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Question: A force \(F=k{{x}^{2}}\) acts on a particle at an angle of \({{60}^{\circ }}\) with the X-axis the w...

A force F=kx2F=k{{x}^{2}} acts on a particle at an angle of 60{{60}^{\circ }} with the X-axis the work done in displacing the particle from X1{{X}_{1}} to X2{{X}_{2}}will be-

Explanation

Solution

given force is given by F=kx2F=k{{x}^{2}} so we can see that force is variable in terms of displacement of a particle so we need to integrate F over a small section of displacement dx from X1{{X}_{1}} to X2{{X}_{2}} to calculate total work done.

Formula used:
W=x1x2F.dsW=\int_{{{x}_{1}}}^{{{x}_{2}}}{F.ds}

Complete Step by step solution:
In the question the force is acting on the particle with an angle of 60{{60}^{\circ }} so we have to its horizontal component by which particle is moving towards X-axis and it is given by,

Given,F=kx2F=k{{x}^{2}}^{{}}

Now total horizontal component of force is given by,
FH=Fcos(θ)=kx2cos(60)=12kx2{{F}_{H}}=F\cdot \cos (\theta )=k{{x}^{2}}\cdot \cos ({{60}^{\circ }})=\dfrac{1}{2}k{{x}^{2}}
cos(60)=12\cos ({{60}^{\circ }})=\dfrac{1}{2}|

Now, work done = X1X2FHdx=12X1X2kx2dx\int\limits_{{{X}_{1}}}^{{{X}_{2}}}{{{F}_{H}}\cdot dx}=\dfrac{1}{2}\int\limits_{{{X}_{1}}}^{{{X}_{2}}}{k{{x}^{2}}\cdot dx}, from the above comment cos(60)=12\cos ({{60}^{\circ }})=\dfrac{1}{2},
since integration of x2{{x}^{2}} is given byx2.dx=x33\int{{{x}^{2}}.dx=\dfrac{{{x}^{3}}}{3}}|

Now by putting limit form X1{{X}_{1}}toX2{{X}_{2}}
12[kx33]X2 X1 =k6[X23X13]\dfrac{1}{2}\left[ \dfrac{k{{x}^{3}}}{3} \right]\begin{matrix} {{X}_{2}} \\\ {{X}_{1}} \\\ \end{matrix}=\dfrac{k}{6}\left[ {{X}_{2}}^{3}-{{X}_{1}}^{3} \right]
So, W=k6[X23X13]W=\dfrac{k}{6}\left[ {{X}_{2}}^{3}-{{X}_{1}}^{3} \right]

So to displace an object from X1{{X}_{1}}toX2{{X}_{2}} work done will be equal to,
W=k6[X23X13]W=\dfrac{k}{6}\left[ {{X}_{2}}^{3}-{{X}_{1}}^{3} \right].M

Additional information:
we solved this question by assuming our surface is smooth and there are no external resistance or frictional forces are there to oppose the motion of an object.
Work done is a scalar quantity, which means that it has no direction associated with it and only magnitude. Hence Work done is a quantity achieved by the dot product.

Note:
Work done is defined as a product of component of force in the direction of displacement and total displacement of a body, and dimension is same as the energy and is given by [ML2T2]\left[ M{{L}^{2}}{{T}^{-2}} \right] and the SI unit of work is joule which is defined as a work done by a force of 1 newton to displace an object by 1 metre in the direction of force.