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Question: Two forces P and Q of magnitude 2F and 3F, respectively, are at an angle 𝛉 with each other. If the ...

Two forces P and Q of magnitude 2F and 3F, respectively, are at an angle 𝛉 with each other. If the force Q is doubled, then their resultant also gets doubled. then, the angle is
A. 30˚
B. 60˚
C. 90˚
D. 120˚

Explanation

Solution

we will use the formula, to find the magnitude of resultant of two vectors.

Complete step by step solution:
In the question we are given two forces P and Q of magnitude;
P=2FP = 2Fand Q=3FQ = 3Fand the angle between the vectors is 𝛉, then it is said that if force Q is doubled then their resultant also get doubled so, we required to find the value of θ
First let us draw the diagram of these vectors


let the resultant of vector P and Q is vector R
SO, P+Q=R\overrightarrow P + \overrightarrow Q = \overrightarrow R and |P+Q=R\overrightarrow P + \overrightarrow Q = |R|=P2+Q2+2PQCOSθ\sqrt {{P^2} + {Q^2} + 2PQCOS\theta }
Here, P=2FP = 2Fand Q=3FQ = 3F so put the value in above equation
R=(2F)2+(3F)2+2(2F)(3F)COSθR = \sqrt {{{(2F)}^2} + {{(3F)}^2} + 2(2F)(3F)COS\theta } =13(F)2+12(F)2COSθ\sqrt {13{{(F)}^2} + 12{{(F)}^2}COS\theta }
now the vectors Q gets doubled, so, Q= 6F and the resultant vector also get doubled, so ,
R1=213(F)2+12(F)2COSθ{R_1} = 2\sqrt {13{{(F)}^2} + 12{{(F)}^2}COS\theta } …………..(1)
And the magnitude of new resultant is given as R1=(2F)2+(6F)2+2(2F)(6F)COSθ{R_1} = \sqrt {{{(2F)}^2} + {{(6F)}^2} + 2(2F)(6F)COS\theta }
=40(F)2+24(F)2COSθ\sqrt {40{{(F)}^2} + 24{{(F)}^2}COS\theta }
From equation 1 40(F)2+24(F)2COSθ\sqrt {40{{(F)}^2} + 24{{(F)}^2}COS\theta } =213(F)2+12(F)2COSθ2\sqrt {13{{(F)}^2} + 12{{(F)}^2}COS\theta }
Now squaring both side, we get
40(F)2+24(F)2COSθ40{(F)^2} + 24{(F)^2}COS\theta =4(13(F)2+12(F)2COSθ)4\,(13{(F)^2} + 12{(F)^2}COS\theta )
On simplifying we get

40F2+24F2COSθ =52F2+48F2COSθ40{F^2} + 24{F^2}COS\theta {\text{ }} = 52{F^2} + 48{F^2}COS\theta
12F2= 24F2COSθ- 12{F^2} = {\text{ }}24{F^2}COS\theta
cos θ =  12cos{\text{ }}\theta {\text{ }} = \; - \dfrac{1}{2}

Hence, θ=120\theta = 120^\circ

Note: If two vectors acting simultaneously at a point can be represented both in magnitude and direction by the adjacent sides of a parallelogram drawn from a point, then the resultant vector is represented both in magnitude and direction by the diagonal of the parallelogram passing through that point.