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# A bead of mass m is located on a parabolic wire with its axis vertical and vertex directed towards as shown in the figure and whose equation is ${x^2} = ay$. If the coefficient of friction is $\mu$, the maximum height above the x-axis at which the particle will be in equilibrium is:A) $\mu a$B) ${\mu ^2}a$C) $\dfrac{{{\mu ^2}a}}{4}$D) $\dfrac{{\mu a}}{2}$

Last updated date: 09th Sep 2024
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Hint: The coefficient of friction can be calculated and expressed in terms of the equation of motion. This can be done by drawing the free-body diagram of the bead and computing the forces acting on the bead when it is in motion along the curve.

Friction is a force that resists the relative motion between two solid surfaces, fluid layers, or material elements moving against one another. The frictional force acting on the body is dependent on the normal force acted upon by the surface on the body.
Frictional force,
$F \propto N$
By removing the constant of proportionality, we have –
$F = \mu N$
where $\mu =$coefficient of friction of the surface.
Consider a bead moving on the parabolic wire of equation ${x^2} = ay$ as shown.

The forces act alongside the tangent drawn on the curve at the point where mass m is situated. The forces acting on the bead are:
i) Weight mg whose component $mg\sin \theta$ acts along the tangent in the downward direction
ii) Frictional force acting in the opposite direction along the tangent, equal to $\mu mg\cos \theta$.
Since the bead is in equilibrium along the direction of the tangent, we have –
$mg\sin \theta = \mu mg\cos \theta$
$\Rightarrow \dfrac{{\sin \theta }}{{\cos \theta }} = \mu$
$\Rightarrow \tan \theta = \mu$
The slope of the tangent at any point is given by the tan of the angle made by the tangent with the horizontal.
However, the slope of the tangent is equal to the differential of the curve at the point. We have –
$\dfrac{{dy}}{{dx}} = \tan \theta$
The equation of the parabola is –
${x^2} = ay$
$\Rightarrow y = \dfrac{{{x^2}}}{a}$
Differentiating the above equation, we get –
$\Rightarrow \dfrac{{dy}}{{dx}} = \dfrac{d}{{dx}}\left( {\dfrac{{{x^2}}}{a}} \right) = \dfrac{{2x}}{a}$
Therefore, we have –
$\Rightarrow \dfrac{{2x}}{a} = \tan \theta$
Substituting the result of $\tan \theta$ from the derived equation, we have –
$\Rightarrow \dfrac{{2x}}{a} = \mu$
$\Rightarrow x = \dfrac{{\mu a}}{2}$
The maximum distance above the x-axis travelled by the bead is equal to: $x = \dfrac{{\mu a}}{2}$

Hence, the correct option is Option D.

Note: Students generally, confuse while writing the horizontal and vertical components of a vector. You can use a simple and handy thumb rule as shown here:

Consider a vector $\vec a$ inclined at angle $\theta$ as shown in the above figure:
- The line that is attached to the angle $\theta$ is designated as $\cos \theta$.
- The other line that is not attached to the angle $\theta$ is designated as $\sin \theta$.