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Question: Three particles, each of mass \(M\) , are placed at the three corners of an equilateral triangle of ...

Three particles, each of mass MM , are placed at the three corners of an equilateral triangle of side ll. What is the force due to this system of particles on another particle of mass mm placed at the midpoint of any side?
A.3GMm4l2 B.4GMm3l2 C.GMm4l2 D.4GMml2 \begin{aligned} & A.\dfrac{3GMm}{4{{l}^{2}}} \\\ & B.\dfrac{4GMm}{3{{l}^{2}}} \\\ & C.\dfrac{GMm}{4{{l}^{2}}} \\\ & D.\dfrac{4GMm}{{{l}^{2}}} \\\ \end{aligned}

Explanation

Solution

Hint: Calculate the force exerted by each of the particles of mass MM placed at the corners of the equilateral triangle to the particle of mass mm placed at the midpoint of any side of the triangle.

Formula Used:
F=Gm1m2r2F=\dfrac{G{{m}_{1}}{{m}_{2}}}{{{r}^{2}}}

Complete step by step answer:
We know that the force exerted between two particles, placed at a distance apart from each other is called gravitational force.
Gravitational Force is directly proportional to the product of mass of two particles or objects and inversely proportional to the square of their distance. It is a vector quantity that has both magnitude and direction.
Mathematically gravitational force is given by:
F=Gm1m2r2F=\dfrac{G{{m}_{1}}{{m}_{2}}}{{{r}^{2}}}

Where:
F=F= Gravitational Force between two objects.
m1={{m}_{1}}= mass of one object
m2={{m}_{2}}= mass of another object
r=r=distance between the object
In our question three particles of mass MM are placed at the corners of the equilateral triangle and one particle of mass mm place at the midpoint at any side of the triangle.

Therefore force exerted particle placed at corner B to the particle of mass mm placed at midpoint D is given by
FBD=GMm(l2)2(i){{F}_{BD}}=\dfrac{GMm}{{{\left( \dfrac{l}{2} \right)}^{2}}}(-i)

Because D is the midpoint of side BC therefore distance becomes l2\dfrac{l}{2}, and here i-irepresents the direction of force which is in the negative x axis.
Force exerted particle placed at corner C to the particle of mass mm placed at midpoint D is given by:
FCD=GMm(l2)2(i){{F}_{CD}}=\dfrac{GMm}{{{\left( \dfrac{l}{2} \right)}^{2}}}(i)
Here ii represents the direction of force which is in the positive x axis.
Also, the force exerted by particle placed at corner A of mass MM to the particle placed at midpoint D:

FAD=GMm(3l2)2(j) FAD=4GMm3l2(j) \begin{aligned} & {{F}_{AD}}=\dfrac{GMm}{{{\left( \dfrac{\sqrt{3}l}{2} \right)}^{2}}}(-j) \\\ & {{F}_{AD}}=\dfrac{4GMm}{3{{l}^{2}}}(-j) \\\ \end{aligned}

Here the distance between corner A and midpoint D which is on side BC is given by 3l2\dfrac{\sqrt{3}l}{2} because triangle is equilateral and equilateral triangle has altitude 3l2\dfrac{\sqrt{3}l}{2}. Which can be found by Pythagoras Theorem.
And here j-jrepresents the direction of force which is in negative y direction.
Therefore the net force is the vector sum of all the forces acting on particle placed at D is given by:
Fnet=FAD+FBD+FCD Fnet=4GMm3l2(j)+GMm(l2)2(i)+GMm(l2)2(i) Fnet=4GMm3l2(j) \begin{aligned} & {{F}_{net}}={{F}_{AD}}+{{F}_{BD}}+{{F}_{CD}} \\\ & {{F}_{net}}=\dfrac{4GMm}{3{{l}^{2}}}(-j)+\dfrac{GMm}{{{\left( \dfrac{l}{2} \right)}^{2}}}(-i)+\dfrac{GMm}{{{\left( \dfrac{l}{2} \right)}^{2}}}(i) \\\ & {{F}_{net}}=\dfrac{4GMm}{3{{l}^{2}}}(-j) \\\ \end{aligned}
Taking the magnitude of this net force.
Fnet=4GMm3l2{{F}_{net}}=\dfrac{4GMm}{3{{l}^{2}}}
Hence, the correct answer is option B.

Note: While doing such types of questions students must remember to take care on the direction of forces. To deal with it simply use vector notation to find your answer more accurately. For vector notation use i, j, k position vectors.