As we have discussed Basics of BPT and its various type. We can
proceed for governing equations and numerical analysis.
From the below figure it is clear that water will stagnant
in the inverted siphon portion (from point C to D) in no flow condition. As the steady state flow Qo enters to the
BPT, filling of the liquid will start from upper portion of the inverted siphon
(from point C to towards BPT). This coming water will create head difference to
push the stagnant water to move towards the delivery reservoir. As the water
starts filling, it will continue up to the BPT to attain steady state condition.
Now this situation can be described by Continuity Equation and conservation of
Momentum equation in the following cases.
Case –1: Filling
starts from upper portion of the inverted siphon.
1.
Continuity
Equation (Conservation of Mass)
2.
Conservation of momentum.
Change of momentum of stagnant liquid = Force applied in the
liquid due to static head of fluid.
Or, Change of
momentum of fluid = Static Head – Frictional Head.
Writing the terms
Case –2: Filling starts from Bottom of the BPT.
3.
Continuity Equation (Conservation of Mass)
4.
Conservation of momentum.
In usual practice pipe line does not leave to drain out. Because
once pipe got empty, its takes time to refill the pipeline and required demand
will not deliver to the delivery reservoir. This happens, when pipeline inclination
θ is very less and pipeline length is long. Therefore delivery valve turned off
in such a way that next time filling starts from bottom of the BPT.
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