2R} \right)^2} = {\left( {2 \times 3P} \right)^2} + 4{P^2} + 24{P^2}\cos \theta
By simplifying the above step, we get
(2R)2=(6P)2+4P2+24P2cosθ{\left( {2R} \right)^2} = {\left( {6P} \right)^2} + 4{P^2} + 24{P^2}\cos \theta
By further simplification,
4R2=(6P)2+4P2+24P2cosθ4{R^2} = {\left( {6P} \right)^2} + 4{P^2} + 24{P^2}\cos \theta -------(2)
In order to equate the equation (1) and (2), multiply the equation (1) into 44
4R2=52P2+48P2cosθ4{R^2} = 52{P^2} + 48{P^2}\cos \theta --------(3)
Solving the equation (2) and (3), we get
(6P)2+4P2+24P2cosθ=52P2+48P2cosθ{\left( {6P} \right)^2} + 4{P^2} + 24{P^2}\cos \theta = 52{P^2} + 48{P^2}\cos \theta
By doing the addition and the subtraction at a necessary point to do the simplification,
12P2=24P2cosθ12{P^2} = - 24{P^2}\cos \,\theta
cosθ=12P224P2\cos \theta = \dfrac{{12{P^2}}}{{24{P^2}}}
By cancelling the similar terms in the right hand side of the equation,
cosθ=12\cos \theta = - \dfrac{1}{2}
θ=cos1(12)\Rightarrow \theta = {\cos ^{ - 1}}\left( {\dfrac{1}{2}} \right).

Hence, the angle between the two forces is 120{120^ \circ }.

Note: The force is said to be vector, if it possesses both magnitude and direction. The angle between the forces matters much, this is because the two forces can act in two different directions, the resultant must be in the direction of the average of the two directions.