Stage 3 – Page 7
Simple Harmonic Motion (SHM) – Springs, Elastic Strings & Hybrid Systems


1. Springs in Series (IIT Favorite)

When two or more springs are connected in series:

1 / keq = 1 / k1 + 1 / k2 + ...

Time period:

T = 2π √(m / keq)

Series connection increases time period


2. Springs in Parallel

For springs attached side by side:

keq = k1 + k2 + ...

Time period:

T = 2π √(m / keq)

Parallel connection decreases time period


3. Mixed Spring Systems (Advanced)

In complex networks:

  • Reduce step-by-step
  • Never assume symmetry blindly

Always find equivalent spring constant first


4. Elastic String – Important Difference

Elastic string:

  • No force when slack
  • Force only when stretched

Tension = kx (only if stretched)

Motion may NOT be SHM for entire cycle


5. SHM with Elastic String (Vertical Motion)

If equilibrium lies in stretched region:

  • Motion about equilibrium is SHM

ω = √(k / m)

Key: equilibrium must be in stretched part


6. Variable Mass Systems (Conceptual)

In most IIT problems:

  • Mass change is slow
  • SHM approximation still valid

Variable mass rarely changes ω directly


7. SHM with Two Masses & One Spring

System:

  • Two masses connected by a spring
  • Both are free

Effective mass:

μ = (m1 m2) / (m1 + m2)

Angular frequency:

ω = √(k / μ)


8. SHM of Pulley–Spring Hybrid

Key ideas:

  • Use constraint equations
  • Convert multiple motions into one variable

Constraint reduces degrees of freedom


9. Common IIT Advanced Traps

  • Assuming elastic string always active
  • Ignoring spring mass (when specified)
  • Wrong equivalent spring calculation

Stage 3 – Page 7 Key Takeaways

✔ Equivalent spring constant controls SHM
✔ Elastic string ≠ spring
✔ Hybrid systems require constraint thinking


— Stage 3 | Advanced SHM Systems —

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