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Question: When a force \(F\) acts on a body of mass \(m\), the acceleration produced in the body is a. If thre...

When a force FF acts on a body of mass mm, the acceleration produced in the body is a. If three equal forces F1,F2{F_1},{F_2} and F3{F_3} which are related as F1=F2=F3=F{F_1} = {F_2} = {F_3} = F act on the body as shown in the figure. Then the acceleration produced is:

A. ( 21\sqrt 2 - 1 ) aa
B. ( 2+1\sqrt 2 + 1 ) aa
C. ( 2\sqrt 2 ) aa
D. aa

Explanation

Solution

Whenever a body is acted by some force it gets accelerated which in mathematical form it’s called Newton’s second law of motion as F=maF = ma here, we will find the net force acting on the body and its direction then will find the net acceleration of the body.

Complete step by step answer:
Let us find the net magnitude of forces F1{F_1} and F2{F_2} which are perpendicular to each other and this net force be written as F12{F_{12}} so,
F12=F2+F2{F_{12}} = \sqrt {{F^2} + {F^2}}
F12=2F{F_{12}} = \sqrt 2 F Which will be in direction just opposite to that of F3{F_3} .
Now, two forces acting on the body of mass m respectively F12=2F{F_{12}} = \sqrt 2 F and F3=F{F_3} = F.
Both forces are in opposite direction,
Hence net force act on the body of mass mm is,
Fnet=2FF{F_{net}} = \sqrt 2 F - F
Fnet=(21)F\Rightarrow {F_{net}} = (\sqrt 2 - 1)F
Now, let us assume that net acceleration is denoted by aa' then by newton’ second law we have:
(21)F=ma(\sqrt 2 - 1)F = ma'
We also know that, F=maF = ma put this value in above equation, we get,
(21)a=a(\sqrt 2 - 1)a = a'
Net acceleration is a=(21)aa' = (\sqrt 2 - 1)a

Hence, the correct option is A.

Note: It should be remembered that, Force is a vector quantity and its added always using vector algebra which is given as Fnet=F12+F22+2F1F2cosθ{F_{net}} = \sqrt {{F_1}^2 + {F_2}^2 + 2{F_1}{F_2}\cos \theta } and the direction of two equal vectors resultant is in the middle of the angle between them. And it can also be calculated with the general formula tanβ=F2sinθF1+F2cosθ\tan \beta = \dfrac{{{F_2}\sin \theta }}{{{F_1} + {F_2}\cos \theta }}.