Step 1: Recall the standard equation for velocity in Simple Harmonic Motion (SHM).
For a particle executing Simple Harmonic Motion, the relationship between its velocity ($v$), displacement ($x$), and amplitude ($A$) is given by:
\[ v = \omega \sqrt{A^2 - x^2} \]
where $\omega$ is the angular frequency of oscillation.
Step 2: Rearrange the given equation to match the standard form.
The given equation is:
\[ 4v^2 = 25 - x^2 \]
Divide by 4 to isolate $v^2$:
\[ v^2 = \frac{25 - x^2}{4} \]
\[ v^2 = \frac{1}{4}(25 - x^2) \]
Take the square root of both sides:
\[ v = \sqrt{\frac{1}{4}(25 - x^2)} \]
\[ v = \frac{1}{2}\sqrt{25 - x^2} \]
Step 3: Compare with the standard SHM velocity equation to find $\omega$ and $A$.
Comparing $v = \frac{1}{2}\sqrt{25 - x^2}$ with $v = \omega \sqrt{A^2 - x^2}$:
We can directly identify the angular frequency ($\omega$) and the square of the amplitude ($A^2$):
\[ \omega = \frac{1}{2} \text{ rad/s} \]
And
\[ A^2 = 25 \quad \Rightarrow \quad A = 5 \text{ m} \]
(The amplitude A = 5 m, but we only need $\omega$ for the time period).
Step 4: Calculate the time period ($T$).
The time period ($T$) of a particle executing SHM is related to its angular frequency ($\omega$) by the formula:
\[ T = \frac{2\pi}{\omega} \]
Substitute the value of $\omega$:
\[ T = \frac{2\pi}{\frac{1}{2}} \]
\[ T = 2\pi \times 2 \]
\[ T = 4\pi \text{ s} \]
The final answer is $\boxed{4\pi \text{ s}}$.