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NEET PHYSICSMedium

A particle of mass 10 g10 \text{ g} moves along a circle of radius 6.4 cm6.4 \text{ cm} with a constant tangential acceleration. What is the magnitude of this acceleration, if the kinetic energy of the particle becomes equal to 8×104 J8 \times 10^{-4} \text{ J} by the end of the second revolution after the beginning of the motion?

A

0.15 m/s20.15 \text{ m/s}^2

B

0.18 m/s20.18 \text{ m/s}^2

C

0.2 m/s20.2 \text{ m/s}^2

D

0.1 m/s20.1 \text{ m/s}^2

Step-by-Step Solution

  1. Concept: According to the Work-Energy Theorem, the work done by the net force on a particle is equal to the change in its kinetic energy (W=ΔKW = \Delta K) . In non-uniform circular motion, the tangential force FtF_t does work over the distance covered.
  2. Formulas:
  • Tangential Force: Ft=matF_t = m a_t
  • Work Done: W=Fts=matsW = F_t \cdot s = m a_t s
  • Distance covered in nn revolutions: s=n×2πRs = n \times 2\pi R
  1. Given Values:
  • Mass (mm) = 10 g=102 kg10 \text{ g} = 10^{-2} \text{ kg}
  • Radius (RR) = 6.4 cm=6.4×102 m6.4 \text{ cm} = 6.4 \times 10^{-2} \text{ m}
  • Kinetic Energy (KK) = 8×104 J8 \times 10^{-4} \text{ J} (Initial Ki=0K_i = 0)
  • Revolutions (nn) = 2
  1. Calculation:
  • Distance (ss) = 2×2π×(6.4×102)=4π(6.4×102) m2 \times 2\pi \times (6.4 \times 10^{-2}) = 4\pi (6.4 \times 10^{-2}) \text{ m}
  • Applying Work-Energy Theorem: mats=Km a_t s = K (102)at[4π(6.4×102)]=8×104(10^{-2}) a_t [4\pi (6.4 \times 10^{-2})] = 8 \times 10^{-4} at=8×104102×4π×6.4×102a_t = \frac{8 \times 10^{-4}}{10^{-2} \times 4\pi \times 6.4 \times 10^{-2}} at=8×1044π×6.4×104=825.6πa_t = \frac{8 \times 10^{-4}}{4\pi \times 6.4 \times 10^{-4}} = \frac{8}{25.6 \pi} at=13.2π13.2×3.1416110.05a_t = \frac{1}{3.2 \pi} \approx \frac{1}{3.2 \times 3.1416} \approx \frac{1}{10.05} at0.1 m/s2a_t \approx 0.1 \text{ m/s}^2
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