Physics·Revision Notes

Simple Pendulum — Revision Notes

NEET UG
Version 1Updated 22 Mar 2026

⚡ 30-Second Revision

  • Definition:Point mass (bob) on massless, inextensible string.
  • SHM Condition:Small angles (sinθapproxθsin\theta approx \theta).
  • Restoring Force:F=mgsinθapproxmgθF = -mg sin\theta approx -mg\theta.
  • Time Period Formula:T=2pisqrtLgT = 2pi sqrt{\frac{L}{g}}
  • Frequency Formula:f=1T=12pisqrtgLf = \frac{1}{T} = \frac{1}{2pi} sqrt{\frac{g}{L}}
  • Dependencies:TproptosqrtLT propto sqrt{L}, Tpropto1sqrtgT propto \frac{1}{sqrt{g}}.
  • Independence:TT is independent of mass and amplitude (for small angles).
  • Effective Length (L):Distance from suspension point to center of mass of bob.
  • Lift Accelerating Up (a):geff=g+aimpliesTg_{eff} = g+a implies T decreases.
  • Lift Accelerating Down (a):geff=gaimpliesTg_{eff} = g-a implies T increases.
  • Free Fall ($a=g$):geff=0impliesTinftyg_{eff} = 0 implies T \to infty (no oscillation).
  • In Liquid:g_{eff} = g left(1 - \frac{\rho_{liquid}}{\rho_{bob}}\right) implies T increases.
  • Temperature Increase:LL increases due to thermal expansion impliesTimplies T increases.

2-Minute Revision

The simple pendulum is a fundamental system for understanding oscillations. It consists of a point mass (bob) suspended by a massless, inextensible string. For its motion to approximate Simple Harmonic Motion (SHM), the angular displacement must be small (typically less than 10circ15circ10^circ-15^circ).

Under this condition, the restoring force, which is the tangential component of gravity (mgsinθmgsin\theta), can be approximated as mgθ-mg\theta, making it proportional to displacement. The time period for one complete oscillation is given by T=2pisqrtLgT = 2pi sqrt{\frac{L}{g}}, where LL is the effective length (from suspension to the bob's center of mass) and gg is the acceleration due to gravity.

Crucially, the time period is independent of the bob's mass and the amplitude of oscillation (for small angles). Remember that TT increases with increasing length and decreases with increasing gravity.

Common NEET variations include pendulums in accelerating lifts (where gg becomes gpmag pm a), in fluid mediums (where buoyancy reduces effective gg), and effects of temperature on the string's length due to thermal expansion.

Always identify the effective LL and gg for any given scenario.

5-Minute Revision

Let's consolidate our understanding of the simple pendulum, a cornerstone of oscillatory motion. An ideal simple pendulum is a point mass 'bob' attached to a massless, inextensible string, oscillating under gravity.

Its motion is SHM only for small angular displacements (hetale10circ15circheta le 10^circ-15^circ). The restoring force is F=mgsinθF = -mgsin\theta. Using the small angle approximation, sinθapproxθsin\theta approx \theta, this becomes FapproxmgθF approx -mg\theta, which is proportional to displacement, satisfying SHM criteria.

The time period TT for one complete oscillation is given by T=2pisqrtLgT = 2pi sqrt{\frac{L}{g}}.

Key Takeaways:

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  1. Independence:The time period TT is independent of the bob's mass and the amplitude of oscillation (for small angles). This is a frequent conceptual trap.
  2. 2
  3. Dependencies:TT is directly proportional to sqrtLsqrt{L} and inversely proportional to sqrtgsqrt{g}. Longer pendulums swing slower; stronger gravity makes them swing faster.
  4. 3
  5. Effective Length (L):Always measure LL from the point of suspension to the center of mass of the bob. If the bob has a radius RR, L=Lstring+RL = L_{string} + R.

Common NEET Scenarios:

  • Pendulum in a Lift:If the lift accelerates upwards with 'a', geff=g+ag_{eff} = g+a, so TT decreases. If downwards, geff=gag_{eff} = g-a, so TT increases. In free fall (a=ga=g), geff=0g_{eff}=0, so TinftyT \to infty (no oscillation).

* *Example:* A pendulum in a lift accelerating upwards at g/3g/3. geff=g+g/3=4g/3g_{eff} = g + g/3 = 4g/3. New T=2pisqrtL4g/3=Tsqrt34=sqrt32TT' = 2pi sqrt{\frac{L}{4g/3}} = T sqrt{\frac{3}{4}} = \frac{sqrt{3}}{2}T. The time period decreases.

  • Pendulum in a Fluid:The buoyant force reduces the effective weight. geff=g(1ρfluidρbob)g_{eff} = g(1 - \frac{\rho_{fluid}}{\rho_{bob}}). Since geff<gg_{eff} < g, the time period TT increases.

* *Example:* Bob density 2ρfluid2\rho_{fluid}. geff=g(1ρfluid2ρfluid)=g(11/2)=g/2g_{eff} = g(1 - \frac{\rho_{fluid}}{2\rho_{fluid}}) = g(1 - 1/2) = g/2. New T=2pisqrtLg/2=Tsqrt2T' = 2pi sqrt{\frac{L}{g/2}} = Tsqrt{2}. The time period increases by sqrt2sqrt{2} times.

  • Effect of Temperature:If the string is metallic, its length LL changes with temperature due to thermal expansion (L=L(1+alphaDeltaT)L' = L(1 + alpha Delta T)). An increase in temperature increases LL, thus increasing TT.

* *Example:* A pendulum clock runs slow in summer because LL increases, making TT increase.

Always be mindful of units and the specific conditions mentioned in the problem. Practice applying the core formula and its variations to build speed and accuracy.

Prelims Revision Notes

The simple pendulum is a critical topic for NEET, primarily testing your understanding of Simple Harmonic Motion (SHM) and its practical applications. The fundamental formula for its time period is T=2pisqrtLgT = 2pi sqrt{\frac{L}{g}}.

Remember that LL is the effective length, measured from the point of suspension to the center of mass of the bob. For a spherical bob of radius RR attached to a string of length ll, L=l+RL = l+R. The condition for SHM is small angular displacement, typically less than 10circ10^circ to 15circ15^circ, where sinθapproxθsin\theta approx \theta.

This approximation is crucial for the restoring force to be proportional to displacement.

Key dependencies: TproptosqrtLT propto sqrt{L} and Tpropto1/sqrtgT propto 1/sqrt{g}. This means if you double the length, the time period increases by sqrt2sqrt{2} times. If gravity quadruples, the time period halves. Crucially, the time period is independent of the mass of the bob and the amplitude of oscillation (for small angles). These are common conceptual traps in MCQs.

Be prepared for variations:

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  1. In a Lift:Upward acceleration 'a' means geff=g+ag_{eff} = g+a (T decreases). Downward acceleration 'a' means geff=gag_{eff} = g-a (T increases). Free fall (a=ga=g) means geff=0g_{eff}=0 (T becomes infinite, no oscillation).
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  3. In a Fluid:Buoyant force reduces the effective weight. geff=g(1ρfluid/ρbob)g_{eff} = g(1 - \rho_{fluid}/\rho_{bob}). Since geff<gg_{eff} < g, the time period increases.
  4. 3
  5. Temperature Change:If the string is metallic, its length LL changes with temperature due to thermal expansion (L=L(1+alphaDeltaT)L' = L(1 + alpha Delta T)). An increase in temperature increases LL, leading to an increase in TT.
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  7. Seconds Pendulum:A pendulum with a time period of 2 seconds. Its length is approximately 1 meter on Earth.

For numerical problems, ensure unit consistency. For percentage change problems, use the direct calculation for accuracy, especially for larger changes. For small changes, TproptosqrtLT propto sqrt{L} implies if LL changes by xx%, TT changes by approximately x/2x/2%. Always identify the effective LL and gg for any given problem scenario.

Vyyuha Quick Recall

Long Gravity Takes Time: Length and Gravity affect Time Tperiod. (Longer L, longer T; Stronger G, shorter T).

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