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. 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.

, 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 1_Caduta_libera_Parte_2_

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 At the peak of its trajectory, its instantaneous

): The constant maximum speed an object reaches during its fall. Choose whether "up" or "down" is the positive

Choose whether "up" or "down" is the positive direction (usually up is positive, making negative). Identify initial conditions: Determine

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 (