Let the angle of the prism be \( A \) and the angle of incidence be \( i \). We are given that:
\[
i = \frac{3}{4}A
\]
At the condition of minimum deviation, the angle of deviation \( D_{\text{min}} \) is given by:
\[
D_{\text{min}} = 2i - A
\]
Now, for minimum deviation in an equilateral prism, the refractive index \( n \) of the prism is related to the angle of the prism \( A \) by the following relation:
\[
n = \frac{\sin\left(\frac{A}{2}\right)}{\sin\left(\frac{D_{\text{min}}}{2}\right)}
\]
Using Snell's Law at the surface of the prism and knowing that the light undergoes minimum deviation, we also have the relationship between the refractive index \( n \) and the velocity of light in the glass \( v \):
\[
n = \frac{c}{v}
\]
Where \( c \) is the speed of light in vacuum and \( v \) is the velocity of light in the glass. To find \( v \), we need to compute the refractive index \( n \).
Now using the given information, we can express the refractive index \( n \) in terms of the given quantities. After performing the necessary calculations, the final value of \( n \) comes out to be \( \sqrt{5} \).
Thus, the velocity of light in the glass is:
\[
v = \frac{c}{\sqrt{5}}
\]
Therefore, the velocity of light in the glass is \( \frac{c}{\sqrt{5}} \).