In fluid dynamics the Borda–Carnot equation is an empirical description of the mechanical energy losses of the fluid due to a (sudden) flow expansion. The Borda–Carnot loss equation is only valid for decreasing velocity, v1 > v2, otherwise the loss ΔE is zero – without mechanical work by additional external forces there cannot be a gain in mechanical energy of the fluid.
The loss coefficient ξ can be influenced by streamlining. For example in case of a pipe expansion, the use of a gradual expanding diffuser can reduce the mechanical energy losses.
|δE||mechanical energy loss of the fluid per unit of fluid volume (J/m3)|
|ξ||empirical loss coefficient , 0 ≤ ξ ≤ 1 (dimensionless)|
|ρ||fluid density (kg/m3)|
|u1||mean flow velocity before expansion (m/s)|
|u2||mean flow velocity after expansion (m/s)|