Step 1: Define initial velocity components.
Let the initial speed be \(u\).
\[
u_x = u\cos 30^\circ = \frac{\sqrt{3}}{2}u, \qquad
u_y = u\sin 30^\circ = \frac{1}{2}u.
\]
Step 2: Equation of vertical motion.
Vertical displacement after time \(t\):
\[
y(t) = 2 + u_y t - \tfrac{1}{2}gt^2.
\]
At ground hit, \(y(t)=0\):
\[
0 = 2 + \tfrac{1}{2}u t - 5t^2. \tag{1}
\]
Step 3: Horizontal motion condition.
Horizontal displacement after time \(t\):
\[
x(t) = u_x t = \tfrac{\sqrt{3}}{2} u t = 6. \tag{2}
\]
Step 4: Express \(t\) in terms of \(u\).
From (2):
\[
t = \frac{12}{\sqrt{3}u} = \frac{4\sqrt{3}}{u}.
\]
Step 5: Substitute in vertical equation.
From (1):
\[
0 = 2 + \tfrac{1}{2}u\left(\frac{4\sqrt{3}}{u}\right) - 5\left(\frac{4\sqrt{3}}{u}\right)^2.
\]
\[
0 = 2 + 2\sqrt{3} - \frac{240}{u^2}.
\]
Step 6: Solve for \(u^2\).
\[
\frac{240}{u^2} = 2+2\sqrt{3}.
\]
\[
u^2 = \frac{240}{2(1+\sqrt{3})} = \frac{120}{1+\sqrt{3}}.
\]
Multiply numerator and denominator by \((1-\sqrt{3})\):
\[
u^2 = \frac{120(1-\sqrt{3})}{1-3} = -60(1-\sqrt{3}) = 60(\sqrt{3}-1).
\]
Numerically: \(\sqrt{3}\approx1.732\).
\[
u^2 \approx 60(0.732) = 43.92 \Rightarrow u \approx 6.63\ \text{m/s}.
\]
Step 7: Recheck horizontal range.
With \(u=6.63\), \(t=\tfrac{4\sqrt{3}}{6.63}\approx1.04\) s.
Then \(x=u_x t = (6.63\cos30^\circ)(1.04)\approx(5.74)(1.04)=5.97\approx6\ \text{m}. \checkmark\)
Thus \(u \approx 6.6\ \text{m/s}\).
Final Answer: \(6.6\ \text{m/s}\)