Rotational Motion – JEE Mains Physics

1. Centre of Mass

  • Centre of Mass (COM) is the point where the entire mass of a system appears to be concentrated.
  • For a two-particle system:
    xcom = (m₁x₁ + m₂x₂) / (m₁ + m₂)
  • For a rigid body, COM depends on the shape and mass distribution.

2. Basic Concepts of Rotational Motion

  • Rotational motion involves a body rotating about a fixed axis.
  • Angular Displacement (θ), Angular Velocity (ω), and Angular Acceleration (α) describe rotational motion.

3. Moment of a Force (Torque)

  • Torque (τ) is the rotational analog of force.
  • Torque is given by:
    τ = r × F
    where r = position vector and F = force vector.

4. Angular Momentum

  • Angular momentum (L) for a particle is given by:
    L = r × p
    where p = linear momentum.
  • For a rotating rigid body:
    L = Iω
    where I = moment of inertia and ω = angular velocity.

5. Conservation of Angular Momentum

  • If no external torque acts on a system, its angular momentum remains conserved.
  • Applications:
    • Ice skater pulling arms inward to spin faster.
    • Neutron stars spinning rapidly after collapsing.

6. Moment of Inertia

  • Moment of Inertia (I) is the rotational analog of mass in linear motion.
  • Depends on the mass distribution about the axis of rotation:
    I = Σ mᵢrᵢ²

7. Radius of Gyration

  • Radius of gyration (k) is defined as:
    k = √(I/M)
    where I = moment of inertia and M = total mass.

8. Values of Moments of Inertia for Simple Objects

  • Thin Rod (about center) =
    I = (1/12)ML²
  • Ring (about center) =
    I = MR²
  • Solid Sphere (about diameter) =
    I = (2/5)MR²
  • Solid Cylinder (about axis) =
    I = (1/2)MR²

9. Parallel and Perpendicular Axes Theorems

  • Parallel Axis Theorem:
    I = Icm + Md²
    where d = distance between axes.
  • Perpendicular Axis Theorem (for planar bodies):
    Iz = Ix + Iy

10. Equilibrium of Rigid Bodies

  • For a body to be in mechanical equilibrium:
    • Net external force = 0 (translational equilibrium).
    • Net external torque = 0 (rotational equilibrium).

11. Rigid Body Rotation and Equations of Rotational Motion

  • Rotational analogs of linear equations:
    ω = ω₀ + αt
    θ = ω₀t + (1/2)αt²
    ω² = ω₀² + 2αθ

12. Comparison of Linear and Rotational Motions

  • Linear Motion ↔ Rotational Motion
  • Displacement (x) ↔ Angular displacement (θ)
  • Velocity (v) ↔ Angular velocity (ω)
  • Acceleration (a) ↔ Angular acceleration (α)
  • Mass (m) ↔ Moment of inertia (I)
  • Force (F) ↔ Torque (τ)

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