diff --git a/docs/documentation/sizing/propulsion_design/engineering_principles.md b/docs/documentation/sizing/propulsion_design/engineering_principles.md
index 51bfec5078b40bedaf18567a72e1a32ca2dd9877..1c15b66df77fefedbedba84afe35e6cca961df0a 100644
--- a/docs/documentation/sizing/propulsion_design/engineering_principles.md
+++ b/docs/documentation/sizing/propulsion_design/engineering_principles.md
@@ -47,15 +47,15 @@ The _scale factor_ is necessary because (as conceptual aircraft designer), we us
 
 So, the scaling is based on continuity principle assuming that the operating condition is constant (commonly known station numbering; assuming no pressure drop).
 
-$ \textcolor{white}{T = \dot{m} \cdot (V_9 - V_0)} $
+$$ \textcolor{white}{T = \dot{m} \cdot (V_9 - V_0)} $$
 
 Therefore, thrust $T$ is proportional to the mass flow $\textcolor{white}{\dot{m}}$, which is related to the cross-sectional area $A$ of the engine.
 
-$ \textcolor{white}{\dot{m}} = \rho \cdot V \cdot A = \rho \cdot V \cdot \pi \left(\frac{d}{2}\right)^2 $
+$$ \textcolor{white}{\dot{m}} = \rho \cdot V \cdot A = \rho \cdot V \cdot \pi \left(\frac{d}{2}\right)^2 $$
 
 Because area $A$ is proportional to the square of the diameter $d$ , it follows that the diameter should be proportional to the square root of the scale factor. 
 
-$ \textcolor{white} d_{new} = d_{ref} \cdot ( \frac{T_{new}}{T_{ref}} )^{0.5} $
+$$ \textcolor{white} d_{new} = d_{ref} \cdot ( \frac{T_{new}}{T_{ref}} )^{0.5} $$
 
 An exemplary simplified calculation (data from the V2527-A5): the current engine provides $127.27~kN$ as sea level static thrust, but for the design only $100~kN$ are needed. The scaling factor would be $0.7857$. Assuming an initial diameter $2~m$, the new diameter would be $1.773~m$ with the scaling factor of $(0.7857)^{0.5} = 0.8864$.