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NEET PHYSICSMedium

A block of mass mm is in contact with the cart C as shown in the figure. The coefficient of static friction between the block and the cart is μ\mu. The acceleration α\alpha of the cart that will prevent the block from falling satisfies:

A

α>mgμ\alpha > \frac{mg}{\mu}

B

α>gμm\alpha > \frac{g}{\mu m}

C

αgμ\alpha \ge \frac{g}{\mu}

D

α<gμ\alpha < \frac{g}{\mu}

Step-by-Step Solution

  1. Identify Forces:
  • Vertical Direction: The block has a tendency to fall downwards due to gravity (mgmg). To prevent this, the static friction force (fsf_s) must act upwards.
  • Horizontal Direction: The cart accelerates with α\alpha. The block moves with the cart, so a normal reaction force (NN) from the cart acts on the block to providing the necessary acceleration. N=mαN = m\alpha [NCERT Class 11, Physics Part I, Sec 5.5].
  1. Condition for Equilibrium (No slipping): For the block not to fall, the upward friction must balance the downward weight: fs=mgf_s = mg.
  2. Limiting Friction: The static friction is self-adjusting but has a maximum limit given by fsμsNf_s \le \mu_s N (where μ\mu is the coefficient of static friction) [NCERT Class 11, Physics Part I, Sec 5.9, Eq 4.14].
  3. Derivation: Substitute the values into the inequality: mgμNmg \le \mu N mgμ(mα)mg \le \mu (m\alpha) Cancel mass mm from both sides (since m>0m > 0): gμαg \le \mu \alpha αgμ\alpha \ge \frac{g}{\mu}
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