Topics covered: Simple Harmonic Motion (SHM), kinematics, energy, spring–mass systems, pendulums and physical pendulum (JEE Main focus).


1. Introduction to SHM

  • Motion is oscillatory when it repeats periodically about a stable equilibrium position.
  • In SHM, restoring force is directly proportional to displacement and directed towards mean position.

F ∝ x

F = −kx

Using Newton’s second law:

d²x/dt² = −(k/m)x = −ω²x

Angular frequency:

ω = √(k/m)


2. Kinematics of SHM

Displacement:

x = A sin(ωt + φ)

  • A = amplitude
  • φ = initial phase
  • (ωt + φ) = phase

Time period:

T = 2π / ω

Frequency:

ν = 1 / T

Angular frequency:

ω = 2πν


3. Velocity in SHM

v = dx/dt = ωA cos(ωt + φ)

v = ω √(A² − x²)

  • Maximum velocity: vmax = ωA (at x = 0)
  • Velocity is zero at x = ±A

4. Acceleration in SHM

a = dv/dt = −ω²A sin(ωt + φ)

a = −ω²x

  • Acceleration is maximum at x = ±A
  • Acceleration is zero at x = 0

5. Velocity–Displacement Relation

v² = ω² (A² − x²)

  • Graph of v vs x is an ellipse
  • Graph of a vs x is a straight line with slope −ω²

6. Energy in SHM

Kinetic Energy (K)

K = ½ mv² = ½ mω² (A² − x²)

  • Kmax = ½ mω²A² (at x = 0)
  • K = 0 at x = ±A

Potential Energy (U)

U = ½ kx² = ½ mω²x²

  • Umax = ½ mω²A² (at x = ±A)
  • U = 0 at x = 0

Total Energy (E)

E = K + U = ½ mω²A² (constant)


7. Time Period of SHM

Linear SHM

T = 2π √(m / k)

Angular SHM

T = 2π √(I / k)

General form:

T = 2π √(Inertia factor / Force factor)


8. Spring–Mass System

(a) Series Combination

1 / keq = 1 / k₁ + 1 / k₂

T = 2π √(m / keq)

(b) Parallel Combination

keq = k₁ + k₂

T = 2π √(m / keq)


9. Relation Between Spring Length and Stiffness

k ∝ 1 / l

If a spring of length l is cut into parts l₁ and l₂:

k₁ = K (l / l₁)

k₂ = K (l / l₂)


10. Simple Pendulum

Time period (small oscillations):

T = 2π √(l / g)

  • Independent of mass
  • Seconds pendulum: T = 2 s

Effective gravity cases

  • Lift accelerating upwards: geff = g + a
  • Lift accelerating downwards: geff = g − a
  • Horizontal acceleration: geff = √(g² + a²)
  • Free-falling lift: geff = 0 → no oscillation

T = 2π √(l / geff)


11. Physical Pendulum

Restoring torque:

τ = −mgdθ

Equation of motion:

I d²θ/dt² = −mgdθ

Time period:

T = 2π √(I / mgd)

Special cases

  • Rod of length l about one end:
    T = 2π √(2l / 3g)
  • Ring of radius R pivoted at rim:
    T = 2π √(2R / g)
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