Substitute ( t_P ) back into the vertical equation to find the maximum height ( h ):
( h = \frac{(v_0 \sin(\alpha))^2}{2g} )
Time to Reach Point S
Time to hit the ground ( t_S = 2t_P = \frac{2v_0 \sin(\alpha)}{g} )
This is based on symmetry of the projectile motion.
Distance Traveled (Range)
Range ( OS = v_{0x} \times t_S )
Substitute to find:
( OS = \frac{v_0^2 \sin(2\alpha)}{g} )
This expression shows the dependence on ( v_0^2 ) and ( \sin(2\alpha) ).
Importance of Uncertainties
Measurement uncertainties must be acknowledged in experiments.
Example: Measuring the height of a projectile to determine initial velocity and its uncertainties.
Angle of Projection Effects
Projectiles launched at different angles (30°, 45°, 60°):
Predicts hit point on a target based on calculated distances.
Higher angles provide different trajectories and distances.
Practical Application of Predictions
Experimental verification of trajectory calculations with actual projectile launches.
Use of a metal ball and spring gun to demonstrate principles.
Tragic Scenario: Monkey and Hunter
A hunter shoots at a monkey; the monkey drops when the gun fires.
The trajectory of the bullet and the falling monkey are analyzed:
The bullet follows a parabolic path while the monkey falls straight down.
Elaborates on the independence of speed and angle in this scenario.
Perspective from the Monkey
The monkey’s point of view is analyzed in a falling elevator scenario.
Both the bullet and the monkey fall together, creating a straight line situation.
Conclusion
The lecture concludes with an experimental demonstration involving the monkey and the bullet's trajectory, emphasizing the calculations and uncertainties involved in projectile motion.