1_caduta_libera_parte_2_ -

, it decelerates until it reaches its maximum height. At the peak of its trajectory, its instantaneous velocity is Set in the first equation: Maximum Height ( Hmaxcap H sub m a x end-sub ): Substitute tmaxt sub m a x end-sub into the position equation: 2. Visualize the Trajectory The graph below illustrates the position of an object thrown upward at

For an object returning to its starting height, the time spent rising equals the time spent falling, and the final impact speed equals the initial launch speed. Final Conclusion

The motion of an object in free fall (Caduta Libera) is a type of uniformly accelerated motion where the acceleration is constant and equal to gravity, denoted as 1_Caduta_libera_Parte_2_

✅In vertical motion, the maximum height reached is determined solely by the initial velocity and gravity , following the relation

Choose whether "up" or "down" is the positive direction (usually up is positive, making negative). Identify initial conditions: Determine , it decelerates until it reaches its maximum height

. Note the parabolic shape, where the peak represents the moment the object begins to fall back down.

. In "Parte 2" of this study, we typically move beyond simple downward drops to analyze objects thrown vertically upward and the effects of air resistance. Final Conclusion The motion of an object in

In real-world scenarios (Parte 2 often introduces this), air resistance Fdcap F sub d acts against the motion. As speed increases, Fdcap F sub d increases until it equals the gravitational force Fgcap F sub g When , the acceleration becomes zero. Terminal Velocity (