Concept:
This problem models horizontal projectile motion. In the absence of air resistance, there is no force acting horizontally, so the horizontal acceleration is $0$ ($a_x = 0$). This ensures the horizontal velocity component remains constant throughout the flight time. Vertically, the object is subject to a constant gravitational acceleration downward ($a_y = g$).
Step 1: Evaluate the horizontal component of velocity ($v_x$).
The object is kicked with an initial horizontal velocity $u_x = 19.6\text{ m s}^{-1}$. Since $a_x = 0$:
\[
v_x = u_x = 19.6\text{ m s}^{-1}
\]
Step 2: Evaluate the vertical component of velocity ($v_y$) at $t = 2\text{ s}$.
Initially, the projectile has no vertical movement, so $u_y = 0$. Using the first equation of motion along the vertical axis:
\[
v_y = u_y + gt
\]
Substitute $u_y = 0$, $g = 9.8\text{ m s}^{-2}$, and $t = 2\text{ s}$:
\[
v_y = 0 + (9.8 \times 2) = 19.6\text{ m s}^{-1}
\]
Step 3: Compute the ratio of horizontal to vertical components.
The desired ratio is:
\[
\text{Ratio} = \frac{v_x}{v_y} = \frac{19.6}{19.6} = \frac{1}{1} \implies 1:1
\]