I have increased the space between my text and equations by placing these lines right after
\begin{document}
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\setlength{\abovedisplayskip}{16pt}
\setlength{\belowdisplayskip}{16pt}
The code I used is this.
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The basic aspect of the problem lies now in quantifying the coefficient of discharge~$C_d$. He showed that $C_d$ is a unique function of:
\begin{equation}
C_d = f(\Lambda_e,\overline{p}_t,geo)
\end{equation}
in which $geo$ stands for the entrance gap geometrical properties. The entrance number $\Lambda_e$ depends on the supply pressure, geometry of the bearing problem and its fluid properties:
\begin{equation}
\Lambda_e = \frac{\mu r_f}{p_s h^2}\sqrt{\frac{\Re Ts}{\kappa}}
\end{equation}
As a result, the original entrance