When string cut → tension disappears → only gravity acts → parabolic projectile motion
Trajectory depends on position and velocity at cut instant
● Ceiling
|
| L = 2 m
\ ● Bob (θ_max or mean)
String CUT → Parabolic path
At extreme: velocity = 0 (momentarily stops)
$$\vec{v} = 0 \, \text{m/s} \quad \text{(both components zero)}$$
Result: Pure free fall → straight down under gravity
At mean position: maximum horizontal speed = 1 m/s
$$v_\text{horizontal} = 1 \, \text{m/s}, \quad v_\text{vertical} = 0$$
Projectile motion:
$$x(t) = (1)t, \quad y(t) = -( \frac{1}{2}gt^2)$$
Result: Parabolic trajectory (horizontal velocity + vertical free fall)
$$mgL(1-\cos\theta_\text{max}) = \frac{1}{2}mv_\text{max}^2$$ $$v_\text{max} = \sqrt{2gL(1-\cos\theta_\text{max})} = 1 \, \text{m/s}$$
| Position | Velocity at Cut | Trajectory |
|---|---|---|
| Extreme | \(v_x = 0, v_y = 0\) | Vertical fall |
| Mean | \(v_x = 1, v_y = 0\) | Parabola |
