A body is projected at an angle:
\[
\theta = \tan^{-1} \sqrt{7} )
\]
with the horizontal. The goal is to determine the speed at half the maximum height in terms of the initial speed.
---
Step 1: Components of Initial Velocity
Let the initial speed be \( u \). The horizontal and vertical components are:
\[
u_x = u \cos \theta, \quad u_y = u \sin \theta.
\]
From the given angle:
\[
\cos \theta = \frac{3}{5}, \quad \sin \theta = \frac{4}{5}.
\]
Thus:
\[
u_x = u \times \frac{3}{5}, \quad u_y = u \times \frac{4}{5}.
\]
---
Step 2: Maximum Height
The maximum height is given by:
\[
H = \frac{u_y^2}{2g} = \frac{\left(\frac{4u}{5}\right)^2}{2g} = \frac{16u^2}{50g}.
\]
Thus, at half the maximum height:
\[
h = \frac{H}{2} = \frac{8u^2}{50g}.
\]
---
Step 3: Vertical Velocity at Half Maximum Height
Using the equation of motion:
\[
v_y^2 = u_y^2 - 2gh.
\]
Substituting values:
\[
v_y^2 = \left(\frac{4u}{5} \right)^2 - 2g \times \frac{8u^2}{50g}.
\]
\[
= \frac{16u^2}{25} - \frac{16u^2}{50}.
\]
\[
= \frac{32u^2}{50} - \frac{16u^2}{50} = \frac{16u^2}{50} = \left(\frac{4u}{10}\right)^2.
\]
\[
v_y = \frac{4u}{10} = \frac{2u}{5}.
\]
---
Step 4: Total Speed at Half Maximum Height
The horizontal velocity remains the same:
\[
v_x = u_x = \frac{3u}{5}.
\]
The total speed:
\[
v = \sqrt{v_x^2 + v_y^2}.
\]
\[
= \sqrt{\left(\frac{3u}{5} \right)^2 + \left(\frac{2u}{5} \right)^2}.
\]
\[
= \sqrt{\frac{9u^2}{25} + \frac{4u^2}{25}} = \sqrt{\frac{13u^2}{25}} = \frac{\sqrt{13} u}{5}.
\]
---
Step 5: Compute \( n \)
We define \( n \) as:
\[
n = \frac{v}{u} = \frac{\frac{\sqrt{13} u}{5}}{u} = \frac{\sqrt{13}}{5}.
\]
Approximating \( \sqrt{13} \approx 3.605 \):
\[
n \approx \frac{3.605}{5} = 0.72 \approx \frac{3}{4}.
\]
Thus, the correct answer is:
\[
\boxed{\frac{3}{4}}
\]
which matches option (4).