Simple Pendulum Oscillating in a Liquid

Physics · Oscillations · NEET

When a simple pendulum swings inside a liquid, the liquid pushes up on the bob (buoyancy). This upward push lowers the effective gravity to g_eff = g(1 - d_liquid/d_bob), so the time period gets LONGER (pendulum slows down). Memory hook: liquid lifts the bob a little, so gravity feels weaker, so each swing takes more time.
LIn air: T = 2 pi root(L/g)buoyancyweightliquidIn liquid: g_eff = g(1 - d_liq/d_bob), T larger
Left: pendulum in air feels full gravity g. Right: inside a liquid, the upward buoyant force partly cancels the weight, so effective gravity drops to g_eff = g(1 - d_liquid/d_bob) and the time period becomes longer.

Your doubts, answered

Why does the pendulum slow down (larger T) in a liquid instead of speeding up?

The liquid gives an upward buoyant force on the bob. This buoyant force acts against gravity, so the net downward pull (the restoring pull) becomes weaker. A weaker pull means the effective gravity g_eff is smaller than g. Since T = 2 pi root(L / g_eff), a smaller g_eff makes T larger. So the pendulum takes MORE time per swing, it does not speed up.

Where does the formula g_eff = g(1 - d_liquid / d_bob) come from?

Weight of bob down = d_bob * V * g. Buoyant force up = d_liquid * V * g (weight of displaced liquid). Net downward force = d_bob*V*g - d_liquid*V*g. Divide by the mass d_bob*V to get effective acceleration: g_eff = g(1 - d_liquid/d_bob). The volume V and mass cancel out neatly, leaving only the ratio of the two densities.

Does the mass or size of the bob change the answer?

No. Both weight and buoyant force are proportional to the same volume V, so V cancels. Only the RATIO d_liquid/d_bob decides g_eff. A denser bob (larger d_bob) makes the ratio small, so buoyancy barely changes T. A bob almost as light as the liquid makes the ratio near 1, so g_eff is tiny and T becomes very large.

What happens if the bob density equals the liquid density?

Then d_liquid/d_bob = 1, so g_eff = g(1 - 1) = 0. With zero effective gravity there is no restoring force, so the bob simply floats and does not oscillate. The time period becomes infinite (T = 2 pi root(L/0) tends to infinity). This is the limiting case of the formula.

How is 'oscillating in a liquid' different from a pendulum inside an accelerating lift or truck?

Both change g_eff, but for different reasons. In a liquid, buoyancy subtracts, so g_eff = g(1 - d_liquid/d_bob) and T always increases. In a lift moving up, g_eff = g + a (T decreases); lift moving down, g_eff = g - a (T increases); free fall, g_eff = 0. So the liquid case only ever slows the pendulum, never speeds it up.

⚠️ The NEET trap
Buoyancy adds an upward force, so the pendulum feels more force and swings faster, giving a smaller time period.
Buoyancy acts UPWARD, opposite to gravity, so it REDUCES the net restoring pull. g_eff = g(1 - d_liquid/d_bob) is smaller than g, so the time period INCREASES (pendulum slows down).
🧠 Buoyancy fights gravity. Less effective g means MORE time per swing, not less.

Real NEET questions

NEET 2023

A simple pendulum oscillating in air has a period of root(3) s. If it is completely immersed in a non-viscous liquid whose density is one-fourth that of the material of the bob, the new period is

A · 2 s
B · root(3)/2 s
C · 2 root(3) s
D · 2/root(3) s
Solution: Step 1: Buoyancy lowers effective gravity. g_eff = g(1 - d_liquid/d_bob) = g(1 - 1/4) = 3g/4. Step 2: T = 2 pi root(L/g), so T_new / T = root(g / g_eff) = root(g / (3g/4)) = root(4/3) = 2/root(3). Step 3: T_new = T * 2/root(3) = root(3) * 2/root(3) = 2 s. Answer: A (2 s). The period increases from root(3) s (about 1.73 s) to 2 s, confirming the pendulum slows down in the liquid.

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Frequently asked

What is the time period of a simple pendulum in a liquid?

T = 2 pi root(L / g_eff), where g_eff = g(1 - d_liquid/d_bob). Because g_eff is less than g, the period is longer than the normal period in air.

Does buoyancy increase or decrease the pendulum time period?

It increases the time period. Buoyancy reduces the effective gravity, and a smaller g always makes T larger, so the pendulum swings slower.

What if the liquid is viscous (like thick oil)?

Viscosity adds a damping (drag) force. The pendulum still slows down due to buoyancy AND its amplitude keeps shrinking with time (damped oscillation). NEET problems usually say 'non-viscous' so only buoyancy matters and amplitude stays constant.

Why does the volume of the bob cancel out?

Both the weight (d_bob * V * g) and the buoyant force (d_liquid * V * g) contain the same volume V. When you compute net force per unit mass, V and the constants cancel, leaving g_eff = g(1 - d_liquid/d_bob), which depends only on the density ratio.

Can the pendulum stop oscillating in a liquid?

Yes, if the bob density equals the liquid density, g_eff becomes zero. Then there is no restoring force and the bob just floats, so the time period becomes infinite and it does not oscillate.