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Draft Tube Flow
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Swirl at the outlet from Francis runners
b2 c2 w2 c2u u2 c2 w2 u2 b2 c2 c2m w2 c2u u2 b2 c2m w2 c2
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Phenomenon in the draft tube flow
Swirl flow Flow in bend Positive pressure gradient in the diffuser - separation
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Swirl flow in draft tubes
Strong coupling between the flow field and the pressure gradients Anisotropic turbulence The turbulence is influenced by the geometry and the velocity The draft tube flow is sensitive to the inlet conditions (velocity and pressure) A vortex filament is present
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Swirl flow
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Swirl flow Mean Axial Velocity
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Vortex breakdown Vortex breakdown is present when a negative axial velocity occurs in the center of the flow. Vortex breakdown occurs when S > 1
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Swirl flow Rankine Vortex
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Swirl flow
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Swirl flow Vortex filament at part load Vortex filament at full load
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Flow in bends A - A A A
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Flow in bends Newton’s 2 law From Bernoulli’s equation Free Vortex
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Positive pressure gradient in the diffuser
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Results: The hydraulic design of the draft tube gives secondary flow and therefore a reduced efficiency
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The Navier Stokes equations in Cylindrical coordinates
r-direction: q-direction: z-direction:
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Euler equations r-direction: q-direction: z-direction:
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r-direction Assume steady state solution Assume axis symmetry
Assume g-force to be neglectible
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Pressure distribution at the inlet
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0,1 m Pressure [Pa]
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0,1 m Pressure [Pa] Radius [m]
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400 mm
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Pressure distribution at the inlet
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0,2 m Pressure [Pa]
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0,2 m Pressure [Pa] Radius [m]
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0,4 m Pressure [Pa]
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0,4 m Pressure [Pa] Radius [m]
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Static Pressure at the inlet
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Velocity at the inlet to the draft tube
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Velocity
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