To solve this problem, we need to consider the motion of the stone in two dimensions: horizontally (c-component) and vertically (y-component).
(c) The equation for the c-component of velocity remains constant since the stone is thrown horizontally. Therefore, the equation for the c-component of velocity of the stone with time is:
v_c(t) = v_O
where v_O is the initial velocity in the horizontal direction (12.5 m/s).
The equation for the y-component of velocity can be determined using the kinematic equation for horizontal motion:
v_y(t) = v_{y0} - g \cdot t
where v_{y0} is the initial vertical velocity (0 m/s) and g is the acceleration due to gravity (-9.8 m/s^2).
(d) The equations for the position of the stone with time can be obtained by integrating the velocity equations with respect to time.
The equation for the horizontal position (c-coordinate) of the stone with time is:
x(t) = v_O \cdot t + x_0
where x_0 is the initial horizontal position (0 m).
The equation for the vertical position (y-coordinate) of the stone with time is:
y(t) = v_{y0} \cdot t - \frac{1}{2} \cdot g \cdot t^2 + y_0
where y_0 is the initial vertical position (38.0 m).
Answer:
(c) v_c(t) = v_O
v_y(t) = v_{y0} - g \cdot t
(d) x(t) = v_O \cdot t + x_0
y(t) = v_{y0} \cdot t - \frac{1}{2} \cdot g \cdot t^2 + y_0