A particle of mass 2.5 kg hangs at the end of a string, 0.9 m long, the other end of which is attached to a fixed point. The particle is projected horizontally with a velocity 8 m/sec. Find the velocity of the particle and tension in the string when the string is (i) horizontal (ii) vertically upward.
Technique
Energy conservation for speed; radial Newton’s-second-law for tension (centripetal equation).
Solution
Setup.m=2.5 kg, ℓ=0.9 m, u=8 m/s, g=9.8 m/s². Let θ be the angle the string makes with the downward vertical (so θ=0 at start, θ=π/2 horizontal, θ=π vertically up).
Step 1 — Energy conservation to find speed at angle θ
The particle rises by ℓ(1−cosθ) from the starting point. Conservation of energy:
21mv2+mgℓ(1−cosθ)=21mu2⟹v2=u2−2gℓ(1−cosθ).
Step 2 — Centripetal equation
At angle θ, the centripetal force toward the pivot is mv2/ℓ, supplied by tension T and the radial component of gravity. With “outward” defined as away from the pivot:
Tension T acts radially inward (toward pivot).
Gravity’s radial component: mgcosθ outward when the particle is below the pivot (θ<π/2), zero at horizontal, −mg∣cosθ∣=mgcosθ inward when above (θ>π/2).
A clean unified form (taking inward as positive): T−mgcosθ=mv2/ℓ for θ≤π/2. For θ>π/2 (particle above pivot), gravity also points inward (downward, same direction as tension when string vertical-up), so T+mg∣cosθ∣=mv2/ℓ.