In projectile motion, the maximum height \( H \) is given by:
\[
H = \frac{v_0^2 \sin^2(\theta)}{2g}
\]
and the range \( R \) is given by:
\[
R = \frac{v_0^2 \sin(2\theta)}{g}
\]
The speed at the maximum height is the horizontal component, which is \( v_0 \cos(\theta) \). According to the problem, this is \( \frac{\sqrt{3}}{2} v_0 \), so:
\[
\cos(\theta) = \frac{\sqrt{3}}{2}
\]
This implies \( \theta = 30^\circ \).
Substituting \( \theta = 30^\circ \) into the range equation, we get:
\[
R = \frac{v_0^2 \sin(60^\circ)}{g} = \frac{v_0^2 \cdot \frac{\sqrt{3}}{2}}{g}
\]
The maximum height is:
\[
H = \frac{v_0^2 \sin^2(30^\circ)}{2g} = \frac{v_0^2 \cdot \frac{1}{4}}{2g} = \frac{v_0^2}{8g}
\]
Given that the range is \( n \) times the maximum height:
\[
R = n \cdot H
\]
Substituting the expressions for \( R \) and \( H \), we get:
\[
\frac{v_0^2 \cdot \frac{\sqrt{3}}{2}}{g} = n \cdot \frac{v_0^2}{8g}
\]
Simplifying:
\[
\frac{\sqrt{3}}{2} = \frac{n}{8}
\]
Solving for \( n \):
\[
n = 4\sqrt{3}
\]
Thus, the value of \( n \) is \( 4\sqrt{3} \).