Why speed changes in a vertical circle
In a horizontal circle the speed can stay the same. In a vertical circle, gravity does negative work when the ball goes up and positive work when it comes down. So the ball is fastest at the bottom and slowest at the top. This is non-uniform circular motion.
Take θ as the angle from the lowest point. Energy conservation gives: v² = u² − 2gr(1 − cos θ), where u is the speed at the bottom.
Tension at any point, bottom and top
Towards the centre, the net force must be mv²/r. At angle θ: T − mg cos θ = mv²/r, so T = mv²/r + mg cos θ.
- Bottom (θ = 0): T_L = mu²/r + mg. Largest tension (a string breaks here first).
- Side (θ = 90°): T = mv²/r.
- Top (θ = 180°): T_H = mv²/r − mg. Smallest tension.
Using u² = v² + 4gr: T_L − T_H = 6mg.
Minimum speeds: √(gr) at the top and √(5gr) at the bottom
- A string can pull but not push, so T ≥ 0 everywhere.
- T is smallest at the top: mv²/r − mg ≥ 0 → v_top ≥ √(gr).
- Energy from bottom to top (height 2r): ½mu² = ½mv² + mg(2r) → u² = v² + 4gr.
- Put v² = gr: u_min = √(5gr).
- At the side (θ = 90°): v² = u² − 2gr = 3gr, so v = √(3gr).
If a ball is on a rigid rod (which can push), it only needs to reach the top with v ≥ 0, so u ≥ √(4gr) = 2√(gr).
What if the speed is too low?
- u < √(2gr): the ball swings like a pendulum and never goes above the centre level.
- √(2gr) < u < √(5gr): the ball goes above the centre, but T becomes zero somewhere in the upper half. The string slackens and the ball follows a parabola (projectile) path.
- u ≥ √(5gr): full loop.
Try it at home
Tie a small plastic bottle with a little water to a string (outside, safely). Swing it in a vertical circle, first slowly, then fast. Slowly, the string goes loose near the top and water may splash. Fast, the string stays tight and no water falls. Feel the pull in your hand: strongest at the bottom.
Exam corner
CBSE asks: derive the minimum speed at the lowest and highest points (3–5 marks), find T at top and bottom, and "why does water not fall from a bucket" type reasoning. Remember T_L − T_H = 6mg and v at the side = √(3gr).
Key formulas and definitions
- v² = u² − 2gr(1 − cos θ)
- T = mv²/r + mg cos θ
- Bottom: T_L = mu²/r + mg; Top: T_H = mv²/r − mg
- v_top(min) = √(gr), u_bottom(min) = √(5gr), v_side = √(3gr)
- T_L − T_H = 6mg
- Rigid rod: u_min = √(4gr)
Worked examples
1. Find the minimum speed at the top of a vertical circle of radius 0.9 m (g = 10 m/s²).
Step 1: v_top = √(gr). Step 2: = √(10 × 0.9) = √9 = 3 m/s.
2. For r = 2 m, find the minimum speed at the lowest point.
Step 1: u = √(5gr). Step 2: = √(5 × 10 × 2) = √100 = 10 m/s.
3. A 0.2 kg stone on a 1 m string moves at 6 m/s at the bottom. Find the tension there.
Step 1: T = mg + mu²/r. Step 2: = 0.2 × 10 + 0.2 × 36 / 1 = 2 + 7.2. Answer: 9.2 N.
4. A 0.5 kg ball on a 1 m string has 8 m/s at the bottom. Find its speed and tension at the top.
Step 1: v² = u² − 4gr = 64 − 40 = 24, v ≈ 4.9 m/s. Step 2: T = mv²/r − mg = 0.5 × 24 − 5 = 7 N.
5. For the ball above, check T_L − T_H = 6mg.
Step 1: T_L = 0.5 × 64 + 5 = 37 N. Step 2: T_L − T_H = 37 − 7 = 30 N. Step 3: 6mg = 6 × 0.5 × 10 = 30 N. ✔
6. A bucket of water is whirled in a vertical circle of radius 1.6 m. What is the least number of rotations per minute at the top so that no water falls?
Step 1: v = √(gr) = √16 = 4 m/s. Step 2: ω = v/r = 2.5 rad/s. Step 3: rpm = ω × 60 / 2π ≈ 23.9. So at least about 24 rpm (at the top).
7. A string can bear 50 N. A 1 kg ball moves on it in a vertical circle of radius 1 m. Find the largest speed allowed at the bottom.
Step 1: T is largest at the bottom: mg + mu²/r ≤ 50. Step 2: 10 + u² ≤ 50 → u² ≤ 40. Answer: u ≤ 6.32 m/s. (This is less than √(5gr) = 7.07, so this string cannot give a full loop!)
Common mistakes
- Using constant speed in a vertical circle. Speed changes because gravity does work.
- Writing T = mg + mv²/r at the top. At the top both forces point to the centre: T + mg = mv²/r.
- Saying the minimum speed at the bottom is √(gr). That is the top; at the bottom it is √(5gr).
- Using √(5gr) for a rod. A rod can push, so only √(4gr) is needed at the bottom.