diff --git a/OpenHPL/Resources/Images/besad.png b/OpenHPL/Resources/Images/besad.png deleted file mode 100644 index 9b6e2de..0000000 Binary files a/OpenHPL/Resources/Images/besad.png and /dev/null differ diff --git a/OpenHPL/Resources/Images/besad.svg b/OpenHPL/Resources/Images/besad.svg new file mode 100644 index 0000000..cf579d0 --- /dev/null +++ b/OpenHPL/Resources/Images/besad.svg @@ -0,0 +1,1731 @@ + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + Inputs from tailwater + + + + + Outputs to tail water + + + + + Inputs from head water + + + + + Outputs to head water + + + + + Penstock + + + + + Control Volume for momentum balance + + + + + Control Volume for mass balance or continuity + + + + + + + + + + + + + + + + + + + + + + diff --git a/OpenHPL/Waterway/Penstock.mo b/OpenHPL/Waterway/Penstock.mo index 1c9c836..82f7b62 100644 --- a/OpenHPL/Waterway/Penstock.mo +++ b/OpenHPL/Waterway/Penstock.mo @@ -87,6 +87,6 @@ equation Documentation(info="

This is a more detaied model of the pipe that can be use for proper modeling of penstock. (This model does not work well. Instead PenstockKP model can be used.)

The model for the penstock with the elastic walls and compressible water with simple discretization method (Staggered grid). The geometry of the penstock is described due to figure:

Conservation laws are usually solved by Finite-volume methods. With the Finite volume method, we divide the grid into small control volumes or control cells and then apply the conservation laws. The discretization method is based on Staggered grid scheme, where the penstock is divided in N segments, with input and output pressure as a boundary conditions. Can be describe as the follow figure:

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+

")); end Penstock;