Concept:
In standard two-dimensional projectile kinematics neglecting atmospheric friction resistance forces, gravity acts purely along the vertical field line. Consequently, the horizontal velocity component remains completely uniform throughout the trajectory:
\[
u_x = v_x \implies V\cos\theta_1 = v\cos\theta_2
\]
Step 1: Equating independent horizontal projection vectors.
Given parameters:
• Initial angle \( \theta_1 = 60^{\circ} \)
• Mid-flight angular tilt \( \theta_2 = 30^{\circ} \)
• Mid-flight speed magnitude \( v = 10 \, ms^{-1} \)
Applying component conservation:
\[
V \cos(60^{\circ}) = 10 \cos(30^{\circ})
\]
Step 2: Evaluating trigonometric values.
\[
V \left(\frac{1}{2}\right) = 10 \left(\frac{\sqrt{3}}{2}\right)
\]
Cancelling out the common factor of 2 from both sides:
\[
V = 10\sqrt{3} \, ms^{-1}
\]