JEE Challenger
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Toppling versus Sliding of a Block on an Increasing Incline

A block of base 10 cm×10 cm10\text{ cm} \times 10\text{ cm} and height 15 cm15\text{ cm} is kept on an inclined plane. The coefficient of friction between them is 3\sqrt{3}. The inclination θ\theta of this inclined plane from the horizontal plane is gradually increased from 0∘0^\circ. Then

Options

A

at θ=30∘\theta = 30^\circ, the block will start sliding down the plane

B

the block will remain at rest on the plane up to certain θ\theta and then it will topple

Correct
C

at θ=60∘\theta = 60^\circ, the block will start sliding down the plane and continue to do so at higher angles

D

at θ=60∘\theta = 60^\circ, the block will start sliding down the plane and on further increasing θ\theta, it will topple at certain θ\theta

Step-by-Step Solution

To determine whether the block slides or topples first as the angle of inclination θ\theta is gradually increased, we evaluate the critical angles for both sliding and toppling.

1. Condition for Sliding:
The block begins to slide when the component of gravity acting down the inclined plane exceeds the maximum static frictional force:
mgsin⁡θ≥fmax=μmgcos⁡θmg \sin\theta \ge f_{\text{max}} = \mu mg \cos\theta
tan⁡θ≥μ\tan\theta \ge \mu
Given that μ=3\mu = \sqrt{3}:
tan⁡θs=3  ⟹  θs=60∘\tan\theta_s = \sqrt{3} \implies \theta_s = 60^\circ
Thus, sliding would occur at an angle of θs=60∘\theta_s = 60^\circ if the block does not topple earlier.

2. Condition for Toppling:
Let the width of the base along the incline be b=10 cmb = 10\text{ cm} and the height of the block be h=15 cmh = 15\text{ cm}. The center of mass is located at a distance of h2\frac{h}{2} perpendicular to the incline and b2\frac{b}{2} parallel to the incline from the lower edge.

As θ\theta increases, the normal force shifts toward the lower edge of the base to provide a counter-torque against the toppling torque produced by the component of gravity down the plane (mgsin⁡θmg \sin\theta).

At the verge of toppling, the normal force acts right at the lowest edge of the block. Taking torque about this lower edge:
τtoppling=(mgsin⁡θ)(h2)\tau_{\text{toppling}} = (mg \sin\theta) \left(\frac{h}{2}\right)
τrestoring=(mgcos⁡θ)(b2)\tau_{\text{restoring}} = (mg \cos\theta) \left(\frac{b}{2}\right)

For rotational equilibrium:
(mgsin⁡θ)h2≤(mgcos⁡θ)b2(mg \sin\theta)\frac{h}{2} \le (mg \cos\theta)\frac{b}{2}
tan⁡θ≤bh\tan\theta \le \frac{b}{h}

Hence, the critical angle for toppling is:
tan⁡θt=bh=1015=23  ⟹  θt=arctan⁡(23)≈33.7∘\tan\theta_t = \frac{b}{h} = \frac{10}{15} = \frac{2}{3} \implies \theta_t = \arctan\left(\frac{2}{3}\right) \approx 33.7^\circ

Conclusion:
Comparing the two critical angles:
θt≈33.7∘<θs=60∘\theta_t \approx 33.7^\circ < \theta_s = 60^\circ

Since θt<θs\theta_t < \theta_s, as θ\theta is gradually increased from 0∘0^\circ, the angle for toppling is reached first. Therefore, the block will remain at rest on the plane up to θ=arctan⁡(2/3)\theta = \arctan(2/3) and then it will topple without sliding.

Hence, the correct option is B.