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JEE Advanced 2017 · System of Particles and Rotational Motion

Consider regular polygons with number of sides n=3,4,5,…n = 3, 4, 5, \ldots as shown in the figure. The center of mass of all the polygons is at height hh from the ground. They roll on a horizontal surface about the leading vertex without slipping and sliding as depicted. The maximum increase in height of the locus of the center of mass for each polygon is Δ\Delta. Then Δ\Delta depends on nn and hh as

Answer: B. Δ=h(1cos⁡(πn)−1)\Delta = h \left(\frac{1}{\cos\left(\frac{\pi}{n}\right)} - 1\right)

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Written solution

Step 1: Relate the initial height to the circumradius of the polygon.

When the regular nn-gon rests flat on one of its sides, the height hh of its center of mass (CM) from the ground is equal to its apothem. Let RR be the circumradius (the distance from the center of mass to any vertex).

h=Rcos⁡(πn)h = R \cos\left(\frac{\pi}{n}\right)

Solving for RR gives:

R=hcos⁡(πn)R = \frac{h}{\cos\left(\frac{\pi}{n}\right)}

Step 2: Determine the maximum height of the center of mass during rotation.

As the polygon rolls about its leading vertex, this vertex acts as a fixed pivot on the ground. The distance from this pivot to the center of mass remains constant and equal to RR. Consequently, the center of mass traces a circular arc of radius RR.

The maximum height of the center of mass occurs when it is positioned directly above the pivot vertex.

hmax=Rh_{\text{max}} = R

Step 3: Calculate the maximum increase in height.

The maximum increase in height Δ\Delta is the difference between the maximum height and the initial height.

Δ=R−h\Delta = R - h

Substitute the expression for RR in terms of hh and nn:

Δ=hcos⁡(πn)−h\Delta = \frac{h}{\cos\left(\frac{\pi}{n}\right)} - h Δ=h(1cos⁡(πn)−1)\Delta = h \left( \frac{1}{\cos\left(\frac{\pi}{n}\right)} - 1 \right)

This can also be expressed using the secant function:

Δ=h(sec⁡(πn)−1)\Delta = h \left( \sec\left(\frac{\pi}{n}\right) - 1 \right)

Answer: The maximum increase in height is Δ=h(1cos⁡(πn)−1)\Delta = h \left( \dfrac{1}{\cos\left(\frac{\pi}{n}\right)} - 1 \right) or Δ=h(sec⁡(πn)−1)\Delta = h \left( \sec\left(\frac{\pi}{n}\right) - 1 \right).

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