. 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_
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 ( At the peak of its trajectory, its instantaneous
Choose whether "up" or "down" is the positive direction (usually up is positive, making negative). Identify initial conditions: Determine Terminal Velocity ( Choose whether "up" or "down"
): The constant maximum speed an object reaches during its fall.
