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JEE Advanced 2006 · Laws of Motion

A circular disc with a groove along its diameter is placed horizontally on a rough surface. A block of mass 1 kg1\,\text{kg} is placed as shown. The co-efficient of friction between the block and all surfaces of groove and horizontal surface in contact is μ=25\mu = \frac{2}{5}. The disc has an acceleration of 25 m/s225\,\text{m/s}^{2} towards left. Find the acceleration of the block with respect to disc. Given cos⁡θ=45\cos \theta = \frac{4}{5}, sin⁡θ=35\sin \theta = \frac{3}{5}.

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Written solution

Step 1: Identify the given parameters.

The mass of the block, the coefficient of friction, the acceleration of the disc, and the trigonometric values are given.

m=1 kgm = 1\text{ kg} μ=25=0.4\mu = \frac{2}{5} = 0.4 a=25 m/s2a = 25\text{ m/s}^2 cos⁡θ=45\cos\theta = \frac{4}{5} sin⁡θ=35\sin\theta = \frac{3}{5}

Step 2: Calculate the pseudo force in the frame of the disc.

Since the disc accelerates to the left, a pseudo force acts on the block to the right.

F∗=maF^* = ma F∗=1×25=25 NF^* = 1 \times 25 = 25\text{ N}

Step 3: Resolve the pseudo force along and perpendicular to the groove.

The components of the pseudo force relative to the groove are determined by the angle θ\theta.

F∥∗=macos⁡θF^*_{\parallel} = ma\cos\theta F∥∗=25×45=20 NF^*_{\parallel} = 25 \times \frac{4}{5} = 20\text{ N} F⊥∗=masin⁡θF^*_{\perp} = ma\sin\theta F⊥∗=25×35=15 NF^*_{\perp} = 25 \times \frac{3}{5} = 15\text{ N}

Step 4: Determine the normal forces acting on the block.

The normal force from the wall of the groove balances the perpendicular component of the pseudo force.

N=F⊥∗=15 NN = F^*_{\perp} = 15\text{ N}

The normal force from the horizontal floor is equal to the weight of the block.

Nfloor=mgN_{\text{floor}} = mg Nfloor=1×10=10 NN_{\text{floor}} = 1 \times 10 = 10\text{ N}

Step 5: Calculate the friction forces.

Friction forces act on the block from both the vertical wall of the groove and the horizontal floor.

fwall=μNf_{\text{wall}} = \mu N fwall=0.4×15=6 Nf_{\text{wall}} = 0.4 \times 15 = 6\text{ N} ffloor=μmgf_{\text{floor}} = \mu mg ffloor=0.4×10=4 Nf_{\text{floor}} = 0.4 \times 10 = 4\text{ N}

Step 6: Verify if the block slides.

Compare the driving force along the groove with the maximum total friction force.

fmax=fwall+ffloorf_{\text{max}} = f_{\text{wall}} + f_{\text{floor}} fmax=6+4=10 Nf_{\text{max}} = 6 + 4 = 10\text{ N}

Since F∥∗=20 N>10 NF^*_{\parallel} = 20\text{ N} > 10\text{ N}, the block slides along the groove.

Step 7: Calculate the acceleration of the block relative to the disc.

Apply Newton's second law along the direction of the groove.

marel=F∥∗−ffloor−fwallma_{\text{rel}} = F^*_{\parallel} - f_{\text{floor}} - f_{\text{wall}} marel=20−4−6=10 Nma_{\text{rel}} = 20 - 4 - 6 = 10\text{ N} arel=101=10 m/s2a_{\text{rel}} = \frac{10}{1} = 10\text{ m/s}^2

Answer: 10 m/s210\text{ m/s}^2 along the groove, toward the lower-right end.

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